1981
DOI: 10.1103/physreva.23.2496
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Analytic solutions to the two-state problem for a class of coupling potentials

Abstract: A class of pulse functions is found for which analytic solutions to the problem of two levels coupled by these pulse functions is obtained. The hyperbolic-secant coupling pulse is included in this class of functions leading to the Rosen-Zener solution, but all other pulses belonging to the class function are asymmetric. The asymmetric pulses lead to qualitatively new features in the solutions; in general, it is impossible to have a zero-transition probability with such asymmetric pulses.

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Cited by 208 publications
(134 citation statements)
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“…The phenomenon of pulsed perturbations that return the full amplitude/occupation to the initial state has been studied in the context of atom-laser interactions. [29][30][31][32] In Figs. 4-6, we compare our semiclassical estimate ͑35͒ with results from numerical simulations of the exact quantum mechanical time FIG.…”
Section: ͑36͒mentioning
confidence: 99%
“…The phenomenon of pulsed perturbations that return the full amplitude/occupation to the initial state has been studied in the context of atom-laser interactions. [29][30][31][32] In Figs. 4-6, we compare our semiclassical estimate ͑35͒ with results from numerical simulations of the exact quantum mechanical time FIG.…”
Section: ͑36͒mentioning
confidence: 99%
“…On the other hand, the κ = 0.5 case is sensitive to the condition |Λ 1 | = |Λ 2 |. The filter function (20) with κ = 0.5 can also be achieved by using a constant detuning ∆ω and an asymmetric field coupling g(t) in the Hamiltonian (3), see [11].…”
Section: The Adiabatic Limitmentioning
confidence: 99%
“…The coherence Bloch vector R ν is widely used in the theory of the magnetic resonance and characterizes the qudit behavior. In the case of the consistent field, as the expansion of the Rabi model, the solution (with the initial matrix elements ρ 1,1 (t = 0) = 1 and other ones are equal to zero) at resonance ω = H for the spin components of qubit or qutrit is the following: R = r B (sn(ωt|k) sin ht, − cn(ωt|k) sin ht, cos ht), (5) where r B = 3S/(S + 1) is the Bloch sphere radius. For higher spins, the direct calculation looks the same (5) only if k = 0.…”
Section: Master Equationmentioning
confidence: 99%
“…Such field modulation under the changing of the elliptic modulus k from 0 to 1 describes the whole class of field forms from trigonometric [4] (k = 0) to the exponentially impulse ones (k = 1) [5]. The elliptic functions cn(ωt|k) and sn(ωt|k) have a real period 4K/ω, while the function dn(ωt|k) has a period of half a duration.…”
Section: Introductionmentioning
confidence: 99%