forked from lijiext/lammps
Switched the sign of spherical harmonics for m odd
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@ -48,14 +48,17 @@ For each atom, :math:`Q_l` is a real number defined as follows:
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\bar{Y}_{lm} = & \frac{1}{nnn}\sum_{j = 1}^{nnn} Y_{lm}( \theta( {\bf r}_{ij} ), \phi( {\bf r}_{ij} ) ) \\
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Q_l = & \sqrt{\frac{4 \pi}{2 l + 1} \sum_{m = -l}^{m = l} \bar{Y}_{lm} \bar{Y}^*_{lm}}
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The first equation defines the spherical harmonic order parameters.
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The first equation defines the local order parameters as averages
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of the spherical harmonics :math:`Y_{lm}` for each neighbor.
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These are complex number components of the 3D analog of the 2D order
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parameter :math:`q_n`, which is implemented as LAMMPS compute
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:doc:`hexorder/atom <compute_hexorder_atom>`.
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The summation is over the *nnn* nearest
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neighbors of the central atom.
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The angles theta and phi are the standard spherical polar angles
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The angles :math:`theta` and :math:`phi` are the standard spherical polar angles
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defining the direction of the bond vector :math:`r_{ij}`.
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The phase and sign of :math:`Y_{lm}` follow the standard conventions,
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so that :math:`{\rm sign}(Y_{ll}(0,0)) = (-1)^l`.
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The second equation defines :math:`Q_l`, which is a
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rotationally invariant non-negative amplitude obtained by summing
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over all the components of degree *l*\ .
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@ -98,8 +101,8 @@ structures are given in Table I of :ref:`Steinhardt <Steinhardt>`, and these
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can be reproduced with this keyword.
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The optional keyword *components* will output the components of the
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normalized complex vector :math:`\bar{Y}_{lm}` of degree *ldegree*\ , which must be
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explicitly included in the keyword *degrees*\ . This option can be used
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*normalized* complex vector :math:`\hat{Y}_{lm} = \bar{Y}_{lm}/|\bar{Y}_{lm}|` of degree *ldegree*\,
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which must be included in the list of order parameters to be computed. This option can be used
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in conjunction with :doc:`compute coord_atom <compute_coord_atom>` to
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calculate the ten Wolde's criterion to identify crystal-like
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particles, as discussed in :ref:`ten Wolde <tenWolde2>`.
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@ -141,11 +144,15 @@ If the keyword *wl/hat* is set to yes, then the :math:`\hat{W}_l`
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values for each atom will be added to the output array, which are real numbers.
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If the keyword *components* is set, then the real and imaginary parts
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of each component of (normalized) :math:`\bar{Y}_{lm}` will be added to the
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output array in the following order: :math:`Re(\bar{Y}_{-m}) Im(\bar{Y}_{-m})
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Re(\bar{Y}_{-m+1}) Im(\bar{Y}_{-m+1}) ... Re(\bar{Y}_m) Im(\bar{Y}_m)`. This
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way, the per-atom array will have a total of *nlvalues*\ +2\*(2\ *l*\ +1)
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columns.
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of each component of *normalized* :math:`\hat{Y}_{lm}` will be added to the
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output array in the following order: :math:`{\rm Re}(\hat{Y}_{-m}), {\rm Im}(\hat{Y}_{-m}),
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{\rm Re}(\hat{Y}_{-m+1}), {\rm Im}(\hat{Y}_{-m+1}), \dots , {\rm Re}(\hat{Y}_m), {\rm Im}(\hat{Y}_m)`.
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In summary, the per-atom array will contain *nlvalues* columns, followed by
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an additional *nlvalues* columns if *wl* is set to yes, followed by
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an additional *nlvalues* columns if *wl/hat* is set to yes, followed
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by an additional 2\*(2\* *ldegree*\ +1) columns if the *components*
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keyword is set.
