All notable changes to this project will be documented in this file.
The format is based on Keep a Changelog, and this project adheres to Semantic Versioning once we hit release version 1.0.0.
-
astype
for sparse matrices, enables one to change data-types, #865 This should be preferred over transform which can't do real->complex of spin matrices. -
added ADOS extraction of PDOS data in
sisl.viz
-
enabled submodule access without imports:
import sisl sisl.geom.graphene
-
added Nambu spin configuration, this is still experimental
-
enabled
...
when extracting slices of MD steps in siesta output files. Here it is the same as:
. But it also allows inline arguments:read_scf(imd=...)
whereimd=:
is not allowed, partly fixes #835 -
enabled
...
foratoms=
arguments. Selects all atoms. -
clarified gauge, lattice vs. atomic is clearer than cell vs. atom. The old values are still respected.
projection
arguments of several functions has been streamlinedorbitals
arguments with slices without ends returned up togeometry.na
, now it correctly returns up to the maximum number of orbitals.
- internal Cython code for performance improvements. This yield significant perf. improvements for DFT sparse matrices with many edges in the sparse matrix, but a perf. hit for very small TB matrices.
- dtype removed from
Spin
class
- added
timesSileSiesta
which can read siesta TIMES output - Parsing of total Mulliken charges in
stdoutSileSiesta
, #691
- reading charges from Siesta 5.2 output files, #856
- a read problem for very big simulations (related to
orbindxSileSiesta
) - bug-fix for
tbtSileTBtrans.Eindex
handling of integers, #829 This is a regression fix, integers will now be handled differently than prior releases. A warning is raised to inform users. - fixed warning raised when reading electronic structure without Ef, #826
- fixed precision writing of energies in GF files (siesta), #827
- fixed reading
HSetupOnly
HSX files from Siesta, #828 - fixed reading stresses and forces from
stdoutSileSiesta
Note that generally the forces/stresses in the Final section of the output will not be returned. Only if there are no other forces/stresses in the output file.
tbtSileTBtrans.Eindex
changed, see #829 for details.
- enabled
lowdin
to return the Lowdin transformation matrix, and also allow it to be calculated using SVD
- bugfix for wrong call
Lattice.to.cuboid
which caused wrong densities, #821
-
conversion of list-like elements to
Lattice
-
vacuum argument for all
sisl.geom
methods that can use it -
Geometry.find_nsc
, alternate method for calculatingnsc
with more options -
sisl._debug_info
for more complete debug information -
axes
argument added toderivative
to only calculate on a subset of directions (can greatly improve performance for some systems) -
operator
argument added toderivative
to apply an operator todHk
anddSk
matrices. of directions (can greatly improve performance for some systems) -
added
apply_kwargs
to methods which uses aBrillouinZone
object. This enables one to leverage parallel processing for calculations. -
SISL_PAR_CHUNKSIZE=25
, new default parameter for parallel processing. Can greatly improve parallel processing of BZ integrations -
added
vectorsSileSiesta
to read vibra eigenmode output -
added
dihedral
toGeometry
, #773 -
ability to retain sub-classes through
<class>.new
calls -
added
Listify
to ensure arguments behaves as iterables -
setter for
Lattice.pbc
to specify it through an array -
Lattice.volumef
to calculate a subset volume based on axes -
added
write_grid
to Siesta binary grid files -
added the
goldene
2D lattice, ahexagonal
Gold 2D structure -
added the
hexagonal
2D lattice, close-packed FCC(111) surface -
improved
atom
projections of states, #750 -
improved typing system
-
units
toread_*
for someSile
s, #726 -
enabled reading the Hamiltonian from the Wannier90 _tb.dat file, #727
-
"Hz", "MHz", "GHz", "THz", and "invcm" as valid energy units, #725
-
added
read_gtensor
andread_hyperfine_coupling
totxtSileORCA
, #722 -
enabled
AtomsArgument
andOrbitalsArgument
to acceptbool
for all or none -
enabled
winSileWannier90.read_hamiltonian
to read the_tb.dat
files -
atoms
argument toDensityMatrix.spin_align
to align a subset of atoms (only diagonal elements between the atoms orbitals) -
added an efficient neighbor finder, #393
-
enabled reading DFTB+ output Hamiltonian and overlap matrices, #579
-
bond_order
forDensityMatrix
objects, #507 -
better error messages when users request quantities not calculated by Siesta/TBtrans
-
functional programming of the basic sisl classes Now many of the
Geometry|Lattice|Grid.*
manipulation routines which returns new objects, are subjected to dispatch methods. E.g.sisl.tile(geometry, 2, axis=1) geometry.tile(2, axis=1)
will call the same method. The first uses a dispatch method, and a
SislError
will be raised if the dispatch argument is not implemented. -
SparseCSR.toarray
to comply with array handling (equivalent totodense
) -
enabled
Grid.to|new
with the most basic stuff str|Path|Grid|pyamg -
Shape.translate
, to easily translate entire shape constructs, #655 -
Creation of chiral GNRs (
kind=chiral
insisl.geom.nanoribbon
/sisl.geom.graphene_nanoribbon
as well assisl.geom.cgnr
) -
Creation of [n]-triangulenes (
sisl.geom.triangulene
) -
added
offset
argument inGeometry.add_vacuum
to enable shifting atomic coordinates -
A new
AtomicMatrixPlot
to plot sparse matrices, #668
- PEP-585 compliant
- buildable for numpy>2, #791
BrillouinZone.tocartesian()
now defaults tok=self.k
- reading XV/STRUCT files from fdf siles could cause problems, #778
Geometry.[ao][us]c2[su]c
methods now retains the input shapes (unlessunique=True
)- lots of
Lattice
methods did not consistently copy over BC BrillouinZone.volume
fixed to actually return BZ volume useLattice.volume
for getting the lattice volume.- xsf files now only respect
lattice.pbc
for determining PBC, #764 - fixed
CHGCAR
spin-polarized density reads, #754 - dispatch methods now searches the mro for best matches, #721
- all
eps
arguments has changed toatol
- methods with
axis
arguments now accepts the str equivalent 0==a - documentation links to external resources
- fixed
chgSileVASP.read_grid
for spinful calculations txtSileOrca.info.no
used a wrong regex, added a test- raises error when requesting isosurface for complex valued grids, #709
- some attributes associated with
Sile.info.*
will now warn instead of raising information - reading matrices from HSX files with weird labels, should now work (fingers-crossed)
Atom(Z="1000")
will now correctly work, #708AtomUnknown
now also has a default mass of 1e40- changed
read_force_constant
toread_hessian
, the old methods are retained with deprecation warnings. pdosSileSiesta
plotting produced wrong spin components for NC/SOCtqdm
changed API in 2019,eta=True
in Notebooks should now workSparseCSR
ufunc handling, in some corner cases could the dtype casting do things wrongly.- fixed corner cases where the
SparseCSR.diags(offsets=)
would add elements in non-existing elements - some cases of writing orthogonal matrices to TSHS/nc file formats #661
BDOS
from TBtrans calculations now returns the full DOS of all (Bloch-expanded) atomsLattice
objects now issues a warning when created with 0-length vectors- HSX file reads should respect input geometry arguments
- enabled slicing in matrix assignments, #650
- changed
Shape.volume()
toShape.volume
- growth direction for zigzag heteroribbons
BandStructure
points can now automatically add thensc == 1
axis as would be done for assigning matrix elements (it fills with 0's).
