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Unformatted text preview: PHYS851 Quantum Mechanics I, Fall 2009 HOMEWORK ASSIGNMENT 5 1. In problem 4.3, we used a change of variables to map the equations of motion for a sinusoidally driven twolevel system onto the timeindependent Rabi model. Here we will investigate how this change of variables can be treated more formally as a unitary transformation. Unitary operators are those which, when acting on (transforming) any state, always preserve the norm of the state. Any Hermitian operator, G can be used to generate a unitary transformation, via the Unitary operator U G = e iG . The Unitary transformation is then defined by  ψ ′ ( t ) ) = U G  ψ ( t ) ) , where  ψ ( t ) ) is the original statevector, and  ψ ′ ( t ) ) is the state vector in the new ‘frame of reference’. For the case of a timedependent Hamiltonian, H ( t ) and a timedependent generator G ( t ), we would like to determine the effective Hamiltonian, H ′ ( t ), which governs the evolution of the state  ψ ′ ( t ) ) . (a) Begin by differentiating both sides of the equation  ψ ′ ( t ) ) = U G ( t )  ψ ( t ) ) with respect to time. Use Schr¨odinger’s equation to eliminate d dt  ψ ( t ) ) . (Tip: keep in mind that in general [ H ( t ) ,G ( t )] negationslash = 0)  ˙ ψ ′ ) = ˙ U G  ψ ) + U G  ˙ ψ ) (1) = ˙ U G  ψ ) − i planckover2pi1 U G H  ψ ) (2) (b) The effective Hamiltonian in the new ’frame of reference’ must satisfy the equation: i planckover2pi1 d dt  ψ ′ ( t ) ) = H ′ ( t )  ψ ′ ( t ) ) . Use the fact that U † G U G = I , and your result from 1a, to give an expression for H ′ ( t ) in terms of H ( t ) and G ( t ). d dt  ψ ′ ) = ˙ U G U † G ( U G  ψ ) ) − i planckover2pi1 U G HU † G ( U G  ψ ) ) (3) = − i planckover2pi1 bracketleftBig U G HU † G + i planckover2pi1 ˙ U G U † G bracketrightBig  ψ ′ ) (4) Thus we see that H ′ = U G HU † G + i planckover2pi1 ˙ U G U † G (5) (c) What is H ′ ( t ) in the special case where G is not explicitly timedependent? What is H ′ in the case where H and G are both timeindependent and [ H,G ] = 0? If G is not timedependent, then ˙ U G = 0, so that H ′ = U G HU † G (6) If [ H,G ] = 0, then it follows that [ U G ,H ] = 0, so that H ′ = U G HU † G = HU G U † G = H (7) 1 (d) By definition, H ( t ) negationslash = H ′ ( t ) is defined as the energy operator. In general, would it be safe to assume that the eigenstates of H ′ ( t ) are the energy eigenstates of the system? No, it would not be a safe assumption, because H ′ is not just a unitary transformation on H , due to the addition of the ˙ U G term. Thus H ′ and H ′ will likely not have the same spectrum....
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This note was uploaded on 12/02/2010 for the course PHYSICS 851 taught by Professor M.moore during the Fall '09 term at Michigan State University.
 Fall '09
 M.Moore
 mechanics, Work

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