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Condon-Shortley-Wigner phase convention

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Condon-Shortley-Wigner phase convention [¦kän·dən ¦shȯrt·lē ¦wig·nər ′fās kən‚ven·shən]
(quantum mechanics)
Convention relating the phases of states having the same eigenvalue ofJ2=Jx2+Jy2+Jz2, and different eigenvalues ofJz, whereJis the total angular momentum, according to which the matrix elements ofJ+=Jx+iJyandJ-=Jx-iJybetween such states are real.


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