degenerate
argument invelocity
/derivative
, they do not belong therexvSileSiesta.read_geometry(species_as_Z)
, deprecated in favor ofatoms=
structSileSiesta.read_geometry(species_as_Z)
, deprecated in favor ofatoms=
Atom.radii
is removed,Atom.radius
is the correct invocationsisl.plot
is removed (sisl.viz
is replacing it!)cell
argument forGeometry.translate/move
(it never worked)- removed
Selector
andTimeSelector
, they were never used internally
- internal test structure, should improve future progress
Lattice.parameters
now returns a 2-tuple oflength, angles
- units of
conductivity
has changed to S / Ang conductivity
is deprecated, useahc
andshc
insteadberry_curvature
has completely changed, checks it API- BZ apply methods are now by default parallel (if
SISL_NUM_PROCS>1
) hsxSileSiesta.read_hamiltonian
now implicitly shifts Fermi-level to 0 (for newer HSX versions)- deprecated
periodic
toaxes
argument inBrillouinZone.volume
- changed
Eigenmode.displacement
shape, please read the documentation - bumped minimal Python version to 3.9, #640
- documentation build system on RTD is updated, #745
gauge
arguments now accept 'cell' and 'orbital' in replacements for 'R' and 'r', respectivelysiesta.*.read_basis
now defaults to read anAtoms
object with all atomsatoms.specie
changed toatoms.species
, generally species is the singular formin_place
arguments changed toinplace
- renamed
stdoutSileVASP
tooutcarSileVASP
, #719 - deprecated scale_atoms in favor of scale_basis in
Geometry.scale
- changed default number of eigenvalues calculated in sparse
eigsh
, from 10 to 1 stdoutSileSiesta.read_*
now defaults to read the next entry, and not the laststdoutSileSiesta.read_*
changed MD output functionality, see #586 for detailsAtomNeighbours
changed name toAtomNeighbor
to follow #393- changed method name
spin_squared
tospin_contamination
- removed
Lattice.translate|move
, they did not make sense, and so their usage should be deferred toLattice.add
instead. vacuum
is now an optional parameter for all ribbon structures- enabled
array_fill_repeat
with custom axis, to tile along specific dimensions - Importing
sisl.viz
explicitly is no longer needed, as it will be lazily loaded whenever it is required.
- Creation of honeycomb flakes (
sisl.geom.honeycomb_flake
,sisl.geom.graphene_flake
), #636 - added
Geometry.as_supercell
to create the supercell structure, thanks to @pfebrer for the suggestion - added
Lattice.to
andLattice.new
to function the same asGeometry
, added Lattice.to["Cuboid"] - added
Atom.to
, currently onlyto.Sphere()
- enabled
Geometry.to|new.Sile(...)
- added logging in some modules, to be added in more stuff to allow easier debugging.
- marked all
toSphere|toEllipsoid|...
as deprecated - a simple extensionable method to add
Sile.info.<attr>
by exposing attributes through an object on each class. The info_attributes contains a list of attributes that can be discovered while reading ascii files see #509
- fixed cases where
Geometry.close
would not catch all neighbours, #633
- sisl now enforces the black style
Lattice
now holds the boundary conditions (notGrid
), see #626- Some siles exposed certain properties containing basic information
about the content, say number of atoms/orbitals etc.
These will be moved to
sile.info.<attr>
instead to reduce the number of methods exposed on each sile.
- problems in the sisl.viz module got fixed
- xarray is now a full dependency (this also implies pandas)
-
added SISL_UNIT_SIESTA to select between legacy or codata2018 units (since Siesta 5) New default is codata2018, may create inconsistencies until Siesta 5 is widely adopted.
-
added --remove to sgeom for removing single atoms
-
added a EllipticalCylinder as a new shape
-
added basis-enthalpy to the stdoutSiestaSile.read_energy routine
-
added
read_trajectory
to read cell vectors, atomic positions, and forces from VASP OUTCAR -
slicing io files multiple output (still WIP), see #584 for details Intention is to have all methods use this method for returning multiple values, it should streamline the API.
-
allowed xyz files to read Origin entries in the comment field
-
allowed sile specifiers to be more explicit:
-
"hello.xyz{contains=}" equivalent to "hello.xyz{}"
-
"hello.xyz{startswith=}" class name should start with
<name>
-
"hello.xyz{endswith=}" class name should end with
<name>
This is useful for defining a currently working code:SISL_IO_DEFAULT=siesta
-
-
added environment variable
SISL_IO_DEFAULT
which appends a sile specifier if not explicitly added. I.e.get_sile("hello.xyz")
is equivalent toget_sile("hello.xyz{os.environ["SISL_IO_DEFAULT"]}"
. Fixes #576 -
added a context manager for manipulating the global env-vars in temporary locations.
with sisl_environ(SISL_IO_DEFAULT=...)