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These values can be accessed by any command that uses per-atom values
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from a compute as input. See the :doc:`Howto output <Howto_output>` doc
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@ -456,21 +456,26 @@ void ComputeOrientOrderAtom::calc_boop(double **rlist,
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for (int il = 0; il < nqlist; il++) {
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int l = qlist[il];
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// calculate spherical harmonics
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// Ylm, -l <= m <= l
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// sign convention: sign(Yll(0,0)) = (-1)^l
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qnm_r[il][l] += polar_prefactor(l, 0, costheta);
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double expphim_r = expphi_r;
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double expphim_i = expphi_i;
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for(int m = 1; m <= +l; m++) {
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double prefactor = polar_prefactor(l, m, costheta);
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double c_r = prefactor * expphim_r;
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double c_i = prefactor * expphim_i;
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qnm_r[il][m+l] += c_r;
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qnm_i[il][m+l] += c_i;
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double ylm_r = prefactor * expphim_r;
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double ylm_i = prefactor * expphim_i;
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qnm_r[il][m+l] += ylm_r;
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qnm_i[il][m+l] += ylm_i;
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if(m & 1) {
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qnm_r[il][-m+l] -= c_r;
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qnm_i[il][-m+l] += c_i;
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qnm_r[il][-m+l] -= ylm_r;
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qnm_i[il][-m+l] += ylm_i;
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} else {
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qnm_r[il][-m+l] += c_r;
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qnm_i[il][-m+l] -= c_i;
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qnm_r[il][-m+l] += ylm_r;
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qnm_i[il][-m+l] -= ylm_i;
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}
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double tmp_r = expphim_r*expphi_r - expphim_i*expphi_i;
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double tmp_i = expphim_r*expphi_i + expphim_i*expphi_r;
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@ -505,19 +510,6 @@ void ComputeOrientOrderAtom::calc_boop(double **rlist,
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qn[jj++] = qnormfac * sqrt(qm_sum);
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}
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// TODO:
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// 1. [done]Need to allocate extra memory in qnarray[] for this option
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// 2. [done]Need to add keyword option
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// 3. [done]Need to calculate Clebsch-Gordan/Wigner 3j coefficients
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// (Can try getting them from boop.py first)
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// 5. [done]Compare to bcc values in /Users/athomps/netapp/codes/MatMiner/matminer/matminer/featurizers/boop.py
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// 6. [done]I get the right answer for W_l, but need to make sure that factor of 1/sqrt(l+1) is right for cglist
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// 7. Add documentation
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// 8. [done] run valgrind
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// 9. [done] Add Wlhat
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// 10. Update memory_usage()
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// 11. Add exact FCC values for W_4, W_4_hat
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// calculate W_l
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if (wlflag) {
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@ -554,7 +546,6 @@ void ComputeOrientOrderAtom::calc_boop(double **rlist,
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idxcg_count++;
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}
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}
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// Whats = [w/(q/np.sqrt(np.pi * 4 / (2 * l + 1)))**3 if abs(q) > 1.0e-6 else 0.0 for l,q,w in zip(range(1,max_l+1),Qs,Ws)]
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if (qn[il] < QEPSILON)
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qn[jj++] = 0.0;
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else {
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@ -565,7 +556,7 @@ void ComputeOrientOrderAtom::calc_boop(double **rlist,
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}
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}
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// Calculate components of Q_l, for l=qlcomp
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// Calculate components of Q_l/|Q_l|, for l=qlcomp
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if (qlcompflag) {
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int il = iqlcomp;
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@ -619,6 +610,7 @@ double ComputeOrientOrderAtom::polar_prefactor(int l, int m, double costheta)
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/* ----------------------------------------------------------------------
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associated legendre polynomial
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sign convention: P(l,l) = (2l-1)!!(-sqrt(1-x^2))^l
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------------------------------------------------------------------------- */
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double ComputeOrientOrderAtom::associated_legendre(int l, int m, double x)
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@ -628,9 +620,9 @@ double ComputeOrientOrderAtom::associated_legendre(int l, int m, double x)
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double p(1.0), pm1(0.0), pm2(0.0);
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if (m != 0) {
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const double sqx = sqrt(1.0-x*x);
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const double msqx = -sqrt(1.0-x*x);
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for (int i=1; i < m+1; ++i)
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p *= static_cast<double>(2*i-1) * sqx;
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p *= static_cast<double>(2*i-1) * msqx;
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}
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for (int i=m+1; i < l+1; ++i) {
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