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Author SHA1 Message Date
Alex Selimov 8e924e1658 Latest updates
2 years ago
Kevin C d6f11590f3
fixed pycac format output to use correct atom tags, fixed mode_da syntax
3 years ago
Alex Selimov cffb460e09 Add periodic boundaries to metric calculation and energy to vtk out
3 years ago
Alex Selimov 8fd2a7f65b Updated dislocation analysis and fix to alloy opt_group option
3 years ago
Alex Selimov 612cea3891 Fix group implementation to abide by new atom type formulation
3 years ago
Alex Selimov a9833f53bf Change bubble code from pressure to ratio
3 years ago
Alex Selimov 044bfe7e7f Fix bug in neighbors
3 years ago
Alex Selimov d5d20e468c Improve dislocation analysis in coarse-grained regions and add character analysis
3 years ago
Alex Selimov 59a0c18779 Change implementation to make atom types a bit better
3 years ago
Alex Selimov f9e7f68676 Add ability for even numbered elements
3 years ago
Alex Selimov a712db3274 Quick fix to README
3 years ago
Alex Selimov f857c96931 Quick fix to README
3 years ago
Alex Selimov de8b4e168a Refactor to remove sub boxes from CACmb code, functionality was not useful and became detrimental for generation of new models
3 years ago
Alex Selimov 971e0a5e8d Update to README
3 years ago
Alex Selimov d9920bbef0 Lots of accumulated fixes to various functionality with cacmb
3 years ago
Alex Selimov 1114a46c60 Add velocity reading to pycac_out files and fix to interp_atoms
3 years ago
Alex Selimov f0fd76f12d Latest working version of cacmb
3 years ago
Alex Selimov fbaca5859b Fix to box bound
3 years ago
Alex Selimov 8eac9be895 Fix stress calculation
3 years ago
Alex Selimov 586c1f002c Another fix to overlap command
3 years ago
Alex Selimov 3ad5e0f5e6 Merge branch 'development' of gitlab.com:aselimov/cacmb into development
3 years ago
Alex Selimov b530b15397 Fix opt_delete overlap
3 years ago
Alex Selimov 0aa4e70653 Update .gitlab-ci.yml
3 years ago
Alex Selimov 80c2fd1d8a Update .gitlab-ci.yml
3 years ago
Alex Selimov 200116665a Update mkdocs.yml
3 years ago
Alex Selimov 20238b5f55 Update mkdocs.yml
3 years ago
Alex Selimov 79fa4b3cb7 Merge branch 'development' of gitlab.com:aselimov/cacmb into development
3 years ago
Alex Selimov 7979ad1093 Fix overlap command
3 years ago
Alex Selimov 3210523eb9 Update .gitlab-ci.yml
3 years ago
Alex Selimov ecdabe23a6 Update .gitlab-ci.yml
3 years ago
Alex Selimov 5c50ce8765 Add first/last flag
3 years ago
Alex Selimov 30dbd3bfc7 Latest working version of cacmb
3 years ago
Alex Selimov a54215d024 Fix all_new option
3 years ago
Alex Selimov 8fd45dc461 Add all new option
3 years ago
Alex Selimov 4b9589e7b3 Fix to dynamic allocation
3 years ago
Alex Selimov c84383b5e1 Makefile.dep
3 years ago
Alex Selimov 66645c8dfc Added opt_bubble
3 years ago
Alex Selimov 8733dfe2e0 Update dependencies for building
3 years ago
Alex Selimov 0e41c7acc9 Lots of updates to cacmb
3 years ago
Alex Selimov b684e0754b Add mode_da and fixes to io
4 years ago
Alex Selimov d2aeb5a7f6 Add documentation
4 years ago
Alex Selimov e3dba9029a Fix bug for writing to .xyz file after delete
4 years ago
Alex Selimov 7ee87c767f Merge in insert command for group option
4 years ago
Alex Selimov 6119366b24 Remove debug statement
4 years ago
Alex Selimov 7a39612164 Add norefine option
4 years ago
Alex Selimov db8428113d Changes to restart file format
4 years ago
Alex Selimov 8298c21503 Updates to metric and emrge and adding read_lmp
4 years ago
Alex Selimov 85135e7c95 More compatability fixes for new version of CAC
4 years ago
Alex Selimov f9ffd4ddb1 Current working version of insert group
4 years ago

@ -0,0 +1,27 @@
image: python:3.8-buster
before_script:
- pip install -r requirements.txt
stages:
- tests
- deploy
pagestests:
stage: tests
script:
- mkdocs build --strict --verbose --site-dir test
artifacts:
paths:
- test
except:
- development
pages:
stage: deploy
script:
- mkdocs build --strict --verbose
artifacts:
paths:
- public
only:
- development

@ -3,378 +3,7 @@
This is a tool for building models in CAC. Commands and usage options are below. This code is intended to follow the atomsk code fairly closely.
## Modes
Documentation is available at: [aselimov.gitlab.io/cacmb](https://aselimov.gitlab.io/cacmb)
The modes follow similarly to the modes you find when using atomsk. The modes will be listed below alongside their syntax and other usage instructions. As a note, if a mode is being used then it has to come first.
A paper describing the use of this tool is currently in preparation.
### Mode Create
```
cacmb --create name element_type lattice_parameter esize
```
Mode create has the following parameters:
`name` - User defined name that either defines the atom type or the lattice type if using the basis option
`element_type` - Specifies which element type to use, this dictates the crystal being build. Current acceptable options for element_type are:
* FCC - Uses the Rhombohedral primitive fcc unit cell as the finite element.
`lattice_parameter` - The lattice parameter for the crystal structure.
`esize` - Number of atoms per edge of the finite element. A value of 2 signifies full atomistic resolution and is the lowest number acceptable.
**Example**
```
cacmb --create Cu fcc 3.615 11
```
Creates a copper element with a lattice parameter of 3.615 with 11 atoms per side
#### Optional keywords
**Orient**
``` orient [hkl] [hkl] [hkl]
orient [hkl] [hkl] [hkl]
```
Default orientation is `[100] [010] [001]`. If this keyword is present then the user must provide the orientation matrix in form `[hkl] [hkl] [hkl]`.
*Example:* `orient [-112] [110] [-11-1]`
**Duplicate**
```
duplicate numx numy numz
```
Default duplicate is `1 1 1`. This is used to replicate the element along each dimensions. This cannot be used if the keyword dimensions is included. By default jagged edges along boundaries are filled if duplicate is greater than `1 1 1`.
*Example:* `duplicate 10 10 10`
**Dimensions**
```
dim dimx dimy dimz
```
There is no default dimensions as duplicate is the default option. This command assigns a box with user-assigned dimensions and fills it with the desired element. By default atoms fill in the jagged edges at the boundaries if the dimensions command is included.
Example: `dimensions 100 100 100`
**Origin**
```
origin x y z
```
Default origin is `0 0 0`. This command just sets the origin for where the simulation cell starts building.
*Example:* `origin 10 0 1`
**Basis**
```
basis basisnum bname bx by bz
```
This function allows you to define a custom basis. `bname bx by bz` must be repeated `basisnum` times.
**efill**
```
efill xyz
```
This command will rerun the creation algorithm with multiple times starting with an esize of `esize` and decreasing it by half on every iteration in an effort to maximize the reduction of degrees of freedom in the system. You must specify which dimensions will be filled. The code accepts `x`, `y`, `z`, `xy`, `yz`, `xz`, and `xyz` specifying which boundaries to fill in.
### Mode Convert
```
cacmb --convert infile outfile
```
This mode converts a file `infile` to a file of `outfile`. The extensions determine the conversion process.
### Mode Merge
```
cacmb --merge dim N infiles outfile
```
This mode merges multiple data files and creates one big simulation cell. The parameters are:
`N` - The number of files which are being read
`dim` - the dimension they are to be stacked along, can be either `x`, `y`, or `z`. If the argument `none` is passed then the cells are just overlaid. Future options will include a delete overlap command.
**Additional options:**
**Shift**
```
shift x y z
```
If the shift command is passed to mode merge then each file after the first file in the merge command is displaced by the vector `[x, y, z]`. This is additive so if you are merging three files and this command is passed then the second file is shifted by `[x,y,z]` and the third file is shifted by `2*[x,y,z]`.
Example: `cacmb --merge z 2 Cu.mb Cu2.mb Cu3.mb Cumerged.mb shift 2 0 0` will shift the atomic and element positions in the `Cu2.mb` file by `[2,0,0]` and the positions in `Cu3.mb` by `[4,0,0]`.
**Wrap**
```
wrap
```
This will wrap atomic positions back inside the box. Effectively as if periodic boundary conditions are applied so that atoms which exit from one side of the simulation cell enter back in through the other.
###Mode Metric
```
--metric cmetric nfiles {filepaths}
```
## Options
Options are additional portions of code which have additional functionality. Options are performed in the order that they appear in the argument list and can be added to any mode. If wanting to use strictly options use `--convert` to specify input and output files.
### Option dislgen
```
-dislgen [ijk] [hkl] x y z burgers char_angle poisson
```
This options adds an arbitrarily oriented dislocation into your model based on user inputs using the volterra displacement fields. The options are below
`[ijk]` - The vector for the line direction
`[hkl]` - The vector for the slip plane
`burgers` - The magnitude of the burgers vector for the dislocation to be inserted
`x y z` - The position of the dislocation centroid
`char_angle` - Character angle of the dislocation (0 is screw and 90 is edge)
`poisson` - Poisson's ratio used for the displacement field.
### Option disloop
````
-disloop loop_normal radius x y z bx by bz poisson
````
This option imposes the displacement field for a dislocation in order to create a loop. This loop is unstable and will close if stress isn't applied.
`loop_normal` - The box dimension which defines the normal to the loop plane. As of now this dimension must be a closed back direction, meaning that for fcc a box dimension has to be of the (111) family of planes. Either `x`, `y`, or `z`.
`n` - The number of atoms to delete on the loop plane
`x y z` - The centroid of the loop.
`bx by bz` - The burgers vector for the dislocation
`poisson` - Poisson ratio for continuum solution
### Option vacancy_disloop
```
-vacancydisloop loop_normal radius x y z
```
This option creates a circular planar vacancy cluster of radius `radius` normal to the `loop_normal` centered on position `x y z`. Upon relaxing or energy minimization this cluster should become a prismatic dislocation loop.
### Option Group
`-group select_type group_shape shape_arguments additional keywords`
This option selects a group of either elements or atoms and applies some transformation to them.
`select_type` - Either `atoms`, `elements`, or 'both'. `elements` selects elements based on whether the element center is within the group. `both` selects elements based on the element center and atoms based on their position.
`group_shape` - Specifies what shape the group takes and dictates which options must be passed. Each shape requires different arguments and these arguments are represented by the placeholder `shape_arguments`. The accepted group shapes and arguments are below:
*Block:*
`-group atoms block xlo xhi ylo yhi zlo zhi`
This selects a group residing in a block with edges perpendicular to the simulation cell. The block boundaries are given by `xlo xhi ylo yhi zlo zhi`.
`additional keywords`- Represents the various transformations which can be performed on a group. These additional keywords are given below.
*Wedge:*
`-group atoms wedge dim1 dim2 bx by bz bw`
This selects a group which are within a wedge shape. The options are given as follows:
`dim1` - The dimension containing the plane normal of the wedge base.
`dim2` - The thickness dimension. Wedge groups are currently required to span the entire cell thickness in one dimensions which is normal to the triangular face. This through thickness dimension is dim2.
`bx by bz` - Centroid of the center of the base
`bw` - Base width
*Notch:*
`-group atoms notch dim1 dim2 bx by bz bw tr`
This shape is similar to a wedge shape except instead of becoming atomically sharp, it finishes in a rounded tip with tip radius `tr`. Options are as follows.
`dim1` - The dimension containing the plane normal of the wedge base.
`dim2` - The thickness dimension. Wedge groups are currently required to span the entire cell thickness in one dimensions which is normal to the triangular face. This through thickness dimension is dim2.
`bx by bz` - Centroid of the center of the base
`bw` - Base width
`tr` - Tip radius
*Sphere*
`-group atoms sphere x y z r`
This shape selects all atoms within a sphere centered at `(x,y,z)` with radius `r`.
**Displace:**
```
displace x y z
```
This is similar to the mode merge `-shift` argument. This simply shift atoms and elements within the group by a vector `[x,y,z]`.
**Wrap**
```
wrap
```
This command wraps atoms back into the simulation cell as though periodic boundary conditions are being used.
**Remesh**
```
remesh esize
```
This command remeshes the atoms/elements within the group to the new element size `esize`.
**Max**
```
max
```
This command attempts to reduce the degrees of freedom in the model by replacing them with graded elements. This code works by starting at elements with size `esize` and then checks all degrees of freedom to see which ones can be replaced by inserting the element. It then iterates over elements of `esize-2` to `esize=2` which is full atomic resolution.
**Delete**
```
delete
```
This command deletes all selected atoms and elements within the group.
**Random**
```
random n
```
This command selects `n` random atoms and `n` random elements within your group bounds. If using group type `atoms` or `elements` then only `n` random atoms or elements are selected. This random atoms/elements then form the new group.
**Nodes**
```
nodes
```
This keyword changes the selection criteria when using `elements` or `both` to element nodes instead of element centroids.
**Flip**
```
flip
```
This keyword changes the group selection criteria from the atoms/elements inside a region to the atoms/elements outside the group.
### Option overwrite
```
-ow
```
If this option is passed then all files are automatically overwritten without asking the user.
### Option boundary
```
-boundary box_bc
```
This allows the user to specify the boundary conditions for the model being outputted. The format is a 3 character string with `p` indicating periodic and `s` indicating shrink-wrapped.
**Example:** `-boundary psp`
### Option Delete
```
-delete keywords
```
Delete requires the usage of additional keywords to specify which delete action will be taken. These additional keywords are below:
**overlap**
```
-delete overlap rc_off
```
This command will delete all overlapping atoms within a specific cutoff radius `rc_off`. This currently does not affect elements.
### Option sbox_ori
```
-sbox_ori sbox [hkl] [hkl] [hkl]
```
This option is primarily used when reading data from non .mb formats. This code simply sets the orientation variable for the specified sub box `sbox`.
### Option redef_box
```
-redef_box redef_dim {xlo xhi} {ylo yhi} {zlo zhi}
```
This option allows for the user to redefine box boundaries deleting atoms/elements outside of the new box boundaries. Elements are refined to atmoistics if they intersect the newly defined box boundaries.
The arguments are described below:
`redef_dim` - The dimensions to be redefined. Can be any permutation of `x`, `y`, `z`, `xy`, `yz`, `xz`, `xyz`. The order of the dimensions dictates the order that the new dimensions must be defined
****
## Position Specification
Specifying positions in cacmb can be done through a variety of ways. Examples of each format is shown below.
`val` - Where `val` is a number, then that value in Angstroms is used as the position. As an example, `11.1` would be read in as a position of 11.1 $\AA$.
`-inf` - This specifies the lower box boundary in the specific dimension. The vector `-inf -inf -inf` specifies the bottom corner of the simulation cell which also acts as the simulation cell origin. The vector `-inf 10 3` instead puts only the x position at the simulation cell origin.
`inf` - Similar to `-inf` but references the upper boundary of the box in that dimension
`inf-val` - Using a minus sign reduces the position from the **upper boundary** by `val`. `inf-10` would be at a distance of $10 \AA$ from the upper boundary in that dimension.
`inf+val` - This increases the position from the **lower boundary**. `inf+10` would be a position $10\AA$ from the lower boundary within the cell.
`inf*val` - This gives you a fractional position in the simulation cell. As an example `inf*0.5` gives you the center point of the simulation cell.
`rand` - Returns a random position that lies within the simulation cell.
`rand[val1:val2]` - returns a random position that lies within the range
`rande[facenum]` - Returns a random position in an interelement boundary which is offset of the element face `facenum`. Face numbers are based on the which vertices comprise the face. Vertex numbers are shown in the figure below for the primitive fcc unit cell which is what the fcc rhombohedral element is based from. The face numbers are:
Face 1: [1,2,3,4]
Face 2: [1,2,6,5]
Face 3: [2,3,7,6]
Face 4: [3,4,8,7]
Face 5: [1,4,8,5]
Face 6: [5,6,7,8]
Image for vertex numbers is:
![](/home/alexselimov/Documents/CACmb/Numbered_element.png)

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# CuNi Bicrystal Interface
This example builds a bicrystal of CuNi with a semi-coherent interface. The interface region is rendered at full atomistic resolution and the bulk of the layers are coarse-grained.
```sh
#!/bin/bash
#Build Copper CG region and atom pad
cacmb --create Cu fcc 3.615 25 orient [-21-1] [011] [11-1] duplicate 7.44 6 4 Cu_cg.mb -ow
cacmb --create Cu fcc 3.615 2 orient [-21-1] [011] [11-1] duplicate 93 75 3 Cu_atom.mb -ow
#Build Nickel CG region and atom pad
cacmb --create Ni fcc 3.52 25 orient [-21-1] [011] [11-1] duplicate 7.6409 6.16 4 Ni_cg.mb -ow
cacmb --create Ni fcc 3.52 2 orient [-21-1] [011] [11-1] duplicate 95.511 77 3 Ni_atom.mb -ow
#Merge all into one block keeping full atomistic resolution at the interface
cacmb --merge z 4 Ni_cg.mb Ni_atom.mb Cu_atom.mb Cu_cg.mb -boundary pps cac_in.restart cac_in.xyz -ow
#Delete leftover files
rm Ni_cg.mb Ni_atom.mb Cu_atom.mb Cu_cg.mb
```
Below are the .xyz file render which shows the atomistic and coarse-grained regions and the common neighbor analysi of the interface.
![xyz bicrystal render](../img/CuNi_xyz.png)
![interface structure for bicrystal model](../img/CuNi_int.png)

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# Getting Started
The CACmb tool separates commands into two general groups, modes and options.
Modes are the main commands which conduct primary operations, these are listed below:
* [Mode Convert](Modes/convert.md)
* [Mode Create](Modes/create.md)
* [Mode Merge](Modes/merge.md)
To start a cacmb run, it is required to run one of the available modes and only one mode can be run at a time.
Additionally one can use options in order to adjust the model during any of the mode runs and unlimited number of options may be used.
While single line commands may be used satisfactorily to build a model, in order to build more complex models it is required to run multiple commands.
Currently CACmb only supports rhombehedral FCC finite elements with faces aligned to {111} slip planes.
This finite element is the primitive unit cell for the FCC crystal and is shown below:
![Rhombohedral Element](img/rhomb.png)
## Simple Example 1
For example, to build a model with an atomistic region bound by a coarse-grained region the following commands should be run:
```
cacmb --create Cu fcc 3.615 15 duplicate 4 2 1 orient [112] [1-10] [11-1] Cu_cg.mb -ow
cacmb --create Cu fcc 3.615 2 duplicate 30 15 2 orient [112] [1-10] [11-1] Cu_at.mb -ow
cacmb --merge z 3 Cu_cg.mb Cu_at.mb Cu_cg.mb model.xyz -ow
```
When visualizing the model.xyz file using ovito we see our desired model (where the red atoms represent the element nodes and blue atoms are atomistic regions):
![Simple example 1 render](img/simple_example_1.png)
**Important Note: In order to fully utilize the cacmb capabilites use the .mb format when running multiple model build steps**
A description of each build step is below:
1. Build a coarse grained model with elements that have 15 atoms per edge. Orientation is set to `[112] [1-10] [11-1]`. We save it to `Cu_cg.mb` and pass `-ow` which is the flag to overwrite existing files with that name.
2. Build an atomistic model with the same dimensionsin the x and y directions as the coarse grained model. *A general way to match dimensions is by setting the duplicate value of the atoms to `esize*duplicate/2`. So for the x dimension we do `15*4/2` which is 30 and for the y dimension `15*2/2` which is 15.
3. Merge the models by stacking the coarse-grained and atomistic models. We start the stacking sequence from the bottom so the first region is the `Cu_cg.mb`, followed by the `Cu_at.mb` model in the middle, followed by another `Cu_cg.mb` region. We output it to model.xyz which renders the atoms and nodes of the model for visualization.
This whole process can be easily run as a shell script as long as cacmb is on your path.
```sh
#!/bin/sh
cacmb --create Cu fcc 3.615 15 duplicate 4 2 1 orient [112] [1-10] [11-1] Cu_cg.mb -ow
cacmb --create Cu fcc 3.615 2 duplicate 30 15 2 orient [112] [1-10] [11-1] Cu_at.mb -ow
cacmb --merge z 3 Cu_cg.mb Cu_at.mb Cu_cg.mb model.xyz -ow
```

