2002
DOI: 10.1103/physrevb.66.201303
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Thermopower of a multiprobe ballistic conductor

Abstract: The thermopower of a multiprobe ballistic conductor in the form of caterpillarlike Sinai billiard is experimentally investigated. The magnetic-field dependence of both longitudinal thermopower and Nernst-Ettingshausen effect exhibits commensurability oscillations, which are more pronounced than the corresponding oscillations in the magnetoresistance. Results of computer calculations based on the generalized Landauer-Büttiker approach are in agreement with experiment. The observed features in the thermopower or… Show more

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Cited by 15 publications
(15 citation statements)
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“…This method is not a highly efficient way to heat the lattice and the magnitude of the heating current was 1000 times larger than typical current values used in diffusion thermopower experiments [2][3][4]. We are nevertheless certain that we did measure the phonon drag and not the diffusion thermopower for the three following reasons.…”
Section: Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…This method is not a highly efficient way to heat the lattice and the magnitude of the heating current was 1000 times larger than typical current values used in diffusion thermopower experiments [2][3][4]. We are nevertheless certain that we did measure the phonon drag and not the diffusion thermopower for the three following reasons.…”
Section: Methodsmentioning
confidence: 99%
“…The resistance [1] and the diffusion thermopower [2][3][4][5][6] of mesoscopic systems has been investigated intensively, yet no experiment to date has revealed the benefits of using the phonon-drag thermopower (PDTP) to study confined electron and phonon systems. This lack of interest can be partly traced to earlier studies of bulk semiconductors [7] and twodimensional electron gases (2DEGs) [8] that showed the phonon drag to depend only on the electron-phonon coupling and phonon parameters, not the electrical conductivity (or its derivative) as in the resistance (or the diffusion thermopower, respectively).…”
Section: Introductionmentioning
confidence: 99%
“…Например, в магнетосопротивлении решeток антиточек проявляют-ся так называемые соизмеримые осцилляции, которые обусловлены совпадением в определeнных магнитных полях размеров решeтки и циклотронного диаметра орбиты электронов -возникновением геометрических резонансов [6]. Кроме того, обнаружен аномальный рост нелокального сопротивления [7] в магнитных полях, при которых выполняются условия соизмеримости, изучены магнетополевые осцилляции диффузионной термоэдс, имеющие ту же природу, что и осцилляции магне-тосопротивления [8]. Исследованы также нелинейные эффекты при пропускании большого постоянного тока и показано, что влияние постоянного электрического поля не сводится только к эффектам разогрева, а приводит также к разрушению устойчивых электронных траек-торий за счeт дрейфа в скрещенных электрическом и магнитном полях [9].…”
Section: Introductionunclassified
“…The qualitative behavior of TP in our device agrees well with that expected from ref. 17 (not shown). As expected, the strength of the feature diminishes when V tg changes from −35 V to −21 V. Figure 3(b) clearly shows a shift in its position when V tg is held constant and V pg is changed from 0 V to −0.34 V. In addition to the (1/B)-periodic SdH oscillations, we observe highly reproducible oscillations in TP at low B (< 0.3 T), which are periodic in B [boxed region in Figure 3(a)].…”
mentioning
confidence: 99%