-
enabled
Geometry.append|prepend
insgeom
command (reads other files) -
added
fdfSileSiesta.write_brillouinzone
to easily write BandLines to the fdf output, see #141 -
added
aniSileSiesta
for MD output of Siesta, #544 -
mdSileOpenMX
for MD output of OpenMX -
Atoms.formula
to get a chemical formula, currently only Hill notation -
unified the index argument for reading Grids,
read_grid
, this influences Siesta and VASP grid reads. -
sisl.mixing
:AndersonMixer
enables the popular and very simple linear-like mixerStepMixer
allows switching between different mixers, for instance this enabled restart capabilities among other things.- Enabled composite mixers (simple math with mixers)
-
BrillouinZone.merge
allows simple merging of several objects, #537
- updated the viz module, #476
- allowing ^ negation in order arguments for siles
- internal change to comply with scipy changes, use issparse instead of spmatrix, see #598
- netCDF4 is now an optional dependency, #595
- interface for Sparse*.nonzero(), arguments suffixed with 's'
stdoutSileVASP
will not acceptall=
argumentsstdoutSileVASP.read_energy
returns as default the next item (no longer the last)txtSileOrca
will not acceptall=
arguments, see #584stdoutSileOrca
will not acceptall=
arguments, see #584xyzSile
out from sisl will now default to the extended xyz file-format Explicitly adding the nsc= value makes it compatible with other exyz file formats and parseable by sisl, this is an internal change- default of
Geometry.translate2uc
, now only periodic axes are default to be moved - all out files have been renamed to stdout to clarify they are user determined output file names, suggestion by @tfrederiksen
- bumped Python requirement to >=3.8
- orbitals
R
arguments will now by default determine the minimal radii that contains 99.99% of the function integrand. The argument now accepts values -1:0 which is a fraction of the integrand that the function should contain, a positive value will explicitly set the range #574 - Added printout of the removed couplings in the
RecursiveSI
SuperCell
class is officially deprecated in favor ofLattice
, see #95 for details The old class will still be accessible and usable for some time (at least a year)- Enabled EigenState.wavefunction(grid) to accept grid as the initialization of
the grid argument, so one does not need to produce the
Grid
on before-hand Geometry.rotate(only=)
to(what=)
, this is to unify the interfaces across, #541 Also changed the default value to be "xyz" if atoms is Not nonetbtncSileTBtrans(only=)
arguments are changed to (what=) #541SelfEnergy.scattering_matrix
is changed toSelfEnergy.broadening_matrix
ince the scattering matrix is an S-matrix usage. Also changedse2scat
tose2broadening
#529- allow
BrillouinZone
initialization with scalar weights for all k-points #537 Geometry.swapaxes
andSuperCell.swapaxes
, these are now more versatile by allowing multiple swaps in a single run, #539- deprecated
set_sc
- internal build-system is changed to
scikit-build-core
, thedistutils
will be deprecated in Python>=3.12 so it was a needed change. This resulted in a directory restructuring.
- fixed Mulliken calculations for polarized calculations due to missing copy, #611
- fixed single argument
ret_isc=True
ofclose
, #604 and #605 - tiling Grid now only possible for commensurate grids (grid.lattice % grid.geometry.lattice)
- rare cases for non-Gamma calculations with actual Gamma matrices resulted in crashes #572
MonkhorstPack.replace
now checks for symmetry k-points if the BZ is using trs. Additionally the displacements are moved to the primitive point before comparing, this partly fixed #568- spin-orbit Hamiltonians in
RealSpaceSE
andRealSpaceSI
, fixes #567 - ufunc reductions on
SparseGeometry
whereaxis
arguments reduces dimensionality - interaction with pymatgen
fdfSileSiesta.includes
would fail when empty lines were present, #555 fixed and added test- Documentation now uses global references
Geometry.swapaxes
would not swap latticevector cartesian coordinates, #539
- calculation of scattering matrices
Geometry.apply
apply functions to slices of data depending on the geometry- enabled Gaussian and Slater type orbitals, #463 Please give feedback!
- deltancSileTBtrans.merge allowing easy merging of several delta siles, #513
- implemented reading of output files from ORCA, #500
- HydrogenicOrbital is added for simple handling of 1-valence electron orbitals, #499
- Bohr radius to constants
- enabled ASCII siles to read from file-handles and buffers, #484
- enabled unit specification for lengths in cube-files
- added
kwargs
passed to eigenstate functions inberry_phase
andconductivity
- ensured that non-orthogonal
transform
will copy over overlap matrix in case the matrix is only touching the non-overlap elements - enabled dictionary entries for the
Atoms
initialization in place ofatoms
argument. Both in the list-like entry, or as the only argument.
- rare compiler bug, #512
within_inf
with periodic arguments, #511- reading TranSiesta data from outSileSiesta
- regression from 80f27b05, reading version 0 HSX content, #492
- delta-files (netCDF) would always have diagonal components, this has now been removed since it only needs the elements with values
- Siesta sparse matrices could in some cases set wrong diagonal components
- too large energies in Siesta files could result in crash, #482
- orbital quantum numbers from HSX file was wrong in v1, #462
- corrected sign for spin-Y direction,
PDOS
,spin_moment
, #486 - RealSpaceSI for right semi-infinite directions, #475
- tbtrans files now have a separate entry in the documentation
- removed all deprecated routines, #495
- oplist now can do in-place operations on generators
- significant performance improvement for COOP calculations, thanks to Susanne Leitherer for discovering the issue
- changed argument order of ElectronState.COP
- index ordering of spin and coordinate quantities are now changed to have these as the first indices. This ensures consistency across return types and allows easier handling. Note that non-polarized PDOS calculations now has an extra dimension for coherence with non-colinear spin. (see #501)
- ensured all units are now CODATA-2018 values
cell_length
changed tocell2length
with new axes argument- enabled orbitals up to the h-shell, #491
- swapped order of
honeycomb
(graphene
derivatives) lattice vectors, to ensure the vectors are following right-hand-rule, #488 - changed DIIS solver to assume the matrix is symmetric (it is)
- tbtncSileTBtrans and its derivates has changed, drastically.
This will accommodate changes related to #477 and #478.
Now
*_transmission
refers to energy resolved transmissions and*_current
reflects bias-window integrated quantities. The defaults and argument order has changed drastically, so users should adapt their scripts depending onsisl
version. A check can be made,if sisl.__version_tuple__[:3] >= (0, 13, 0):
- To streamline argument order the
*_ACO[OH]P
routines have changedelec
andE
argument order. This makes them compatible withorbital_transmission
etc.
- enabled parsing geometry.in files from FHIaims
- added
batched_indices
for memory-reduced location of array values - enabled manifold extractions
sisl.physics.yield_manifolds
- enabled center of mass for periodic systems (chooses best COM)
- enabled returning the overlap matrix from
berry_phase
- added
rocksalt
@tfrederiksen - slab geometry creations,
fcc_slab
,bcc_slab
androcksalt_slab
@tfrederiksen - added
Geometry.translate2uc
to shift everything into the unit-cell @tfrederiksen - added
Geometry.unrepeat
to reverserepeat
calls (and tosgeom
) - added
SparseGeometry.unrepeat
to reverserepeat
calls
- enabled reading HSX file version 1, #432
- major performance boost for reading GULP FC files
- cleaned mixing methods and decoupled the History and Mixers
- incorrect handling of
atoms
argument inGeometry.center
calls
- State*.outer corrected to the same interface as State*.inner
- all
sisl.geom
geometries are now callingoptimize_nsc
if needed SparseGeometry.cut
->SparseGeometry.untile
- much faster
- many more checks to warn about wrong usage
cut
is now deprecated (removed in 0.13)- changed the --cut flag in
sgeom
to--untile
, deprecated flag
- enabled in/out arguments to tbt siles (easier to remember meaning)
- return spin moment from SCF output files of Siesta
- read_fermi_level to siesta.PDOS files
- MacOS builds
sdata
handling of siesta.PDOS* files, much more versatily now- masking import of xarray
- Fixes to sisl.viz module related to 3.10 and other details
- Geometry.sub_orbital is added
- BrillouinZone.volume enables easy calculation of volumes for BZ integrals
- State.sub|remove are now allowed to be done inplace
- State.derivative can now correctly calculate 1st and 2nd order derivatives #406
- Enabled discontinuity jumps in band-structures (pass points as None)
- COOP and COHP calculations for eigenstates
- inverse participation ration calculations (with arbitrary q)
- origin point for mirror functionality (Geometry)
- degenerate_dir for
velocity
directions State.remove
complementary toState.sub
- copying Dispatchers for subclasses.
