hexrd.material.crystallography module
- hexrd.material.crystallography.LoadFormFactorData()[source]
Script to read in a csv file containing information relating the magnitude of Q (sin(th)/lambda) to atomic form factor
Notes: Atomic form factor data gathered from the International Tables of Crystallography:
Brown, A. G. Fox, E. N. Maslen, M. A. O’Keefec and B. T. M. Willis,
- “Chapter 6.1. Intensity of diffracted intensities”, International Tables
for Crystallography (2006). Vol. C, ch. 6.1, pp. 554-595
- class hexrd.material.crystallography.PlaneData(hkls, *args, **kwargs)[source]
Bases:
object
Careful with ordering: Outputs are ordered by the 2-theta for the hkl unless you get self.__hkls directly, and this order can change with changes in lattice parameters (lparms); setting and getting exclusions works on the current hkl ordering, not the original ordering (in self.__hkls), but exclusions are stored in the original ordering in case the hkl ordering does change with lattice parameters
if not None, tThWidth takes priority over strainMag in setting two-theta ranges; changing strainMag automatically turns off tThWidth
- calcStructFactor(atominfo)[source]
Calculates unit cell structure factors as a function of hkl
USAGE:
FSquared = calcStructFactor(atominfo,hkls,B)
INPUTS:
1) atominfo (m x 1 float ndarray) the first threee columns of the matrix contain fractional atom positions [uvw] of atoms in the unit cell. The last column contains the number of electrons for a given atom
2) hkls (3 x n float ndarray) is the array of Miller indices for the planes of interest. The vectors are assumed to be concatenated along the 1-axis (horizontal)
3) B (3 x 3 float ndarray) is a matrix of reciprocal lattice basis vectors,where each column contains a reciprocal lattice basis vector ({g}=[B]*{hkl})
OUTPUTS:
1) FSquared (n x 1 float ndarray) array of structure factors, one for each hkl passed into the function
- exclude(dmin=None, dmax=None, tthmin=None, tthmax=None, sfacmin=None, sfacmax=None, pintmin=None, pintmax=None)[source]
Set exclusions according to various parameters
Any hkl with a value below any min or above any max will be excluded. So to be included, an hkl needs to have values between the min and max for all of the conditions given.
Note that method resets the tThMax attribute to None.
PARAMETERS
- dmin: float > 0
minimum lattice spacing (angstroms)
- dmax: float > 0
maximum lattice spacing (angstroms)
- tthmin: float > 0
minimum two theta (radians)
- tthmax: float > 0
maximum two theta (radians)
- sfacmin: float > 0
minimum structure factor as a proportion of maximum
- sfacmax: float > 0
maximum structure factor as a proportion of maximum
- pintmin: float > 0
minimum powder intensity as a proportion of maximum
- pintmax: float > 0
maximum powder intensity as a proportion of maximum
- property exclusions
- getDD_tThs_lparms()[source]
derivatives of tThs with respect to lattice parameters; have not yet done coding for analytic derivatives, just wimp out and finite difference
- getHKLID(hkl, master=False)[source]
Return the unique ID of a list of hkls.
Parameters
- hklint | tuple | list | numpy.ndarray
The input hkl. If an int, or a list of ints, it just passes through (FIXME). If a tuple, treated as a single (h, k, l). If a list of lists/tuples, each is treated as an (h, k, l). If an numpy.ndarray, it is assumed to have shape (3, N) with the N (h, k, l) vectors stacked column-wise
- masterbool, optional
If True, return the master hklID, else return the index from the external (sorted and reduced) list.
Returns
- retvallist
The list of requested hklID values associate with the input.
Notes
TODO: revisit this weird API???
Changes:
2020-05-21 (JVB) – modified to handle all symmetric equavlent reprs.
- getHKLs(*hkl_ids, **kwargs)[source]
Returns the powder HKLs subject to specified options.
Parameters
- *hkl_idsint
Optional list of specific master hklIDs.
