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Solutions to Physics Homework Problems: 325, #6 and #16, Assignments of Quantum Mechanics

The solutions to two problems from a physics 325 textbook. The first problem involves finding the first and second order approximations of the time evolution of two coupled harmonic oscillators. The second problem deals with the time evolution of a quantum mechanical system in the presence of a time-dependent potential. The document also includes the derivation of the unperturbed energy eigenstates and the calculation of the probability of finding the system in a particular excited state after a certain time.

Typology: Assignments

Pre 2010

Uploaded on 03/11/2009

koofers-user-078
koofers-user-078 🇺🇸

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Download Solutions to Physics Homework Problems: 325, #6 and #16 and more Assignments Quantum Mechanics in PDF only on Docsity! 1 Physics 325 Solution to Homework Problems #6 Winter 2004 1. Your textbook Prob. 9.5 We start with: ċa = 1 ih̄ H ′abe −iω0tcb ċb = 1 ih̄ H ′bae iω0tca with ca(0) = a, cb(0) = b For the first order result, we substitute ci(0) into the right side of the equations: ċ(1)a ≈ 1 ih̄ H ′abe −iω0tcb(0) = b ih̄ H ′abe −iω0t => c(1)a (t) ≈ b ih̄ ∫ t 0 H ′ab(t ′)e−iω0t ′ dt′ Similarly c(1)b (t) ≈ a ih̄ ∫ t 0 H ′ba(t ′)eiω0t ′ dt′ For second order, we use the first order results for ci(t) in the right hand side of the exact equations: ċ(2)a (t) ≈ 1 ih̄ H ′abe −iω0tc (1) b = 1 ih̄ H ′abe −iω0t a ih̄ ∫ t 0 H ′ba(t ′)eiω0t ′ dt′ = − a h̄2 H ′abe −iω0t ∫ t 0 H ′ba(t ′)eiω0t ′ dt′ => c(2)a (t) ≈ − a h̄2 ∫ t 0 H ′ab(t ′)e−iω0t ′ [ ∫ t′ 0 H ′ba(t ′′)eiω0t ′′ dt′′ ] dt′ Similarly, c(2)b ≈ − b h̄2 ∫ t 0 H ′ba(t ′)eiω0t ′ [ ∫ t′ 0 H ′ab(t ′′)e−iω0t ′′ dt′′ ] dt′ To second order, ca(t) ≈ a+ c(1)a + c(2)a , cb(t) ≈ b+ c(1)b + c (2) b . 2. Your textbook Prob. 9.16 (a) We start with the exact equation, Eq. 9.82: ċm = 1 ih̄ ∑ n cnH ′ mne iωmnt where ωmn = (Em −En)/h̄ And next compute H ′mn where H ′ = V0(t): H ′mn = 〈ψm(x)|V0(t)|ψn(x)〉 = V0(t)〈ψm(x)|ψn(x)〉 = V0(t)δmn because H ′ is constant over x, and the energy eigenstates are orthonormal. Therefore, ċm = 1 ih̄ cmH ′ mm = 1 ih̄ cmV0(t) Because we started in state N , for m 6= N , cm(0) = 0 and ċm = 0, leaving cm(t) = 0 for all t. Therefore no transitions take place and the only non-vanishing equation is then: ċN = 1 ih̄ cNV0(t); d(ln cN) dt = ċN cN = 1 ih̄ V0(t) => ln cN (t) = 1 ih̄ ∫ t 0 V0(t′)dt′ => cN (t) = e 1 ih̄ ∫ t 0 V0(t ′)dt′ Therefore only the phase of cN changes. The total phase change is : φ(T ) = 1 ih̄ ∫ T 0 V0(t′)dt′
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