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• W75451856 abstract "Before going further with our study of angular momentum, it will be advantageous to study the general behavior of physical systems under rotations in our 3-D space. If a state vector which describes the state of a physical system is specified by ❘ψ〉, the state vector for the rotated system will be specified by ❘ψrot.〉 = R❘ψ〉. (We use the subscript, rot., in place of a prime, which is often used for the rotated state, because primes are also often used on quantum labels.) The operator, R, is the operator that rotates the system. Recall from the theory of translation operators, two possible points of view exist for such operators: (1) The active point of view, in which R is used to rotate the system. (2) The passive point of view, in which the system is left unchanged and R is used to rotate the coordinate system (in the opposite sense) to view the system from a rotated reference frame. We shall use the active point of view in this chapter. The operator R is a linear, unitary operator:" @default.
• W75451856 created "2016-06-24" @default.
• W75451856 creator A5007125097 @default.
• W75451856 date "2000-01-01" @default.
• W75451856 modified "2023-09-23" @default.
• W75451856 title "Invariance of Physical Systems Under Rotations" @default.
• W75451856 doi "https://doi.org/10.1007/978-1-4612-1272-0_29" @default.
• W75451856 hasPublicationYear "2000" @default.
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