Phonon assisted resonant tunneling and its phonons control
- Авторлар: Kusmartsev F.V.1, Yamamoto K.2, Egorov I.A.1, Krevchik P.V.1, Zaytsev R.V.1, Pyataev N.A.3, Nikolaev A.V.4,5, Dakhnovsky Y.6, Bukharaev A.A.7,8, Shorokhov A.V.3, Filatov D.O.9, Semenov M.B.1, Krevchik V.D.1, Aringazin A.K.10
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Мекемелер:
- Department of Physics
- Research Institute
- Mordovia State University
- Skobeltsyn Institute of Nuclear Physics
- Moscow Institute of Physics and Technology (State University)
- Department of Physics and Astronomy
- Zavoisky Institute for Physics and Technology, Kazan Scientific Center
- Kazan Federal University
- Lobachevsky State University of Nizhny Novgorod
- Institute for Basic Research
- Шығарылым: Том 104, № 6 (2016)
- Беттер: 392-397
- Бөлім: Condensed Matter
- URL: https://bakhtiniada.ru/0021-3640/article/view/159528
- DOI: https://doi.org/10.1134/S0021364016180016
- ID: 159528
Дәйексөз келтіру
Аннотация
We observe a series of sharp resonant features in the tunneling differential conductance of InAs quantum dots. We found that dissipative quantum tunneling has a strong influence on the operation of nanodevices. Because of such tunneling the current–voltage characteristics of tunnel contact created between atomic force microscope tip and a surface of InAs/GaAs quantum dots display many interesting peaks. We found that the number, position, and heights of these peaks are associated with the phonon modes involved. To describe the found effect we use a quasi-classical approximation. There the tunneling current is related to a creation of a dilute instanton–anti-instanton gas. Our experimental data are well described with exactly solvable model where one charged particle is weakly interacting with two promoting phonon modes associated with external medium. We conclude that the characteristics of the tunnel nanoelectronic devices can thus be controlled by a proper choice of phonons existing in materials, which are involved.
Авторлар туралы
F. Kusmartsev
Department of Physics
Хат алмасуға жауапты Автор.
Email: F.Kusmartsev@lboro.ac.uk
Ұлыбритания, Loughborough, LE11 3TU
K. Yamamoto
Research Institute
Email: F.Kusmartsev@lboro.ac.uk
Жапония, 2-25-22-304 Kohinata Bunkyo-ku, Tokyo
I. Egorov
Department of Physics
Email: F.Kusmartsev@lboro.ac.uk
Ресей, Penza, 440026
P. Krevchik
Department of Physics
Email: F.Kusmartsev@lboro.ac.uk
Ресей, Penza, 440026
R. Zaytsev
Department of Physics
Email: F.Kusmartsev@lboro.ac.uk
Ресей, Penza, 440026
N. Pyataev
Mordovia State University
Email: F.Kusmartsev@lboro.ac.uk
Ресей, Saransk, 430005
A. Nikolaev
Skobeltsyn Institute of Nuclear Physics; Moscow Institute of Physics and Technology (State University)
Email: F.Kusmartsev@lboro.ac.uk
Ресей, Moscow, 119991; Dolgoprudnyi, Moscow region, 141700
Y. Dakhnovsky
Department of Physics and Astronomy
Email: F.Kusmartsev@lboro.ac.uk
АҚШ, Laramie, WY, 82071
A. Bukharaev
Zavoisky Institute for Physics and Technology, Kazan Scientific Center; Kazan Federal University
Email: F.Kusmartsev@lboro.ac.uk
Ресей, Kazan, 420029; Kazan, 420008
A. Shorokhov
Mordovia State University
Email: F.Kusmartsev@lboro.ac.uk
Ресей, Saransk, 430005
D. Filatov
Lobachevsky State University of Nizhny Novgorod
Email: F.Kusmartsev@lboro.ac.uk
Ресей, Nizhny Novgorod, 603950
M. Semenov
Department of Physics
Email: F.Kusmartsev@lboro.ac.uk
Ресей, Penza, 440026
V. Krevchik
Department of Physics
Email: F.Kusmartsev@lboro.ac.uk
Ресей, Penza, 440026
A. Aringazin
Institute for Basic Research
Email: F.Kusmartsev@lboro.ac.uk
Қазақстан, Astana, 010008
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