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#Convert
```
cacmb --convert infile outfile(s)
```
This mode converts a file `infile` to different files `outfile(s)`.
The extensions on both files determine which read and write subroutines are called.
This mode can also be used to apply options to a file by setting `infile` and `outfile` to the same value such as:
```
cacmb --convert cac.mb cac.mb {-options}
```

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# Create
```
cacmb --create name element_type lattice_parameter esize
```
Mode create has the following parameters:
`name` - User defined name that either defines the atom type or the lattice type if using the basis option. If the basis command is not called then name must be an element.
`element_type` - Specifies which element type to use, this dictates the crystal being build. Current acceptable options for element_type are:
* FCC - Uses the Rhombohedral primitive fcc unit cell as the finite element.
`lattice_parameter` - The lattice parameter for the crystal structure.
`esize` - Number of atoms per edge of the finite element. A value of 2 signifies full atomistic resolution and is the lowest number acceptable.
**Example**
```
cacmb --create Cu fcc 3.615 11
```
Creates a copper fcc element with a lattice parameter of 3.615 with 11 atoms per side
## Optional keywords
Below are optional keywords that must directly follow after the esize command and before any options or filenames are passed
### Orient
```
orient [hkl] [hkl] [hkl]
```
The default orientation that is built is `[100] [010] [001]`.
If this keyword is present then the user must provide the orientation matrix in form `[hkl] [hkl] [hkl]` without spaces.
Currently only accepts whole number values for `[hkl]`.
*Example:* `orient [-112] [110] [-11-1]`
### Duplicate
```
duplicate numx numy numz
```
The default duplicate is `1 1 1`.
This is used to replicate elements along each dimension.
The unit of duplication is the lattice periodicity length times the size of elements being duplicated.
`numx numy numz` dicate the number of duplications units in the x,y, and z dimensions.
This keyword **cannot** be used with the `dim` command.
*Example:* `duplicate 10 10 10`
### Dim
```
dim dimx dimy dimz
```
There is no default `dim` as `duplicate` is the default option.
This command assigns a box with user-assigned dimensions and fills it with the desired element size.
**Note:** using dim may not result in periodic cells unless the origin of the cell is shifted from 0,0,0.
*Example:* `dimensions 100 100 100`
### Origin
```
origin x y z
```
This keyword is used to set the origin of the simulation cell.
When using the `duplicate` command, the origin is set to the minimum position of the rotated element.
When using the `dim` command the default origin is `(0,0,0)`.
When using the `dim` command for building it may become necessary to shift the origin of the simulation cell in order to produce a periodic simulation.
This origin can be retrieved by first running `--create` with `duplicate 1 1 1`.
*Example:* `origin 10 0 1`
### Basis
```
basis basisnum bname bx by bz
```
This function allows you to define a custom basis to be used at every lattice point.
The parameters for this keyword are:
- `basisnum` - The number of atoms in the basis
- `bname` - The type of the basis atom (e.g. Cu or Si)
- `bx by bz` - The position of the basis atom.
`bname bx by bz` must be repeated `basisnum` times for this command.
*Example:*
`basis 2 Si 0 0 0 Si 1.35775 1.35775 1.35775` when used with the `fcc` element produces a diamond structure with Si.
### efill
```
efill
```
This command attempts to maximize the degree of coarse-graining by iterating through esizes smaller than the user specified when filling in the jagged boundaries to create a periodic block.
This command will iterate through element sizes from the user specified `esize-2` to a minimum esize of 11.
Below is an example of a model without efill and a model with efill.
*Model without efill*
![Model without efill command](../img/not_efilled_vtk.png)
*Model with efill*
![Model with efill command](../img/efilled_vtk.png)

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# Merge
```
cacmb --merge dim N infiles
```
This mode merges multiple data files and creates one big simulation cell. The parameters are:
`dim` - the dimension they are to be stacked along, can be either `x`, `y`, or `z`. If the argument `none` is passed then the cells are just overlaid.
`N` - The number of files which are being read
`infiles` - The input files which are to be merged. There must be `N` of them.
## Additional options:
### Shift
```
shift x y z
```
If the shift command is passed to mode merge then each file after the first file in the merge command is displaced by the vector `[x, y, z]`. This is additive so if you are merging three files and this command is passed then the second file is shifted by `[x,y,z]` and the third file is shifted by `2*[x,y,z]`.
Example: `cacmb --merge z 2 Cu.mb Cu2.mb Cu3.mb Cumerged.mb shift 2 0 0` will shift the atomic and element positions in the `Cu2.mb` file by `[2,0,0]` and the positions in `Cu3.mb` by `[4,0,0]`.

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# Boundary
```
-boundary box_bc
```
This allows the user to specify the boundary conditions for the model being outputted. The format is a 3 character string with `p` indicating periodic and `s` indicating shrink-wrapped.
**Example** `ppp` - is a fully periodic model, `pss` is periodic in the x dimension and shrink wrapped in y and z.

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# Deform
```
-deform dim dl
```
This command is used to apply a uniaxial strain unto a simulation cell.
The argument `dim` takes the values of `x, y, or z` and the argument `dl` is the change in length to be applied (in Angstroms.

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# Delete Overlap
```
-delete overlap rc_off
```
This delete option removes overlapping atoms.
For every neighboring pair of atoms, the distance between them is checked.
If the distance is less than `rc_off` then the atom with the higher index in the data arrays is deleted.

@ -0,0 +1,52 @@
# Dislocation
There are various options for creating dislocations.
These are listed below.
## dislgen
```
-dislgen [ijk] [hkl] x y z burgers char_angle poisson
```
This options adds an arbitrarily oriented dislocation into your model based on user inputs using the volterra displacement fields. The options are below
`[ijk]` - The vector for the line direction
`[hkl]` - The vector for the slip plane
`burgers` - The magnitude of the burgers vector for the dislocation to be inserted
`x y z` - The position of the dislocation centroid
`char_angle` - Character angle of the dislocation (0 is screw and 90 is edge)
`poisson` - Poisson's ratio used for the displacement field.
## disloop
````
-disloop loop_normal radius x y z bx by bz poisson
````
This option imposes the displacement field for a dislocation in order to create a loop. This loop is unstable and will close if stress isn't applied.
`loop_normal` - The box dimension which defines the normal to the loop plane. As of now this dimension must be a close packed direction, meaning that for fcc a box dimension has to be of the (111) family of planes. Either `x`, `y`, or `z`.
`radius` - The radius of the loop in Angstroms.
`x y z` - The centroid of the loop.
`bx by bz` - The burgers vector for the dislocation
`poisson` - Poisson ratio for continuum solution
## vacancy disloop
```
-vacancydisloop loop_normal radius x y z
```
This option creates a circular planar vacancy cluster of radius `radius` normal to the `loop_normal` centered on position `x y z`. Upon relaxing or energy minimization this cluster should become a prismatic dislocation loop.

@ -0,0 +1,129 @@
# Group
```
-group select_type group_shape shape_arguments
```
This option selects a group of either elements or atoms and applies some transformation to them.
`select_type` - Either `atoms`, `elements`, or 'both'. `elements` selects elements based on whether the element center is within the group. `both` selects elements based on the element center and atoms based on their position.
`group_shape` - Specifies what shape the group takes and dictates which options must be passed. Each shape requires different arguments and these arguments are represented by the placeholder `shape_arguments`. The accepted group shapes and arguments are below:
## Group Shapes
These are the allowed group shapes
### Block
```
-group atoms block xlo xhi ylo yhi zlo zhi
```
This selects a group residing in a block with edges perpendicular to the simulation cell. The block boundaries are given by `xlo xhi ylo yhi zlo zhi`.
`additional keywords`- Represents the various transformations which can be performed on a group. These additional keywords are given below.
### Wedge
```
-group atoms wedge dim1 dim2 bx by bz bw
```
This selects a group which are within a wedge shape. The options are given as follows:
`dim1` - The dimension containing the plane normal of the wedge base.
`dim2` - The thickness dimension. Wedge groups are currently required to span the entire cell thickness in one dimensions which is normal to the triangular face. This through thickness dimension is dim2.
`bx by bz` - Centroid of the center of the base
`bw` - Base width
### Notch
```
-group atoms notch dim1 dim2 bx by bz bw tr
```
This shape is similar to a wedge shape except instead of becoming atomically sharp, it finishes in a rounded tip with tip radius `tr`. Options are as follows.
`dim1` - The dimension containing the plane normal of the wedge base.
`dim2` - The thickness dimension. Wedge groups are currently required to span the entire cell thickness in one dimensions which is normal to the triangular face. This through thickness dimension is dim2.
`bx by bz` - Centroid of the center of the base
`bw` - Base width
`tr` - Tip radius
### Sphere
```
-group atoms sphere x y z r
```
This shape selects all atoms within a sphere centered at `(x,y,z)` with radius `r`.
## Group selection operators
The following are a list of group operations which alter how the atoms/elements in the group are selected.
### Random
```
random n
```
This command selects `n` random atoms and `n` random elements within your group bounds.
If using group type `atoms` or `elements` then only `n` random atoms or elements are selected.
These random atoms/elements then form the new group.
*Example:*
```
group atoms block -inf inf -inf inf inf*0.5 inf random 10
```
The above example selects 10 random atoms from the specified group.
These atoms will all have z values which place them in the top half of the cell.
### Node
```
nodes
```
This keyword changes the selection criteria when using `elements` or `both` to element nodes instead of element centroids.
### Flip
```
flip
```
This keyword changes the group selection criteria from the atoms/elements inside a region to the atoms/elements outside the group.
### Notsize
```
notsize esize
```
Notsize filters out elements of size `esize` when determining the group. For example, if the user runs `notsize 25` and the group bounds contain elements with esizes of 13, 15, 25 (from the efill command for example) then only the elements with esize 13 and 15 are selected as part of the group.
## Group modification operators
These modifiers operate on selected atoms and elements to adjust their properties.
### Displace
```
displace x y z
```
This operation shifts all grouped atoms/nodes by a vector `(x,y,z)`.
### Delete
```
delete
```
This command deletes all selected atoms and elements within the group.
### Type
```
type atom_type
```
This command changes all atoms and basis atoms at element nodes for the group elements and atoms to type `atom_type`.
`atom-type` should be two characters which describe the atomic element (such as `Cu` or `Ni`)
### Refine
```
refine
```
This command refines all elements within the group to full atomistic resolution.

@ -0,0 +1,18 @@
# Orient
```
-orient [hkl] [hkl] [hkl]
```
This command transforms the simulation cell into the specified orientation.
This can be useful when attempting to view the model along different slip planes.
In general the dimensions will not be periodic as the box will not have flat surfaces along the x, y, and z dimensions.
*Example:* `-orient [-112] [110] [-11-1]`
This command also comes with a sub command `unorient`.
## Unorient
```
-unorient
```
This removes the orientation applied by an orient command during the current cacmb run.

@ -0,0 +1,7 @@
# Overwrite
```
-ow
```
If this option is passed then all files are automatically overwritten without asking the user.

@ -0,0 +1,8 @@
# Redefine Box Boundaries
```
-redef_box redef_dim {xlo xhi} {ylo yhi} {zlo zhi}
```
This option allows for the user to redefine box boundaries deleting atoms/elements outside of the new box boundaries. Elements are refined to atmoistics if they intersect the newly defined box boundaries.
The arguments are described below:
`redef_dim` - The dimensions to be redefined. Can be any permutation of `x`, `y`, `z`, `xy`, `yz`, `xz`, `xyz`. The order of the dimensions dictates the order that the new dimensions must be defined

@ -0,0 +1,20 @@
# Define Orientation
```
-sbox_ori sbox [hkl] [hkl] [hkl]
```
This option is primarily used when reading data from non .mb formats.
This code sets the orientation of the elements and atoms that are part of the sub_box `sbox` to the user provided orientation.
This doesn't change anything about the model, but is required in order to accurately use the `dislgen` or `orient` options when operating on non .mb files.
*Example:*
```
cacmb --create Cu fcc 3.615 2 orient [112] [1-10] [11-1] duplicate 10 10 10 cac.lmp
cacmb --convert cac.lmp cac_out.lmp -sbox_ori 1 [112] [1-10] [11-1] -dislgen [112] [11-1] inf*0.5 inf*0.5 inf*0.5 2.556 90 0.3
```
The above command attempts to insert a dislocation using the `dislgen` option.
In order to do the coordinate transformation, the code needs to know what the orientation of the model originally and so the sbox_ori command sets the sbox information.
To better understand how the sub_boxes work, please view sub_box in the Getting Started guide.

@ -0,0 +1,14 @@
# Slip Plane
```
-slip_plane dim pos
```
This command forces a slip plane at position `pos` along dimension `dim` by finding which elements that plane intersects and refining them to full atomistics.
## Optional Arguments
### efill
```
-slip_plane dim pos efill
```
The efill option attempts to remesh the elements that are refined while ensuring an element discontinuity on the prescribed slip plane

@ -0,0 +1,8 @@
# Wrap
```
-wrap
```
This will wrap atomic positions back inside the box.
Effectively as if periodic boundary conditions are applied so that atoms which exit from one side of the simulation cell enter back in through the other.

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@ -0,0 +1,31 @@
# CACmb: The Concurent Atomistic-Continuum Model Builder
CACmb is a tool used to build coarse-grained atomistic models for use with the PyCAC and LammpsCAC toolkits.
This tool also allows for the creation of equivalent atomistic models to be used in lammps throught the .lmp data format.
![cacmb image](img/demo.gif)
## Requirements
CACmb requires only a fortran compiler and does not need any external libraries.
This code has been tested using both gfortran and ifort fortran compilers solely on linux.
## Build instructions
CACmb can be built by the following commands:
```
git clone https://gitlab.com/aselimov/cacmb
cd cacmb/src
make
```
You can also install cacmb to /usr/local/bin by running:
```
sudo make install
```
Otherwise make sure your cacmb executable is available on your system path.
Please view the [Getting Started](Getting_Started.md) guide for an introduction and basic usage instructions.
## License
This tool is available under the MIT license which is printed below, a full copy of which is available at the cacmb [Gitlab repository.](https://gitlab.com/aselimov/cacmb/-/blob/development/LICENSE)

@ -0,0 +1,10 @@
site_name: "CACmb: The Concurrent Atomistic Continuum Model Builder"
site_url: https://aselimov.gitlab.io/cacmb
site_dir: public
theme: readthedocs
use_directory_urls: false
extra_javascript:
- https://cdnjs.cloudflare.com/ajax/libs/mathjax/2.7.0/MathJax.js?config=TeX-AMS-MML_HTMLorMML

@ -0,0 +1,6 @@
# Documentation static site generator & deployment tool
mkdocs>=1.1.2
# Add your custom theme if not inside a theme_dir
# (https://github.com/mkdocs/mkdocs/wiki/MkDocs-Themes)
# mkdocs-material>=5.4.0

@ -2,7 +2,8 @@
.DEFAULT_GOAL := all
FC=mpif90
FFLAGS=-Wall -mcmodel=large -O0 -g -fbacktrace -fcheck=all -ffpe-trap=invalid,zero,overflow,underflow,denormal
#FFLAGS=-Wall -mcmodel=large -O0 -g -fbacktrace -fcheck=all -ffpe-trap=invalid,zero,overflow,underflow,denormal
FFLAGS=-O3 -g
OBJDIR=obj
SRCS := $(wildcard *.f90)
@ -32,7 +33,7 @@ $(OBJDIR)/%.o: %.f90
deps:
@fortdepend -o Makefile.dep -i mpi -b obj -w
@makedepf90 -b obj *.f90 > Makefile.dep
#----------------- CLEAN UP -----------------#

@ -11,9 +11,11 @@ obj/main : \
obj/mode_calc.o \
obj/mode_convert.o \
obj/mode_create.o \
obj/mode_da.o \
obj/mode_merge.o \
obj/mode_metric.o \
obj/neighbors.o \
obj/opt_bubble.o \
obj/opt_deform.o \
obj/opt_delete.o \
obj/opt_disl.o \
@ -39,8 +41,10 @@ obj/caller.o : \
obj/mode_calc.o \
obj/mode_convert.o \
obj/mode_create.o \
obj/mode_da.o \
obj/mode_merge.o \
obj/mode_metric.o \
obj/opt_bubble.o \
obj/opt_deform.o \
obj/opt_delete.o \
obj/opt_disl.o \
@ -51,6 +55,7 @@ obj/caller.o : \
obj/parameters.o
obj/elements.o : \
obj/atoms.o \
obj/box.o \
obj/functions.o \
obj/parameters.o \
@ -94,10 +99,17 @@ obj/mode_create.o : \
obj/parameters.o \
obj/subroutines.o
obj/mode_da.o : \
obj/elements.o \
obj/io.o \
obj/neighbors.o \
obj/parameters.o
obj/mode_merge.o : \
obj/atoms.o \
obj/elements.o \
obj/io.o \
obj/neighbors.o \
obj/parameters.o \
obj/subroutines.o
@ -108,11 +120,19 @@ obj/mode_metric.o : \
obj/parameters.o
obj/neighbors.o : \
obj/box.o \
obj/elements.o \
obj/functions.o \
obj/parameters.o \
obj/subroutines.o
obj/opt_bubble.o : \
obj/atoms.o \
obj/box.o \
obj/elements.o \
obj/opt_group.o \
obj/parameters.o
obj/opt_deform.o : \
obj/box.o \
obj/elements.o \
@ -132,9 +152,11 @@ obj/opt_disl.o : \
obj/subroutines.o
obj/opt_group.o : \
obj/atoms.o \
obj/box.o \
obj/elements.o \
obj/parameters.o \
obj/sorts.o \
obj/subroutines.o
obj/opt_orient.o : \
@ -164,4 +186,5 @@ obj/str.o :
obj/subroutines.o : \
obj/box.o \
obj/functions.o \
obj/parameters.o
obj/parameters.o \
obj/str.o

