Interface States in Space-Time Photonic Crystals: Topological Origin, Propagation, and Amplification. [PDF]
Caballero A, Allard TF, Huidobro PA.
europepmc +1 more source
Angle-Dependent Terahertz Circular Dichroism and Full-Space Polarization Manipulation via Extrinsic Chiral Metasurfaces. [PDF]
Wan M +11 more
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Conformational chirality in buckled molecular silicenes: a precursor for chiral magnets. [PDF]
Muskan, Bhattacharya D, Shil S.
europepmc +1 more source
Wavelength-tunable high-Q circular dichroism based on the hybrid chiral phase-change metasurface. [PDF]
Zhou X +7 more
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Chiral Metal Halide Perovskites for Spin-Polarized Light-Emitting Diodes. [PDF]
Gaurav A +8 more
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Chiral Magnon Dynamics in a Kitaev Magnet Revealed by Magneto-Optics
Bachar N +15 more
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Chiral symmetry breaking on the lattice [PDF]
We review important aspects of QCD in the continuum and on the lattice and take a look at the fate of its symmetries with an emphasis on chiral symmetry breaking on the lattice.
Manfried Faber, Roman Hollwieser
exaly +3 more sources
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Dilaton and Chiral-Symmetry Breaking
Physical Review Letters, 1986The spontaneous breaking of chiral symmetry in certain gauge models may also imply the spontaneous breaking of an approximate scale symmetry. This breaking will produce the dilaton as a pseudo-Goldstone boson of spontaneously broken scale invariance.
, Bardeen, , Leung, , Love
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Spontaneous Breakings of Chiral Symmetries
Physical Review D, 1970We analyze in detail the spontaneous breakings of chiral $\mathrm{SU}(3)\ensuremath{\bigotimes}\mathrm{SU}(3)$ and $\mathrm{SU}(2)\ensuremath{\bigotimes}\mathrm{SU}(2)$. We determine the directions along which the two groups may break spontaneously.
CICOGNA, GIAMPAOLO +2 more
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Chiral-symmetry breaking at finite temperatures
Physical Review D, 1988A Dyson equation approach is used to investigate chiral-symmetry breaking at finite temperatures for an effective QCD Hamiltonian. Coupled equations for the quasiparticle energy and chiral gap angle are derived. The resulting gap equation is no longer form invariant under shifts of the effective quark-quark potential by a constant.
, Klevansky, , Lemmer
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