Symmetry-transformed overlap integrals

doc/docs/Scheme_User_Interface.md

@@ -571,6 +571,31 @@ Returns a list of the group-velocity components (units of *c*) in the given *dir
           
 As above, but returns the group velocity or component thereof only for band `which-band`.
 
+### Band symmetry
+
+MPB can compute the "characters" of a symmetry operation $g$ applied to a field at a particular point, i.e. MPB can compute the overlap integrals:
+
+```math
+(\mathbf{F}|g\mathbf{F}') = \int \mathbf{F}(\mathbf{r})^\dagger [g\mathbf{F}'(\mathbf{r})] \, \mathrm{d}\mathbf{r} = \int \mathbf{F}(\mathbf{r})^\dagger (g\mathbf{F}')(g^{-1}\mathbf{r}) \, \mathrm{d}\mathbf{r}
+```
+
+where **F** denotes either the **E**- or **H**-field and **F**′ denotes the associated **D**- or **B**-field (including Bloch phases) and integration is over the unit cell.
+The space group operation $g$ may include both rotational ($W$) and translational ($w$) parts, and are specified by the associated matrix-column pair $g = \{W,w\}$ acting on points as $\{W,w\}\mathbf{r} = W\mathbf{r} + w$.
+$W$ and $w$ should be supplied as `matrix3x3` and `vector3` variables in the basis of the lattice (listings of space group operations are available e.g. on the [Bilbao Crystallographic Server](https://www.cryst.ehu.es/)).
+(Note that $g$ transforms both the vectorial components of **F**′ as well as its coordinates: if **F**′ refers to a **B**-field, an additional factor of $\mathop{\mathrm{det}}W$ is incorporated to account for its pseudovectorial nature.)
+
+Given the character tables associated with the little groups of a considered photonic crystal, this functionality can e.g. be used to infer which irreducible representation (irrep) a given band (or band grouping) transforms as across the Brillouin zone.
+
+**`(compute-symmetry which_band W w)`**
+Compute the $(\mathbf{H}|g\mathbf{B})$ character for `which-band` under a symmetry operation with rotation `W` and translation `w`, returning a complex number.
+
+**`(compute-symmetries W w)`**
+Equivalent to `compute-symmetry`, but returns characters for *all* computed bands, returning a list of complex numbers.
+
+**`(transformed_overlap W w)`**
+Sets **F**′ to `curfield` (must be either a **D**- or **B**-field) and computes the associated character under the symmetry operation specified by `W` and `w`, returning a complex number.
+Usually, it will be more convenient to call `compute-symmetry` (which wraps `transformed_overlap` with an initialization of `curfield` via `get-bfield`).
+
 Field Manipulation
 ------------------
 

mpb/Makefile.am

@@ -20,7 +20,7 @@ EXTRA_DIST = mpb.scm.in epsilon.c mu.c
 
 nodist_pkgdata_DATA = $(SPECIFICATION_FILE)
 
-MY_SOURCES = medium.c epsilon_file.c field-smob.c fields.c	\
+MY_SOURCES = transform.c medium.c epsilon_file.c field-smob.c fields.c	\
 material_grid.c material_grid_opt.c matrix-smob.c mpb.c field-smob.h matrix-smob.h mpb.h my-smob.h
 
 MY_LIBS = $(top_builddir)/src/matrixio/libmatrixio.a $(top_builddir)/src/libmpb@[email protected] $(NLOPT_LIB) -lctl $(GUILE_LIBS)

mpb/fields.c

@@ -706,32 +706,31 @@ number get_energy_point(vector3 p)
      return f_interp_val(p, mdata, (real *) curfield, 1, 0);
 }
 
-cvector3 get_bloch_field_point(vector3 p)
+void get_bloch_field_point_(scalar_complex *field, vector3 p)
 {
-     scalar_complex field[3];
-     cvector3 F;
-
      CHECK(curfield && strchr("dhbecv", curfield_type),
 	   "field must be must be loaded before get-*field*-point");
      field[0] = f_interp_cval(p, mdata, &curfield[0].re, 6);
      field[1] = f_interp_cval(p, mdata, &curfield[1].re, 6);
      field[2] = f_interp_cval(p, mdata, &curfield[2].re, 6);
-     F.x = cscalar2cnumber(field[0]);
-     F.y = cscalar2cnumber(field[1]);
-     F.z = cscalar2cnumber(field[2]);
-     return F;
+}
+
+cvector3 get_bloch_field_point(vector3 p)
+{
+     scalar_complex field[3];
+     cvector3 F;
+
+     get_bloch_field_point_(field, p);
+
+     return cscalar32cvector3(field);
 }
 
 cvector3 get_field_point(vector3 p)
 {
      scalar_complex field[3], phase;
      cvector3 F;
 
