Consider a one-dimensional infinite square well potential of width L. The potential V(x) is V(x)=0 for 0≤x≤L and V(x)=∞ elsewhere.
The stationary states of a particle of mass m confined in this potential are described by the Schrödinger equation.
In the ground state of this particle, the square of the product of the position uncertainty Δx and the momentum uncertainty Δp is expressed in the following form:
(ΔxΔp)2=(CAπ2+B)ℏ2Here, Δx=⟨x2⟩−⟨x⟩2, Δp=⟨p2⟩−⟨p⟩2, and ⟨⋅⟩ denotes the expectation value. ℏ is the Dirac constant.
Given that A and C are coprime positive integers and B is a negative integer, find the value of the product A×∣B∣×C.
Give the result of A×∣B∣×C as a positive integer.