- **kwargsdict
- One or more of the following keyword arguments:
- asStrbool
If True, return a list of strings. The default is False.
- thisTThscalar | None
If not None, only return hkls overlapping the specified 2-theta (in radians). The default is None.
- allHKLsbool
If True, then ignore exlcusions. The default is False.
Raises
- TypeError
If an unknown kwarg is passed.
- RuntimeError
If an invalid hklID is passed.
Returns
- retvallist | numpy.ndarray
Either a list of hkls as strings (if asStr=True) or a vstacked array of hkls.
Notes
- !!! the shape of the return value when asStr=False is the _transpose_
of the typical return value for self.get_hkls() and self.hkls! This _may_ change to avoid confusion, but going to leave it for now so as not to break anything.
- 2022/08/05 JVB:
Added functionality to handle optional hklID args
Updated docstring
- getMergedRanges(cullDupl=False)[source]
return indices and ranges for specified planeData, merging where there is overlap based on the tThWidth and line positions
- getSymHKLs(asStr=False, withID=False, indices=None)[source]
new function that returns all symmetric hkls
- getTThRanges(strainMag=None, lparms=None)[source]
Return 2-theta ranges for included hkls
return array is n x 2
- get_hkls()[source]
do not do return self.__hkls, as everywhere else hkls are returned in 2-theta order; transpose is to comply with lparm convention
- property hedm_intensity
- property hkls
do not do return self.__hkls, as everywhere else hkls are returned in 2-theta order; transpose is to comply with lparm convention
- property latVecOps
gets lattice vector operators as a new (deepcopy)
- property laueGroup
This is the Schoenflies tag
- property lparms
- static makePlaneData(hkls, lparms, qsym, symmGroup, strainMag, wavelength)[source]
hkls : need to work with crystallography.latticePlanes lparms : need to work with crystallography.latticePlanes laueGroup : see symmetry module wavelength : wavelength strainMag : swag of strian magnitudes
- static makeScatteringVectors(hkls, rMat_c, bMat, wavelength, chiTilt=None)[source]
Static method for calculating g-vectors and scattering vector angles for specified hkls, subject to the bragg conditions specified by lattice vectors, orientation matrix, and wavelength
FIXME: must do testing on strained bMat
- property powder_intensity
- set_laue_and_lparms(laueGroup, lparms)[source]
Set the Laue group and lattice parameters simultaneously
When the Laue group changes, the lattice parameters may be incompatible, and cause an error in self.__calc(). This function allows us to update both the Laue group and lattice parameters simultaneously to avoid this issue.
- property strainMag
- property structFact
- property tThMax
- property wavelength
- hexrd.material.crystallography.RetrieveAtomicFormFactor(elecNum, magG, sinThOverLamdaList, ffDataList)[source]
Interpolates between tabulated data to find the atomic form factor for an atom with elecNum electrons for a given magnitude of Q
USAGE:
ff = RetrieveAtomicFormFactor(elecNum,magG,sinThOverLamdaList,ffDataList)
INPUTS:
elecNum, (1 x 1 float) number of electrons for atom of interest
magG (1 x 1 float) magnitude of G
sinThOverLamdaList (n x 1 float ndarray) form factor data is tabulated in terms of sin(theta)/lambda (A^-1).
ffDataList (n x m float ndarray) form factor data is tabulated in terms of sin(theta)/lambda (A^-1). Each column corresponds to a different number of electrons
OUTPUTS:
ff (n x 1 float) atomic form factor for atom and hkl of interest
NOTES: Data should be calculated in terms of G at some point
- hexrd.material.crystallography.convert_MillerBravias_direction_to_Miller(UVW)[source]
Converts 4-index hexagonal Miller-Bravais direction indices to 3-index Miller direction indices.
Parameters
- UVWarray_like
The (n, 3) array of non-redundant Miller-Bravais direction indices to convert.
Returns
- numpy.ndarray
The (n, 3) array of Miller direction indices associated with the input Miller-Bravais indices.
Notes
NOT for plane normals!!!