- dispatchers to
Shape
Spin.spinor
to get number of spinor componentssc
argument toxyzSile.read_geometry
for user defined cells- tiling a State object, #354 and #355
- replacing atoms in SparseOrbital geometries #139
- direction now accepts
abc
andxyz
keywords to retrieve vectors depending on direction input. - replacing atoms in SparseOrbital geometries #139
- reading from STRUCT_* files (Siesta input/output) #308
- reading the SuperCell block from fdf
- reading PAO.Basis blocks from both out and fdf files, almost complete functionality #90
- generic
transform
method for matrix transformations - doing ufunc.reduce on SparseCSR matrices; wrong values for e.g. np.prod, generally be CAUTIOUS with reduction operations
- transposing a SparseCSR matrix
- added pymatgen conversion (Geometry.to/new.pymatgen)
- atom indexing by shapes #337
sub_orbital
allows lists of orbitalsberry_phase
now works for non-orthogonal basis sets (uses Lowdin transformation) This may require sufficiently small dk for accurateness.degenerate
argument forconductivity
to enable decoupling of states- BandStructure.lineark now always starts from 0
- reading coordinates from siesta.out when bands are calculated #362
- complex warning for spin_moment #360 and #363
- partially fixed #102 (
wavefunction
forfxyz
outside box, related to #365 and how origin is interpreted in the code - non-collinear PDOS plotting
- improvement for BandStructure setup, arguments more stringent
- several fixes for
sisl.viz
; #368, #376 and #382 - empty array handlings in
_sanitize_*
#370 - ensured AtomicOrbital can be instantiated without specifying m (default to 0)
- fixed bug when copying orbitals
- fixed reading atomic labels in xsf files #402
- fixed hpc parameters #403
- order of arguments for
nanoribbon
it was not consistent with the others - removed cell argument in
Geometry.sub
- removed
Sile.exist
, refer toSile.file
which always will be apathlib.Path
instance berry_phase
now uses the gauge=R convention, the code became much simplerBrillouinZone.parametrize
function changed interface to allow more dimensionsEigenStateElectron.inner
does not use the overlap matrix by default, norm2 is for exactly this behaviour- changed license to MPLv2 makes toolboxes easier to contribute under different license
- renamed origo to origin, see #365
- default parallel calculations are disabled
- changed
State.align_*
routines to alignself
rather thanother
- doc fixes for recommending
python -m pip
- removed keywords align for State.inner|outer, manually use
align
if required - removed method
State.expectation
- calculation of scattering states and eigenchannels
- multiple variants of scattering state methods
-
Major addition: plotly backend for plotting and interaction with output. This is still a work in progress made by Pol Febrer. Many thanks to @pfebrer!
-
Added unzip argument to BZ.apply methods to unzip multiple return values, also added documentation to reflect this
-
Fixed reading data-arrays from Siesta-PDOS files
-
Enabled minimization method for basis information and pseudo generation
-
Enabled plotting grids using the command-line
-
Bug in how non-colinear matrices are dealt with, now fixed Thanks to Xe Hu for discovering this.
-
Allowed reading the geometry for supercell HSX files Atomic coordinates and nsc are determined from xij arrays
-
Basic implementation of Hermitian construct. It now ensures a correct Hermitian matrix for simple cases
-
Added more return from close/within, supercell offsets may be queried (ret_isc)
-
Added more transposing functionality for spin matrices
-
Fixed wfsxSileSiesta returning proper k-points if a geometry is passed (i.e. reduced k-points). Otherwise warns users
-
Huge performance increase for finalizing very large structures
-
Fixed writing %block in fdf files
-
Enabled reading Fermi level from VASP DOSCAR files
-
Cleaned siesta and VASP reading of completed jobs, #287
-
added Geometry.new allowing easy type-lookups to convert to Geometry e.g. Geometry.new("RUN.fdf") and Geometry.new(ase_atoms) automatically figures out which method to call and how to interpret the objects. added Geometry.to allowing easy type-lookups to convert to other objects #282
-
enabled calculating supercell matrices with phases, format=sc: returns in supercell matrix form (no, no_s)
-
removed support for int and long as matrix types, only float/complex
-
Enabled
sgrid
to write tables of data -
Merged spin_orbital_moment(deleted) and spin_moment with optional argument project
-
Enabled orbital resolved velocities
-
Added outSileSiesta.read_energy to read final energies in a property-dict (works both as a property (
energy.fermi
) and a dictionary (energy["fermi"]
) -
Ensured ghost atoms in Siesta are handled with separate class, AtomGhost, #249
-
Using
si.RealspaceSI
withunfold=(1,1,1)
no longer results innsc
on the given surface hamiltonian being set to(1,1,1)
. -
Added calculation of isosurfaces, #246
-
Added
sisl.WideBandSE
for self-energies with constant diagonals -
Enabled more user control over categories, #242
-
Improved interpolation function for Grid's, and also added filters
-
Bugfix for periodic directions for ASE conversion, #231
-
Fixed tuples for
_sanitize_atoms
, #233 -
Fixed reading correct unit from deltanc files, #234
-
Enabled berry-phase calculations for NC+SOC, #235
-
Added tiling to Grid, #238
-
Added Atoms.group_data which nicely splits an array holding orbital information into atomic contributions (a list since each sub-list may be unequal in length)
-
Many small bug-fixes and performance improvements
-
Exposing sisl_toolbox as a module for external contributions Now stuff contributed from 3rd parties can easily be included in a toolbox which is a separate module.
