Comparative analysis of minority carrier transport in npn bipolar transistors with Si, Si1-xGex, and Si1-yCy base layers

Research output: Contribution to journalConference articleResearchpeer review

Authors

  • B. Heinemann
  • D. Knoll
  • G. G. Fischer
  • P. Schley
  • H. J. Osten

External Research Organisations

  • Leibniz Institute for High Performance Microelectronics (IHP)
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Details

Original languageEnglish
Pages (from-to)347-351
Number of pages5
JournalTHIN SOLID FILMS
Volume369
Issue number1
Publication statusPublished - 3 Jul 2000
Externally publishedYes
EventInternational Joint Conference on Silicon Epitaxyand Heterostructures (IJC-SI) - Miyagi, Japan
Duration: 12 Sept 199917 Sept 1999

Abstract

Here we present a comparative analysis of vertical minority carrier transport in Si, