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Within the framework of quantum mechanics (Eqs. (9.26) and what follows). show that the following are Hermitian operators: (a) momentum 𝐩=-i ħ∇≡-i (h)/(2 π) ∇; and (b) angular momentum 𝐋=-i ħ𝐫 ×∇≡-i (h)/(2 π) 𝐫 ×∇. Hint. In Cartesian form L is a linear combination of noncommuting Hermitian operators. | Numerade
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