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Unformatted text preview: PHYS 507 Homework V (Fall ’05) Assigned: November 7, 2005, Monday. Due: November 16, 2005, Wednesday, at 5:00 pm. Note: First Midterm exam is on November 19, Saturday at 14:00 somewhere in the Physics Dept. 1. The Virial Theorem: Consider the Hamiltonian for a particle in 1D, H = p 2 2 m + V ( x ) = T + V , where T is the kinetic energy operator. We assume that the potential V ( x ) is of such a nature that H has bounded eigenstates  ϕ n i with discrete energies E n . In that case  ϕ n i can be normalized to unity, h ϕ n  ϕ n i = 1. Denote the expectation values in state  ϕ n i by h i n . (a) Show that h [ H,A ] i n =0 for any operator A . (b) Consider the operator A = xp + px . Compute [ T,A ] and [ V,A ]. Using these expressions and part (a), find a relationship between h T i n and h xV ( x ) i n (this is called the virial theorem). (c) Apply the theorem to potentials of the form V ( x ) = c  x  α , where c and α are constants, and express h T i n and h V i n in terms of the energy eigenvalue...
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This note was uploaded on 02/11/2012 for the course MATH 435 taught by Professor Starg during the Spring '11 term at Al Ahliyya Amman University.
 Spring '11
 starg

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