2018
DOI: 10.1002/qua.25667
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The effect of stochastic barrier fluctuation on semiclassical transmission probability and Shannon entropy of a symmetric double well potential

Abstract: Stochastic fluctuation of barrier height and width of a symmetric double well plays a very significant role in the corresponding dynamics by increasing the semiclassical transmission probability and Shannon entropy of the system. The population of the system has been observed to be spread into several under barrier states starting from the W L or W R [W L;R 5 1 ffiffi 2 p W 1 6W 2 ð Þ , where W 1 and W 2 are the wave functions describing the two lowest degenerate states] in presence of the stochastic fluctuati… Show more

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Cited by 4 publications
(3 citation statements)
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“…The monochromatic pulse shape is regular, whereas irregularity in the time profile is the basic character of the polychromatic pulse. In our previous works, we have found out that the basic irregularity is the reason of the excess energy which is delivered to the system [11, 13, 26, 27]. Now, for achieving a specific goal like photodetachment, we need a specific amount of energy to be delivered to the system.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…The monochromatic pulse shape is regular, whereas irregularity in the time profile is the basic character of the polychromatic pulse. In our previous works, we have found out that the basic irregularity is the reason of the excess energy which is delivered to the system [11, 13, 26, 27]. Now, for achieving a specific goal like photodetachment, we need a specific amount of energy to be delivered to the system.…”
Section: Resultsmentioning
confidence: 99%
“…But here we have taken the field strength ε to be gaussian function, that is, ε=αeβtτ2, the field structure will reach maxima at t = τ and as time proceeds the field strength will decrease exponentially [24, 25]. For this type of field, the S ( t ) can be written as S()t=αeβtτ2cos()ωt Similarly for a polychromatic pulse [26, 27], where the field strengths are of Gaussian shape S()t=iαi0.5emcos()ωiteβitτ2 Now, the matrix elements of V 12 can be written as V12italicij=σ〈〉|ϕiχj σ 〈 ϕ i | χ j 〉 is simply the square root of the Frank‐Condon (F‐C) factor and σ is a constant term which indicates the strength of coupling between the two electronic states. 〈〉|ϕiχj=pwpiwfalse˜pj The photodetachment probability ( P d ) is given by, Pd=iDit2 The dissociation probability ( P diss ) is given by, Pdiss=1()i=1nb1…”
Section: Theoretical Methodsmentioning
confidence: 99%
“…Having control over a chemical event has been an important topic of contemporary research . Both theoreticians and experimentalists are involved in developing methodologies which can have control over chemical phenomena . One of the common ways to get selective control is by the use of electromagnetic radiation.…”
Section: Introductionmentioning
confidence: 99%