Let x and p denote, respectively, the coordinate and momentum operators satisfying the canonical commutation relation [x, p]=i in natural units (ħ = 1). Then the commutator [x, pe P] is (a) i(1-p)e (b) i(1-p)e (c) i(1-eP) (d) ineP
Let x and p denote, respectively, the coordinate and momentum operators satisfying the canonical commutation relation [x, p]=i in natural units (ħ = 1). Then the commutator [x, pe P] is (a) i(1-p)e (b) i(1-p)e (c) i(1-eP) (d) ineP
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![Let x and p denote, respectively, the coordinate and momentum operators satisfying the canonical commutation
relation [x, p]=i in natural units (h =1). Then the commutator [x, pe¯P] is
(a) i(1-p)e
(b) i(1-p?)e
(c) i(1-e"P)
(d) ipe P](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2F08e9d4fd-8438-4c25-b12e-9acf7c201044%2F909d852d-95f9-46d9-b0ea-4f329f904fb5%2Fpdp8plj_processed.jpeg&w=3840&q=75)
Transcribed Image Text:Let x and p denote, respectively, the coordinate and momentum operators satisfying the canonical commutation
relation [x, p]=i in natural units (h =1). Then the commutator [x, pe¯P] is
(a) i(1-p)e
(b) i(1-p?)e
(c) i(1-e"P)
(d) ipe P
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