1964
DOI: 10.1063/1.3051398
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Mécanique quantique, Vol. 2 and Quantum Mechanics

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Cited by 135 publications
(219 citation statements)
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“…The identification of the two parts of equation (6) with spin and orbital angular momenta is tempting due to the appearance of the operator L = −ir × ∇ and the relationship of the cross-product in S t with the spin-1 matrices representing S. But, since L and S are not operators in M, the question arises of which are the operators corresponding to the two parts of equation (6). In his book on Quantum Mechanics, Messiah [22,Ch. XXI,problem 7] offers an expression which corresponds to the second quantization of the first part of equation (6).…”
Section: The Separation Of L and Smentioning
confidence: 99%
“…The identification of the two parts of equation (6) with spin and orbital angular momenta is tempting due to the appearance of the operator L = −ir × ∇ and the relationship of the cross-product in S t with the spin-1 matrices representing S. But, since L and S are not operators in M, the question arises of which are the operators corresponding to the two parts of equation (6). In his book on Quantum Mechanics, Messiah [22,Ch. XXI,problem 7] offers an expression which corresponds to the second quantization of the first part of equation (6).…”
Section: The Separation Of L and Smentioning
confidence: 99%
“…Note that this current is independent of the potential V (φ) and up to a prefactor, it is just the momentum density of the boson field 43 . Consequently, translation invariance implies that the total thermal current J e is conserved.…”
Section: E the Massive Boson Modelmentioning
confidence: 99%
“…Using the Baker-Campbell-Hausdorff formula (see, e.g. [15]), in the permuted computational basis the quantum evolution is described by the two decoupled equations…”
Section: Typical Class Of Constraintsmentioning
confidence: 99%