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Nov
18
answered Interacting representation of the Poincaré group
Nov
12
revised Aharonov-Bohm Effect and Integer Quantum Hall Effect
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Nov
12
answered Aharonov-Bohm Effect and Integer Quantum Hall Effect
Nov
6
revised Symmetries of spacetime and objects over it
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Nov
6
revised Symmetries of spacetime and objects over it
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Nov
6
comment Symmetries of spacetime and objects over it
@Qmechanic Thank you
Nov
6
answered Symmetries of spacetime and objects over it
Nov
6
revised Relation between electric charge and gauge parameter of the moduli space of monopoles
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Nov
6
answered Relation between electric charge and gauge parameter of the moduli space of monopoles
Oct
30
revised Path integral and geometric quantization
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Oct
30
revised Kugo and Ojima's Canonical Formulation of Yang-Mills using BRST
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Oct
30
answered Kugo and Ojima's Canonical Formulation of Yang-Mills using BRST
Oct
29
answered Path integral and geometric quantization
Oct
29
answered Weinberg angle measurement methods
Oct
20
answered How to apply Noether's theorem
Oct
16
comment Mathematically challenging areas in Quantum information theory and quantum cryptography
Coherent states which are widely used in quantum cryptography, have a geometric origin (Bargmann space). Please see for example Ma's thesis: web.williams.edu/go/math/sjmiller/public_html/crypto/handouts/…
Oct
15
answered Mathematically challenging areas in Quantum information theory and quantum cryptography
Oct
11
revised Dimensional reduction and Schwarzschild solution
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Oct
11
answered Dimensional reduction and Schwarzschild solution
Oct
4
comment How to construct the charge conjugation matrix for any given dimension?
I can show you how to construct in this particular case, but can you please check your calculations because in your expressions $(\Gamma^1)^2=(\Gamma^2)^2=1$ while $(\Gamma^3)^2=(\Gamma^4)^2=-1$, i.e., you are working in a signature $(1, 1, -1, -1)$. Is this really the case you need.