11 SSM If orbital angular momentum L is measured along, say, az axis to obtain a value for L, show that (L; + L32 = [((e + 1) – mēj1?h is the most that can be said about the other two components of the orbital angular momentum.

Modern Physics
3rd Edition
ISBN:9781111794378
Author:Raymond A. Serway, Clement J. Moses, Curt A. Moyer
Publisher:Raymond A. Serway, Clement J. Moses, Curt A. Moyer
Chapter3: The Quantum Theroy Of Light
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11 SSM If orbital angular momentum L is measured along, say,
az axis to obtain a value for L, show that
(L; + L32 = [((e + 1) – mēj1?h
is the most that can be said about the other two components of the
orbital angular momentum.
Transcribed Image Text:11 SSM If orbital angular momentum L is measured along, say, az axis to obtain a value for L, show that (L; + L32 = [((e + 1) – mēj1?h is the most that can be said about the other two components of the orbital angular momentum.
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