-     CHECK(curfield && strchr("dhbecv", curfield_type),
-	   "field must be must be loaded before get-*field*-point");
-     field[0] = f_interp_cval(p, mdata, &curfield[0].re, 6);
-     field[1] = f_interp_cval(p, mdata, &curfield[1].re, 6);
-     field[2] = f_interp_cval(p, mdata, &curfield[2].re, 6);
+     get_bloch_field_point_(field, p);
 
      if (curfield_type != 'v') {
 	  double phase_phi = TWOPI *
@@ -744,10 +743,8 @@ cvector3 get_field_point(vector3 p)
 	  CASSIGN_MULT(field[2], field[2], phase);
      }
 
-     F.x = cscalar2cnumber(field[0]);
-     F.y = cscalar2cnumber(field[1]);
-     F.z = cscalar2cnumber(field[2]);
-     return F;
+	 F = cscalar32cvector3(field);
+	 return F;
 }
 
 cnumber get_bloch_cscalar_point(vector3 p)

mpb/mpb.h

@@ -74,6 +74,7 @@ extern int kpoint_index;
 extern void compute_field_squared(void);
 void get_efield(integer which_band);
 real mean_medium_from_matrix(const symmetric_matrix *eps_inv);
+void get_bloch_field_point_(scalar_complex *field, vector3 p);
 
 /**************************************************************************/
 

mpb/mpb.scm.in

@@ -211,6 +211,13 @@
 (define-external-function compute-energy-in-object-list false false
   'number (make-list-type 'geometric-object))
 
+(define-external-function transformed-overlap false false 
+  'cnumber 'matrix3x3 'vector3)
+(define-external-function compute-symmetries false false
+  (make-list-type 'cnumber) 'matrix3x3 'vector3)
+(define-external-function compute-symmetry false false
+  'cnumber 'integer 'matrix3x3 'vector3)
+
 (define-external-function output-field-to-file false false
   no-return-value 'integer 'string)  
 