- hexrd.material.crystallography.convert_Miller_direction_to_MillerBravias(uvw, suppress_redundant=True)[source]
Converts 3-index hexagonal Miller direction indices to 4-index Miller-Bravais direction indices.
Parameters
- uvwarray_like
The (n, 3) array of 3-index hexagonal Miller indices to convert.
- suppress_redundantbool, optional
Flag to suppress the redundant 3rd index. The default is True.
Returns
- numpy.ndarray
The (n, 3) or (n, 4) array – depending on kwarg – of Miller-Bravis components associated with the input Miller direction indices.
Notes
NOT for plane normals!!!
- hexrd.material.crystallography.convert_Miller_direction_to_cartesian(uvw, a=1.0, c=1.0, normalize=False)[source]
Converts 3-index hexagonal Miller direction indices to components in the crystal reference frame.
Parameters
- uvwarray_like
The (n, 3) array of 3-index hexagonal indices to convert.
- ascalar, optional
The a lattice parameter. The default value is 1.
- cscalar, optional
The c lattice parameter. The default value is 1.
- normalizebool, optional
Flag for whether or not to normalize output vectors
Returns
- numpy.ndarray
The (n, 3) array of cartesian components associated with the input direction indices.
Notes
The [uv.w] the Miller-Bravais convention is in the hexagonal basis {a1, a2, a3, c}. The basis for the output, {o1, o2, o3}, is chosen such that
o1 || a1 o3 || c o2 = o3 ^ o1
- hexrd.material.crystallography.cosineXform(a, b, c)[source]
Spherical trig transform to take alpha, beta, gamma to expressions for cos(alpha*). See ref below.
- [1] R. J. Neustadt, F. W. Cagle, Jr., and J. Waser, ``Vector algebra and
the relations between direct and reciprocal lattice quantities’’. Acta Cryst. (1968), A24, 247–248
- hexrd.material.crystallography.getDparms(lp, lpTag, radians=True)[source]
Utility routine for getting dparms, that is the lattice parameters without symmetry – ‘triclinic’
- hexrd.material.crystallography.getFriedelPair(tth0, eta0, *ome0, **kwargs)[source]
Get the diffractometer angular coordinates in degrees for the Friedel pair of a given reflection (min angular distance).
AUTHORS:
Bernier – 10 Nov 2009
USAGE:
- ome1, eta1 = getFriedelPair(tth0, eta0, *ome0,
display=False, units=’degrees’, convention=’hexrd’)
INPUTS:
tth0 is a list (or ndarray) of 1 or n the bragg angles (2theta) for the n reflections (tiled to match eta0 if only 1 is given).
eta0 is a list (or ndarray) of 1 or n azimuthal coordinates for the n reflections (tiled to match tth0 if only 1 is given).
ome0 is a list (or ndarray) of 1 or n reference oscillation angles for the n reflections (denoted omega in [1]). This argument is optional.
Keyword arguments may be one of the following:
Keyword Values|{default} Action ————– ————– ————– ‘display’ True|{False} toggles display to cmd line ‘units’ ‘radians’|{‘degrees’} sets units for input angles ‘convention’ ‘fable’|{‘hexrd’} sets conventions defining
the angles (see below)
- ‘chiTilt’ None the inclination (about Xlab) of
the oscillation axis
OUTPUTS:
ome1 contains the oscialltion angle coordinates of the Friedel pairs associated with the n input reflections, relative to ome0 (i.e. ome1 = <result> + ome0). Output is in DEGREES!
eta1 contains the azimuthal coordinates of the Friedel pairs associated with the n input reflections. Output units are controlled via the module variable ‘outputDegrees’
NOTES:
- !!!: The ouputs ome1, eta1 are written using the selected convention, but
the units are alway degrees. May change this to work with Nathan’s global…
- !!!: In the ‘fable’ convention [1], {XYZ} form a RHON basis where X is
downstream, Z is vertical, and eta is CCW with +Z defining eta = 0.