-
Changed asarray (as*) methods for SparseGeometry Now we have a dispatch class which enables one to store the behaviour as variables and then post-process
-
Using
*.geom
orgeometry.atom
is now deprecated, use*.geometry
andgeometry.atoms
instead (respectively) -
Added spin-rotation for density matrices, this will enable sisl to manipulate DM and write them for Siesta calculations
-
Enabled all numpy.ufuncs (np.exp(H))
-
Added nanoribbons construction (@tfrederiksen)
-
Internal change to pathlib for files and paths
-
Added velocity calculations for NC+SOC Hamiltonians
-
Sparse pattern transposes of non-full matrices, fixed bug
-
Changed Geometry.sort to be more diverse (this may break old code) This new way of sorting is way more flexible and allows very fine control, fixes #191, #197
-
Added a bilayer geometry which can create twisted bilayers #181, #186
-
Enabled VASP
*CAR
files to write/read dynamic specifications #185 -
Enabled
xarray.DataArray
returning from BrillouinZone objects #182 -
Several improvements to outSileSiesta.read_scf #174, #180
-
A huge performance increase for data extraction in tbtncSileTbtrans (thanks to Gaetano Calogero for finding the bottleneck)
-
Added preliminary usage of Mixers, primarily intented for extending sisl operations where SCF are used (may heavily change).
-
Lots of small bug-fixes
-
Now sisl is Python >=3.6 only, #162
This release was helped by the following committers (THANKS):
- Thomas Frederiksen
- Pol Febrer
- Jonas Lundholm Bertelsen
- Bernhard Kretz
-
fixed #160 by removing all(?) TRS k-points in a Monkhorst Pack grid
-
fixed repeat for SparseGeometryOrbital #161
-
changed lots of places for einsum in electron.py for increased performance
-
added AHC conductivity calculations
conductivity
(not tested) -
added Berry curvature calculations
berry_flux
(not tested) -
added Overlap class to directly use overlap matrices (without having a second matrix).
-
fixed geometry align issue when reading geometries from Siesta output #153
-
fixed pickling a sparse matrix #150
-
Fixed TSV.nc write-out for grid files (see poisson_explicit.py)
-
Fixed fermi level calculation for non-polarized calculations
-
Reverted Fermi calculation routine for more stable implementation
-
fixed DynamiclMatrix reading for number of atoms not divisable by 4 #145
A huge thanks to Jonas L. B. for fixes, suggestions etc.
-
Bug-fix for reading geometries in outSiesta
-
Enabled reading the fermi level from the output, fixes #126
-
Enabled Siesta STM and STS output
-
Fixed an inheritance issue in
axsfSile
which meant it was unusable until now -
Maintenance fix for looping sparse matrices. Now the default is to loop the sparse non-zero elements. If one wishes to loop all atoms/orbitals one should use
iter_orbitals()
NOTE: This may break some codes if they used loops on sparse matrices -
Fixed reading VASP CAR files with constraints (thanks to T. Frederiksen)
-
Added
overlap
method toGeometry
to find overlapping atoms between two geometries. -
Added Siesta LDOS charge handling
-
Changed edges method to not exclude it-self by default. This is because it is not intuitive given the default exclude=None
Note: this may break compatibility with other software/scripts.
-
Added mulliken charge calculations and orbital angular momentum for SO DM, fixes #136
-
Fixed reading overlap matrix in conjunction with DM from fdf-sile
-
Performance increase for the real-space self-energy calculations
-
Fixed transposing of the spin-box for NC and SO matrices
-
Enabled TRS handler for SO matrices, fixes #125
-
Enabled better b-casting assignments for sparse-matrices, fixes #134
-
Upgraded documentation to a layout that obeys numpydoc
-
Fixed reading ASE xyz outputs, thanksto JL. Bertelsen,
-
Fixed a typo in fdf reading onlyS, thanks to JL. Bertelsen, #135
-
Enabled reading arbitrary self-energy by requesting an energy and k-point from TSGF files.
-
Upgraded handling of TBT.*.nc files to conform with the >=Siesta-4.1-b5 releases where all files contain the same device + electrode meta-data.
-
Deprecated TBTGFSileTBtrans (use tbtgfSileTBtrans instead)
-
Forced align=False in inner such that users should take care of this
-
Added align_norm to swap states such that they more or less correspond to the same band (which should have a closer residual for on-site coefficients).
-
Removed norm2 and made norm equal to norm2 for states. This is the more natural thing, besides. Doing norm() ** 0.5 shouldn't be too much of a problem.
-
Officially added real-space self-energy calculations
-
Cleaned TBT vs. PHT for class name structures
-
Bugfix for reading MD output from Siesta out-files #130
-
Bugfix for tbtse files when requesting pivoting indices using this combination
in_device=True, sort=False
which in most cases return wrong indices, thanks to J. Bertelsen for bug-find! -
Added several routines for retrieving transposed coupling elements. When having connections
i -> j
it may be beneficial to easily get the transposed connectionj -> i
by taking into account the supercell.Geometry.a2transpose
enables this functionality making construct functions much simpler when having edges/boundaries. -
Bug-fix for reading white-space prefixed keywords in XSF files, #127
-
Performance increase for self-energy calculations for very small systems
-
Huge memory reduction for
Geometry.o2a
with very large system -
Enabled pickling on
BrillouinZone
objects -
Added
spin_moment
toHamiltonian
-
Removed
rotate[abc]
methods since they were cluttering the name-space Codes should simply replace with:geometry.rotate(angle, geometry.cell[{012}, :], *)
for the same effect.
-
Finally removed deprecated
write_geom
from the API -
Enabled calculation of
<S^2>
for spin-polarized calculations, this may be used for calculating spin-contaminations -
added checks for
SparseCSR
to disallow out-of-bounds keys -
Bug fixed for reading POSCAR files from VASP (only when multiple species are used in a non-ordered fashion)
-
added
sisl
command line utility, it is exactly the same assdata
-
Enabled pickling sparse matrices, this allows dask usage of sparse matrices
-
Performance increase for sparse matrix handling
-
Fixed a problem with Fortran IO + Jupyter notebooks, now the file-handles are re-used if a code block is terminated before closing the file
-
Added
SparseOrbital
append
+transpose
This enables appending Hamiltonian's (append) and makes hermiticity checks possible (transpose) -
Enabled complex averaged calculations using
oplist
Theoplist
object is a container allowing inter-element operations>>> l1 = oplist([0, 1]) >>> l2 = oplist([2, 3]) >>> l = l1 + l2 >>> print(l) [2, 4]
This is extremely handy for
BrillouinZone.asaverage
/assum
when calculating multiple values usingeigenstate
objects. -
Added reflection calculation to
tbtncSileTBtrans
-
Added more distribution functions (step and heaviside)
-
Removed numpy deprecated class numpy.matrix, now everything is array
-
Removed possibility of using
kavg=list(...)