@ -1162,6 +1162,267 @@ END SELECT
!
END SUBROUTINE ATOMMASSSPECIES
!
subroutine realatomspecies(smass,species)
!
IMPLICIT NONE
CHARACTER(LEN=2),INTENT(OUT):: species
INTEGER:: mass
REAL(dp),INTENT(IN):: smass
if(mass_is_equal(smass,1.008d0)) then
species = 'H'
else if(mass_is_equal(smass,2.014101777d0)) then
species = 'D'
else if(mass_is_equal(smass,4.002602d0)) then
species = 'He'
else if(mass_is_equal(smass,6.94d0)) then
species = 'Li'
else if(mass_is_equal(smass,9.012182d0)) then
species = 'Be'
else if(mass_is_equal(smass,10.81d0)) then
species = 'B'
else if(mass_is_equal(smass,12.011d0)) then
species='C'
else if(mass_is_equal(smass,14.007d0)) then
species='N'
else if(mass_is_equal(smass,15.999d0)) then
species='O'
else if(mass_is_equal(smass,18.9984032d0)) then
species='F'
else if(mass_is_equal(smass,20.1797d0)) then
species='Ne'
!
! n=3
else if(mass_is_equal(smass,22.98976928d0)) then
species = 'Na'
else if(mass_is_equal(smass,24.305d0)) then
species='Mg'
else if(mass_is_equal(smass,26.9815386d0)) then
species='Al'
else if(mass_is_equal(smass,28.085d0)) then
species='Si'
else if(mass_is_equal(smass,30.973762d0)) then
species='P'
else if(mass_is_equal(smass,32.06d0)) then
species='S'
else if(mass_is_equal(smass,35.45d0)) then
species='Cl'
else if(mass_is_equal(smass,39.948d0)) then
species='Ar'
!
! n=4
else if(mass_is_equal(smass,39.0983d0)) then
species='K'
else if(mass_is_equal(smass,40.078d0)) then
species='Ca'
else if(mass_is_equal(smass,44.955912d0)) then
species='Sc'
else if(mass_is_equal(smass,47.867d0)) then
species='Ti'
else if(mass_is_equal(smass,50.9415d0)) then
species='V'
else if(mass_is_equal(smass,51.9961d0)) then
species='Cr'
else if(mass_is_equal(smass,54.938045d0)) then
species='Mn'
else if(mass_is_equal(smass,55.845d0)) then
species='Fe'
else if(mass_is_equal(smass,58.933195d0)) then
species='Co'
else if(mass_is_equal(smass,58.6934d0)) then
species='Ni'
else if(mass_is_equal(smass,63.546d0)) then
species='Cu'
else if(mass_is_equal(smass,65.38d0)) then
species='Zn'
else if(mass_is_equal(smass,69.723d0)) then
species='Ga'
else if(mass_is_equal(smass,72.63d0)) then
species='Ge'
else if(mass_is_equal(smass,74.9216d0)) then
species='As'
else if(mass_is_equal(smass,78.96d0)) then
species='Se'
else if(mass_is_equal(smass,79.904d0)) then
species='Br'
else if(mass_is_equal(smass,83.798d0)) then
species='Kr'
!
! n=5
else if(mass_is_equal(smass,85.4678d0)) then
species='Rb'
else if(mass_is_equal(smass,87.62d0)) then
species='Sr'
else if(mass_is_equal(smass,88.90585d0)) then
species='Y'
else if(mass_is_equal(smass,91.224d0)) then
species='Zr'
else if(mass_is_equal(smass,92.90638d0)) then
species='Nb'
else if(mass_is_equal(smass,95.96d0)) then
species='Mo'
else if(mass_is_equal(smass,98.906d0)) then
species='Tc'
else if(mass_is_equal(smass,101.07d0)) then
species='Ru'
else if(mass_is_equal(smass,102.90550d0)) then
species='Rh'
else if(mass_is_equal(smass,106.42d0)) then
species='Pd'
else if(mass_is_equal(smass,107.8682d0)) then
species='Ag'
else if(mass_is_equal(smass,112.411d0)) then
species='Cd'
else if(mass_is_equal(smass,114.818d0)) then
species='In'
else if(mass_is_equal(smass,118.71d0)) then
species='Sn'
else if(mass_is_equal(smass,121.76d0)) then
species='Sb'
else if(mass_is_equal(smass,127.60d0)) then
species='Te'
else if(mass_is_equal(smass,126.90447d0)) then
species='I'
else if(mass_is_equal(smass,131.293d0)) then
species='Xe'
!
! n=6
else if(mass_is_equal(smass,132.9054519d0)) then
species='Cs'
else if(mass_is_equal(smass,137.327d0)) then
species='Ba'
! Lanthanides
else if(mass_is_equal(smass,138.90547d0)) then
species='La'
else if(mass_is_equal(smass,140.116d0)) then
species='Ce'
else if(mass_is_equal(smass,140.90765d0)) then
species='Pr'
else if(mass_is_equal(smass,144.242d0)) then
species='Nd'
else if(mass_is_equal(smass,144.91d0)) then
species='Pm'
else if(mass_is_equal(smass,150.36d0)) then
species='Sm'
else if(mass_is_equal(smass,151.964d0)) then
species='Eu'
else if(mass_is_equal(smass,157.25d0)) then
species='Gd'
else if(mass_is_equal(smass,158.92535d0)) then
species='Tb'
else if(mass_is_equal(smass,162.50d0)) then
species='Dy'
else if(mass_is_equal(smass,164.93032d0)) then
species='Ho'
else if(mass_is_equal(smass,167.259d0)) then
species='Er'
else if(mass_is_equal(smass,168.93421d0)) then
species='Tm'
else if(mass_is_equal(smass,173.054d0)) then
species='Yb'
else if(mass_is_equal(smass,174.9668d0)) then
species='Lu'
! End of Lanthanides
else if(mass_is_equal(smass,178.49d0)) then
species='Hf'
else if(mass_is_equal(smass,180.94788d0)) then
species='Ta'
else if(mass_is_equal(smass,183.84d0)) then
species='W'
else if(mass_is_equal(smass,186.207d0)) then
species='Re'
else if(mass_is_equal(smass,190.23d0)) then
species='Os'
else if(mass_is_equal(smass,192.217d0)) then
species='Ir'
else if(mass_is_equal(smass,195.084d0)) then
species='Pt'
else if(mass_is_equal(smass,196.966569d0)) then
species='Au'
else if(mass_is_equal(smass,200.59d0)) then
species='Hg'
else if(mass_is_equal(smass,204.38d0)) then
species='Tl'
else if(mass_is_equal(smass,207.2d0)) then
species='Pb'
else if(mass_is_equal(smass,208.9804d0)) then
species='Bi'
else if(mass_is_equal(smass,209.98d0)) then
species='Po'
else if(mass_is_equal(smass,209.99d0)) then
species='At'
else if(mass_is_equal(smass,222.02d0)) then
species='Rn'
!
! n=7
else if(mass_is_equal(smass,233.d0)) then
species='Fr'
else if(mass_is_equal(smass,226.d0)) then
species='Ra'
! Actinides
else if(mass_is_equal(smass,227.d0)) then
species='Ac'
else if(mass_is_equal(smass,232.03806d0)) then
species='Th'
else if(mass_is_equal(smass,231.03588d0)) then
species='Pa'
else if(mass_is_equal(smass,238.02891d0)) then
species='U'
else if(mass_is_equal(smass,237.d0)) then
species='Np'
else if(mass_is_equal(smass,244.d0)) then
species='Pu'
else if(mass_is_equal(smass,243.d0)) then
species='Am'
else if(mass_is_equal(smass,247.d0)) then
species='Cm'
else if(mass_is_equal(smass,247.d0)) then
species='Bk'
else if(mass_is_equal(smass,251.d0)) then
species='Cf'
else if(mass_is_equal(smass,252.d0)) then
species='Es'
else if(mass_is_equal(smass,257.d0)) then
species='Fm'
else if(mass_is_equal(smass,258.d0)) then
species='Md'
else if(mass_is_equal(smass,259.d0)) then
species='No'
else if(mass_is_equal(smass,262.d0)) then
species='Lr'
! End of actinides
else if(mass_is_equal(smass,265.d0)) then
species='Rf'
else if(mass_is_equal(smass,268.d0)) then
species='Db'
else if(mass_is_equal(smass,271.d0)) then
species='Sg'
else if(mass_is_equal(smass,270.d0)) then
species='Bh'
else if(mass_is_equal(smass,277.d0)) then
species='Hs'
else if(mass_is_equal(smass,276.d0)) then
species='Mt'
else if(mass_is_equal(smass,281.d0)) then
species='Ds'
else if(mass_is_equal(smass,280.d0)) then
species='Rg'
else if(mass_is_equal(smass,285.17d0)) then
species='Cn'
else if(mass_is_equal(smass,284.d0)) then
species='Uu'
else if(mass_is_equal(smass,289.d0)) then
species='Fl'
else if(mass_is_equal(smass,288.d0)) then
species='Mc'
else if(mass_is_equal(smass,293.d0)) then
species='Lv'
else if(mass_is_equal(smass,294.d0)) then
species='Ts'
else if(mass_is_equal(smass,294.d0)) then
species='Og'
!
end if
end subroutine realatomspecies
END MODULE atoms

@ -5,14 +5,11 @@ module box
implicit none
real(kind=dp) :: box_bd(6) !Global box boundaries
real(kind=dp) :: box_ori(3,3) !Box orientation
character(len=3) :: box_bc !Box boundary conditions (periodic or shrinkwrapped)
logical :: bound_called
!The subbox variables contain values for each subbox, being the boxes read in through some
!command. Currently only mode_merge will require sub_boxes, for mode_create it will always
!allocate to only 1 sub_box
integer :: sub_box_num = 0
real(kind=dp), allocatable :: sub_box_ori(:,:,:)!Orientations for each of the subboxes
real(kind=dp), allocatable :: sub_box_bd(:,:)!Boundaries for each of the sub_boxes
!command.
!Below are some simulation parameters which may be adjusted if reading in restart files
integer :: timestep=0
@ -29,42 +26,6 @@ module box
bound_called=.false.
end subroutine box_init
subroutine alloc_sub_box(n)
!Allocate the sub_box variables
integer, intent(in) :: n
integer :: i
allocate(sub_box_ori(3,3,n), sub_box_bd(6,n))
do i = 1, n
sub_box_ori(:,:,i) = identity_mat(3)
sub_box_bd(:,i) = 0.0_dp
end do
end subroutine alloc_sub_box
subroutine grow_sub_box(n)
!Grows sub box arrays, this is only called when a new file is read in
integer, intent(in) :: n
integer, allocatable :: temp_array_bd(:,:,:), temp_file(:)
real(kind=dp), allocatable :: temp_ori(:,:,:), temp_bd(:,:)
!Allocate temporary arrays
allocate(temp_ori(3,3,sub_box_num+n),temp_bd(6,sub_box_num+n), &
temp_array_bd(2,2,sub_box_num+n), temp_file(sub_box_num+n))
!Move allocation for all sub_box_arrays
temp_ori(:,:,1:sub_box_num) = sub_box_ori
temp_ori(:,:,sub_box_num+1:) = 0.0_dp
call move_alloc(temp_ori, sub_box_ori)
temp_bd(:, 1:sub_box_num) = sub_box_bd
temp_bd(:, sub_box_num+1:) = 0.0_dp
call move_alloc(temp_bd, sub_box_bd)
return
end subroutine grow_sub_box
subroutine grow_box(temp_box_bd)
!This function takes in a temporary box boundary and adjusts the overall box boundaries
!to include it
@ -85,24 +46,6 @@ module box
return
end subroutine grow_box
subroutine in_sub_box(r, which_sub_box)
!This returns which sub_box a point is in. It returns the first sub_box with boundaries which
!contain the point.
real(kind=dp), dimension(3), intent(in) :: r
integer, intent(out) :: which_sub_box
integer :: i
do i = 1, sub_box_num
if( in_block_bd(r, sub_box_bd(:,i))) then
which_sub_box = i
exit
end if
end do
return
end subroutine in_sub_box
subroutine reset_box
!This subroutine just resets the box boundary and position
box_bc = "ppp"
@ -115,4 +58,5 @@ module box
box_volume = (box_bd(2) - box_bd(1)) * (box_bd(4) - box_bd(3))*(box_bd(6) - box_bd(5))
return
end function
end module box

@ -1,6 +1,7 @@
module caller
!this module just calls modes and options
use mode_da
use mode_create
use mode_convert
use mode_merge
@ -14,6 +15,7 @@ module caller
use opt_delete
use opt_redef_box
use opt_slip_plane
use opt_bubble
use box
@ -37,6 +39,8 @@ module caller
call metric(arg_pos)
case('--calc')
call calc(arg_pos)
case('--da')
call da(arg_pos)
case default
print *, "Mode ", trim(adjustl(mode)), " currently not accepted. Please check documentation for ", &
"accepted modes and rerun."
@ -56,8 +60,14 @@ module caller
call group(arg_pos)
case('-ow')
arg_pos = arg_pos + 1
case('-novel')
arg_pos = arg_pos+1
case('-wrap')
arg_pos = arg_pos + 1
case('-norefine')
arg_pos = arg_pos + 1
case('-all_new')
arg_pos = arg_pos + 1
case('-orient')
call orient_opt(arg_pos)
case('-unorient')
@ -68,8 +78,8 @@ module caller
call get_command_argument(arg_pos, box_bc)
arg_pos=arg_pos+1
bound_called = .true.
case('-sbox_ori')
call sbox_ori(arg_pos)
case('-box_ori')
call set_box_ori(arg_pos)
case('-deform')
call deform(arg_pos)
case('-delete')
@ -82,6 +92,8 @@ module caller
call redef_box(arg_pos)
case('-slip_plane')
call run_slip_plane(arg_pos)
case('-bubble')
call bubble(arg_pos)
case default
print *, 'Option ', trim(adjustl(option)), ' is not currently accepted.'
stop 3