mpb/transform.c

@@ -0,0 +1,210 @@
+/* Copyright (C) 1999-2014 Massachusetts Institute of Technology.
+ *
+ * This program is free software; you can redistribute it and/or modify
+ * it under the terms of the GNU General Public License as published by
+ * the Free Software Foundation; either version 2 of the License, or
+ * (at your option) any later version.
+ *
+ * This program is distributed in the hope that it will be useful,
+ * but WITHOUT ANY WARRANTY; without even the implied warranty of
+ * MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE.  See the
+ * GNU General Public License for more details.
+ *
+ * You should have received a copy of the GNU General Public License
+ * along with this program; if not, write to the Free Software
+ * Foundation, Inc., 59 Temple Place, Suite 330, Boston, MA  02111-1307  USA
+ */
+
+
+#include <stdio.h>
+#include <stdlib.h>
+#include <math.h>
+
+#include "config.h"
+#include <mpiglue.h>
+#include <mpi_utils.h>
+#include <check.h>
+
+#include "mpb.h"
+#include <ctl-io.h>
+#include <xyz_loop.h>
+#include <maxwell.h>
+
+
+
+/* If `curfield` is the real-space D-field (of band-index i), computes the overlap 
+ *       ∫ Eᵢ†(r){W|w}Dᵢ(r) dr  =  ∫ Eᵢ†(r)(WDᵢ)({W|w}⁻¹r) dr,
+ * for a symmetry operation {W|w} with rotation W and translation w; each specified 
+ * in the lattice basis. The vector fields Eᵢ and Dᵢ include Bloch phases.
+ * If `curfield` is the real-space B-field, the overlap
+ *       ∫ Hᵢ†(r){W|w}Bᵢ(r) dr  =  det(W) ∫ Hᵢ†(r)(WBᵢ)({W|w}⁻¹r) dr,
+ * is computed instead. Note that a factor det(W) is then included since B & H are
+ * pseudovectors. As a result, the computed symmetry expectation values are
+ * independent of whether the D- or B-field is used.
+ * No other choices for `curfield` are allowed: to set `curfield` to the real-space
+ * B- or D-field use the `get-bfield` and `get-dfield` Scheme functions or the
+ * `get_bfield` and `get_dfield` in C functions.                   
+ * Usually, it will be more convenient to use the wrapper `compute_symmetry(i, W, w)`
+ * which defaults to the B-field (since μ = 1 usually) and takes a band-index `i`.
+ */
+cnumber transformed_overlap(matrix3x3 W, vector3 w)
+{
+    int n1, n2, n3;
+    real s1, s2, s3, c1, c2, c3;
+    cnumber integral = {0,0}, integral_sum;
+    number detW;
+    vector3 kvector = cur_kvector;
+    matrix3x3 invW, Wc;
+
+    if (!curfield || !strchr("db", curfield_type)) {
+        mpi_one_fprintf(stderr, "curfield must refer to either a B- or D-field\n");
+        return integral;
+    }
+
+    #ifndef SCALAR_COMPLEX
+        CHECK(0, "transformed_overlap(..) is not yet implemented for mpbi");
+        /* NOTE: Not completely sure why the current implementation does not work for mpbi
+         * (i.e for assumed-inversion): one clue is that running this with mpbi and the
+         * error-check off gives symmetry eigenvalues whose norm are ≈(ni÷2+1)/ni (where
+         * ni=n1=n2=n3) instead of near-unity (as they should be). This suggests we are not
+         * counting the number of grid points correctly somehow: I think the root issue is
+         * that we use the LOOP_XYZ macro, which has special handling for mbpi (i.e. only
+         * "visits" the "inversion-reduced" part of the unitcell): but here, we actually
+         * really want to (or at least assume to) visit _all_ the points in the unitcell. 
+         */
+    #endif
+    #ifdef HAVE_MPI
+        CHECK(0, "transformed_overlap(..) is not yet implemented for MPI");
+        /* NOTE: It seems there's some racey stuff going on with the MPI implementation,
+         * unfortunately, so it doesn't end giving consistent (or even meaningful) results.
+         * The issue could be that both `LOOP_XYZ` is distributed over workers _and_ that
+         * `get_bloch_field_point_` also is (via the interpolation). I'm imagining that such
+         * a naive "nested parallelism" doesn't jive here.
+         * Long story short: disable it for now.
+         */
+    #endif
+
+    /* prepare before looping ... */
+    n1 = mdata->nx; n2 = mdata->ny; n3 = mdata->nz;
+
+    s1 = geometry_lattice.size.x / n1; /* pixel spacings */
+    s2 = geometry_lattice.size.y / n2;
+    s3 = geometry_lattice.size.z / n3;
+    c1 = n1 <= 1 ? 0 : geometry_lattice.size.x * 0.5; /* offsets (negative) */
+    c2 = n2 <= 1 ? 0 : geometry_lattice.size.y * 0.5;
+    c3 = n3 <= 1 ? 0 : geometry_lattice.size.z * 0.5;
+
+    detW = matrix3x3_determinant(W);
+    if (fabs(fabs(detW) - 1.0) > 1e-12) {
+        mpi_one_fprintf(stderr, "valid symmetry operations {W|w} must have |det(W)| = 1.0\n");
+        return integral;
+    }
+    invW = matrix3x3_inverse(W);
+    /* W is specified in the lattice basis, but field *vectors* evaluated in real-space
+     * are in a Cartesian basis: when we transform the vector components, we must account
+     * for this difference. We transform W to a Cartesian basis Wc = RWR⁻¹ (with
+     * R = geometry_lattice.basis, a matrix w/ columns of Cartesian basis vectors) and
+     * then use Wc to transform vector fields.
