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=J_x²+J_y²+J_z², and different eigenvalues ofJ_z, whereJis the total angular momentum, according to which the matrix elements ofJ₊=J_x+iJ_yandJ_-=J_x-iJ_ybetween such states are real.

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