@ -2,6 +2,7 @@ module elements
!This module contains the elements data structures, structures needed for building regions
!and operations that are done on elements
use atoms
use parameters
use functions
use subroutines
@ -11,10 +12,10 @@ module elements
!Data structures used to represent the CAC elements. Each index represents an element
character(len=100), allocatable :: type_ele(:) !Element type
integer, allocatable :: size_ele(:), lat_ele(:), sbox_ele(:), tag_ele(:) !Element size
integer, allocatable :: size_ele(:), lat_ele(:), tag_ele(:) !Element size
real(kind=dp), allocatable :: r_node(:,:,:,:) !Nodal position array
!Element result data structures
real(kind=dp), allocatable :: force_node(:,:,:,:), virial_node(:,:,:,:), energy_node(:,:,:)
real(kind=dp), allocatable :: force_node(:,:,:,:), virial_node(:,:,:,:), energy_node(:,:,:), vel_node(:,:,:,:)
integer, save :: ele_num !Number of elements
integer, save :: node_num !Total number of nodes
@ -22,19 +23,21 @@ module elements
!Data structure used to represent atoms
integer, allocatable :: type_atom(:)!atom type
integer, allocatable :: sbox_atom(:), tag_atom(:)
integer, allocatable :: tag_atom(:)
real(kind =dp),allocatable :: r_atom(:,:) !atom position
integer :: atom_num=0 !Number of atoms
!Atom result data structures information
real(kind=8), allocatable :: force_atom(:,:), virial_atom(:,:), energy_atom(:)
real(kind=8), allocatable :: force_atom(:,:), virial_atom(:,:), energy_atom(:), vel_atom(:,:)
!Mapping atom type to provided name
character(len=2), dimension(10) :: type_to_name
integer :: atom_types = 0
real(kind=dp) :: masses(10)
!Variables for creating elements based on primitive cells
real(kind=dp) :: cubic_cell(3,8), fcc_cell(3,8), fcc_mat(3,3), fcc_inv(3,3), bcc_cell(3,8), bcc_mat(3,3), bcc_inv(3,3)
integer :: cubic_faces(4,6)
real(kind=dp) :: cubic_cell(3,8), fcc_cell(3,8), fcc_mat(3,3), fcc_inv(3,3), bcc_cell(3,8), bcc_mat(3,3), bcc_inv(3,3), &
cube20(3,20)
integer :: cubic_faces(4,6), oneonetwopairs(2,6)
!Below are lattice type arrays which provide information on the general form of the elements.
!We currently have a limit of 10 lattice types for simplicities sake but this can be easily increased.
@ -43,7 +46,7 @@ module elements
integer :: max_esize=0 !Maximum number of atoms per side of element
real(kind=dp) :: lapa(10)
!These variables contain information on the basis, for simplicities sake we limit
!These variables contain informatione on the basis, for simplicities sake we limit
!the user to the definition of 10 lattice types with 10 basis atoms at each lattice point.
!This can be easily increased with no change to efficiency
integer :: max_basisnum, basisnum(10) !Max basis atom number, number of basis atoms in each lattice type
@ -72,14 +75,45 @@ module elements
0.0_dp, 1.0_dp, 1.0_dp /), &
shape(fcc_cell))
!Now initialize the 20 node cube element
cube20 = reshape((/ 0.0_dp, 0.0_dp, 0.0_dp, &
1.0_dp, 0.0_dp, 0.0_dp, &
1.0_dp, 1.0_dp, 0.0_dp, &
0.0_dp, 1.0_dp, 0.0_dp, &
0.0_dp, 0.0_dp, 1.0_dp, &
1.0_dp, 0.0_dp, 1.0_dp, &
1.0_dp, 1.0_dp, 1.0_dp, &
0.0_dp, 1.0_dp, 1.0_dp, &
0.5_dp, 0.0_dp, 0.0_dp, &
1.0_dp, 0.5_dp, 0.0_dp, &
0.5_dp, 1.0_dp, 0.0_dp, &
0.0_dp, 0.5_dp, 0.0_dp, &
0.0_dp, 0.0_dp, 0.5_dp, &
1.0_dp, 0.0_dp, 0.5_dp, &
1.0_dp, 1.0_dp, 0.5_dp, &
0.0_dp, 1.0_dp, 0.5_dp, &
0.5_dp, 0.0_dp, 1.0_dp, &
1.0_dp, 0.5_dp, 1.0_dp, &
0.5_dp, 1.0_dp, 1.0_dp, &
0.0_dp, 0.5_dp, 1.0_dp /), &
shape(cube20))
!Now we create a list containing the list of vertices needed to describe the 6 cube faces
cubic_faces(:,1) = (/ 1, 2, 3, 4 /)
cubic_faces(:,2) = (/ 1, 2, 6, 5 /)
cubic_faces(:,3) = (/ 2, 3, 7, 6 /)
cubic_faces(:,4) = (/ 3, 4, 8, 7 /)
cubic_faces(:,5) = (/ 1, 4, 8, 5 /)
cubic_faces(:,4) = (/ 1, 4, 8, 5 /)
cubic_faces(:,5) = (/ 4, 3, 7, 8 /)
cubic_faces(:,6) = (/ 5, 6, 7, 8 /)
!Now mark which node pairs represent the 112 directions. This is used for the dislocation analysis.
oneonetwopairs(:,1) = (/ 1, 3 /)
oneonetwopairs(:,2) = (/ 1, 6 /)
oneonetwopairs(:,3) = (/ 2, 7 /)
oneonetwopairs(:,4) = (/ 1, 8 /)
oneonetwopairs(:,5) = (/ 4, 7 /)
oneonetwopairs(:,6) = (/ 5, 7 /)
!!Now initialize the fcc primitive cell
fcc_cell = reshape((/ 0.0_dp, 0.0_dp, 0.0_dp, &
0.5_dp, 0.5_dp, 0.0_dp, &
@ -119,6 +153,7 @@ module elements
max_basisnum = 0
basisnum(:) = 0
basis_type(:,:) = 0
ng_node(:) = 0
node_num = 0
node_atoms = 0
@ -179,7 +214,7 @@ module elements
!Allocate element arrays
if(n > 0) then
allocate(type_ele(n), tag_ele(n), size_ele(n), lat_ele(n), sbox_ele(n), r_node(3,max_basisnum, max_ng_node,n), &
allocate(type_ele(n), tag_ele(n), size_ele(n), lat_ele(n), r_node(3,max_basisnum, max_ng_node,n), &
stat=allostat)
if(allostat > 0) then
print *, "Error allocating element arrays in elements.f90 because of: ", allostat
@ -189,7 +224,7 @@ module elements
if(m > 0) then
!Allocate atom arrays
allocate(type_atom(m), sbox_atom(m), tag_atom(m), r_atom(3,m), stat=allostat)
allocate(type_atom(m), tag_atom(m), r_atom(3,m), stat=allostat)
if(allostat > 0) then
print *, "Error allocating atom arrays in elements.f90 because of: ", allostat
stop
@ -233,11 +268,6 @@ module elements
temp_int(ele_size+1:) = 0
call move_alloc(temp_int, size_ele)
allocate(temp_int(n+ele_size+buffer_size))
temp_int(1:ele_size) = sbox_ele(1:ele_size)
temp_int(ele_size+1:) = 0
call move_alloc(temp_int, sbox_ele)
allocate(char_temp(n+ele_size+buffer_size))
char_temp(1:ele_size) = type_ele(1:ele_size)
call move_alloc(char_temp, type_ele)
@ -265,11 +295,6 @@ module elements
temp_int(atom_size+1:) = 0
call move_alloc(temp_int, tag_atom)
allocate(temp_int(m+atom_size+buffer_size))
temp_int(1:atom_size) = sbox_atom
temp_int(atom_size+1:) = 0
call move_alloc(temp_int, sbox_atom)
allocate(temp_real(3,m+atom_size+buffer_size))
temp_real(:,1:atom_size) = r_atom
temp_real(:, atom_size+1:) = 0.0_dp
@ -280,11 +305,11 @@ module elements
end if
end subroutine
subroutine add_element(tag, type, size, lat, sbox, r)
subroutine add_element(tag, type, size, lat, r)
!Subroutine which adds an element to the element arrays
integer, intent(in) :: size, lat, sbox, tag
integer, intent(in) :: size, lat, tag
character(len=100), intent(in) :: type
real(kind=dp), intent(in) :: r(3, max_basisnum, max_ng_node)
real(kind=dp), intent(in) :: r(:,:,:)
integer :: newtag
@ -304,15 +329,14 @@ module elements
type_ele(ele_num) = type
size_ele(ele_num) = size
lat_ele(ele_num) = lat
sbox_ele(ele_num) = sbox
r_node(:,:,:,ele_num) = r(:,:,:)
end subroutine add_element
subroutine add_atom(tag, type, sbox, r)
subroutine add_atom(tag, type, r)
!Subroutine which adds an atom to the atom arrays
integer, intent(in) :: type, sbox, tag
integer, intent(in) :: type, tag
real(kind=dp), intent(in), dimension(3) :: r
integer :: newtag
@ -325,29 +349,38 @@ module elements
end if
!Check to see if we need to grow the arrays
call grow_ele_arrays(0,1)
tag_atom(atom_num) = tag
tag_atom(atom_num) = newtag
type_atom(atom_num) = type
r_atom(:,atom_num) = r(:)
sbox_atom(atom_num) = sbox
end subroutine add_atom
subroutine add_atom_type(type, inttype)
subroutine add_atom_type(mass, inttype, force_new)
!This subroutine adds a new atom type to the module list of atom types
character(len=2), intent(in) :: type
real(kind=dp), intent(in) :: mass
integer, intent(out) :: inttype
logical, optional, intent(in) :: force_new
integer :: i
logical :: exists
logical :: exists, force
if(present(force_new)) then
force = force_new
else
force = .false.
end if
exists = .false.
do i=1, 10
if(type == type_to_name(i)) then
exists = .true.
inttype = i
exit
end if
end do
if(.not.force) then
do i=1, 10
if(is_equal(mass, masses(i))) then
exists = .true.
inttype = i
exit
end if
end do
end if
if (exists.eqv..false.) then
atom_types = atom_types+1
@ -355,7 +388,8 @@ module elements
print *, "Defined atom types are greater than 10 which is currently not supported."
stop 3
end if
type_to_name(atom_types) = type
call atommassspecies(mass, type_to_name(atom_types))
masses(atom_types) = mass
inttype = atom_types
end if
return
@ -374,6 +408,8 @@ module elements
ng_node(i) = 8
case('bcc')
ng_node(i) = 8
case('20fcc')
ng_node(i) = 20
end select
if(ng_node(i) > max_ng_node) max_ng_node = ng_node(i)
@ -393,18 +429,18 @@ module elements
!This subroutine returns the interpolated atoms from the elements.
!Arguments
character(len=100), intent(in) :: type !The type of element that it is
character(len=*), intent(in) :: type !The type of element that it is
integer, intent(in) :: esize !The number of atoms per side
integer, intent(in) :: lat_type !The integer lattice type of the element
real(kind=dp), dimension(3,max_basisnum, max_ng_node), intent(in) :: r_in !Nodal positions
integer, dimension(max_basisnum*max_esize**3), intent(out) :: type_interp !Interpolated atomic positions
real(kind=dp), dimension(:,:,:), intent(in) :: r_in !Nodal positions
integer, dimension(:), intent(out) :: type_interp !Interpolated atomic positions
real(kind=dp), dimension(3, max_basisnum*max_esize**3), intent(out) :: r_interp !Interpolated atomic positions
real(kind = dp), optional, intent(in) :: eng(max_basisnum, max_ng_node), f(3, max_basisnum, max_ng_node), &
v(6, max_basisnum, max_ng_node)
real(kind=dp), dimension(10, max_basisnum*max_esize**3), optional,intent(out) :: data_interp !Interpolated atomic positions
real(kind = dp), optional, intent(in) :: eng(:,:), f(:,:,:), &
v(:,:,:)
real(kind=dp), dimension(:,:), optional,intent(out) :: data_interp !Interpolated atomic positions
!Internal variables
integer :: it, is, ir, ibasis, inod, ia, bnum, lat_type_temp
integer :: it, is, ir, ibasis, inod, ia, bnum, lat_type_temp, adjust
real(kind=dp) :: a_shape(max_ng_node)
real(kind=dp) :: t, s, r
@ -426,8 +462,36 @@ module elements
lat_type_temp = lat_type
end select
select case(trim(adjustl(type)))
select case(type)
case('fcc','bcc')
!Now loop over all the possible sites
do it = 1, esize
t=-1.0_dp +(it-1)*(2.0_dp/(esize-1))
do is =1, esize
s=-1.0_dp +(is-1)*(2.0_dp/(esize-1))
do ir = 1, esize
r=-1.0_dp +(ir-1)*(2.0_dp/(esize-1))
call rhombshape(r,s,t,a_shape)
do ibasis = 1, bnum
ia = ia + 1
do inod = 1, 8
type_interp(ia) = basis_type(ibasis,lat_type_temp)
r_interp(:,ia) = r_interp(:,ia) + a_shape(inod) * r_in(:,ibasis,inod)
if(present(data_interp)) then
!If data is present then interpolate data arrays as well
data_interp(1,ia) = data_interp(1,ia) + eng(ibasis, inod)*a_shape(inod)
data_interp(2:4,ia) = data_interp(2:4,ia) + f(:, ibasis, inod)*a_shape(inod)
data_interp(5:10,ia) = data_interp(5:10,ia) + v(:, ibasis, inod)*a_shape(inod)
end if
end do
end do
end do
end do
end do
case('20fcc')
!Now loop over all the possible sites
do it = 1, esize
t = (1.0_dp*(it-1)-(esize-1)/2)/(1.0_dp*(esize-1)/2)
@ -435,11 +499,11 @@ module elements
s = (1.0_dp*(is-1)-(esize-1)/2)/(1.0_dp*(esize-1)/2)
do ir = 1, esize
r = (1.0_dp*(ir-1) - (esize-1)/2)/(1.0_dp*(esize-1)/2)
call rhombshape(r,s,t,a_shape)
call quad_rhombshape(r,s,t,a_shape)
do ibasis = 1, bnum
ia = ia + 1
do inod = 1, 8
do inod = 1, 20
type_interp(ia) = basis_type(ibasis,lat_type_temp)
r_interp(:,ia) = r_interp(:,ia) + a_shape(inod) * r_in(:,ibasis,inod)
@ -464,6 +528,68 @@ module elements
return
end subroutine interpolate_atoms
subroutine interpolate_vel(type, esize, lat_type, vel_in, vel_interp)
!This subroutine returns the interpolated atoms from the elements.
!Arguments
character(len=*), intent(in) :: type !The type of element that it is
integer, intent(in) :: esize !The number of atoms per side
integer, intent(in) :: lat_type !The integer lattice type of the element
real(kind=dp), dimension(:,:,:), intent(in) :: vel_in !Nodal positions
real(kind=dp), dimension(3, max_basisnum*max_esize**3), intent(out) :: vel_interp !Interpolated atomic positions
!Internal variables
integer :: it, is, ir, ibasis, inod, ia, bnum, lat_type_temp, adjust
real(kind=dp) :: a_shape(max_ng_node)
real(kind=dp) :: t, s, r
!Initialize some variables
vel_interp(:,:) = 0.0_dp
ia = 0
!Define bnum based on the input lattice type. If lat_type=0 then we are interpolating lattice points which means
!the basis is 0,0,0, and the type doesn't matter
select case(lat_type)
case(0)
bnum=1
lat_type_temp = 1
case default
bnum = basisnum(lat_type)
lat_type_temp = lat_type
end select
select case(type)
case('fcc','bcc')
!Now loop over all the possible sites
do it = 1, esize
t=-1.0_dp +(it-1)*(2.0_dp/(esize-1))
do is =1, esize
s=-1.0_dp +(is-1)*(2.0_dp/(esize-1))
do ir = 1, esize
r=-1.0_dp +(ir-1)*(2.0_dp/(esize-1))
call rhombshape(r,s,t,a_shape)
do ibasis = 1, bnum
ia = ia + 1
do inod = 1, 8
vel_interp(:,ia) = vel_interp(:,ia) + a_shape(inod) * vel_in(:,ibasis,inod)
end do
end do
end do
end do
end do
end select
if (ia /= bnum*esize**3) then
print *, "Incorrect interpolation"
stop 3
end if
return
end subroutine interpolate_vel
subroutine rhombshape(r,s,t, shape_fun)
!Shape function for rhombohedral elements
real(kind=8), intent(in) :: r, s, t
@ -482,6 +608,42 @@ module elements
return
end subroutine rhombshape
subroutine quad_rhombshape(r,s,t, shape_fun)
!Shape function for 20 node quadratic rhombohedral elements
real(kind=8), intent(in) :: r, s, t
real(kind=8), intent(out) :: shape_fun(:)
!Corner nodes
shape_fun(1) = (1.0_dp-r)*(1.0_dp-s)*(1.0_dp-t)*(-r-s-t-2)/8.0_dp
shape_fun(2) = (1.0_dp+r)*(1.0_dp-s)*(1.0_dp-t)*(r-s-t-2)/8.0_dp
shape_fun(3) = (1.0_dp+r)*(1.0_dp+s)*(1.0_dp-t)*(r+s-t-2)/8.0_dp
shape_fun(4) = (1.0_dp-r)*(1.0_dp+s)*(1.0_dp-t)*(-r+s-t-2)/8.0_dp
shape_fun(5) = (1.0_dp-r)*(1.0_dp-s)*(1.0_dp+t)*(-r-s+t-2)/8.0_dp
shape_fun(6) = (1.0_dp+r)*(1.0_dp-s)*(1.0_dp+t)*(r-s+t-2)/8.0_dp
shape_fun(7) = (1.0_dp+r)*(1.0_dp+s)*(1.0_dp+t)*(r+s+t-2)/8.0_dp
shape_fun(8) = (1.0_dp-r)*(1.0_dp+s)*(1.0_dp+t)*(-r+s+t-2)/8.0_dp
!Side nodes, first node r is zero
shape_fun(9) = (1-r*r)*(1-s)*(1-t)/4.0_dp
shape_fun(11) = (1-r*r)*(1+s)*(1-t)/4.0_dp
shape_fun(17) = (1-r*r)*(1-s)*(1+t)/4.0_dp
shape_fun(19) = (1-r*r)*(1+s)*(1+t)/4.0_dp
!node s is zero
shape_fun(10) = (1+r)*(1-s*s)*(1-t)/4.0_dp
shape_fun(12) = (1-r)*(1-s*s)*(1-t)/4.0_dp
shape_fun(18) = (1+r)*(1-s*s)*(1+t)/4.0_dp
shape_fun(20) = (1-r)*(1-s*s)*(1+t)/4.0_dp
!node t is zero
shape_fun(13) = (1-r)*(1-s)*(1-t*t)/4.0_dp
shape_fun(14) = (1+r)*(1-s)*(1-t*t)/4.0_dp
shape_fun(15) = (1+r)*(1+s)*(1-t*t)/4.0_dp
shape_fun(16) = (1-r)*(1+s)*(1-t*t)/4.0_dp
end subroutine quad_rhombshape
subroutine delete_atoms(num, in_index)
!This subroutine deletes atoms from the atom arrays
integer, intent(in) :: num
@ -533,19 +695,18 @@ module elements
!accidentally overwrite values which need to be deleted
do i = num, 1, -1
node_num = node_num - ng_node(lat_ele(sorted_index(i)))
node_atoms = node_atoms - ng_node(lat_ele(sorted_index(i)))*basisnum(lat_ele(sorted_index(i)))
if(sorted_index(i) == ele_num) then
r_node(:,:,:,sorted_index(i)) = 0.0_dp
type_ele(sorted_index(i)) =''
size_ele(sorted_index(i)) = 0
lat_ele(sorted_index(i)) = 0
sbox_ele(sorted_index(i)) = 0
tag_ele(sorted_index(i)) = 0
else
r_node(:,:,:,sorted_index(i)) = r_node(:,:,:,ele_num)
type_ele(sorted_index(i)) = type_ele(ele_num)
size_ele(sorted_index(i)) = size_ele(ele_num)
lat_ele(sorted_index(i)) = lat_ele(ele_num)
sbox_ele(sorted_index(i)) = sbox_ele(ele_num)
tag_ele(sorted_index(i)) = tag_ele(ele_num)
end if
ele_num = ele_num - 1
@ -555,12 +716,47 @@ module elements
subroutine wrap_atoms
!This subroutine wraps atoms back into the simulation cell if they have exited for any reason
integer :: i
do i = 1, atom_num
call apply_periodic(r_atom(:,i))
end do
end subroutine wrap_atoms
subroutine wrap_elements
integer :: i, inod, ibasis, j, node_in_bd(3,max_ng_node)
real(kind =dp) :: box_len(3)
do j = 1, 3
box_len(j) = box_bd(2*j) - box_bd(2*j-1)
end do
print *, box_bd
do i = 1, ele_num
node_in_bd = 0
do inod = 1, ng_node(lat_ele(i))
do ibasis = 1, basisnum(lat_ele(i))
do j = 1, 3
if(r_node(j,ibasis,inod,i) < box_bd(2*j-1)) then
node_in_bd(j,inod) = 1
else if(r_node(j,ibasis,inod,i) > box_bd(2*j)) then
node_in_bd(j,inod) = -1
end if
end do
end do
end do
do j = 1, 3
if(all(node_in_bd(j,:) == 1)) then
r_node(j,:,:,i) = r_node(j,:,:,i) + box_len(j)
else if(all(node_in_bd(j,:) == -1)) then
r_node(j,:,:,i) = r_node(j,:,:,i) - box_len(j)
end if
end do
end do
end subroutine wrap_elements
subroutine def_new_box
!This subroutine calculates new box boundaries based on minimum and maximum nodal/atomic positions
integer :: i, j, inod, ibasis
@ -613,6 +809,9 @@ do i = 1, atom_num
else if(trim(adjustl(pos_string)) == '-inf') then
pos=box_bd(2*i-1)
else if(trim(adjustl(pos_string)) == 'mid') then
pos=(box_bd(2*i)+box_bd(2*i-1))/2
else if (trim(adjustl(pos_string)) == 'rand') then
call random_number(rand)
pos = (box_bd(2*i)-box_bd(2*i-1))*rand + box_bd(2*i-1)
@ -636,7 +835,6 @@ do i = 1, atom_num
end do
end if
read(cone, *) face
if ((face < 1).or.(face > 6)) stop "Current face number must be 1,2,3,4,5,6. Please check documentation"
!Now get the position
call offset_pos(ele, face, rand_ele_pos)
@ -659,6 +857,15 @@ do i = 1, atom_num
end if
pos = box_bd(2*i) - pos
else if ((index(pos_string,'-') > 0).and.(index(pos_string,'mid')>0)) then
!Now extract the number we are reducing from midinity
if(index(pos_string,'mid') < index(pos_string,'-')) then
read(pos_string(index(pos_string,'-')+1:), *, iostat=iospara) pos
else
read(pos_string(1:index(pos_string,'-')-1), *, iostat=iospara) pos
end if
pos = (box_bd(2*i)+box_bd(2*i-1))/2.0_dp - pos
else if ((index(pos_string,'+') > 0).and.(index(pos_string,'inf')>0)) then
!Now extract the number we are reducing from infinity
if(index(pos_string,'inf') < index(pos_string,'+')) then
@ -668,6 +875,15 @@ do i = 1, atom_num
end if
pos = box_bd(2*i-1) + pos
else if ((index(pos_string,'+') > 0).and.(index(pos_string,'mid')>0)) then
!Now extract the number we are reducing from midinity
if(index(pos_string,'mid') < index(pos_string,'+')) then
read(pos_string(index(pos_string,'+')+1:), *, iostat=iospara) pos
else
read(pos_string(1:index(pos_string,'+')-1), *, iostat=iospara) pos
end if
pos = (box_bd(2*i)+box_bd(2*i-1))/2.0_dp + pos
else if ((index(pos_string,'*') > 0).and.(index(pos_string,'inf')>0)) then
!Now extract the number we are reducing from infinity
if(index(pos_string,'inf') < index(pos_string,'*')) then
@ -721,11 +937,11 @@ do i = 1, atom_num
case('fcc')
!First we have to extract the element lattice parameter
call matrix_inverse(sub_box_ori(:,:,sbox_ele(ie)),3,ori_inv)
call matrix_inverse(box_ori(:,:),3,ori_inv)
r_cubic_node = r_node(:,1,:,ie)
r_cubic_node = matmul(fcc_inv,matmul(ori_inv,r_cubic_node))
lp = (maxval(r_cubic_node(1,:))-minval(r_cubic_node(1,:)))/(esize-1)
pos = matmul(sub_box_ori(:,:,sbox_ele(ie)),matmul(fcc_mat,pos))*lp
pos = matmul(box_ori,matmul(fcc_mat,pos))*lp
pos = pos + r_node(:,1, 1, ie)
case default
@ -830,14 +1046,71 @@ do i = 1, atom_num
end subroutine
subroutine alloc_vel_arrays(n,m)
!This subroutine used to provide initial allocation for the atom and element data arrays
integer, intent(in) :: n,m !n-size of element arrays, m-size of atom arrays
integer :: allostat
!Allocate element arrays
if (n > 0) then
if (allocated(vel_node)) then
deallocate(vel_node)
end if
allocate(vel_node(3,max_basisnum,max_ng_node,n), stat=allostat)
if(allostat > 0) then
print *, "Error allocating element data arrays in mode_metric because of:", allostat
stop
end if
end if
if (m > 0) then
if (allocated(vel_atom)) then
deallocate(vel_atom)
end if
allocate(vel_atom(3,m), stat=allostat)
if(allostat > 0) then
print *, "Error allocating atom data arrays in mode_metric because of:", allostat
stop
end if
end if
end subroutine alloc_vel_arrays
subroutine add_atom_data(ia, eng, force, virial)
!Function which sets the atom data arrays
integer, intent(in) :: ia
real(kind=dp), intent(in) :: eng, force(3), virial(6)
real(kind=dp), intent(in) :: eng, force(:), virial(:)
integer :: size_atom_array
real(kind=dp), allocatable :: tmp_eng(:), tmp_force(:,:), tmp_virial(:,:)
size_atom_array=size(tag_atom)
if(ia > atom_num) then
stop "ia in add_atom_dat shouldn't be larger than atom_num"
else if(ia > size(energy_atom)) then
allocate(tmp_eng(size(energy_atom)+1024))
allocate(tmp_force(3, size(energy_atom)+1024))
allocate(tmp_virial(6, size(energy_atom)+1024))
tmp_eng=0.0_dp
tmp_eng(1:size(energy_atom)) = energy_atom
call move_alloc(tmp_eng, energy_atom)
tmp_force=0.0_dp
tmp_force(:, 1:size(force_atom, 2)) = force_atom
call move_alloc(tmp_force, force_atom)
tmp_virial=0.0_dp
tmp_virial(:, 1:size(virial_atom,2)) = virial_atom
call move_alloc(tmp_virial, virial_atom)
end if
energy_atom(ia) = eng
force_atom(:,ia) = force(:)
virial_atom(:,ia) = virial(:)
vflag = .true.
return
end subroutine add_atom_data
@ -848,10 +1121,12 @@ do i = 1, atom_num
real(kind=dp), intent(in) :: eng(max_basisnum, max_ng_node), &
force(3,max_basisnum, max_ng_node), &
virial(6,max_basisnum,max_ng_node)
integer :: inod
vflag = .true.
energy_node(:,:,ie) = eng
force_node(:,:,:,ie) = force
virial_node(:,:,:,ie) = virial
return
end subroutine add_element_data
@ -862,4 +1137,27 @@ do i = 1, atom_num
node_num = 0
end subroutine reset_data
function ele_in_bounds(bd, etype, esize, lat_type, r_in )
real(kind=dp), intent(in) :: bd(6), r_in(3, max_basisnum, max_ng_node)
integer, intent(in) :: lat_type, esize
character(len=*), intent(in) :: etype
integer :: i
real(kind=dp) :: rinterp(3, max_basisnum*max_esize**3)
integer :: tinterp(max_basisnum*max_esize**3)
logical :: ele_in_bounds
ele_in_bounds=.false.
call interpolate_atoms(etype, esize, lat_type, r_in, tinterp, rinterp)
do i=1, esize**3
if(in_block_bd(rinterp(:,i), bd))then
ele_in_bounds = .true.
exit
end if
end do
return
end function ele_in_bounds
end module elements