- !!!: In the ‘hexrd’ convention [2], {XYZ} form a RHON basis where Z is
upstream, Y is vertical, and eta is CCW with +X defining eta = 0.
REFERENCES:
- [1] E. M. Lauridsen, S. Schmidt, R. M. Suter, and H. F. Poulsen,
``Tracking: a method for structural characterization of grains in powders or polycrystals’’. J. Appl. Cryst. (2001). 34, 744–750
- [2] J. V. Bernier, M. P. Miller, J. -S. Park, and U. Lienert,
``Quantitative Stress Analysis of Recrystallized OFHC Cu Subject to Deformed In Situ’’, J. Eng. Mater. Technol. (2008). 130. DOI:10.1115/1.2870234
- hexrd.material.crystallography.hexagonalIndicesFromRhombohedral(hkl)[source]
converts rhombohedral hkl to hexagonal indices
- hexrd.material.crystallography.latticeParameters(lvec)[source]
Generates direct and reciprocal lattice vector components in a crystal-relative RHON basis, X. The convention for fixing X to the lattice is such that a || x1 and c* || x3, where a and c* are direct and reciprocal lattice vectors, respectively.
- hexrd.material.crystallography.latticePlanes(hkls, lparms, ltype='cubic', wavelength=1.54059292, strainMag=None)[source]
Generates lattice plane data in the direct lattice for a given set of Miller indices. Vector components are written in the crystal-relative RHON basis, X. The convention for fixing X to the lattice is such that a || x1 and c* || x3, where a and c* are direct and reciprocal lattice vectors, respectively.
USAGE:
planeInfo = latticePlanes(hkls, lparms, **kwargs)
INPUTS:
hkls (3 x n float ndarray) is the array of Miller indices for the planes of interest. The vectors are assumed to be concatenated along the 1-axis (horizontal).
lparms (1 x m float list) is the array of lattice parameters, where m depends on the symmetry group (see below).
The following optional keyword arguments are recognized:
- *) ltype=(string) is a string representing the symmetry type of
the implied Laue group. The 11 available choices are shown below. The default value is ‘cubic’. Note that each group expects a lattice parameter array of the indicated length and order.
latticeType lparms ———– ———— ‘cubic’ a ‘hexagonal’ a, c ‘trigonal’ a, c ‘rhombohedral’ a, alpha (in degrees) ‘tetragonal’ a, c ‘orthorhombic’ a, b, c ‘monoclinic’ a, b, c, beta (in degrees) ‘triclinic’ a, b, c, alpha, beta, gamma (in degrees)
- *) wavelength=<float> is a value represented the wavelength in
Angstroms to calculate bragg angles for. The default value is for Cu K-alpha radiation (1.54059292 Angstrom)
*) strainMag=None
OUTPUTS:
planeInfo is a dictionary containing the following keys/items:
- normals (3, n) double array array of the components to the
unit normals for each {hkl} in X (horizontally concatenated)
- dspacings (n, ) double array array of the d-spacings for
each {hkl}
- 2thetas (n, ) double array array of the Bragg angles for
each {hkl} relative to the specified wavelength
NOTES:
- *) This function is effectively a wrapper to ‘latticeVectors’.
See ‘help(latticeVectors)’ for additional info.
- *) Lattice plane d-spacings are calculated from the reciprocal
lattice vectors specified by {hkl} as shown in Appendix 1 of [1].
REFERENCES:
- [1] B. D. Cullity, ``Elements of X-Ray Diffraction, 2
ed.’’. Addison-Wesley Publishing Company, Inc., 1978. ISBN 0-201-01174-3
- hexrd.material.crystallography.latticeVectors(lparms, tag='cubic', radians=False, debug=False)[source]
Generates direct and reciprocal lattice vector components in a crystal-relative RHON basis, X. The convention for fixing X to the lattice is such that a || x1 and c* || x3, where a and c* are direct and reciprocal lattice vectors, respectively.
