2013
DOI: 10.1103/physrevd.87.065029
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Deconstructing supersymmetricSmatrices inD2+1

Abstract: Global supersymmetries of the S-matrices of N = 2, 4, 8 supersymmetric Yang-Mills theories in three spacetime dimensions (without matter hypermultiplets) are shown to be SU (1|1), SU (2|2) and SU (2|2) ⊗ SU (2|2) respectively. These symmetries are not manifest in the off-shell Lagrangian formulations of these theories. A direct map between these symmetries and their representations in terms of the Yang-Mills degrees of freedom and the corresponding quantities in Chern-Simons-Matter theories with N ≥ 4 supersym… Show more

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Cited by 7 publications
(10 citation statements)
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“…It is generally thought that 1/f noise in semiconductors results from a distribution of bistable charge states. Such fluctuators are regularly observed in various solid state platforms [24,[26][27][28][29][30][31][32][33][34][35][36]. A simple model for TLSs causing 1/f noise proposed by McWhorter [37] considers a distribution of TLSs, each of which switches between two states and contributes a Lorentzian power spectrum to the overall noise spectrum.…”
mentioning
confidence: 99%
“…It is generally thought that 1/f noise in semiconductors results from a distribution of bistable charge states. Such fluctuators are regularly observed in various solid state platforms [24,[26][27][28][29][30][31][32][33][34][35][36]. A simple model for TLSs causing 1/f noise proposed by McWhorter [37] considers a distribution of TLSs, each of which switches between two states and contributes a Lorentzian power spectrum to the overall noise spectrum.…”
mentioning
confidence: 99%
“…Here we resort to a variational method based on a partial polaron transformation [48,49]. The idea is that, when the impurity mass is large compared to the Tkachenko boson mass, the bosonic field can instantaneously adjust to the slow motion of the impurity.…”
Section: B Finite Impurity Massmentioning
confidence: 99%
“…12 Such two-level fluctuators involve tunneling between two spatial configurations with nearly equal potential energy and are routinely observed in amorphous materials. [13][14][15][16] These fluctuators have been observed as spurious resonances in the spectrum of superconducting phase qubits, 17 and have been the subject of an extensive literature in the Josephson qubit community. [18][19][20][21][22] Similar two-level fluctuators consisting of a charge hopping between localized states have been observed in the environment of various other solid-state devices, including lateral gated heterostructures [23][24][25][26] and self-assembled quantum dots.…”
Section: Introductionmentioning
confidence: 99%