Transmission and Dwell Time Oscillations Caused by Coexistence of Tunneling and Propagating in a Trapezoidal Barrier

Abstract A refined one of our exactly solvable trapezoidal barrier potential model [Thin Solids Films, 414 (2002) 136)] for metal-insulator-metal tunnel junctions has Seen presented. According to the refined model, the longitudinal kinetic energy (ExL) and the effective mass (m^*L) of the electron8...

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Published inCommunications in theoretical physics Vol. 53; no. 3; pp. 462 - 468
Main Author 舒启清 柳文军 王少明 蒋一 马文淦
Format Journal Article
LanguageEnglish
Published IOP Publishing 01.03.2010
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ISSN0253-6102
DOI10.1088/0253-6102/53/3/11

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Abstract Abstract A refined one of our exactly solvable trapezoidal barrier potential model [Thin Solids Films, 414 (2002) 136)] for metal-insulator-metal tunnel junctions has Seen presented. According to the refined model, the longitudinal kinetic energy (ExL) and the effective mass (m^*L) of the electron8 in the electrode on the left of the barrier distinguish from that on the right. It is found that as ExL is greater than the shorter side of the resultant trapezoidal barrier potential, there will be a coexistence of the tunneling and propagating in the barrier. The results demonstrate that the damped oscillating electron waves localized in the propagating barrier subregion lead to the oscillation and enhancement in the transmission coefficient DT and dwell time TD. For the barrier height φ1=2.6 eV and φ2 = 1.4 eV, the width d=22 A and ExL = 1.0 eV, DT and TD have a maximum of 0.054 and 0.58x10^-15 s at V = 2.04 V and 2.18 V, respectively. This suggests that a real tunneling may be a hybrid.
AbstractList Abstract A refined one of our exactly solvable trapezoidal barrier potential model [Thin Solids Films, 414 (2002) 136)] for metal-insulator-metal tunnel junctions has Seen presented. According to the refined model, the longitudinal kinetic energy (ExL) and the effective mass (m^*L) of the electron8 in the electrode on the left of the barrier distinguish from that on the right. It is found that as ExL is greater than the shorter side of the resultant trapezoidal barrier potential, there will be a coexistence of the tunneling and propagating in the barrier. The results demonstrate that the damped oscillating electron waves localized in the propagating barrier subregion lead to the oscillation and enhancement in the transmission coefficient DT and dwell time TD. For the barrier height φ1=2.6 eV and φ2 = 1.4 eV, the width d=22 A and ExL = 1.0 eV, DT and TD have a maximum of 0.054 and 0.58x10^-15 s at V = 2.04 V and 2.18 V, respectively. This suggests that a real tunneling may be a hybrid.
Author 舒启清 柳文军 王少明 蒋一 马文淦
AuthorAffiliation College of Materials Science and Engineering, Shenzhen University, Shenzhen 518060, China Shenzhen Key Laboratory of Special Functional Materials, Shenzhen University, Shenzhen 518060, China Department of Modern Physics, University of Science and Technology of China, Hefei 230026, China
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Notes tunnel junctions, trapezoidal barrier, coexistence of the tunneling and propagating, dwell time
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Snippet Abstract A refined one of our exactly solvable trapezoidal barrier potential model [Thin Solids Films, 414 (2002) 136)] for metal-insulator-metal tunnel...
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StartPage 462
SubjectTerms 停留时间
固体薄膜
振动传播
阻尼振荡
隧道结
Title Transmission and Dwell Time Oscillations Caused by Coexistence of Tunneling and Propagating in a Trapezoidal Barrier
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