@ -168,11 +168,11 @@ END FUNCTION StrDnCase
do i =1 ,3
!Check upper bound
if(v(i) > (box_bd(2*i)+10.0_dp**(-10)) ) then
if(v(i) > (box_bd(2*i))) then
in_block_bd =.false.
exit
!Check lower bound
else if (v(i) < (box_bd(2*i-1)-10.0_dp**(-10))) then
else if (v(i) < (box_bd(2*i-1))+1d-6) then
in_block_bd = .false.
exit
end if
@ -254,6 +254,19 @@ END FUNCTION StrDnCase
return
end function is_equal
function mass_is_equal(A, B)
!This function checks if too numbers are equal within a tolerance
real(kind=dp), intent(in) :: A, B
logical :: mass_is_equal
if((A>(B - 10.0_dp**(-2))).and.(A < (B+10.0_dp**(-2)))) then
mass_is_equal = .true.
else
mass_is_equal = .false.
end if
return
end function mass_is_equal
pure function unitvec(n,vec)
integer, intent(in) :: n
real(kind=dp), intent(in) :: vec(n)

File diff suppressed because it is too large Load Diff

@ -38,9 +38,11 @@ program main
!Call initialization functions
call lattice_init
call box_init
call random_seed
call init_random_seed
force_overwrite=.false.
norefine=.false.
wrap_flag = .false.
all_new = .false.
end_mode_arg = 0
@ -62,10 +64,15 @@ program main
case('-wrap')
wrap_flag=.true.
case('-norefine')
norefine=.true.
case('-set_cac')
call set_cac(i)
case('-set_types')
call set_types(i)
case('-all_new')
all_new=.true.
end select
end do
!Determine if a mode is being used and what it is. The first argument has to be the mode
@ -106,14 +113,17 @@ program main
end do
!If wrap flag was passed then call the wrap atoms command
if(wrap_flag) call wrap_atoms
if(wrap_flag) then
call wrap_atoms
call wrap_elements
end if
!If we called the boundary command then we adjust the box bounds
if(bound_called) call def_new_box
!Check to make sure a file was passed to be written out and then write out
! Before building do a check on the file
if ((trim(adjustl(mode)) /= "--metric").and.(trim(adjustl(mode)) /= "--calc"))then
if ((trim(adjustl(mode)) /= "--metric").and.(trim(adjustl(mode)) /= "--calc").and.(trim(adjustl(mode)) /= "--da"))then
if ((outfilenum == 0)) then
argument = 'none'
call get_out_file(argument)
@ -121,4 +131,5 @@ program main
call write_out
end if
return
end program main

@ -25,6 +25,9 @@ module mode_calc
case('tot_virial')
allocate(calculated(6))
call calc_tot_virial
case('tot_energy')
allocate(calculated(1))
call calc_tot_energy
case default
print *, trim(adjustl(calc_opt)), " is not accepted as a calc option in mode_calc"
stop 3
@ -67,23 +70,19 @@ module mode_calc
calculated = 0
do i = 1, atom_num
do j = 1, 6
calculated(j) = calculated(j) + virial_atom(j, i)
calculated(j) = calculated(j) - virial_atom(j, i)
end do
end do
!Sum the nodal virials
do i = 1, ele_num
avg_virial(:) = 0
do inod = 1, ng_node(lat_ele(i))
do ibasis = 1, basisnum(lat_ele(i))
do j = 1,6
avg_virial(j) = avg_virial(j) + virial_node(j,ibasis,inod,i)/(basisnum(lat_ele(i))*ng_node(lat_ele(i)))
calculated(j) = calculated(j) - virial_node(j,ibasis,inod,i)*(size_ele(i)**3)/ng_node(lat_ele(i))
end do
end do
end do
end do
!Now add the total virial from the element
calculated = calculated + avg_virial*(esize**3.0_dp)
end do
!Now calculate the total box virial and convert to GPa
@ -91,5 +90,26 @@ module mode_calc
print *, "Total virial is calculated as : (v11, v22, v33, v32, v31, v21)"
print *, calculated
end subroutine
end subroutine calc_tot_virial
subroutine calc_tot_energy
integer :: i, inod, ibasis, j
calculated=0
!Sum atom energies
do i = 1, atom_num
calculated(1) = calculated(1) + energy_atom(i)
end do
!Sum element energies
do i =1, ele_num
do inod=1, ng_node(lat_ele(i))
do ibasis=1, basisnum(lat_ele(i))
calculated(1) = calculated(1) + energy_node(ibasis, inod, i)*(size_ele(i)**3)/ng_node(lat_ele(i))
end do
end do
end do
print *, 'Total energy in eV is:'
print *, calculated(1)
end subroutine calc_tot_energy
end module mode_calc

@ -12,10 +12,10 @@ module mode_create
character(len=100) :: name, element_type
real(kind = dp) :: lattice_parameter, orient(3,3), cell_mat(3,8), box_len(3), basis(3,3), origin(3), maxlen(3), &
orient_inv(3,3), box_vert(3,8), maxbd(3), lattice_space(3), duplicate(3)
orient_inv(3,3), box_vert(3,8), maxbd(3), lattice_space(3), duplicate(3), basis_pos(3,10)
integer :: esize, ix, iy, iz, box_lat_vert(3,8), lat_ele_num, lat_atom_num, bd_in_lat(6), &
basis_pos(3,10), esize_nums, esize_index(10)
logical :: dup_flag, dim_flag, efill
esize_nums, esize_index(10)
logical :: dup_flag, dim_flag, efill, crossb(3)
real(kind=dp), allocatable :: r_lat(:,:,:), r_atom_lat(:,:)
integer, allocatable :: elat(:)
@ -67,7 +67,7 @@ module mode_create
end do
!Now get the rotated box vertex positions in lattice space. Should be integer units and get the new maxlen
select case(trim(adjustl(element_type)))
case('fcc')
case('fcc', '20fcc')
box_lat_vert = int(matmul(fcc_inv, matmul(orient_inv, box_vert)))+1
maxbd = maxval(matmul(orient,matmul(fcc_mat,box_lat_vert)),2)
case('bcc')
@ -79,10 +79,10 @@ module mode_create
do i = 1, 3
box_bd(2*i) = maxval(box_vert(i,:)) - 0.25_dp*lattice_space(i)
box_bd(2*i-1) = origin(i)-0.25_dp*lattice_space(i)
box_len(i) = box_bd(2*i) - box_bd(2*i-1)
end do
else if(dim_flag) then
!As a note everything is defined so that the lattice parameter is multiplied in at the end
!so we have to divide all the real Angstroms units by the lattice parameter
@ -93,7 +93,7 @@ module mode_create
end do
!Now get the rotated box vertex positions in lattice space. Should be integer units
select case(trim(adjustl(element_type)))
case('fcc')
case('fcc', '20fcc')
box_lat_vert = int(matmul(fcc_inv, matmul(orient_inv, box_vert)))+1
case('bcc')
box_lat_vert = int(matmul(bcc_inv, matmul(orient_inv, box_vert)))+1
@ -122,7 +122,7 @@ module mode_create
box_bd(2*i) = maxval(r_node_temp(i,:,:))+10.0_dp**(-6.0_dp)
box_bd(2*i-1) = minval(r_node_temp(i,:,:)) - 10.0_dp**(-6.0_dp)
end do
call add_element(0,element_type, esize, 1, 1, r_node_temp)
call add_element(0,element_type, esize, 1, r_node_temp)
end if
!If we passed the dup_flag or dim_flag then we have to convert the lattice points and add them to the atom/element arrays
@ -131,9 +131,11 @@ module mode_create
!Call the build function with the correct transformation matrix
select case(trim(adjustl(element_type)))
case('fcc')
call build_with_rhomb(box_lat_vert, fcc_mat)
call build_with_rhomb(box_lat_vert, fcc_mat, 8, fcc_inv)
case('bcc')
call build_with_rhomb(box_lat_vert, bcc_mat)
call build_with_rhomb(box_lat_vert, bcc_mat, 8, bcc_inv)
case('20fcc')
call build_with_rhomb(box_lat_vert, fcc_mat, 20, fcc_inv)
case default
print *, "Element type ", trim(adjustl(element_type)), " not accepted in mode create, please specify a supported ",&
"element type"
@ -150,7 +152,7 @@ module mode_create
if(lat_atom_num > 0) then
do i = 1, lat_atom_num
do ibasis = 1, basisnum(1)
call add_atom(0,basis_type(ibasis, 1), 1, (r_atom_lat(:,i)*lattice_parameter)+basis_pos(:,ibasis))
call add_atom(0,basis_type(ibasis, 1), (r_atom_lat(:,i)*lattice_parameter)+basis_pos(:,ibasis))
end do
end do
deallocate(r_atom_lat)
@ -164,16 +166,16 @@ module mode_create
end do
end do
call add_element(0,element_type, elat(i), 1, 1, r_node_temp)
call add_element(0,element_type, elat(i), 1, r_node_temp)
end do
end if
end if
!The last thing we do is setup the sub_box_boundaries
call alloc_sub_box(1)
sub_box_num = 1
sub_box_ori(:,:,1) = orient
sub_box_bd(:,1) = box_bd
!If any elements are fully outside the box then wrap them back in
if (any(crossb)) then
call wrap_elements
end if
box_ori = orient
end subroutine create
!This subroutine parses the command and pulls out information needed for mode_create
subroutine parse_command(arg_pos)
@ -181,9 +183,10 @@ module mode_create
integer, intent(out) :: arg_pos
integer :: ori_pos, i, j, arglen, stat
character(len=100) :: textholder
character(len=20) :: orient_string
character(len=100) :: orient_string
character(len=2) :: btype
logical :: isortho, isrighthanded
logical :: isortho, isrighthanded, bool
real(kind=dp) :: mass
!Pull out all required positional arguments
@ -201,6 +204,7 @@ module mode_create
call get_command_argument(5, textholder, arglen)
if(arglen==0) STOP "Esize missing in mode create"
read(textholder, *, iostat=stat) esize
max_esize = esize
if(stat > 0) STOP "Error reading esize"
arg_pos = 6
@ -248,6 +252,12 @@ module mode_create
read(textholder, *) origin(i)
arg_pos = arg_pos + 1
end do
case('crossb')
do i = 1, 3
call get_command_argument(arg_pos, textholder)
read(textholder, *) crossb(i)
arg_pos = arg_pos + 1
end do
case('basis')
call get_command_argument(arg_pos, textholder)
read(textholder, *) basisnum(1)
@ -256,7 +266,8 @@ module mode_create
do i = 1, max_basisnum
call get_command_argument(arg_pos, btype)
arg_pos = arg_pos+1
call add_atom_type(btype, basis_type(i,1))
call atommass(btype, mass)
call add_atom_type(mass, basis_type(i,1))
do j = 1, 3
call get_command_argument(arg_pos, textholder)
read(textholder, *) basis_pos(j,i)
@ -273,14 +284,16 @@ module mode_create
end select
end do
!Calculate the lattice periodicity length in lattice units
do i = 1, 3
lattice_space(i) = norm2(orient(i,:))
end do
!Now normalize the orientation matrix
orient = matrix_normal(orient,3)
!Check special periodicity relations
select case(trim(adjustl(element_type)))
case('fcc')
case('fcc', '20fcc')
do i = 1,3
!Check if one of the directions is 110
if ((is_equal(abs(orient(i,1)), abs(orient(i,2))).and.(is_equal(orient(i,3),0.0_dp))).or.&
@ -307,8 +320,6 @@ module mode_create
end if
end do
end select
!Now normalize the orientation matrix
orient = matrix_normal(orient,3)
!Now check these to make sure they are right handed and orthogonal
call check_right_ortho(orient, isortho, isrighthanded)
if (.not.isortho) then
@ -325,25 +336,28 @@ module mode_create
if (basisnum(1) == 0) then
max_basisnum = 1
basisnum(1) = 1
call add_atom_type(name, basis_type(1,1)) !If basis command not defined then we use name as the atom_name
call atommass(name, mass)
call add_atom_type(mass, basis_type(1,1)) !If basis command not defined then we use name as the atom_name
basis_pos(:,1) = 0.0_dp
end if
!
end subroutine
subroutine build_with_rhomb(box_in_lat, transform_matrix)
subroutine build_with_rhomb(box_in_lat, transform_matrix, nn, transform_inverse)
!This subroutine returns all the lattice points in the box in r_lat
!Inputs
integer, dimension(3,8), intent(in) :: box_in_lat !The box vertices transformed to lattice space
real(kind=dp), dimension(3,3), intent(in) :: transform_matrix !The transformation matrix from lattice_space to real space
real(kind=dp), dimension(3,3), intent(in) :: transform_inverse !The inverse transform
integer, intent(in) :: nn
!Internal variables
integer :: i, inod, bd_in_lat(6), bd_in_array(6), ix, iy, iz, numlatpoints, ele(3,8), rzero(3), efill_size, &
vlat(3), temp_lat(3,8), m, n, o, j, k, nump_ele, efill_temp_lat(3,8), filzero(3), bd_ele_lat(6),&
efill_ele(3,8), ebd(6)
real(kind=dp) :: v(3), temp_nodes(3,1,8), r(3), centroid_bd(6)
integer :: i, inod, bd_in_lat(6), bd_in_array(6), ix, iy, iz, numlatpoints, ele(3,nn), rzero(3), efill_size, &
vlat(3), temp_lat(3,nn), m, n, o, j, k, nump_ele, efill_temp_lat(3,nn), filzero(3), &
bd_ele_lat(6), efill_ele(3,nn), ebd(6), shift_vec(3), type_interp(max_basisnum*max_esize**3)
real(kind=dp) :: v(3), temp_nodes(3,1,nn), r(3), centroid_bd(6), vreal(3), r_interp(3, max_basisnum*max_esize**3)
logical, allocatable :: lat_points(:,:,:)
logical :: node_in_bd(8), add, lat_points_ele(esize,esize,esize), intersect_bd(3)
logical :: node_in_bd(nn), add, lat_points_ele(esize,esize,esize), intersect_bd(3)
!Do some value initialization
max_esize = esize
@ -360,6 +374,8 @@ module mode_create
numlatpoints = numlatpoints*(bd_in_lat(2*i)-bd_in_lat(2*i-1))
end do
if(numlatpoints < 0) stop "number of lattice points is negative, this can occur if the model is too big"
!Allocate the correct lat variable
select case(esize)
!Atomistics
@ -393,7 +409,12 @@ module mode_create
!If we are working with elements we have to use more complex code
!Initialize finite element
ele(:,:) = (esize-1) * cubic_cell(:,:)
select case(element_type)
case('fcc','bcc')
ele(:,:) = (esize-1) * cubic_cell(:,:)
case('20fcc')
ele(:,:) = (esize-1)*cube20
end select
!Make a 3 dimensional array of lattice points. This array is indexed by the integer lattice position.
!A value of true means that the coordinate is a lattice point which is within the box_bd
@ -414,6 +435,7 @@ module mode_create
end do
end do
!Now we redefine bd_in_lat The first 3 indices contains limits for the lat_points array
bd_in_array(1) = bd_in_lat(2) - bd_in_lat(1) + 10
bd_in_array(2) = bd_in_lat(4) - bd_in_lat(3) + 10
@ -423,7 +445,7 @@ module mode_create
do iy = 1, bd_in_array(2)
do ix = 1, bd_in_array(1)
node_in_bd(:) = .false.
do inod = 1, 8
do inod = 1, nn
vlat = ele(:,inod) + (/ ix, iy, iz /)
!Check to see if the node resides at a position containing a lattice point within the box
@ -445,16 +467,22 @@ module mode_create
!Now build the finite element region
lat_ele_num = 0
lat_atom_num = 0
allocate(r_lat(3,8,numlatpoints/esize), elat(numlatpoints/esize))
allocate(r_lat(3,nn,numlatpoints/esize), elat(numlatpoints/esize))
select case(element_type)
case('fcc','bcc')
ele(:,:) = (esize-1) * cubic_cell(:,:)
case('20fcc')
ele(:,:) = (esize-1)*cube20
end select
ele(:,:) = (esize-1) * cubic_cell(:,:)
!Redefined the second 3 indices as the number of elements that fit in the bounds
do i = 1, 3
bd_in_array(3+i) = bd_in_array(i)/esize
end do
!Now start the element at rzero
do inod=1, 8
do inod=1, nn
ele(:,inod) = ele(:,inod) + rzero
end do
do iz = -bd_in_array(6), bd_in_array(6)
@ -463,7 +491,7 @@ module mode_create
node_in_bd(:) = .false.
temp_nodes(:,:,:) = 0.0_dp
temp_lat(:,:) = 0
do inod = 1, 8
do inod = 1, nn
vlat= ele(:,inod) + (/ ix*(esize), iy*(esize), iz*(esize) /)
!Transform point back to real space for easier checking
! v = matmul(orient, matmul(transform_matrix,v))
@ -479,6 +507,31 @@ module mode_create
!If within array boundaries check to see if it is a lattice point
else if(lat_points(vlat(1),vlat(2),vlat(3))) then
node_in_bd(inod) = .true.
else if(any(crossb)) then
vreal=0
do i = 1, 3
if(crossb(i)) then
if(temp_nodes(i,1,inod) < box_bd(2*i-1)) then
vreal(i) = temp_nodes(i,1,inod)+box_len(i)
else if(temp_nodes(i,1,inod) > box_bd(2*i)) then
vreal(i) = temp_nodes(i,1,inod)-box_len(i)
else
vreal(i) = temp_nodes(i,1,inod)
end if
else
vreal(i) = temp_nodes(i,1,inod)
end if
end do
v = matmul(transform_inverse, matmul(orient_inv, vreal))
do i = 1, 3
vlat(i) = nint(v(i) - bd_in_lat(2*i-1)+5)
end do
if(any(vlat > shape(lat_points)).or.any(vlat < 1)) then
continue
!If within array boundaries check to see if it is a lattice point
else if(lat_points(vlat(1),vlat(2),vlat(3))) then
node_in_bd(inod) = .true.
end if
end if
end do
@ -488,14 +541,50 @@ module mode_create
lat_ele_num = lat_ele_num+1
r_lat(:,:,lat_ele_num) = temp_nodes(:,1,:)
elat(lat_ele_num) = esize
!Now set all the lattice points contained within an element to false
do o = minval(temp_lat(3,:)), maxval(temp_lat(3,:))
do n = minval(temp_lat(2,:)), maxval(temp_lat(2,:))
do m = minval(temp_lat(1,:)), maxval(temp_lat(1,:))
lat_points(m,n,o) = .false.
if(any(crossb)) then
call interpolate_atoms('fcc', esize, 0, temp_nodes, type_interp, r_interp)
j= 0
do o = minval(temp_lat(3,:)), maxval(temp_lat(3,:))
do n = minval(temp_lat(2,:)), maxval(temp_lat(2,:))
do m = minval(temp_lat(1,:)), maxval(temp_lat(1,:))
j=j+1
do i = 1, 3
if(crossb(i)) then
if(r_interp(i,j) < box_bd(2*i-1)) then
vreal(i) = r_interp(i,j)+box_len(i)
else if(r_interp(i,j) > box_bd(2*i)) then
vreal(i) = r_interp(i,j)-box_len(i)
else
vreal(i) = r_interp(i,j)
end if
else
vreal(i) = r_interp(i,j)
end if
end do
v = matmul(transform_inverse, matmul(orient_inv, vreal))
do i = 1, 3
vlat(i) = nint(v(i) - bd_in_lat(2*i-1)+5)
end do
if(lat_points(vlat(1), vlat(2), vlat(3))) then
lat_points(vlat(1), vlat(2), vlat(3)) = .false.
else
print *, "Lat points should be true not false"
stop 2
end if
end do
end do
end do
end do
else
!Now set all the lattice points contained within an element to false
do o = minval(temp_lat(3,:)), maxval(temp_lat(3,:))
do n = minval(temp_lat(2,:)), maxval(temp_lat(2,:))
do m = minval(temp_lat(1,:)), maxval(temp_lat(1,:))
lat_points(m,n,o) = .false.
end do
end do
end do
end if
!If any nodes are in the boundary and we want to efill then run the efill code
else if(any(node_in_bd).and.efill) then
@ -515,8 +604,8 @@ module mode_create
end if
end do
lat_points_ele(1:(bd_ele_lat(2)-bd_ele_lat(1)),1:(bd_ele_lat(4)-bd_ele_lat(3)),&
1:(bd_ele_lat(6)-bd_ele_lat(5)))= lat_points(bd_ele_lat(1):bd_ele_lat(2), &
lat_points_ele(1:(bd_ele_lat(2)-bd_ele_lat(1)+1),1:(bd_ele_lat(4)-bd_ele_lat(3)+1),&
1:(bd_ele_lat(6)-bd_ele_lat(5))+1)= lat_points(bd_ele_lat(1):bd_ele_lat(2), &
bd_ele_lat(3):bd_ele_lat(4), &
bd_ele_lat(5):bd_ele_lat(6))
!Now start looping through elements and try to fit as many as you can
@ -537,7 +626,7 @@ module mode_create
ze: do k = 1, (esize-efill_size)
ye: do j = 1, (esize-efill_size)
xe: do i = 1, (esize-efill_size)
do inod = 1,8
do inod = 1,nn
vlat = efill_ele(:,inod) + (/ i, j, k /)
if (.not.lat_points_ele(vlat(1),vlat(2),vlat(3))) cycle xe
do o = 1,3

