Abstract:SUMMARYAs a promising resonant tunneling structure for reduction of tunneling time, the "asymmetric rectangular double-barrier structure with an acceleration well" is proposed. Analytical expressions are derived for the tunneling transmission coefficient of the electrons and for the resonant condition. Also, the condition for the shortest tunneling time is analytically studied by using the dwell time as the tunneling time. From the resonant condition, the width of each layer can be determined for a given reson… Show more
“…(9) and (10), the outer well widths L w1 , L w2 , and L w3 of the single barrier structure with outer wells can be determined from Eq. (15).…”
Section: Determination Of the Resonant Structurementioning
confidence: 99%
“…Table 3 lists the dwell times τ d (E 1 ) and τ d (E 2 ) of the electrons with resonant energy values of E 1 and E 2 in the triple barrier structure with outer wells and the dwell times for the resonant energies E 1 and E 2 in the triple barrier structure without outer wells. For reference, the dwell time in the triple barrier structure with a prewell is also listed in Table 3 (it is considered possible to reduce the dwell time by a prewell [15]). Table 3 shows that the dwell time in the triple barrier structure with a prewell can be reduced to about 25% for τ d (E 1 ) and about 39% for τ d (E 2 ) in comparison with those in the triple barrier structure without outer wells.…”
Section: Dwell Timementioning
confidence: 99%
“…To date, many studies have been carried out, both theoretically and experimentally [3][4][5][6][7][8][9][10][11][12][13][14][15].…”
SUMMARYThe impact of the outer wells on tunneling characteristics is theoretically studied in a new structure with outer wells consisting of wells on both sides of an asymmetrical triple barrier structure. First, the theoretical equation for the transmission coefficient is derived and the resonance conditions are studied. It is found that resonance is not related to the existence of the outer wells and is governed by the two resonance conditions independently existing in the two wells between the barriers. Second, the dwell time of electrons at the two resonant energy values is analyzed. The dwell time in the triple barrier structure with outer wells is compressed to about 14% at the maximum in comparison with the dwell time in the triple barrier structure without outer wells. Even if the dwell time is compared with that in the structure with a prewell, which is a conventional way of reducing the dwell time, a reduction to about 60% is realized. Also, with regard to the current density versus voltage characteristics for the structure with outer wells, it is found that a large current flows at a lower voltage than in the structure without outer wells.
“…(9) and (10), the outer well widths L w1 , L w2 , and L w3 of the single barrier structure with outer wells can be determined from Eq. (15).…”
Section: Determination Of the Resonant Structurementioning
confidence: 99%
“…Table 3 lists the dwell times τ d (E 1 ) and τ d (E 2 ) of the electrons with resonant energy values of E 1 and E 2 in the triple barrier structure with outer wells and the dwell times for the resonant energies E 1 and E 2 in the triple barrier structure without outer wells. For reference, the dwell time in the triple barrier structure with a prewell is also listed in Table 3 (it is considered possible to reduce the dwell time by a prewell [15]). Table 3 shows that the dwell time in the triple barrier structure with a prewell can be reduced to about 25% for τ d (E 1 ) and about 39% for τ d (E 2 ) in comparison with those in the triple barrier structure without outer wells.…”
Section: Dwell Timementioning
confidence: 99%
“…To date, many studies have been carried out, both theoretically and experimentally [3][4][5][6][7][8][9][10][11][12][13][14][15].…”
SUMMARYThe impact of the outer wells on tunneling characteristics is theoretically studied in a new structure with outer wells consisting of wells on both sides of an asymmetrical triple barrier structure. First, the theoretical equation for the transmission coefficient is derived and the resonance conditions are studied. It is found that resonance is not related to the existence of the outer wells and is governed by the two resonance conditions independently existing in the two wells between the barriers. Second, the dwell time of electrons at the two resonant energy values is analyzed. The dwell time in the triple barrier structure with outer wells is compressed to about 14% at the maximum in comparison with the dwell time in the triple barrier structure without outer wells. Even if the dwell time is compared with that in the structure with a prewell, which is a conventional way of reducing the dwell time, a reduction to about 60% is realized. Also, with regard to the current density versus voltage characteristics for the structure with outer wells, it is found that a large current flows at a lower voltage than in the structure without outer wells.
“…Double-barrier resonant tunneling quantum structures have been extensively investigated due to their potential device http://dx.doi.org/10.1016/j.spmi.2015.05.016 0749-6036/Ó 2015 Elsevier Ltd. All rights reserved. applications [11][12][13][14]. Theoretical studies on tunneling phenomena in asymmetric rectangular double-barrier structures [11,12] have been performed.…”
“…Since then, theoretical works on symmetric double-barrier structures [18,19] and asymmetrical double-barrier structures under an applied bias [20,21] have been performed. Recently, Hamaguchi et al [22] calculated the tunneling-time for an asymmetrical rectangular double-barrier structure with an acceleration well, a structure that is expected to reduce the tunnelingtime. Simanjuntak et al [23] studied the time it takes an electron wave packet to traverse a superlattice with n cells and square-barrier periodic potential.…”
We analyze the tunneling-time of a spatial wave packet which traverses a resonant structure by means of the presence-time formalism. With this method we can evaluate the finite size effects of the corresponding energy probability distribution in the tunneling-time. We show that these effects are not negligible and reduce the tunneling-time by 25%. An expression for the resonant tunneling-time is derived, r 3 /2Γ , where r Γ is the width of the resonance. We confirm numerically this result for two resonant structures: a superlattice with n cells and square-barrier periodic potential, and an asymmetrical rectangular double-barrier potential.
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