2020
DOI: 10.1140/epjp/s13360-020-00632-0
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Effect of the nearby levels on the resonance fluorescence spectrum of the atom–field interaction

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Cited by 3 publications
(6 citation statements)
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“…We consider that the field is approximately tuned to the transition frequency between the levels |g⟩ and |e⟩ of the atom, but detuned from the nearby levels |j⟩ (AC Stark effect). The Hamiltonian that describes this system is [9,12,15,21]…”
Section: Ac Stark Shift Hamiltonianmentioning
confidence: 99%
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“…We consider that the field is approximately tuned to the transition frequency between the levels |g⟩ and |e⟩ of the atom, but detuned from the nearby levels |j⟩ (AC Stark effect). The Hamiltonian that describes this system is [9,12,15,21]…”
Section: Ac Stark Shift Hamiltonianmentioning
confidence: 99%
“…we use χ = 0.5, a value that falls within the validity range of the assumed approximation for the Hamiltonian (1) [15], and we set g = 1. We can observe that for values of ∆ > 0, i.e., when the frequency of the atom is higher than that of the field, the lineshapes rapidly decay towards the initial state of the atom, i.e., there are no transitions between the two levels, regardless of the value of the parameter r. On the other hand, for values of ∆ < 0, we notice that as we increase the negative values of r in ascending order, the lineshapes become distorted and approach the initial state of the atom more rapidly, due to the widening of the probability distribution as the values of r decrease, as shown in Figure 2a.…”
Section: Squeezed Coherent Statesmentioning
confidence: 99%
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“…Suponemos que el campo está aproximadamente en sintonía con la frecuencia de transición entre los niveles |g y |e del átomo, pero fuera de sintonía con los niveles cercanos |j (efecto AC Stark). El Hamiltoniano que describe este sistema se expresa como [22,23,29,30]…”
Section: Modelo De Jaynes-cummings Y Estados Virtuales No Resonantesunclassified
“…Sin embargo, esta diferencia en las formas de línea (cuando el átomo se encuentra en el estado base o excitado) no permite discernir entre estados pares e impares cuando el número promedio de fotones es n > 4. La razón de esta imposibilidad es que el rango de validez del Hamiltoniano (1) está limitado a valores de χ menores que 1 [30], y a que para un numero promedio de fotones lo suficientemente grande, la distribución de probabilidad para los estados coherentes pares e impares son aproximadamente indistinguibles.…”
Section: Estados Gato De Schrödingerunclassified