@ -0,0 +1,312 @@
module mode_da
!This mode is used to calculate the dislocation analysis algorithm for both CG and atomistic regions
use parameters
use io
use elements
use neighbors
implicit none
integer :: num_d_points
integer, allocatable :: is_slipped(:,:,:)
real(kind=dp), allocatable :: disl_line(:,:), disl_data(:)
private :: write_xyz
public
contains
subroutine da(arg_pos)
!This is the main calling subroutine for the dislocation analysis code
integer, intent(out) :: arg_pos
real(kind=dp), dimension(6) :: temp_box_bd
integer :: ppos
character(len=100) :: outfile
!Now call the dislocation analysis code for the coarse-grained elements
call parse_command(arg_pos)
call read_in(1, (/0.0_dp,0.0_dp,0.0_dp/), temp_box_bd)
!Now allocate the necessary variables
if(allocated(is_slipped)) deallocate(is_slipped)
allocate(is_slipped(max_basisnum, max_ng_node, ele_num))
if(allocated(disl_line)) deallocate(disl_line)
num_d_points=0
allocate(disl_line(3,1024))
allocate(disl_data(1024))
call cga_da
!Now create the output file num and write out to xyz format
ppos = scan(trim(infiles(1)),".", BACK= .true.)
if ( ppos > 0 ) then
outfile = 'da_'//infiles(1)(1:ppos)//'vtk'
else
outfile = 'da_'//infiles(1)//'.vtk'
end if
call write_da_vtk(outfile)
ppos = scan(trim(infiles(1)),".", BACK= .true.)
if ( ppos > 0 ) then
outfile = 'da_'//infiles(1)(1:ppos)//'xyz'
else
outfile = 'da_'//infiles(1)//'.xyz'
end if
call write_da_xyz(outfile)
return
end subroutine da
subroutine parse_command(arg_pos)
!This subroutine parses the arguments for mode command
integer, intent(out) :: arg_pos
integer :: i, arglen
character(len = 100) :: textholder
logical :: file_exists
!Read the input file
call get_command_argument(2,textholder, arglen)
if (arglen == 0) stop "Missing file for dislocation analysis"
call get_in_file(textholder)
arg_pos = 3
return
end subroutine parse_command
subroutine cga_da
integer :: i, j, k, l, ibasis, nei, close_neighbors(2,4,6), far_neighbor(4,6), minindex, minindices(2), linevec(3)
integer :: face_types(ele_num*6), face_ele(6*ele_num), diff_pair(2,6)
real(kind = dp) :: face_centroids(3, ele_num*6), r(3), rc, vnode(3, max_basisnum, 4), vnorm, &
max_node_dist, ndiff, rmax(3), rmin(3), rnorm, v1(3), v2(3), v1norm, v2norm, theta1, theta2, &
diff_mag(6), diffvec(3)
real(kind=dp), allocatable :: disl_line_temp(:,:), disl_data_temp(:)
logical :: is_edge
!Initialize variables
l = 0
max_node_dist = 0
!Now save the close and far neighbors of the nodes. This is done to attempt to figure out the character of the dislocation
!by comparing how the burgers vector is distributed over the face.
do j = 1, 6
close_neighbors(1, 1, j) = cubic_faces(4, j)
close_neighbors(2, 1, j) = cubic_faces(2, j)
far_neighbor(1,j) = cubic_faces(3,j)
close_neighbors(1, 2, j) = cubic_faces(1, j)
close_neighbors(2, 2, j) = cubic_faces(3, j)
far_neighbor(2,j) = cubic_faces(4,j)
close_neighbors(1, 3, j) = cubic_faces(2, j)
close_neighbors(2, 3, j) = cubic_faces(4, j)
far_neighbor(3,j) = cubic_faces(1,j)
close_neighbors(1, 4, j) = cubic_faces(3, j)
close_neighbors(2, 4, j) = cubic_faces(1, j)
far_neighbor(4,j) = cubic_faces(2,j)
end do
!First calculate all of the face centroids
do i = 1, ele_num
do j = 1, 6
r(:) = 0.0_dp
rmax= -Huge(1.0)
rmin= Huge(1.0)
do k = 1, 4
do ibasis = 1, basisnum(lat_ele(i))
r = r + r_node(:, ibasis, cubic_faces(k,j), i)
rmax= max(rmax, r_node(:, ibasis, cubic_faces(k,j), i))
rmin= min(rmin, r_node(:, ibasis, cubic_faces(k,j), i))
end do
end do
rnorm=norm2(rmax-rmin)
max_node_dist = max(max_node_dist, rnorm)
r = r/(basisnum(lat_ele(i))*4)
!add the face centroids, the type, and map the elements faces to the face arrays
l = l + 1
face_centroids(:, l) = r
face_types(l) = j
face_ele(l) = i
end do
end do
!Now set the cut off distance as half the distance from opposite nodes in the largest element
rc = 0.5*max_node_dist
call calc_NN(l, face_centroids(:,1:l), rc)
!Now loop overall the faces and make sure the nearest neighbor is the opposite type. If it isn't than we dscard it
is_slipped = 0
do i = 1, l
nei = nn(i)
!Skip if it's 0 or the closest face belongs to the same element
if ((nei == 0).or.(face_ele(i) == face_ele(nei))) cycle
!Check the face types, the way that the faces are laid out in the cubic_faces array face 1's opposite is 6 and
! face 2's opposite is 5 and etc
vnode = 0
if(face_types(i) == (7-face_types(nei))) then
vnorm = 0
do j = 1, 4
do ibasis = 1, basisnum(lat_ele(face_ele(i)))
!Compute the vectors between all nodes at the face.
vnode(:,ibasis,j) = r_node(:,ibasis, cubic_faces(j,face_types(i)), face_ele(i)) - &
r_node(:,ibasis, cubic_faces(j,face_types(nei)), face_ele(nei))
end do
end do
!Now calculate the maximum difference between nodes
vnorm = 0
do j = 1, 4
do k=j,4
v1=vnode(:,1,j) - vnode(:,1,k)
v1norm=norm2(v1)
if (vnorm < v1norm) then
vnorm = v1norm
diffvec= v1
end if
end do
end do
!Now calculate the difference between the largest norm and the smallest norm, if it's larger than 0.5 then mark it
!as slipped. This value probably can be converted to a variable value that depends on the current lattice parameter
!I think 0.5 works ok though.
if (vnorm>0.5_dp) then
print *, "Element number ", face_ele(i), " is dislocated along face ", face_types(i), &
" with neighbor ", face_ele(nei), " with max displacement of ", vnorm
l=0
do j = 1, 4
is_slipped(:, cubic_faces(j,face_types(i)), face_ele(i)) = 1
!This portion of the code is used to determine what the character of the dislocation most likely is
!effectively how this works is we look for the two nodes with the most similar burgers vector.
!The vector between these two nodes is close to the line direction and as a result we can probably estimate
!if it's close to edge, screw, or if it's pretty fairly mixed.
do k = j+1, 4
l=l+1
diff_mag(l) = norm2(vnode(:, 1, j)-vnode(:,1,k))
diff_pair(1,l)=cubic_faces(j, face_types(i))
diff_pair(2,l)=cubic_faces(k, face_types(i))
end do
end do
minindex = minloc(diff_mag,1)
!Now figure out if the min difference between nodes is associated with a 112 direction
is_edge = .false.
do j = 1,6
if((diff_pair(1,minindex) == oneonetwopairs(1,j)).and.(diff_pair(2,minindex)==oneonetwopairs(2,j))) then
is_edge=.true.
exit
else if((diff_pair(2,minindex)==oneonetwopairs(1,j)).and.(diff_pair(1,minindex)==oneonetwopairs(2,j)))then
is_edge=.true.
exit
end if
end do
if(is_edge) then
print *, 'Dislocation has primarily edge character'
else
print *, 'Dislocation has primarily screw character'
end if
if( i < nei) then
num_d_points=num_d_points+2
if(num_d_points > size(disl_line,2)) then
allocate(disl_line_temp(3,size(disl_line,2)+1024))
disl_line_temp=0.0_dp
disl_line_temp(:, 1:size(disl_line,2))=disl_line
call move_alloc(disl_line_temp, disl_line)
end if
if(num_d_points/2 > size(disl_data)) then
allocate(disl_data_temp(size(disl_data)+1024))
disl_data_temp=0
disl_data_temp(1:size(disl_data)) = disl_data
call move_alloc(disl_data_temp, disl_data)
end if
print *, num_d_points/2, vnorm
disl_data(num_d_points/2)=vnorm
disl_line(:,num_d_points-1) =r_node(:, 1, diff_pair(1,minindex), face_ele(i))
disl_line(:,num_d_points) =r_node(:, 1, diff_pair(2,minindex), face_ele(i))
end if
end if
end if
end do
end subroutine cga_da
subroutine write_da_vtk(outfile)
character (len=*), intent(in) :: outfile
integer :: i
open(unit=11, file=outfile, action='write', status='replace', position='rewind')
write(11, '(a)') '# vtk DataFile Version 4.0.1'
write(11, '(a)') 'Dislocation line analyzed via cacmb dislocation analysis'
write(11, '(a)') 'ASCII'
write(11, '(a)') 'DATASET UNSTRUCTURED_GRID'
write(11, *) 'POINTS', num_d_points, 'float'
!Write the points to the file
do i = 1, num_d_points
write(11, '(3f23.15)') disl_line(:, i)
end do
write(11,*) 'CELLS', num_d_points/2, num_d_points/2*3
do i=1, num_d_points, 2
write(11,'(3i16)') 2, i-1, i
end do
write(11,*) 'CELL_TYPES', num_d_points/2
do i=1, num_d_points, 2
write(11,'(i16)') 3
end do
write(11,*) 'CELL_DATA', num_d_points/2
write(11, '(a)') 'SCALARS burgers_vec, float'
write(11, '(a)') 'LOOKUP_TABLE default'
do i=1, num_d_points, 2
write(11, '(f23.15)') disl_data((i+1)/2)
end do
close(11)
end subroutine write_da_vtk
subroutine write_da_xyz(outfile)
!This subroutine write the element positions to a .xyz file and marks whether they are slipped or not
character(len=*), intent(in) :: outfile
integer :: i, ibasis, inod, outn
open(unit=11, file=outfile, action='write', status='replace', position='rewind')
!Write number of node_atoms
write(11, '(i16)') node_atoms
!Write comment
write(11, '(a)') "is_slipped x y z"
!Write nodal positions
outn = 0
do i = 1, ele_num
do inod = 1, ng_node(lat_ele(i))
do ibasis = 1, basisnum(lat_ele(i))
write(11, '(1i16, 3f23.15)') is_slipped(ibasis,inod,i), r_node(:,ibasis,inod,i)
outn = outn + 1
end do
end do
end do
if(outn /= node_atoms) then
print *, "outn", outn, " doesn't equal node_atoms ", node_atoms
end if
close(11)
end subroutine write_da_xyz
end module mode_da

@ -6,18 +6,23 @@ module mode_merge
use io
use subroutines
use elements
use neighbors
implicit none
character(len=4) :: dim
integer :: in_num, new_starts(2)
real(kind=dp) :: shift_vec(3)
logical :: shift_flag
real(kind=dp) :: shift_vec(3), replace_vec(3)
character(len=100) :: replace_str(3)
logical :: shift_flag, replace_flag
real(kind=dp), private, save :: rc_off
public
contains
subroutine merge(arg_pos)
integer, intent(out) :: arg_pos
integer :: i
integer :: i, j
real(kind=dp) :: displace(3), temp_box_bd(6)
print *, '-----------------------Mode Merge---------------------------'
@ -55,7 +60,27 @@ module mode_merge
call read_in(i, displace, temp_box_bd)
end if
if(shift_flag) call shift(new_starts, i)
if(replace_flag.and.(i>1)) then
!Parse the replace vector
do j = 1, 3
call parse_pos(j, replace_str(j), replace_vec(j))
end do
call replace(new_starts, temp_box_bd)
end if
end do
!Now reset tags
do i = 1, atom_num
tag_atom(i) = i
end do
do i = 1, ele_num
tag_ele(i) = i
end do
return
@ -113,6 +138,17 @@ module mode_merge
if (arglen==0) stop "Missing vector component for shift command"
read(textholder, *) shift_vec(i)
end do
case('replace')
replace_flag = .true.
do i = 1,3
arg_pos = arg_pos + 1
call get_command_argument(arg_pos, replace_str(i), arglen)
if (arglen==0) stop "Missing vector component for shift command"
end do
arg_pos = arg_pos+1
call get_command_argument(arg_pos, textholder, arglen)
read(textholder,*) rc_off
case default
!If it isn't an available option to mode merge then we just exit
exit
@ -152,7 +188,7 @@ module mode_merge
end do
!If we don't include the wrap command then we have to increase the size of the box
if(.not.(wrap_flag)) then
if(.not.(wrap_flag).and..not.(trim(adjustl(dim))=='none')) then
do i = 1,3
if (alldims(i:i) /= trim(adjustl(dim))) then
if (current_shift(i) < -lim_zero) then
@ -167,4 +203,147 @@ module mode_merge
end if
end subroutine shift
subroutine replace(array_start, rbox_bd)
integer, intent(in) :: array_start(2)
real(kind = dp), intent(in) :: rbox_bd(6)
integer :: ibasis, inod, del_num, del_index(atom_num), nump_ele, interp_start
integer :: j, ie, type_interp(max_basisnum*max_esize**3), add_atom_num, orig_atom_num, m, n, o, esize, &
ele(3,8), new_ele_num, vlat(3), added_points
real(kind=dp) :: r_interp(3, max_basisnum*max_esize**3), rfill(3,max_basisnum,max_ng_node), ravg(3), ratom(3,max_basisnum)
logical :: in_bd, lat_points(max_esize, max_esize, max_esize)
real(kind=dp) :: del_bd(6)
integer :: i, c(3), ci, cj, ck, num_nei, nei, delete_num
!These are the variables containing the cell list information
integer, dimension(3) :: cell_num
integer, allocatable :: num_in_cell(:,:,:), which_cell(:,:)
integer, allocatable :: cell_list(:,:,:,:)
!First apply the replace vec to all new nodes and elements
do i = array_start(1), atom_num
r_atom(:,i) = r_atom(:, i) + replace_vec
end do
do i = array_start(2), ele_num
do inod = 1, ng_node(lat_ele(i))
do ibasis=1, basisnum(lat_ele(i))
r_node(:, ibasis,inod, i) = r_node(:, ibasis,inod, i) + replace_vec
end do
end do
end do
!Calculate new boundary
do i = 1, 6
del_bd(i) = rbox_bd(i) + replace_vec((i-1)/2 + 1)
end do
del_num = 0
del_index=0
interp_start = atom_num +1
!Now loop over all old elements,
do ie = 1, array_start(2)-1
!If any element points are within the boundary then we run the refine code
if(ele_in_bounds(del_bd, type_ele(ie), size_ele(ie), lat_ele(ie), r_node(:,:,:,ie))) then
added_points=0
del_num = del_num + 1
del_index(del_num) = ie
!Find all possible elements that we can make while making sure they aren't in the group
lat_points(1:size_ele(ie),1:size_ele(ie),1:size_ele(ie)) = .true.
!Now add the leftover lattice points as atoms, only if they aren't within the new boundaries
do o = 1, size_ele(ie)
do n = 1, size_ele(ie)
do m = 1, size_ele(ie)
if(lat_points(m,n,o)) then
call get_interp_pos(m,n,o, ie, ratom(:,:))
do ibasis = 1, basisnum(lat_ele(ie))
call apply_periodic(ratom(:,ibasis))
added_points=added_points + 1
call add_atom(0, basis_type(ibasis,lat_ele(ie)), ratom(:,ibasis))
end do
end if
end do
end do
end do
if (added_points /= (size_ele(ie)**3)) then
print *, "Element ", ie, " is refined incorrectly in refinefill"
end if
end if
end do
!Once all atoms are added we delete all of the elements
call delete_elements(del_num, del_index)
!Now delete overlapping atoms
allocate(which_cell(3,atom_num))
!First pass the atom list and atom num to the algorithm which builds the cell list
print *, rc_off
call build_cell_list(atom_num, r_atom, 4*rc_off, cell_num, num_in_cell, cell_list, which_cell)
!Now loop over every atom and figure out if it has neighbors within the rc_off
del_num = 0
atom_loop: do i = 1, atom_num
!c is the position of the cell that the atom belongs to
c = which_cell(:,i)
!Check to make sure it hasn't already been deleted
if(all(c /= 0)) then
!Now loop over all neighboring cells
do ci = -1, 1, 1
do cj = -1, 1, 1
do ck = -1, 1, 1
if (any((c + (/ ck, cj, ci /)) == 0)) cycle
if( (c(1) + ck > cell_num(1)).or.(c(2) + cj > cell_num(2)).or. &
(c(3) + ci > cell_num(3))) cycle
do num_nei = 1, num_in_cell(c(1) + ck, c(2) + cj, c(3) + ci)
nei = cell_list(num_nei,c(1) + ck, c(2) + cj, c(3) + ci)
!Check to make sure the atom isn't the same index as the atom we are checking
!and that the neighbor hasn't already been deleted
if((nei /= i).and.(nei/= 0)) then
!Now check to see if it is in the cutoff radius, if it is add it to the delete code
if (norm2(r_atom(:,nei)-r_atom(:,i)) < rc_off) then
del_num = del_num + 1
!Make sure to delete the older value
if( (i < array_start(1)).or.(i > interp_start)) then
del_index(del_num) = i
which_cell(:,i) = 0
cycle atom_loop
else
del_index(del_num) = nei
which_cell(:,nei) = 0
cell_list(num_nei,c(1) + ck, c(2) + cj, c(3) + ci) = 0
end if
end if
end if
end do
end do
end do
end do
end if
end do atom_loop
print *, "Replace command deletes ", del_num, " atoms"
!Now delete all the atoms
call delete_atoms(del_num, del_index(1:del_num))
return
end subroutine replace
end module mode_merge