due to complexity, now singlekavg
requests are not k-averaged. -
Bugfix in calculating
shot_noise
,noise_power
andfano
factors intbtncSileSiesta
They were only correct for Gamma-point calculations -
Fixed
*.EIG
sdata
processing when using--dos
-
Fixed reading geometries from grids from VASP (grid values were correct)
-
Toolboxes:
- Added a toolbox to calculate the Poisson solution for arbitrary electrodes for TranSiesta
-
Fixed temperature for phonon output pht*nc files
-
Added tbtprojncSileTBtrans sile for analyzing projected transmissions
-
Removed deprecated dhSileTBtrans
-
Bug fix for binary grid files with Siesta and also reads using fdf-files
-
Changed default self-energy eta values to 1e-4 eV
-
Added Zak-phase calculations (thanks to T. Frederiksen)
-
Updated lots of State methods
-
added Bloch expansion class which can expand any method
-
self-energy calculations:
- Much faster
- enabled left/right self-energies in one method
-
fixed AtomicOrbital copies
-
enabled TSGF reads
-
Added noise-power calculations for TBT.nc files
-
Fixed TBT.SE.nc files, units and scattering matrix retrieval
-
added more VASP files
-
Fixes for the GULP dynamical matrix reads
-
Enabled preliminary reads of OpenMX input file
-
Enabled DOS calculation for the eigenvalue files
-
Added Berry-phase calculation for orthogonal basis sets
-
Added velocity calculation of electronic eigenstates
-
Enabled effective mass tensor in electronic eigenstates (un-tested)
-
High performance increase by moving stuff to Cython.
-
Added Siesta interaction tutorials
-
Added orthogonality checks when reading sparse matrices
-
Lots of fixes for the fdf-file
-
Added Mulliken calculation in DensityMatrix/EnergyDensityMatrix
-
Enabled reading phonons from FC files
-
Added named-groups which enables accessing groups of atoms by names.
Geometry['Hello'] = [2, 3, 4]
-
Changed Hessian to DynamicalMatrix to clarify the units
-
Added new units class to handle complex units.
-
Enabled a Phonon class to calculate group velocities of phonons, DOS and PDOS, displacements
-
Bug-fixes for Siesta binary writes, now the supercell format is always Siesta compliant.
-
Enabled replacing k-points in MonkhorstPack grids.
-
Enabled calculation of band-velocities from eigenstates
-
Made better progress-bars. Using eta= now relies on tqdm It is however still an optional dependency.
-
Fixed Gamma-point periodic wavefunction storage. Creating grids with wave-functions is fully functional for arbitrarily big supercells.
-
BrillouinZone objects:
-
Renamed PathBZ to BandStructure
-
Renamed MonkhorstPackBZ to MonkhorstPack
-
Enabled MonkhorstPack symmetry. This will reduce the number of k-points to roughly half (note symmetry is by default on)
-
Forced MonkhorstPack to create a k-grid which is Gamma centered
-
-
Shapes (backwards compatibility broken)
-
Complete re-write of Shapes
-
Skewed Cuboids, Ellipsoids
-
Set combinations of Shapes (unions, difference sets, etc.)
-
-
Grid
-
Enabled Grid.index for shapes.
-
Fixed grid initialization to create grid spacings fixed by a real. I.e. the voxel spacing.
>>> Grid([10, 10, 10]) # 10 points per lattice vector >>> Grid(0.1) # 0.1 Angstrom spacing
-
Enabled plotting wavefunctions on grids.
-
Enabled plotting charge density on grids.
-
-
Enabled tqdm usage for progressbar. It is fast and easy to use and a small requirement. (still optional)
-
Added intrinsic Sisl exceptions which will be used throughout (at some point)
-
Removed deprecated TightBinding class (use Hamiltonian instead)
-
Added many SislWarning raises which are used to notify the user of potentially important things (say if sisl knows there should be a unit associated but it couldn't find it).
-
Added TSDE file reading in sisl.
-
Siesta reading of grid-related data is now much smarter. It will try and recognize the units of the data so the units become sisl intrinsics (Ry -> eV, Bohr -> Ang, etc.). This means that typically one does not need to do manual unit-conversion. There are however a few cases where sisl cannot figure out the units. Particularly if the files are renamed.
-
Added a new class EigenSystem which holds information regarding eigenvalues and eigenvectors.
- Currently an EigenState class is also enabled which can currently be used to calculate wavefunctions, DOS, PDOS and more to come.
-
Fixed lots of bugs in fdf-reading quantities. Now one is also able to read Hamiltonian and other physical quantities from the fdf-object directly. There is pre-defined orders of which files to read from if there are multiple files eligeble.
Reading the geometry now defaults to the fdf file, but one can query the output files by a boolean.
-
Enabled PDOS calculations for the Hamiltonian. Together with the MonkhorstPack class one can easily calculate k-averaged PDOS quantities.
-
Fixed cube reading/writing of multi-column data.
-
Added siesta PDOS xml parsing, currently this is only scriptable but it manages easy extraction of quantities without the PDOSXML utility. This also enables retrieving the PDOS as an xarray.DataArray.
-
Fixed a bug in writing XV files (only for -100/-200 species)
-
TBtrans / TBT.nc file:
-
Added TBT.SE.nc file to enable easy extraction of self-energies from TBtrans
-
Added COOP and COHP extraction to the TBT.nc files.
-
Added DM and ADM extraction to the TBT.nc files.
-
Reorganized the TBtrans netcdf files (internal changes only)
-
Added shot-noise calculation (and Fano factor). Currently un-tested!
-
-
Several added files
- Various minor bug-fixes
-
Fixed scaling of bond-currents in case 'all' is used, makes comparison with '+' and '-' easier.
-
Updated defaults in bond_current to '+' such that only forward going electrons are captured.
-
Updated defaults in vector_current to '+' such that only forward going electrons are captured.
-
Enabled reading a tabular data-file
-
Lots of updates to the spin-class. It should now be more coherent.
-
Added rij and Rij to the sparse_geometry classes to extract orbital or atomic distance matrices (returing the same sparsity pattern).
-
Renamed
which
keyword inGeometry.center
towhat
-
Added uniq keyword to o2a for better handling of orbitals -> atoms.
-
Fixed a performance bottleneck issue related to the
scipy.linalg.solve
routine which was changed since 0.19.0. -
Changed internal testing scheme to
pytest
-
Lots of bug-fixes here and there
-
Geometry files used in the command-line has updated these arguments:
- tile
- repeat
- rotate
The order of the arguments are interchanged to be similar to the scripting capabilities.
Also fixed an issue related to moving atoms into the unit-cell.
