2020
DOI: 10.1134/s0021364020100069
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Hyper-Poisson Photon Statistics

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Cited by 19 publications
(31 citation statements)
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“…As the magnetic field increases further, the domain wall energy becomes negative and the domain walls form a periodic array with the period that decreases with the field. This state is similar to the 'mixed state' in collinear antiferromagnets [43], except that in our case n rotates through the angle 2π across the wall, since the states with n parallel and antiparallel to ẑ have different energies for K 1 = 0. At the second critical field, H c2 , the transition between the DWA and TS states occurs and the modulation direction, described by ξ, rotates abruptly through 90 • .…”
Section: T S H C2mentioning
confidence: 53%
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“…As the magnetic field increases further, the domain wall energy becomes negative and the domain walls form a periodic array with the period that decreases with the field. This state is similar to the 'mixed state' in collinear antiferromagnets [43], except that in our case n rotates through the angle 2π across the wall, since the states with n parallel and antiparallel to ẑ have different energies for K 1 = 0. At the second critical field, H c2 , the transition between the DWA and TS states occurs and the modulation direction, described by ξ, rotates abruptly through 90 • .…”
Section: T S H C2mentioning
confidence: 53%
“…the magnetic field of ∼ 4 T [38] and another with a constant ψ and n rotating along a direction perpendicular to the field vector. The latter state is similar to the periodic array of domain walls ('mixed state') predicted for collinear chiral antiferromagnets near the flop transition [43]. Here, we use the effective model Eq.…”
Section: Effective Modelmentioning
confidence: 62%
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“…Introduction.-With the experimental observation of a skyrmion lattice in three-dimensional helical magnets MnSi 1 , Fe 1−x Co x Si 2 , and thin films of FeGe 3 , significant attention has been paid to systematic study of noncollinear magnetic states and associated magnetoelectric phenomena, where magnetic skyrmions play a prominent role [4][5][6][7] . Analogous to a topologically protected field-theoretical solution due to Skyrme 8,9 the stability of this particle-like spin texture is guaranteed by topological arguments, making it immune to smooth perturbations [10][11][12] . In chiral magnets, skyrmions are stabilized due to a delicate interplay between direct exchange, favoring collinear ordering, and asymmetric exchange known as Dzyaloshinskii-Moriya interaction (DMI) that results in spin canting 4,5 .…”
mentioning
confidence: 93%
“…In crystals lacking spatial inversion symmetry, the interplay of Heisenberg exchange interaction, antisymmetric Dzyaloshinskii-Moriya interaction, and an external Zeeman field may lead to the formation of vortexlike magnetic SKs. They have been predicted [2][3][4] years before they were experimentally discovered in magnetic layers with a strong spin-orbit interaction [1,5,6].…”
mentioning
confidence: 99%