@ -10,7 +10,7 @@ module mode_metric
integer :: nfiles
character(len=100) :: metric_type
real(kind=dp) :: rc_off
real(kind=dp) :: rc_off, old_box_len(3)
!Save reference positions
integer :: np, npreal, nmet
@ -50,23 +50,31 @@ module mode_metric
end select
!Now set the reference positions
print *, "Combining positions"
call convert_positions(r_zero, npreal)
!Now calculate the neighbor list for the reference configuration
call calc_neighbor(5.0_dp, r_zero, np)
print *, "Getting initial neighbor list"
call calc_neighbor(rc_off, r_zero, np)
!Save box lengths for applying periodic boundaries
do i=1,3
old_box_len(i) = box_bd(2*i) - box_bd(2*i-1)
end do
!Reset element and box
call reset_data
call reset_box
!Now loop over new files
do i = 2, nfiles
call read_in(i, (/ 0.0_dp, 0.0_dp, 0.0_dp /), temp_box_bd)
call convert_positions(r_curr, np_temp)
if (npreal /= np_temp) then
print *, "Error in mode_metric where number of points in ", i, "th file is ", np_temp, " and number of points in" &
// "reference file is", npreal
end if
print *, "Calculating metric for file number ", i
call calc_metric
!Now create the output file num and write out to xyz format
ppos = scan(trim(infiles(i)),".", BACK= .true.)
@ -124,8 +132,11 @@ module mode_metric
!This subroutine calculates the continuum metric that we require
integer :: i, j, k, nei, ip, jp
real(kind=dp) :: def_grad(3,3), omega(3,3), eta(3,3), rij(3), eta_inv(3,3), ftf(3,3), &
U(3,3), R(3,3), Rskew(3,3), oldrij(3)
U(3,3), R(3,3), Rskew(3,3), oldrij(3), box_len(3)
do i = 1, 3
box_len(i) = box_bd(2*i) - box_bd(2*i-1)
end do
!Loop over all points
do ip = 1, np
eta(:,:) = 0.0_dp
@ -134,8 +145,17 @@ module mode_metric
do jp = 1, nei_num(ip)
!Calculate the neighbor vec in current configuration
nei = nei_list(jp, ip)
rij = r_curr(:,nei) - r_curr(:,ip)
oldrij = r_zero(:,nei) - r_zero(:,ip)
rij = r_curr(:,nei) - r_curr(:,ip) +periodvec(:,jp,ip)*box_len
if (norm2(rij) > 5*rc_off) then
do j = 1, 3
if (r_curr(j,nei) > r_curr(j,ip)) then
rij(j) = rij(j) - box_len(j)
else if(r_curr(j,nei) < r_curr(j,ip)) then
rij(j) = rij(j) + box_len(j)
end if
end do
end if
oldrij = r_zero(:,nei) - r_zero(:,ip) + periodvec(:,jp,ip)*old_box_len
!Calculate eta and omega
do i = 1,3
@ -190,9 +210,10 @@ module mode_metric
integer :: i, inod, ibasis
npoints=0
rout = -huge(1.0_dp)
if(atom_num > 0) then
do i = 1, atom_num
call apply_periodic(r_atom(:,i))
rout(:,tag_atom(i)) = r_atom(:,i)
npoints = npoints + 1
end do
@ -202,8 +223,11 @@ module mode_metric
do i = 1, ele_num
do inod = 1, ng_node(lat_ele(i))
do ibasis = 1, basisnum(lat_ele(i))
call apply_periodic(r_node(:,ibasis,inod,i))
rout(:, atom_num+(tag_ele(i)-1)*max_ng_node*max_basisnum + (inod-1)*max_basisnum + ibasis) &
= r_node(:,ibasis,inod,i)
npoints = npoints + 1
end do
end do
@ -223,14 +247,14 @@ module mode_metric
select case(metric_type)
case('def_grad')
write(11,*) "type element x y z F11 F12 F13 F21 F22 F23 F31 F32 F33"
write(11,*) "id type element x y z F11 F12 F13 F21 F22 F23 F31 F32 F33"
case('microrotation')
write(11,*) "type element x y z micro1 micro2 micro3 norm2(micro)"
write(11,*) "id type element x y z micro1 micro2 micro3 norm2(micro)"
end select
if(atom_num > 0) then
do i = 1, atom_num
write(11,*) type_atom(i), 0, r_atom(:,i), met(:,tag_atom(i))
write(11,*) tag_atom(i), type_atom(i), 0, r_atom(:,i), met(:,tag_atom(i))
end do
end if
@ -238,7 +262,8 @@ module mode_metric
do i = 1, ele_num
do inod = 1, ng_node(lat_ele(i))
do ibasis = 1, basisnum(lat_ele(i))
write(11,*) basis_type(ibasis,lat_ele(i)), 1, r_node(:,ibasis,inod,i), &
write(11,*) atom_num+(tag_ele(i)-1)*max_ng_node*max_basisnum + (inod-1)*max_basisnum + ibasis, &
basis_type(ibasis,lat_ele(i)), 1, r_node(:,ibasis,inod,i), &
met(:, atom_num+(tag_ele(i)-1)*max_ng_node*max_basisnum + (inod-1)*max_basisnum + ibasis)
end do
end do

@ -4,10 +4,12 @@ module neighbors
use elements
use subroutines
use functions
use box
integer, allocatable :: nei_list(:,:), nei_num(:)
integer, allocatable :: nei_list(:,:), nei_num(:), nn(:), periodvec(:,:,:)
real(kind=dp), allocatable :: init_vec(:,:,:), output(:), microrotation(:,:)
public
contains
subroutine build_cell_list(numinlist, r_list, rc_off, cell_num, num_in_cell, cell_list, which_cell)
@ -47,22 +49,25 @@ module neighbors
allocate(num_in_cell(cell_num(1),cell_num(2),cell_num(3)), cell_list(cell_lim, cell_num(1), cell_num(2), cell_num(3)))
!Now place points within cell
num_in_cell = 0
do i = 1, numinlist
!Check to see if the current point is a filler point and if so just skip it
if(r_list(1,i) < -huge(1.0_dp)+1) cycle
if(r_list(1,i) < box_bd(1)) cycle
!c is the position of the cell that the point belongs to
do j = 1, 3
c(j) = int((r_list(j,i)-box_bd(2*j-1))/(rc_off/2)) + 1
c(j) = int((r_list(j,i)-box_bd(2*j-1))/(rc_off)) + 1
end do
!Place the index in the correct position, growing if necessary
num_in_cell(c(1),c(2),c(3)) = num_in_cell(c(1),c(2),c(3)) + 1
if (num_in_cell(c(1),c(2),c(3)) > cell_lim) then
allocate(resize_cell_list(cell_lim+10,cell_num(1),cell_num(2),cell_num(3)))
resize_cell_list(1:cell_lim, :, :, :) = cell_list
resize_cell_list(1:cell_lim, :, :, :) = cell_list(1:cell_lim, :, :, :)
resize_cell_list(cell_lim+1:, :, :, :) = 0
call move_alloc(resize_cell_list, cell_list)
cell_lim = cell_lim + 10
end if
cell_list(num_in_cell(c(1),c(2),c(3)),c(1),c(2),c(3)) = i
@ -77,44 +82,70 @@ module neighbors
real(kind=dp), intent(in) :: rc_off
integer, intent(in) :: n
real(kind=dp), dimension(3,n) :: r_list
real(kind=dp), dimension(:, :), intent(in) :: r_list
integer :: i, c(3), ci, cj, ck, num_nei, nei
integer :: i, j, c(3),cn(3), ci, cj, ck, num_nei, nei, v(3), period_dir(3)
!Variables for cell list code
integer, dimension(3) ::cell_num
integer, allocatable :: num_in_cell(:,:,:), cell_list(:,:,:,:)
integer :: which_cell(3,n)
real(kind=dp) :: r(3), box_len(3)
logical :: period_bd(3)
!First reallocate the neighbor list codes
!First reallocate the neighbor list variables
if (allocated(nei_list)) then
deallocate(nei_list,nei_num)
deallocate(nei_list,nei_num, periodvec)
end if
allocate(nei_list(100,n),nei_num(n))
allocate(nei_list(100,n),nei_num(n), periodvec(3,100,n))
nei_list=0
periodvec=0
nei_num=0
!Now first pass the position list and and point num to the cell algorithm
call build_cell_list(n, r_list, rc_off, cell_num, num_in_cell, cell_list, which_cell)
do i=1, 3
if (box_bc(i:i) == 'p') then
period_bd(i) = .true.
else
period_bd(i)=.false.
end if
box_len(i) = box_bd(2*i) - box_bd(2*i-1)
end do
!Now loop over every point and find it's neighbors
pointloop: do i = 1, n
!First check to see if the point is a filler point, if so then skip it
if(r_list(1,i) < -Huge(-1.0_dp)+1) cycle
if(r_list(1,i) < box_bd(1)) cycle
!c is the position of the cell that the point
!c is the position of the cell that the point belongs to
c = which_cell(:,i)
!Loop over all neighboring cells
do ci = -1, 1, 1
do cj = -1, 1, 1
do ck = -1, 1, 1
!First check to make sure that the neighboring cell exists
!First try to apply periodic boundaries
v=(/ ck, cj, ci /)
cn=0
period_dir=0
do j=1, 3
if ((c(j) + v(j) == 0).and.period_bd(j)) then
cn(j) = cell_num(j)
period_dir(j) = 1
else if ((c(j) + v(j) > cell_num(j)).and.period_bd(j)) then
cn(j) = 1
period_dir(j) = -1
else if ((c(j)+v(j) >= 1) .and. (c(j)+v(j) <= cell_num(j))) then
cn(j) = c(j) + v(j)
end if
end do
if(any((c + (/ ck, cj, ci /)) == 0)) cycle
if( (c(1) + ck > cell_num(1)).or.(c(2) + cj > cell_num(2)).or. &
(c(3) + ci > cell_num(3))) cycle
do num_nei = 1, num_in_cell(c(1) + ck, c(2) + cj, c(3) + ci)
nei = cell_list(num_nei,c(1) + ck, c(2) + cj, c(3) + ci)
do num_nei = 1, num_in_cell(cn(1),cn(2),cn(3))
nei = cell_list(num_nei,cn(1),cn(2),cn(3))
!Check to make sure the atom isn't the same index as the atom we are checking
!and that the neighbor hasn't already been deleted
@ -122,10 +153,13 @@ module neighbors
!Now check to see if it is in the cutoff radius, if it is add it to the neighbor list for that
!atom and calculate the initial neighbor vector
if (norm2(r_list(:,nei)-r_list(:,i)) < rc_off) then
r = r_list(:,nei) + period_dir*box_len
if (norm2(r-r_list(:,i)) < rc_off) then
nei_num(i) = nei_num(i) + 1
nei_list(nei_num(i), i) = nei
periodvec(:,nei_num(i),i) = period_dir
end if
end if
@ -139,4 +173,66 @@ module neighbors
return
end subroutine calc_neighbor
subroutine calc_NN(n,points, rc_off)
integer, intent(in) :: n
real(kind=dp), intent(in) :: points(3,n)
real(kind=dp), intent(in) :: rc_off
integer :: i, c(3), ci, cj, ck, nei
!cell arrays
integer, dimension(3) ::cell_num
integer, allocatable :: num_in_cell(:,:,:), cell_list(:,:,:,:)
integer :: which_cell(3,n)
real(kind = dp) :: rmin
!First reallocate the neighbor list codes
if (allocated(nn)) then
deallocate(nn)
end if
allocate(nn(n))
nn=0
!First build the cell lists
call build_cell_list(n, points, rc_off, cell_num, num_in_cell, cell_list, which_cell)
pointloop: do i = 1, n
!First check to see if the point is a filler point, if so then skip it
if(points(1,i) < -Huge(-1.0_dp)+1) cycle
!Get the positon of the cell
c = which_cell(:,i)
!Initialize the min vec
rmin=rc_off
!loop over all neighboring cells
do ci = -1, 1, 1
do cj = -1, 1, 1
do ck = -1, 1, 1
if(any((c + (/ ck, cj, ci /)) == 0)) cycle
if( (c(1) + ck > cell_num(1)).or.(c(2) + cj > cell_num(2)).or. (c(3) + ci > cell_num(3))) cycle
do num_nei = 1, num_in_cell(c(1) + ck, c(2) + cj, c(3) + ci)
nei = cell_list(num_nei,c(1) + ck, c(2) + cj, c(3) + ci)
!Check to make sure the atom isn't the same index as the atom we are checking
if((nei /= i)) then
!If it's the minimum position than we add it to the nearest neighbor list and updat e the min vec
if (norm2(points(:,nei)-points(:,i)) < rmin) then
rmin = norm2(points(:, nei) - points(:,i))
nn(i)=(nei)
end if
end if
end do
end do
end do
end do
end do pointloop
return
end subroutine calc_NN
end module neighbors

@ -0,0 +1,146 @@
module opt_bubble
!This module contains the bubble option which can be used to create voids with specific pressures of certain atoms
use atoms
use parameters
use elements
use box
use opt_group
implicit none
real(kind=dp), private :: br, brat, c(3)
character(len=2), private :: species
public
contains
subroutine bubble(arg_pos)
integer, intent(inout) :: arg_pos
integer :: new_type, n, j, i, atom_num_pre
real(kind = dp) :: p(3), rand, factor, per, vol, mass
print *, '------------------------------------------------------------'
print *, 'Option Bubble'
print *, '------------------------------------------------------------'
!First we parse the bubble command
call parse_bubble(arg_pos)
!Now we use the existing group code to delete a sphere which represents the bubble
centroid=c
radius = br
type='all'
gshape='sphere'
group_nodes = .true.
group_atom_types=0
call get_group
call refine_group
call get_group
atom_num_pre= atom_num
call delete_group
!Now we create a new atom type with the desired species
call atommass(species, mass)
call add_atom_type(mass, new_type)
!Now we calculate the number of atoms we need to add for the desired pressure
!print *, "Creating a bubble with pressure", bp, " at temperature ", bt, " with radius ", br
!
!factor = 1.0e24/6.02214e23
!if (bp <= 10.0) then
! per=factor*(3.29674113+4.51777872*bp**(-0.80473167))
!else if (bp .le. 20.0) then
! per=factor*(4.73419689-0.072919483*bp)
!else
! per=factor*(4.73419689-0.072919483*bp)
! print *, 'warning: pressure is too high'
! print *, 'equation of state is only valid for < 20 GPa'
!endif
!vol = 4.0*pi/3.0*br**3.0
n = brat*(atom_num_pre-atom_num)
print *, "Adding ", n, " atoms of species ", species
!Now add n atoms randomly within the sphere
do i = 1, n
do while(.true.)
do j = 1, 3
call random_number(rand)
p(j) = rand*(2*br) + c(j)-br
end do
if (norm2(p-c) < br) exit
end do
call add_atom(0, new_type, p)
end do
end subroutine bubble
subroutine parse_bubble(arg_pos)
integer, intent(inout) :: arg_pos
integer :: i, arglen
real(kind=dp) :: mass
character(len=100) :: tmptxt
!First read in the bubble centroid
do i = 1, 3
arg_pos = arg_pos + 1
call get_command_argument(arg_pos, tmptxt, arglen)
print *, trim(adjustl(tmptxt))
call parse_pos(i, tmptxt, c(i))
end do
!Now the bubble radius
arg_pos = arg_pos + 1
call get_command_argument(arg_pos, tmptxt, arglen)
print *, trim(adjustl(tmptxt))
if(arglen == 0) stop "Missing bubble radius"
read(tmptxt, *) br
!Now bubble ratio
arg_pos = arg_pos + 1
call get_command_argument(arg_pos, tmptxt, arglen)
print *, trim(adjustl(tmptxt))
if(arglen == 0) stop "Missing bubble ratio"
read(tmptxt, *) brat
!Now the bubble species
arg_pos = arg_pos + 1
call get_command_argument(arg_pos, species, arglen)
print *, species
if(arglen == 0) stop "Missing bubble species"
!OPtional arguments
do while(.true.)
if(arg_pos > command_argument_count()) exit
arg_pos=arg_pos+1
call get_command_argument(arg_pos, tmptxt)
tmptxt=adjustl(tmptxt)
select case(trim(tmptxt))
case('excludetypes')
arg_pos=arg_pos + 1
call get_command_argument(arg_pos, tmptxt, arglen)
if(arglen==0) stop "Missing number of atoms to exclude"
read(tmptxt, *) exclude_num
do i=1,exclude_num
arg_pos = arg_pos + 1
call get_command_argument(arg_pos, tmptxt, arglen)
if(arglen==0) stop "Missing exclude atom types"
call atommass(tmptxt, mass)
call add_atom_type(mass, exclude_types(i))
end do
case default
exit
end select
end do
return
end subroutine parse_bubble
end module opt_bubble

@ -10,6 +10,7 @@ module opt_deform
real(kind=dp), save :: applied_strain
integer, save :: sdim
logical :: percent
public
contains
@ -21,9 +22,11 @@ module opt_deform
character(len=1) :: dims(3)
integer :: i, j, k
real(kind=dp) :: frac_atom(atom_num), frac_node(max_basisnum, max_ng_node, ele_num)
real(kind=dp) :: frac_atom(atom_num), frac_node(max_basisnum, max_ng_node, ele_num), blen
!initialize some variables
percent=.false.
dims(1) = 'x'
dims(2) = 'y'
dims(3) = 'z'
@ -44,7 +47,13 @@ module opt_deform
end do
print *, "Original box bounds in ", dims(sdim), " are ", box_bd(2*sdim-1:2*sdim)
box_bd(2*sdim) = box_bd(2*sdim) + applied_strain
if(percent) then
blen = box_bd(2*sdim) - box_bd(2*sdim-1)
box_bd(2*sdim) = box_bd(2*sdim-1) + blen*applied_strain
else
box_bd(2*sdim) = box_bd(2*sdim) + applied_strain
end if
print *, "New box bounds are ", box_bd(2*sdim-1:2*sdim)
!Now reassign the positions
@ -90,6 +99,25 @@ module opt_deform
if (arg_len == 0) stop "Missing strain in deform command"
read(textholder, *) applied_strain
!Now parse the additional options which may be present
do while(.true.)
if(arg_pos > command_argument_count()) exit
!Pull out the next argument which should either be a keyword or an option
arg_pos=arg_pos+1
call get_command_argument(arg_pos, textholder)
textholder=adjustl(textholder)
!Choose what to based on what the option string is
select case(trim(textholder))
case('percent')
percent=.true.
case default
arg_pos=arg_pos-1
!if it isn't an available option to opt_group then we just exit
exit
end select
end do
arg_pos = arg_pos + 1
end subroutine parse_deform

