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By Miguel Orszag

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Additional resources for Quantum optics : including noise reduction, trapped ions, quantum trajectories, and decoherence ; with 92 problems with hints for solutions

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N! We can see that the phase ignorance washes out the off diagonal elements. 7. Define the characteristic function or “momentum generating function” (see also Chap. 7) as: ∞ CA (ξ) = Show that An = ( (iξ)n n A . n! n=0 ∂ n ) CA (ξ) |ξ=0 , ∂(iξ) CA (ξ) = T r(ρ exp(iξA)), CA (ξ) = P (A´/ρ) exp(iξA´)dA´, where A´is an eigenvalue of A and P (A´/ρ) the corresponding probability density. Hint: To prove the last property, use the second one for a continuous spectrum. 8. 7 be A = γa + γ ∗ a† . For a harmonic oscillator in a pure state α, show that 1 CA (ξ) = exp − ξ 2 γγ ∗ + i(α∗ γ ∗ + αγ) , 2 A = α∗ γ ∗ + αγ, 2 σA = A2 − A P (A´/ρ) = 2 =| γ |2 , 1 (A´− A )2 exp − 2 2 2σA 2πσA .

1 Squeezed States: General Properties and Detection We define the quadrature operators X and Y [1] X= a + a† = 2 ω q, 2 Y = a − a† = 2i 1 p. 2) ω em [X sin(ωt − k · r) − Y cos(ωt − k · r)] , 2εo v thus appearing as factor-operators in front of the sin and cos functions. 3) 1 . 11), one can write (ΔX)2 (ΔY )2 ≥ (ΔX)2 = 1 1 , (ΔY )2 = . 5) From the quadrature perspective, a coherent state is a minimum uncertainty state with equal fluctuations in both quadratures. 42 5. 7) Y )α = Im {α} . Pictorially, a coherent state can be represented, in the complex plane, as an error circle of diameter 12 and its center displaced by α (Fig.

28) are ∓R, where R≡ δ 2 + Ro2 , Eo dba | . 29) Normally, Ro is referred to as the Rabi frequency. 28) is Cb (t) = Ca (t) cos Rt 2 + iδ R sin Rt 2 o dab −i ER sin Rt 2 o dba −i ER sin Rt 2 Cb (0) cos Rt 2 − Ca (0) iδ R sin Rt 2 . 30) To take a simple example, if we start from the lower state [Cb (0) = 1], the transition probability for absorption is | Ca (t) |2 = | Rt Ro 2 | sin2 . 25) describes exactly the interaction between a two-level atom and the radiation field dCb = νCa (t) exp(−iωab t) cos ωt , dt dC i a = ν ∗ Cb (t) exp(iωab t) cos ωt , dt i where ν ≡ Eo dba .

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