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Apr
7
revised Allowed interactions in bosonic string theory
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Apr
7
answered Allowed interactions in bosonic string theory
Mar
31
answered The Lagrangian as a metric
Mar
25
comment Soliton Moduli Spaces and Homotopy Theory
@jamalS cont. There are more applications besides anomalies such as spinc quantization, charge quantization and fractionalization, Brane charges, supersymmetric quantum mechanics, Berezin-Toeplitz quantization and may be more. I don’t know of a single review comprising all these applications.
Mar
25
comment Soliton Moduli Spaces and Homotopy Theory
@jamalS There are analogous computations for the monopole moduli space dimension in the following review arxiv.org/abs/hep-th/0609055v2 by Weinberg and Yi, and for nonAbelian vortices in arxiv.org/abs/hep-th/0306150v1 by Hannay and Tong. There is a more mathematical review of the instanton and Seiberg-Witten moduli spaces dimension computation by David Bleecker milne.ruc.dk/~Booss/A-S-Index-Book/BlckBss_2012_04_25.pdf.
Mar
24
revised Soliton Moduli Spaces and Homotopy Theory
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Mar
24
revised Soliton Moduli Spaces and Homotopy Theory
added 1 characters in body
Mar
24
answered Soliton Moduli Spaces and Homotopy Theory
Mar
24
answered Galilean, SE(3), Poincare groups - Central Extension
Mar
20
comment Lie group of Schrodinger Wave equation
@user35952 I'll try to answer your new question soon, I'll try to clarify the previous "Poincare group vs Galilean group" answer
Mar
19
revised Lie group of Schrodinger Wave equation
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Mar
19
revised Lie group of Schrodinger Wave equation
added 106 characters in body
Mar
19
answered Lie group of Schrodinger Wave equation
Mar
16
revised Significance of magnetic translation operator defined in fractional QHE's description
added 65 characters in body
Mar
16
answered Significance of magnetic translation operator defined in fractional QHE's description
Mar
13
awarded  Nice Answer
Mar
13
comment Which symmetric pure qudit states can be reached within local operations?
@Piotr Migdal Thank you very much
Mar
13
awarded  Nice Answer
Mar
9
comment Lie algebra of axial charges
@gian_25 The matrix representation is just the 4-dimensional fundamental representation of $SO(4) = SU(2) \times SU(2)$, denoting the indices of the 4-space corresponding to $(\sigma, \pi_1, \pi_2, \pi_3)$ by $0,1,2,3$. Then$ (T^{V}_i)_{jk} = i \epsilon_{ijk}, (T^{(A)}_i)_{jk} = i (\delta_{ji}\delta_{k0}+ \delta_{ki}\delta_{i0})$. Please observe that the commutator of two axial generators is a vector generator.
Mar
9
answered Lie algebra of axial charges