@ -8,6 +8,7 @@ module opt_delete
implicit none
real(kind=dp) :: rc_off
logical :: first
public
contains
@ -34,6 +35,7 @@ module opt_delete
character(len=100) :: textholder
arg_pos = arg_pos + 1
first = .true.
call get_command_argument(arg_pos, textholder, arg_len)
if(arg_len==0) stop "Missing argument to delete command"
@ -49,6 +51,24 @@ module opt_delete
end select
arg_pos = arg_pos + 1
do while(.true.)
if(arg_pos > command_argument_count()) exit
!Pull out the next argument which should either be a keyword or an option
arg_pos=arg_pos+1
call get_command_argument(arg_pos, textholder)
textholder=adjustl(textholder)
select case(trim(textholder))
case('first')
first=.true.
case('last')
first=.false.
case default
!if it isn't an available option to opt_group then we just exit
exit
end select
end do
end subroutine parse_delete
subroutine delete_overlap
@ -62,14 +82,16 @@ module opt_delete
integer, dimension(3) :: cell_num
integer, allocatable :: num_in_cell(:,:,:), which_cell(:,:)
integer, allocatable :: cell_list(:,:,:,:)
logical :: deleted_atom(atom_num)
allocate(which_cell(3,atom_num))
!First pass the atom list and atom num to the algorithm which builds the cell list
call build_cell_list(atom_num, r_atom, rc_off, cell_num, num_in_cell, cell_list, which_cell)
call build_cell_list(atom_num, r_atom, 5*rc_off, cell_num, num_in_cell, cell_list, which_cell)
!Now loop over every atom and figure out if it has neighbors within the rc_off
delete_num = 0
deleted_atom=.false.
atom_loop: do i = 1, atom_num
!c is the position of the cell that the atom belongs to
@ -93,22 +115,39 @@ module opt_delete
!Check to make sure the atom isn't the same index as the atom we are checking
!and that the neighbor hasn't already been deleted
if((nei /= i).and.(nei/= 0)) then
if((nei /= i).and.(.not.deleted_atom(nei))) then
!Now check to see if it is in the cutoff radius, if it is add it to the delete code
if (norm2(r_atom(:,nei)-r_atom(:,i)) < rc_off) then
delete_num = delete_num + 1
for_delete(delete_num) = max(i,nei)
if(first) then
for_delete(delete_num) = min(i,nei)
deleted_atom(min(i,nei)) = .true.
else
for_delete(delete_num) = max(i,nei)
deleted_atom(max(i,nei)) = .true.
end if
!Now zero out the larger index
if(i > nei) then
which_cell(:,i) = 0
cycle atom_loop
if(first) then
if(i < nei) then
which_cell(:,i) = 0
cycle atom_loop
else
which_cell(:,nei) = 0
cell_list(num_nei,c(1) + ck, c(2) + cj, c(3) + ci) = 0
end if
else
which_cell(:,nei) = 0
cell_list(num_nei,c(1) + ck, c(2) + cj, c(3) + ci) = 0
if(i > nei) then
which_cell(:,i) = 0
cycle atom_loop
else
which_cell(:,nei) = 0
cell_list(num_nei,c(1) + ck, c(2) + cj, c(3) + ci) = 0
end if
end if
end if
end if
end do

@ -113,7 +113,7 @@ module opt_disl
subroutine disl
!This subroutine creates the actual dislocation
integer :: i, sub_box, inod, ibasis, ix, iy, iz
integer :: i, inod, ibasis, ix, iy, iz
real(kind=dp) :: ss_ori(3,3), ss_inv(3,3), be, bs, slipx(3), disp_transform(3,3), inv_transform(3,3), &
actan, r(3), disp(3)
@ -240,7 +240,7 @@ module opt_disl
subroutine dislgen
!This subroutine creates the actual dislocation
integer :: i, sub_box, inod, ibasis
integer :: i, inod, ibasis
real(kind=dp) :: ss_ori(3,3), ss_inv(3,3), be, bs, slipx(3), disp_transform(3,3), inv_transform(3,3), &
actan, r(3), disp(3)
@ -250,14 +250,6 @@ module opt_disl
be = sin(char_angle*pi/180.0_dp)*b
bs = cos(char_angle*pi/180.0_dp)*b
!Figure out which sub box you are in so you can access it's orientation, this code will not work
!with overlapping sub_boxes
do i = 1, sub_box_num
if(in_block_bd(centroid, sub_box_bd(:,i))) then
sub_box = i
exit
end if
end do
!Construct the slip system orientation matrix in an unrotated system
slipx = cross_product(slip_plane, line)
@ -267,8 +259,7 @@ module opt_disl
call matrix_inverse(ss_ori, 3, ss_inv)
!Apply the rotation
print *, ss_inv
disp_transform = matmul(sub_box_ori(:,:,i), ss_inv)
disp_transform = matmul(box_ori(:,:), ss_inv)
call matrix_inverse(disp_transform,3,inv_transform)
if(atom_num > 0) then
@ -381,18 +372,6 @@ module opt_disl
arg_pos = arg_pos + 1
!Now check to make sure that the dimension selected is actually a 1 1 1 direction.
! call in_sub_box(centroid, sbox)
! if(.not.((abs(sub_box_ori(loop_normal,1,sbox)) == abs(sub_box_ori(loop_normal,2,sbox))).and. &
! (abs(sub_box_ori(loop_normal,2,sbox)) == abs(sub_box_ori(loop_normal,3,sbox))).and. &
! (abs(sub_box_ori(loop_normal,3,sbox)) == abs(sub_box_ori(loop_normal,1,sbox))))) then
! print *, "The selected dimension ", loop_normal, " for sub_box ", sbox, " is ", &
! sub_box_ori(loop_normal,:,sbox), " which is not in the (111) family of planes"
! STOP 3
! end if
end subroutine
!Code for the creation of dislocation loops is based on functions from atomsk
@ -541,7 +520,7 @@ module opt_disl
end do
return
end subroutine
end subroutine disloop
!********************************************************
! SOLIDANGLE
@ -652,18 +631,6 @@ module opt_disl
arg_pos=arg_pos+1
!Now check to make sure that the dimension selected is actually a 1 1 1 direction.
! call in_sub_box(centroid, sbox)
! if(.not.((abs(sub_box_ori(loop_normal,1,sbox)) == abs(sub_box_ori(loop_normal,2,sbox))).and. &
! (abs(sub_box_ori(loop_normal,2,sbox)) == abs(sub_box_ori(loop_normal,3,sbox))).and. &
! (abs(sub_box_ori(loop_normal,3,sbox)) == abs(sub_box_ori(loop_normal,1,sbox))))) then
! print *, "The selected dimension ", loop_normal, " for sub_box ", sbox, " is ", &
! sub_box_ori(loop_normal,:,sbox), " which is not in the (111) family of planes"
! STOP 3
! end if
end subroutine parse_vacancydisloop

File diff suppressed because it is too large Load Diff

@ -10,7 +10,7 @@ module opt_orient
real(kind=dp), save :: new_orient(3,3)
real(kind=dp), dimension(6) :: orig_box_bd
real(kind=dp), allocatable :: orig_sub_box_ori(:,:,:)
real(kind=dp), dimension(3,3) :: orig_box_ori
character(len=3) :: orig_box_bc
public
@ -22,7 +22,7 @@ module opt_orient
integer :: i, j, k, ibasis, inod
logical :: isortho, isrighthanded, matching
real(kind=dp) :: inv_sub_box_ori(3,3,sub_box_num)
real(kind=dp) :: inv_box_ori(3,3)
!First parse the orient command
@ -31,36 +31,25 @@ module opt_orient
!Now rotate the basis. To do this we transform the basis to [100] [010] [001] and then
!transform to user specified basis.
!Find all inverse orientation matrices for all sub_boxes
do i = 1, sub_box_num
call matrix_inverse(sub_box_ori(:,:,i), 3, inv_sub_box_ori(:,:,i))
end do
call matrix_inverse(box_ori(:,:), 3, inv_box_ori(:,:))
!Now transform all atoms
do i = 1, atom_num
r_atom(:,i) = matmul(new_orient,matmul(inv_sub_box_ori(:,:,sbox_atom(i)),r_atom(:,i)))
r_atom(:,i) = matmul(new_orient,matmul(inv_box_ori(:,:),r_atom(:,i)))
end do
!Now transform all elements
do i = 1, ele_num
do inod =1, ng_node(lat_ele(i))
do ibasis = 1, basisnum(lat_ele(i))
r_node(:,ibasis,inod,i) = matmul(new_orient,matmul(inv_sub_box_ori(:,:,sbox_ele(i)),r_node(:,ibasis,inod,i)))
r_node(:,ibasis,inod,i) = matmul(new_orient,matmul(inv_box_ori(:,:),r_node(:,ibasis,inod,i)))
end do
end do
end do
!Now save the original sub_box_ori and overwrite them
if(allocated(orig_sub_box_ori)) deallocate(orig_sub_box_ori)
allocate(orig_sub_box_ori(3,3,sub_box_num))
orig_sub_box_ori = sub_box_ori
!Now overwrite the orientations
do i = 1, sub_box_num
sub_box_ori(:,:,i) = new_orient
end do
!Now save the original box_ori
orig_box_ori = box_ori
box_ori = new_orient
!Save original box boundaries
orig_box_bd = box_bd
@ -70,18 +59,16 @@ module opt_orient
orig_box_bc = box_bc
do i = 1,3
matching=.true.
sbox_loop:do j = 1, sub_box_num
do k = 1, 3
if(.not.is_equal(orig_sub_box_ori(i,k,j), new_orient(i,k))) then
matching = .false.
exit sbox_loop
end if
end do
end do sbox_loop
do k = 1, 3
if(.not.is_equal(orig_box_ori(i,k), new_orient(i,k))) then
matching = .false.
exit
end if
end do
if(.not.matching) box_bc(i:i)='s'
end do
call def_new_box
call def_new_box
end subroutine orient_opt
subroutine parse_orient(arg_pos)
@ -121,24 +108,24 @@ module opt_orient
real(kind=dp) :: inv_ori(3,3)
!Now rotate the basis. To do this we transform the basis to [100] [010] [001] and then
!transform to the original sbox_ele
!transform to the original box_ori
!Find the inverse for the new orientation matrix
call matrix_inverse(new_orient, 3, inv_ori)
!Recover original sub_box_ori
sub_box_ori = orig_sub_box_ori
!Recover original box_ori and box_bd
box_ori = orig_box_ori
!Now transform all atoms
do i = 1, atom_num
r_atom(:,i) = matmul(sub_box_ori(:,:,sbox_atom(i)),matmul(inv_ori(:,:),r_atom(:,i)))
r_atom(:,i) = matmul(box_ori(:,:),matmul(inv_ori(:,:),r_atom(:,i)))
end do
!Now transform all elements
do i = 1, ele_num
do inod =1, ng_node(lat_ele(i))
do ibasis = 1, basisnum(lat_ele(i))
r_node(:,ibasis,inod,i) = matmul(sub_box_ori(:,:,sbox_ele(i)),matmul(inv_ori,r_node(:,ibasis,inod,i)))
r_node(:,ibasis,inod,i) = matmul(box_ori(:,:),matmul(inv_ori,r_node(:,ibasis,inod,i)))
end do
end do
end do
@ -148,29 +135,4 @@ module opt_orient
box_bc = orig_box_bc
end subroutine unorient
subroutine sbox_ori(arg_pos)
integer, intent(inout) :: arg_pos
integer :: i, sbox_in, arg_len
real(kind = dp) :: new_orient(3,3)
character(len=100) :: textholder
character(len=20) :: ori_string
arg_pos = arg_pos + 1
call get_command_argument(arg_pos, textholder,arg_len)
if (arg_len== 0) stop 'Missing sbox in sbox_ori command'
read(textholder,*) sbox_in
do i = 1, 3
arg_pos = arg_pos + 1
call get_command_argument(arg_pos, ori_string, arg_len)
if (arg_len == 0) print *, "Missing orientation vector in -orient option"
call parse_ori_vec(ori_string, new_orient(i,:))
new_orient(i,:) = new_orient(i,:) / norm2(new_orient(i,:))
end do
sub_box_ori(:,:,sbox_in) = new_orient
arg_pos = arg_pos + 1
end subroutine sbox_ori
end module opt_orient

@ -3,6 +3,7 @@ module opt_redef_box
use box
use elements
use subroutines
implicit none
character(len=3) :: redef_dim, new_bc
@ -13,7 +14,8 @@ module opt_redef_box
subroutine redef_box(arg_pos)
!This is the main calling function for opt_redef_box
integer, intent(inout) :: arg_pos
integer :: i, inod, ibasis, iatom, delete_list(atom_num), delete_num, type_interp(max_basisnum*max_esize**3)
integer :: i, j, inod, ibasis, iatom, delete_list(atom_num), delete_num, type_interp(max_basisnum*max_esize**3), &
new_snum
real(kind=dp):: r_interp(3, max_basisnum*max_esize**3)
logical :: node_out(8)
@ -64,7 +66,7 @@ module opt_redef_box
!loop over all interpolated atoms and add them to the system
do iatom = 1, basisnum(lat_ele(i))*size_ele(i)**3
if(in_block_bd(r_interp(:,iatom), new_bd)) then
call add_atom(0,type_interp(iatom), sbox_ele(i), r_interp(:,iatom))
call add_atom(0,type_interp(iatom), r_interp(:,iatom))
end if
end do
end if
@ -128,4 +130,26 @@ module opt_redef_box
arg_pos = arg_pos + 1
end subroutine parse_redef_box
subroutine set_box_ori(arg_pos)
integer, intent(inout) :: arg_pos
integer :: arg_len, i
real(kind=dp) :: new_orient(3,3)
character(len=100) :: textholder
character(len=20) :: ori_string
do i = 1, 3
arg_pos = arg_pos + 1
call get_command_argument(arg_pos, ori_string, arg_len)
if (arg_len == 0) print *, "Missing orientation vector in -orient option"
call parse_ori_vec(ori_string, new_orient(i,:))
new_orient(i,:) = new_orient(i,:) / norm2(new_orient(i,:))
end do
box_ori(:,:) = new_orient
arg_pos = arg_pos + 1
end subroutine set_box_ori
end module opt_redef_box

@ -17,11 +17,13 @@ module opt_slip_plane
!Main calling function for the slip_plane option
integer, intent(inout) :: arg_pos
integer :: ie, ia, slip_enum, old_atom_num, esize, new_ele_num, n, m, o, ele(3,8), nump_ele, inod, vlat(3), ibasis
integer :: ie, ia, slip_enum, old_atom_num, esize, new_ele_num, n, m, o, ele(3,8), nump_ele, inod, vlat(3), ibasis,&
starting_anum
integer, allocatable :: slip_eles(:), temp_int(:)
real(kind=dp) :: r_interp(3, max_basisnum*max_esize**3), rfill(3,max_basisnum, max_ng_node), ratom(3,max_basisnum), &
maxp, minp
maxp, minp, vel_interp(3, max_basisnum*max_esize**3)
real(kind=dp), allocatable :: vel_tmp(:,:)
integer :: type_interp(max_basisnum*max_esize**3)
logical :: lat_points(max_esize,max_esize, max_esize)
@ -58,11 +60,25 @@ module opt_slip_plane
!If we aren't efilling then just refine the element
if(.not.efill) then
starting_anum=atom_num
call interpolate_atoms(type_ele(ie), size_ele(ie), lat_ele(ie), r_node(:,:,:,ie), type_interp, r_interp)
do ia = 1, basisnum(lat_ele(ie)) * size_ele(ie)**3
call apply_periodic(r_interp(:,ia))
call add_atom(0, type_interp(ia), sbox_ele(ie), r_interp(:,ia))
call add_atom(0, type_interp(ia), r_interp(:,ia))
end do
if(allocated(vel_atom)) then
call interpolate_vel(type_ele(ie), size_ele(ie), lat_ele(ie), vel_node(:,:,:,ie), vel_interp)
if(size(vel_atom,2) < size(type_atom)) then
allocate(vel_tmp(3, size(type_atom)))
vel_tmp=0.0_dp
vel_tmp(:, 1:size(vel_atom,2)) = vel_atom
call move_alloc(vel_tmp, vel_atom)
end if
do ia = 1, basisnum(lat_ele(ie)) * size_ele(ie)**3
vel_atom(:, starting_anum+ia) = vel_interp(:, ia)
end do
end if
!If we are efilling then the code is slightly more complex
else
!First populate the lat points array
@ -93,7 +109,7 @@ module opt_slip_plane
if(.not.(spos < maxp).and.(spos > minp))then
nump_ele = nump_ele - esize**3
lat_points(m:m+esize-1, n:n+esize-1, o:o+esize-1) = .false.
call add_element(0, type_ele(ie), esize, lat_ele(ie), sbox_ele(ie), rfill)
call add_element(0, type_ele(ie), esize, lat_ele(ie), rfill)
new_ele_num = new_ele_num + 1
end if
end do latloop
@ -110,7 +126,7 @@ module opt_slip_plane
call get_interp_pos(m,n,o, ie, ratom(:,:))
do ibasis = 1, basisnum(lat_ele(ie))
call apply_periodic(r_atom(:,ibasis))
call add_atom(0, basis_type(ibasis,lat_ele(ie)), sbox_ele(ie), ratom(:,ibasis))
call add_atom(0, basis_type(ibasis,lat_ele(ie)), ratom(:,ibasis))
end do
end if
end do

@ -13,6 +13,7 @@ module parameters
!Numeric constants
real(kind=dp), parameter :: pi = 3.14159265358979323846_dp
real(kind=dp), parameter :: pvt2n = 1362.626470955822
!Mode type that is being called
character(len=100) :: mode

@ -2,6 +2,8 @@ module subroutines
use parameters
use functions
use box
use str
implicit none
integer :: allostat, deallostat
@ -149,29 +151,43 @@ module subroutines
subroutine parse_ori_vec(ori_string, ori_vec)
!This subroutine parses a string to vector in the format [ijk]
character(len=20), intent(in) :: ori_string
character(*), intent(in) :: ori_string
real(kind=dp), dimension(3), intent(out) :: ori_vec
real(kind=dp) :: prefactor
integer :: start, fin
integer :: i, ori_pos, stat
ori_pos=2
do i = 1,3
do while(ori_string(ori_pos:ori_pos)==' ')
ori_pos=ori_pos+1
end do
if (ori_string(ori_pos:ori_pos) == '-') then
ori_pos = ori_pos + 1
read(ori_string(ori_pos:ori_pos), *, iostat=stat) ori_vec(i)
if (stat>0) STOP "Error reading orientation value"
ori_vec(i) = -ori_vec(i)
ori_pos = ori_pos + 1
else
read(ori_string(ori_pos:ori_pos), *, iostat=stat) ori_vec(i)
if(stat>0) STOP "Error reading orientation value"
ori_pos=ori_pos + 1
do i = 1, len(ori_string)
if(ori_string(i:i) == "[") then
start=i+1
else if(ori_string(i:i) == "]") then
fin = i-1
end if
end do
ori_pos=start
if (tok_count(ori_string(start:fin)) == 3) then
read(ori_string(start:fin),*) ori_vec(:)
else
do i = 1,3
do while(ori_string(ori_pos:ori_pos)==' ')
ori_pos=ori_pos+1
end do
if (ori_string(ori_pos:ori_pos) == '-') then
ori_pos = ori_pos + 1
read(ori_string(ori_pos:ori_pos), *, iostat=stat) ori_vec(i)
if (stat>0) STOP "Error reading orientation value"
ori_vec(i) = -ori_vec(i)
ori_pos = ori_pos + 1
else
read(ori_string(ori_pos:ori_pos), *, iostat=stat) ori_vec(i)
if(stat>0) STOP "Error reading orientation value"
ori_pos=ori_pos + 1
end if
end do
end if
return
end subroutine parse_ori_vec
@ -241,5 +257,52 @@ module subroutines
return
end subroutine check_right_ortho
subroutine init_random_seed()
implicit none
integer, allocatable :: seed(:)
integer :: i, n, un, istat, dt(8), pid, t(2), s
integer(8) :: count, tms
call random_seed(size = n)
allocate(seed(n))
! First try if the OS provides a random number generator
open(newunit=un, file="/dev/urandom", access="stream", &
form="unformatted", action="read", status="old", iostat=istat)
if (istat == 0) then
read(un) seed
close(un)
else
! Fallback to XOR:ing the current time and pid. The PID is
! useful in case one launches multiple instances of the same
! program in parallel.
call system_clock(count)
if (count /= 0) then
t = transfer(count, t)
else
call date_and_time(values=dt)
tms = (dt(1) - 1970) * 365_8 * 24 * 60 * 60 * 1000 &
+ dt(2) * 31_8 * 24 * 60 * 60 * 1000 &
+ dt(3) * 24 * 60 * 60 * 60 * 1000 &
+ dt(5) * 60 * 60 * 1000 &
+ dt(6) * 60 * 1000 + dt(7) * 1000 &
+ dt(8)
t = transfer(tms, t)
end if
s = ieor(t(1), t(2))
pid = getpid() + 1099279 ! Add a prime
s = ieor(s, pid)
if (n >= 3) then
seed(1) = t(1) + 36269
seed(2) = t(2) + 72551
seed(3) = pid
if (n > 3) then
seed(4:) = s + 37 * (/ (i, i = 0, n - 4) /)
end if
else
seed = s + 37 * (/ (i, i = 0, n - 1 ) /)
end if
end if
call random_seed(put=seed)
end subroutine init_random_seed
end module subroutines

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