USAGE:
lattice = LatticeVectors(lparms, <symmTag>)
INPUTS:
lparms (1 x n float list) is the array of lattice parameters, where n depends on the symmetry group (see below).
symTag (string) is a case-insensitive string representing the symmetry type of the implied Laue group. The 11 available choices are shown below. The default value is ‘cubic’. Note that each group expects a lattice parameter array of the indicated length and order.
latticeType lparms ———– ———— ‘cubic’ a ‘hexagonal’ a, c ‘trigonal’ a, c ‘rhombohedral’ a, alpha (in degrees) ‘tetragonal’ a, c ‘orthorhombic’ a, b, c ‘monoclinic’ a, b, c, beta (in degrees) ‘triclinic’ a, b, c, alpha, beta, gamma (in degrees)
OUTPUTS:
lattice is a dictionary containing the following keys/items:
- F (3, 3) double array transformation matrix taking
componenents in the direct lattice (i.e. {uvw}) to the reference, X
- B (3, 3) double array transformation matrix taking
componenents in the reciprocal lattice (i.e. {hkl}) to X
- BR (3, 3) double array transformation matrix taking
componenents in the reciprocal lattice to the Fable reference frame (see notes)
- U0 (3, 3) double array transformation matrix
(orthogonal) taking componenents in the Fable reference frame to X
vol double the unit cell volume
- dparms (6, ) double list the direct lattice parameters:
[a b c alpha beta gamma]
- rparms (6, ) double list the reciprocal lattice
parameters: [a* b* c* alpha* beta* gamma*]
NOTES:
- *) The conventions used for assigning a RHON basis,
X -> {x1, x2, x3}, to each point group are consistent with those published in Appendix B of [1]. Namely: a || x1 and c* || x3. This differs from the convention chosen by the Fable group, where a* || x1 and c || x3 [2].
- *) The unit cell angles are defined as follows:
alpha=acos(b’*c/|b||c|), beta=acos(c’*a/|c||a|), and gamma=acos(a’*b/|a||b|).
- *) The reciprocal lattice vectors are calculated using the
crystallographic convention, where the prefactor of 2*pi is omitted. In this convention, the reciprocal lattice volume is 1/V.
- *) Several relations from [3] were employed in the component
calculations.
REFERENCES:
- [1] J. F. Nye, ``Physical Properties of Crystals: Their
Representation by Tensors and Matrices’’. Oxford University Press, 1985. ISBN 0198511655
- [2] E. M. Lauridsen, S. Schmidt, R. M. Suter, and H. F. Poulsen,
``Tracking: a method for structural characterization of grains in powders or polycrystals’’. J. Appl. Cryst. (2001). 34, 744–750
- [3] R. J. Neustadt, F. W. Cagle, Jr., and J. Waser, ``Vector
algebra and the relations between direct and reciprocal lattice quantities’’. Acta Cryst. (1968), A24, 247–248
- hexrd.material.crystallography.lorentz_factor(tth)[source]
05/26/2022 SS adding lorentz factor computation to the detector so that it can be compenstated for in the intensity correction
parameters: tth two theta of every pixel in radians
- hexrd.material.crystallography.polarization_factor(tth, unpolarized=True, eta=None, f_hor=None, f_vert=None)[source]
06/14/2021 SS adding lorentz polarization factor computation to the detector so that it can be compenstated for in the intensity correction
05/26/2022 decoupling lorentz factor from polarization factor
- parameters: tth two theta of every pixel in radians
if unpolarized is True, all subsequent arguments are optional eta azimuthal angle of every pixel f_hor fraction of horizontal polarization (~1 for XFELs) f_vert fraction of vertical polarization (~0 for XFELs)
notice f_hor + f_vert = 1
- hexrd.material.crystallography.processWavelength(arg)[source]
Convert an energy value to a wavelength. If argument has units of length or energy, will convert to globally specified unit type for wavelength (dUnit). If argument is a scalar, assumed input units are keV.
- hexrd.material.crystallography.rhombohedralIndicesFromHexagonal(HKL)[source]
converts hexagonal hkl to rhombohedral indices