[Wannier] Parity-time symmetry

Daniel Kaplan danielkaplan137 at gmail.com
Tue Dec 31 14:26:36 CET 2019


Hello All!

I was wondering if any of you have encountered the following issue when
fitting wannier functions in systems with specific symmetry.

I'm dealing with a magnetic system (but in principle, this could be any
system) which has PT-symmetry. Since [PT, H] = 0, but in general, PT does
not commute with other observables, the spectrum of H should be of
doubly-degenerate bands (much like Kramers' degeneracy). Indeed a
self-consistent VASP run converges to such a spectrum remarkably well, with
the splitting between bands less than 1meV.

The trouble begins when attempting to fit Wannier functions to this system.
While overall the fit is of good quality (see attached spread information;
and band-structure comparisons) in many places along the high-symmetry
lines the splitting between bands amounts to >10meV which is unacceptable
in terms of preserving the symmetry.

More to the point the Wannier90.eig file *DOES *carry the symmetry rather
well (most eigenvalues differ by less than 1meV), but then throughout the
band-structure this is no longer the case.

What would you recommend in this instance?



I was thinking as well about the possibility of imposing this symmetry
directly. Since any Bloch band \phi(k) has a PT-partner PT \phi(k), and
these are naturally degenerate, then it would make a lot of sense (at
least, superficially) to fit the Wannier bands to *half* the spectrum, and
then reconstruct the other half by applying PT on the eigenvectors composed
of the Wannier basis.

Is such a thing at all possible?



Yours thankful,

Daniel Kaplan

Dept. of Condensed Matter Physics

Weizmann Institute of Science
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 Final State
  WF centre and spread    1  (  0.804077,  0.102310,  7.704753 )     6.13299382
  WF centre and spread    2  (  0.082185, -0.995229,  8.438850 )     5.82641191
  WF centre and spread    3  ( -0.556984, -0.688866,  7.673939 )     5.45609639
  WF centre and spread    4  (  0.004711, -0.006884,  6.174897 )     1.48160342
  WF centre and spread    5  ( -0.003941,  0.036428,  6.218878 )     2.24103642
  WF centre and spread    6  (  0.000440,  0.020881,  6.222547 )     1.74400990
  WF centre and spread    7  (  0.002633, -0.001175,  6.077481 )     1.48137326
  WF centre and spread    8  ( -0.013331, -0.078053,  6.020684 )     4.81346904
  WF centre and spread    9  ( -0.047670, -0.613716,  1.634524 )     5.38254812
  WF centre and spread   10  (  0.996041, -0.924214,  3.327170 )     5.39097450
  WF centre and spread   11  ( -0.032994,  1.252665,  4.029649 )     5.79797902
  WF centre and spread   12  ( -0.005517,  0.006678,  3.102633 )     1.49462375
  WF centre and spread   13  (  0.000154, -0.010012,  3.063406 )     1.52701405
  WF centre and spread   14  ( -0.001518, -0.009227,  3.055703 )     1.99828982
  WF centre and spread   15  ( -0.000300, -0.005523,  3.163580 )     1.23192042
  WF centre and spread   16  (  0.015073,  0.076194,  3.251327 )     4.80945433
  WF centre and spread   17  (  0.030989,  0.237591,  0.590173 )     6.60630368
  WF centre and spread   18  ( -1.772519,  0.312462,  0.139756 )     6.46630010
  WF centre and spread   19  (  0.597293,  0.651979, -0.300591 )     6.03041340
  WF centre and spread   20  ( -0.587732,  0.663604, -0.288734 )     5.96616358
  WF centre and spread   21  (  0.738419, -0.075074,  1.552730 )     5.79103262
  WF centre and spread   22  (  0.564951, -0.693327,  0.279969 )     6.06113163
  WF centre and spread   23  (  0.548477, -0.635296, -1.603221 )     5.45568554
  WF centre and spread   24  ( -0.265593, -1.678647, -0.018321 )     6.58644738
  WF centre and spread   25  (  0.046136,  0.629771,  7.651816 )     5.55234929
  WF centre and spread   26  ( -1.003588,  0.899042,  5.894349 )     5.36205748
  WF centre and spread   27  (  0.053748, -1.223677,  5.304028 )     5.65578315
  WF centre and spread   28  (  0.005018, -0.006578,  6.173327 )     1.49567169
  WF centre and spread   29  (  0.000792,  0.009804,  6.211000 )     1.52611206
  WF centre and spread   30  (  0.001658,  0.008597,  6.221223 )     1.99849887
  WF centre and spread   31  (  0.000367,  0.006770,  6.109200 )     1.25106501
  WF centre and spread   32  (  0.001845,  0.006039,  6.173635 )     0.85020681
  WF centre and spread   33  ( -0.780292, -0.083807,  1.577272 )     6.31874999
  WF centre and spread   34  (  0.558295,  0.665169,  1.609991 )     5.51721942
  WF centre and spread   35  ( -0.502955,  0.668043,  1.618807 )     5.41476590
  WF centre and spread   36  ( -0.005656,  0.006442,  3.100879 )     1.48123683
  WF centre and spread   37  (  0.003781, -0.036888,  3.056105 )     2.23419551
  WF centre and spread   38  ( -0.000504, -0.020705,  3.054638 )     1.73936367
  WF centre and spread   39  ( -0.004864,  0.001035,  3.199091 )     1.49755288
  WF centre and spread   40  ( -0.001232, -0.004520,  3.102499 )     0.86077465
  WF centre and spread   41  ( -0.030562, -0.217701, -0.618899 )     6.59640398
  WF centre and spread   42  (  1.755124, -0.337636, -0.142115 )     6.44678022
  WF centre and spread   43  ( -0.599205, -0.652313,  0.301883 )     6.00746636
  WF centre and spread   44  ( -0.707285, -0.821000,  1.266723 )     5.32716531
  WF centre and spread   45  ( -0.715087,  0.039541, -1.558092 )     5.82060536
  WF centre and spread   46  (  0.702607,  0.838813, -1.214371 )     5.34751441
  WF centre and spread   47  ( -0.082374,  1.036800,  0.771103 )     5.88128621
  WF centre and spread   48  (  0.228054,  1.669972,  0.020484 )     6.64394103
  Sum of centres and spreads (  0.021167,  0.026564,148.396357 )   202.60004219

         Spreads (Ang^2)       Omega I      =   130.040382817
        ================       Omega D      =     1.666441675
                               Omega OD     =    70.893217703
    Final Spread (Ang^2)       Omega Total  =   202.600042195
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