Results 271 to 280 of about 1,033,260 (289)
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The SU(4) ⊃ SU(2) ⊗ SU(2) chain
Journal of Mathematical Physics, 1978We consider the physical SU(4) ⊃ SU(2) ⊗ SU(2) chain. With the help of the three vectors (Sα, Ti, Qαi), (VαS, VtT, VαiQ), (WSα, WiT, WαiQ) we can easily write the three fundamental invariants I2, I3, I4; the two operators Ω and Φ (eigenvalues ω and φ) of Moshinsky and Nagel [Phys. Lett.
A. Partensky, C. Maguin
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SU(2) and SU(1,1) interferometers
Physical Review A, 1986A Lie-group-theoretical approach to the analysis of interferometers is presented. Conventional interferometers such as the Mach-Zehnder and Fabry-Perot can be characterized by SU(2). We introduce a class of interferometers characterized by SU(1,1). These interferometers employ active elements such as four-wave mixers or degenerate-parametric amplifiers
, Yurke, , McCall, , Klauder
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Journal of Mathematical Physics, 1988
Matrix elements of the group generators for the totally symmetric irreducible representations of SU(5) are obtained in closed form employing the decomposition chain SU(5)⊇SU(4)×U(1)⊇SO(4)×U(1). The SU(4)≈SU(2)×SU(2) subgroup herein also occurs at the tail of the inclusion chain SU(5)⊇SO(5)⊇SO(4).
J. Vanthournout +2 more
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Matrix elements of the group generators for the totally symmetric irreducible representations of SU(5) are obtained in closed form employing the decomposition chain SU(5)⊇SU(4)×U(1)⊇SO(4)×U(1). The SU(4)≈SU(2)×SU(2) subgroup herein also occurs at the tail of the inclusion chain SU(5)⊇SO(5)⊇SO(4).
J. Vanthournout +2 more
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SU(2) × SU(2) scalars in the enveloping algebra of SU(4)
Journal of Mathematical Physics, 1976We build an integrity basis for the SU(2) × SU(2) scalars belonging to the enveloping algebra of SU(4). We prove that it contains seven independent invariants in addition to the Casimir operators of SU(4) and SU(2) × SU(2). We form a complete set of commuting operators by adding to the latter two linear combinations of the former the operators Ω and ...
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Matrix elements of the labelling operators for SU(4) ⊃ SU(2) × SU(2)
Journal of Physics A: Mathematical and General, 1989A matrix representation of the labelling operators of Moshinsky and Nagel (1963) and of Partensky and Maguin (1978) in the non-orthogonal Draayer basis of SU(4) is derived; this allows one to solve explicitly the missing label problem for the spin-isospin multiplets in the arbitrary SU(4) supermultiplets.
E Norvaisas, S Alisauskas
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