Hot-electron model in doped silicon thermistors

被引:0
|
作者
Liu, D [1 ]
Galeazzi, M [1 ]
McCammon, D [1 ]
Sanders, WT [1 ]
Smith, B [1 ]
Tan, P [1 ]
Boyce, KR [1 ]
Brekosky, R [1 ]
Gygax, JD [1 ]
Kelley, R [1 ]
Mott, DB [1 ]
Porter, FS [1 ]
Stahle, CK [1 ]
Stahle, CM [1 ]
Szymkowiak, AE [1 ]
机构
[1] Univ Wisconsin, Madison, WI 53706 USA
来源
LOW TEMPERATURE DETECTORS | 2002年 / 605卷
关键词
D O I
暂无
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Non-ohmic behavior of doped silicon and germanium can be empirically explained using a hot-electron model, which is motivated by the hot-electron effect in metals at low temperatures. This model assumes that the thermal coupling between electrons and lattice at low temperatures is weaker than the coupling between electrons, so that the electric power applied to the electrons raises them to a higher temperature than the lattice. Although this model seems not suitable for semiconductors in the variable range-hopping regime, where the electrons are localized, it fits quite well the experimental data. To determine whether the hot-electron model in doped semiconductor is just an alternative way to parameterize the data or has some physical validity, we investigated the noise and the frequency-dependence of the impedance of doped silicon thermistors that arc used for low temperature thermal X-ray detectors. The measured excess white noise at low frequencies is consistent with the predicted thermodynamic fluctuations of energy between electron and phonon systems. The non-ohmic behavior shows a characteristic time that can be interpreted as a C/G time constant in the hot-electron model. By measuring this time constant, we get a hot-electron heat capacity C that agrees with the measured excess heat capacity of the implants. These support the assumption of a hot-electron system thermally separated from the lattice system.
引用
收藏
页码:87 / 90
页数:4
相关论文
共 50 条
  • [31] Silicon hot-electron bolometers with single-electron transistor readout
    Stevenson, TR
    Hsieh, WT
    Mitchell, RR
    Isenberg, HD
    Stahle, CM
    Cao, NT
    Schneider, G
    Travers, DE
    Moseley, SH
    Wollack, EJ
    Henry, RM
    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT, 2006, 559 (02): : 591 - 593
  • [32] A MANY-BAND SILICON MODEL FOR HOT-ELECTRON TRANSPORT AT HIGH-ENERGIES
    BRUNETTI, R
    JACOBONI, C
    VENTURI, F
    SANGIORGI, E
    RICCO, B
    SOLID-STATE ELECTRONICS, 1989, 32 (12) : 1663 - 1667
  • [33] A distributed device model for hot-electron bolometers
    Merkel, HF
    Khosropanah, P
    Adam, A
    Cherednichenko, S
    Kollberg, EL
    IEICE TRANSACTIONS ON ELECTRONICS, 2002, E85C (03): : 725 - 732
  • [34] CHANNEL HOT-ELECTRON DEGRADATION MODEL FOR IGFETS
    TROUTMAN, R
    COTTRELL, P
    HARROUN, T
    CHAKRAVARTI, S
    IEEE TRANSACTIONS ON ELECTRON DEVICES, 1979, 26 (11) : 1849 - 1850
  • [35] A distributed device model for hot-electron bolometers
    Merkel, Harald F.
    Khosropanah, Pourya
    Adam, Aurèle
    Cherednichenko, Serguei
    Kollberg, Erik Ludvig
    IEICE Transactions on Electronics, 2002, E85-C (03) : 725 - 732
  • [36] HOT-ELECTRON INTERACTIONS AT THE PASSIVATED GOLD-SILICON INTERFACE
    HALLEN, HD
    HUANG, T
    FERNANDEZ, A
    SILCOX, J
    BUHRMAN, RA
    PHYSICAL REVIEW LETTERS, 1992, 69 (20) : 2931 - 2934
  • [37] HOT-ELECTRON TRANSPORT IN A PULSE-DOPED GAAS STRUCTURE
    NAKAJIMA, S
    KUWATA, N
    NISHIYAMA, N
    SHIGA, N
    HAYASHI, H
    SEMICONDUCTOR SCIENCE AND TECHNOLOGY, 1992, 7 (3B) : B372 - B374
  • [38] Light emission due to hot-electron direct transitions in silicon
    Puritis, T
    ULTRAFAST PHENOMENA IN SEMICONDUCTORS, 1999, 297-2 : 307 - 310
  • [39] HOT-ELECTRON MAGNETORESISTANCE IN N-SILICON INVERSION LAYERS
    HESS, K
    PHYSICA STATUS SOLIDI A-APPLIED RESEARCH, 1975, 31 (02): : 483 - 487
  • [40] EFFECT OF IONIZED IMPURITY SCATTERING ON HOT-ELECTRON DIFFUSION IN SILICON
    CHATTOPADHYAY, D
    NAG, BR
    JOURNAL OF PHYSICS C-SOLID STATE PHYSICS, 1978, 11 (10): : 2055 - 2059