+     */
+    Wc = matrix3x3_mult(matrix3x3_mult(geometry_lattice.basis, W),
+                        matrix3x3_inverse(geometry_lattice.basis));
+
+    /* hoist rescalings outside the loop (maybe licm takes care of it, but do it anyway) */
+    kvector.x *= TWOPI/geometry_lattice.size.x;
+    kvector.y *= TWOPI/geometry_lattice.size.y;
+    kvector.z *= TWOPI/geometry_lattice.size.z;
+
+    /* loop over coordinates (introduces int vars `i1`, `i2`, `i3`, `xyz_index`) */
+    LOOP_XYZ(mdata) { /* implies two opening braces `{{` */
+        vector3 p, pt;
+        scalar_complex F[3], Ft[3], Ftemp[3], integrand, phase;
+        double deltaphi;
+
+        /* current lattice coordinate */
+        p.x = i1 * s1 - c1;
+        p.y = i2 * s2 - c2;
+        p.z = i3 * s3 - c3;
+
+        /* transformed coordinate pt = {W|w}⁻¹p = W⁻¹(p-w) since {W|w}⁻¹={W⁻¹|-W⁻¹w} */
+        pt = matrix3x3_vector3_mult(invW, vector3_minus(p, w));
+
+        /* Bloch field value at transformed coordinate pt: interpolation is needed to 
+         * ensure generality in the case of fractional translations.                  */
+        get_bloch_field_point_(Ftemp, pt); /* assign `Ftemp` to field at `pt` (without eⁱᵏʳ factor) */
+
+        /* define `Ft` as the vector components of `Ftemp` transformed by `Wc`; we just
+         * write out the matrix-product manually here, for both real & imag parts       */
+        Ft[0].re = Wc.c0.x*Ftemp[0].re + Wc.c1.x*Ftemp[1].re + Wc.c2.x*Ftemp[2].re;
+        Ft[0].im = Wc.c0.x*Ftemp[0].im + Wc.c1.x*Ftemp[1].im + Wc.c2.x*Ftemp[2].im;
+        Ft[1].re = Wc.c0.y*Ftemp[0].re + Wc.c1.y*Ftemp[1].re + Wc.c2.y*Ftemp[2].re;
+        Ft[1].im = Wc.c0.y*Ftemp[0].im + Wc.c1.y*Ftemp[1].im + Wc.c2.y*Ftemp[2].im;
+        Ft[2].re = Wc.c0.z*Ftemp[0].re + Wc.c1.z*Ftemp[1].re + Wc.c2.z*Ftemp[2].re;
+        Ft[2].im = Wc.c0.z*Ftemp[0].im + Wc.c1.z*Ftemp[1].im + Wc.c2.z*Ftemp[2].im;
+
+        /* get the Bloch field value at current point `p` (without eⁱᵏʳ factor).
+         * We multiply the input field `F` (either B or D-field) with μ⁻¹ or ε⁻¹ to get
+         * H- or E-fields, as the relevant overlap is ⟨F|Ft⟩ = ⟨H|Bt⟩ or ⟨E|Dt⟩, with
+         * t-postscript denoting a field transformed by {W|w}. Here, we essentially
+         * adapt some boiler-plate code from compute_field_energy_internal in fields.c   */
+        if (curfield_type == 'd') {
+            assign_symmatrix_vector(F, mdata->eps_inv[xyz_index], curfield+3*xyz_index);
+        }
+        else if (curfield_type == 'b' && mdata->mu_inv != NULL) {
+            assign_symmatrix_vector(F, mdata->mu_inv[xyz_index],  curfield+3*xyz_index);
+        }
+        else {
+            F[0] = curfield[3*xyz_index];
+            F[1] = curfield[3*xyz_index+1];
+            F[2] = curfield[3*xyz_index+2];
+        }
+
+        /* inner product of F and Ft={W|w}F in Bloch form */
+        CASSIGN_CONJ_MULT(integrand, F[0], Ft[0]);  /* add adjoint(F)*Ft to integrand */
+        CACCUMULATE_SUM_CONJ_MULT(integrand, F[1], Ft[1]);
+        CACCUMULATE_SUM_CONJ_MULT(integrand, F[2], Ft[2]);
+
+        /* so far, Bloch phases have been excluded; we include them here. It saves two
+         * trigonometric operations if we do them just jointly for `p` and `pt`.        */
+        deltaphi = (kvector.x*(pt.x-p.x) + kvector.y*(pt.y-p.y) + kvector.z*(pt.z-p.z));
+        CASSIGN_SCALAR(phase, cos(deltaphi), sin(deltaphi));
+
+        /* finally, add integrand-contribution to integral, with Bloch phases included */
+        integral.re += CSCALAR_MULT_RE(integrand, phase);
+        integral.im += CSCALAR_MULT_IM(integrand, phase);
+    }}}
+
+    integral.re *= Vol / H.N;
+    integral.im *= Vol / H.N;
+
+    mpi_allreduce(&integral, &integral_sum, 2, number,
+                  MPI_DOUBLE, MPI_SUM, mpb_comm);
+
+    if (curfield_type == 'b') {  /* H & B are pseudovectors => transform includes det(W) */
+        integral_sum.re *= detW;
+        integral_sum.im *= detW;
+    }
+
+    return integral_sum;
+}
+
+cnumber compute_symmetry(int which_band, matrix3x3 W, vector3 w)
+{
+    cnumber symval;
+    get_bfield(which_band);
+    symval = transformed_overlap(W, w);
+
+    return symval;
+}
+
+cnumber_list compute_symmetries(matrix3x3 W, vector3 w)
+{
+    cnumber_list symvals;
+    int ib;
+    symvals.num_items = num_bands;
+    CHK_MALLOC(symvals.items, cnumber, num_bands);
+
+    for (ib = 0; ib < num_bands; ++ib){
+        symvals.items[ib] = compute_symmetry(ib+1, W, w);
+    }
+    return symvals;
+}

src/matrices/scalar.h

@@ -63,6 +63,14 @@ typedef struct {
 		    bbbb_re * cccc_im + bbbb_im * cccc_re); \
 }
 
+/* a = conj(b) * c */
+#define CASSIGN_CONJ_MULT(a, b, c) { \
+     real bbbb_re = (b).re, bbbb_im = (b).im; \
+     real cccc_re = (c).re, cccc_im = (c).im; \
+     CASSIGN_SCALAR(a, bbbb_re * cccc_re + bbbb_im * cccc_im, \
+              bbbb_re * cccc_im - bbbb_im * cccc_re); \
+}
+
 /* a = b / c = b * conj(c) / |c|^2 */
 #define CASSIGN_DIV(a, b, c) { \
      scalar_complex aaaa_tmp; real aaaa_tmp_norm; \