-
Enabled deleting supercell elements of a sparse Geometry. This will come in handy when calculating the self-energies and Green functions. I.e. Hamiltonian.set_nsc(...) will truncate entries based on the new supercell.
-
Preliminary testing of reading Siesta binary output (.RHO, .VT, etc.)
-
Added parsing the Siesta EIG file (easy plotting, reading in Python)
-
Changed interface for BrillouinZone objects. Now a BrillouinZone accepts any object which has cell/rcell entries. Any function call on the BrillouinZone object will transfer the call to the passed object and evaluate that function for all k-points in the BrillouinZone.
-
sisl.io.siesta.tbtrans
-
Added current calculator to TBT.nc sile to calculate the current as TBtrans does it (this requires the latest commit in SIESTA which defines the chemical potential and electronic structure of all electrodes).
-
Bug-fixes for TBT.nc sile, the bond-currents for multi-orbital systems were in some cases wrong.
-
Huge performance increase for TBT.nc data processing. Now the majority of routines are based on array-indexing, rather than sparse loops.
-
Changed the DOS retrieval functions to be more flexible. The default is now to return the summed DOS across the selected atoms.
-
Added a TBTGFSileSiesta which enables one to create external self-energies to be read in by TBtrans (complete electrode control).
-
Added
deltancSileSiesta
as a replacement fordHncSileSiesta
, TBtrans 4.1b4 will have two delta terms, dH (adds to bond-currents) and dSigma (does not add to bond-currents). -
BEWARE, lots of defaults has changed in this release.
-
-
Hamiltonian.tile is now even faster, only utilizing intrinsic numpy array functionality.
-
Greatly speeded up Hamiltonian.remove/sub functions. Now there are no for-loops in the remove/sub routines which will greatly increase performance. It will now be much faster to generate the Hamiltonian for a small reference cell, tile/repeat it, remove atoms.
-
Added the following routines:
SuperCell.fit
routine to determine a new supercell object such that a given set of coordinates are all within AND periodic in the new supercell.SuperCell.parallel
to check whether two objects have parallel latticevectors.Geometry.distance
returns a list of distances from a given set of atoms. I.e. to determine a set of distances required for a subsequent close call. This routine can also be used to group neighbouring atoms in a common fashion.Geometry.optimize_nsc
loops all atoms and minimizesnsc
in case one is not sure of the interaction range.Hamiltonian.shift
enables the shift of the entire electronic structure Fermi-level.- Added new flag to
Hamiltonian.Hk
routinesformat={'csr', 'array', 'dense', ...}
to ensure a consistent return of the data-type.
-
Bug fix for dHncSileSiesta for multiple levels.
-
Performance boost for the sub and remove functions for the Hamiltonian objects. Instead of creating the geometry first, it may now be much faster to generate the small Hamiltonian, tile -> repeat -> sub -> remove.
-
Performance boost for the tile and repeat functions for the Hamiltonian objects. They are now the preferred method for creating large systems.
-
Bug fixed when having extremely long atomic ranges and using tile/repeat. The number of supercells was too large. It did not affect anything, but it was inconsistent.
-
Enabled reading the density matrix and energy density matrix from siesta.
-
Addition of a PerformanceSelector class which enables a dynamic selection of the best routine.
Currently this is enabled in the SparseOrbitalBZ class where constructing a matrix @ k can be done in numerous ways.
-
Bug fixed in supercell specification of the Hamiltonian:
>>> H[io, jo, (-1, 0, 0)]
now works in all cases.
-
Spin-orbit H(k) has been enabled
-
Fixed reading the <>.nc file from SIESTA, the non-zero elements count was wrong.
-
Now H(k) has been tested for non-colinear and spin-orbit coupling and one can now use sisl to perform non-colinear and spin-orbit coupling calculations.
-
API change, all dR keywords has been changed to R for consistency and reduction of ambiguity. Also the
Atoms.dR
is now referred to asAtoms.maxR()
to indicate its meaning.This may break old scripts if one use the
dR
keyword in arguments.
-
Added BrillouinZone class to easily create BrillouinZone plots etc. When calculating the eigenspectrum of a Hamiltonian one may pass the BrillouinZone object instead of the k-point to retrieve all eigenvalues for the k-points in the BrillouinZone object. Say for a PathBZ one can now easily retrieve the band-structure.
-
Enabled specification of Hamiltonian connections across supercells via a tuple index (as the last index):
>>> H[io, jo, (-1, 0, 0)]
Thus connecting orbital
io
andjo
across the -1 first lattice vector -
Enabled tbtrans files to attach a geometry (to get correct species).
-
API change of:
read/write_geom => read/write_geometry read/write_sc => read/write_supercell read/write_es => read/write_hamiltonian
Moved
quantity
tophysics
. -
Enabled slice deletion in
SparseCSR
Enabled eliminate_zeros() to remove unneeded values.
-
Added ScaleUp compatibility. sisl now acceps ScaleUp files which is a 2nd principles code for large scale calculations using Wannier functions.
-
Added Hamiltonian.sub/remove/tile for easy extension of Hamiltonian without having to construct the larger geometries. This should speed up the creation of really large structures as one may then simply "update" the Hamiltonian elements subsequently.
-
Fixed bug in __write_default (should have been _write_default)
-
API change in
close
functions, now ret_coord => ret_xyz, ret_dist => ret_rij -
Added
SparseCSR
math operations work on otherSparseCSR
matrices Thus one may now do:>>> a, b = SparseCSR(...), SparseCSR(...) >>> aMb, aPb = a * b, a + b
Which makes many things much easier. If this is used, you are encouraged to assert that the math is correct. Currently are the routines largely untested. Assistance is greatly appreciated in creating tests.
-
Geometries now always create a supercell. This was not the case when an atom with no defined orbital radius was used. Now this returns a supercell with 10 A of vacuum along each Cartesian direction.
-
Fixed reading _hr.dat from Wannier90, now the band-structure of SrTiO3 (Junquera's test example) is correct.
-
Speeded up tbtrans.py analyzing methods enourmously by introducing faster sparse iterators. Now one can easily perform data-analysis on systems in excess of 10.000 atoms very fast.
-
Added the TBT.AV.nc file which is meant to be created by
sisl
from the TBT.nc files (i.e. create the k-averaged output). This enables users to run tbtrans, create the k-averaged output, and then delete the old file to heavily reduce disk-usage.An example:
tbtrans RUN.fdf > TBT.out sdata siesta.TBT.nc --tbt-av rm siesta.TBT.nc
after this
siesta.TBT.AV.nc
exists will all k-averaged quantites. If one is not interested in k-resolved quantities this may be very interesting. -
Updated the TBT.nc sile for improved readability.
