2014
DOI: 10.1103/physrevb.90.035135
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Constraints on Jones transmission matrices from time-reversal invariance and discrete spatial symmetries

Abstract: Optical spectroscopies are most often used to probe dynamical correlations in materials, but they are also a probe of symmetry. Polarization anisotropies are of course sensitive to structural anisotropies, but have been much less used as a probe of more exotic symmetry breakings in ordered states. In this paper a Jones transfer matrix formalism is discussed to infer the existence of exotic broken symmetry states of matter from their electrodynamic response for a full complement of possible broken symmetries in… Show more

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Cited by 61 publications
(55 citation statements)
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“…In fact, for all reciprocal materials and excluding any nonlinear effects, the Jones matrix in backward propagation direction corresponds to the transpose of the Jones transmission direction in forward direction [62]. Therefore, polarizationconserving transmittances, that is, the diagonal elements of the Jones transmission matrix, are identical for forward and backward propagation.…”
Section: Circular Polarization Convertermentioning
confidence: 99%
“…In fact, for all reciprocal materials and excluding any nonlinear effects, the Jones matrix in backward propagation direction corresponds to the transpose of the Jones transmission direction in forward direction [62]. Therefore, polarizationconserving transmittances, that is, the diagonal elements of the Jones transmission matrix, are identical for forward and backward propagation.…”
Section: Circular Polarization Convertermentioning
confidence: 99%
“…Such a high degree of symmetry may not be compatible with any lattice distortion caused by atomic displacements. In this case, it will be difficult to detect the electronic gyrotropic order with conventional methods [19][20][21][22].…”
Section: Prl 115 026401 (2015) P H Y S I C a L R E V I E W L E T T Ementioning
confidence: 99%
“…The complex transmission is represented by a 2 × 2 Jones matrix. Because of the threefold rotational symmetry of the lattice, this reduces to an antisymmetric matrix for the transmission of a linearly polarized pulse [70]. By diagonalizing this antisymmetric matrix, we can convert the transmission matrix from the linear basis into a circular basis (see SM Sec.…”
Section: B Analysis Of the Tdts Datamentioning
confidence: 99%