-
Easier script data-extraction from TBT.nc files due to easier conversion between atomic indices and pivoting orbitals.
For this:
-
a2p returns the pivoting indices for the given atoms (complete set)
-
o2p returns the pivoting indices for the given orbitals
-
Added
atom
keyword for retrieving DOS for a given set of atoms -
sdata
andTBT.nc
files now enable the creation of the TBT.AV.nc file which is the k-averaged file of TBT.nc
-
-
Faster bond-current algorithms (faster iterator)
-
Initial template for TBT.Proj files for sdata processing
-
Geometry:
-
Enabled multiplying geometries with integers to emulate
repeat
ortile
functions:>>> geometry * 2 == geometry.tile(2, 0).tile(2, 1).tile(2, 2) >>> geometry * [2, 1, 2] == geometry.tile(2, 0).tile(2, 2) >>> geometry * [2, 2] == geometry.tile(2, 2) >>> geometry * ([2, 1, 2], 'repeat') == geometry.repeat(2, 0).repeat(2, 2) >>> geometry * ([2, 1, 2], 'r') == geometry.repeat(2, 0).repeat(2, 2) >>> geometry * ([2, 0], 'r') == geometry.repeat(2, 0) >>> geometry * ([2, 2], 'r') == geometry.repeat(2, 2)
This may be considered an advanced feature but useful nonetheless.
-
Enabled "adding" geometries in a similar way as multiplication I.e. the following applies:
>>> A + B == A.add(B) >>> A + (B, 1) == A.append(B, 1) >>> A + (B, 2) == A.append(B, 2) >>> (A, 1) + B == A.prepend(B, 1)
-
Added
origo
andatom
argument to rotation functions. Previously this could be accomblished by:rotated = geometry.move(-origo).rotate(...).move(origo)
while now it is:
rotated = geometry.rotate(..., origo=origo)
The origo argument may also be a single integer in which case the rotation is around atom
origo
.Lastly the
atom
argument enables only rotating a sub-set of atoms. -
Geometry[..] is now calling axyz if
..
is pure indices, if it is aslice
it does not work with super-cell indices -
Added
rij
functions to the Geometry for retrieving distances between two atoms (orij
for orbitals) -
Renamed iter_linear to iter
-
Added argument to iter_species for only looping certain atomic indices
-
Added iter_orbitals which returns an iterator with atomic and associated orbitals. The orbitals are with respect to the local orbital indices on the given atom
>>> for ia, io in Geometry.iter_orbitals(): >>> Geometry.atom[ia].R[io]
works, while
>>> for ia, io in Geometry.iter_orbitals(local=False): >>> Geometry.atom[ia].R[io]
does not work because
io
is globally defined. -
Changed argument name for
coords
,atom
instead of the oldidx
. -
Renamed function
axyzsc
toaxyz
-
-
SparseCSR:
-
Added
iter_nnz(i=None)
which loops on sparse elements connecting to rowi
(or default to loop on all rows and columns). -
ispmatrix
to iterate through ascipy.sparse.*_matrix
(and theSparseCSR
matrix).
-
-
Hamiltonian:
-
Added
iter_nnz
which is theHamiltonian
equivalent ofSparseCSR.iter_nnz
. It enables explicit looping on atomic couplings, or orbital couplings. I.e. one may specify a subset of atoms or orbitals to loop over. -
Preliminary implementation of the non-collinear spin-case. Needs testing.
-
-
Fix a bug when reading non-Gamma TSHS files, now the supercell information is correct.
-
tbtncSileSiesta now distinguishes between: electronic_temperature [K] and kT [eV] where the units are not the same.
-
Fixed TBT_DN.nc TBT_UP.nc detection as a
Sile
-
Added information printout for the TBT.nc files
sdata siesta.TBT.nc --info
will print out what information is contained in the file.
-
Atoms
overhauled with a lot of the utility routines inherent to theGeometry
object. It is now much faster to perform operations on this object. -
The FDF sile now allows setting and retrieving variables from the fdf file. Hence one may now set specific fdf flags via:
sdata RUN.fdf --set SolutionMethod Transiesta
-
Changed default output precision for TXT files to .8f. Additionally one may use flag
--format
insgeom
to define the precision. -
Shape
have been added. There are now several Shapes which may be used to easily find atoms within a given Shape. This should in principle allow construction of very complex Shapes and easier construction of complex Hamiltonians
This release introduces many API changes and a much more stream-lined interface for interacting with sisl.
You are heavily encouraged to update your distribution.
Here is a compressed list of changes:
-
sdata is now an input AND output dependent command. It first reads the input and output files, in a first run, then it determines the options for the given set of files. Secondly, the sdata command uses "position dependent" options. This means that changing the order of options may change the output.
-
tbtncSile
- Correct vector currents (for xsf files)
- bug-fix for Gamma-only calculations
- returned DOS is now correctly in 1/eV (older versions returned 1/Ry)
- fixed sdata atomic[orbital] ranges such that, e.g.
--atom [1-2][3-5]
(for atom 1 and 2 and only orbitals 3, 4 and 5 on those atoms.) - DOS queries now has an extra argument (E) which returns only for the given energy.
- When storing tables in sdata this now adds information regarding each column at the top (instead of at the bottom). Furthermore, the information is more descriptive
-
Changed all
square
named arguments toorthogonal
-
Added nsc field to xyz files (to retain number of supercells)
-
Added
move
function for geometry (same as translate) -
Added
prepend
function, equivalent toappend
, but adding the atoms in the beginning instead of the end -
Fixed many bugs related to the use of Python-ranges (as opposed to numpy ranges)
-
SparseCSR now enables operations:
a = SparseCSR(...) a = a * 2 + 2
is now viable. This enables easy scaling, translation etc. using the sparse matrix format (very handy for magnetic fields).
-
Enabled
del
for SparseCSR, i.e.del SparseCSR(..)[0, 1]
will remove the element, completely. -
Enabled reading of the TSHS file from SIESTA 4.1, now we may easily interact with SIESTA.
-
Moved version.py to info.py
-
Moved scripts to
entry_points
, this makes scripts intrinsic in the module and one may import and use the commands as their command-line equivalents. -
Hamiltonian.construct now takes a single argument which is the function for the inner loop. The old behaviour may be achieved by doing either:
>>> func = Hamiltonian.create_construct(R, param) >>> Hamiltonian.construct(func)
or
>>> Hamiltonian.construct((R, param))
-
The atoms contained in the Geometry are now not duplicated in case of many similar Atom objects. This should reduce overhead and increase throughput. However, the efficiency is not optimal yet.
-
Added many more tests, thus further stabilizing sisl
I would really like help with creating more tests! Please help if you can!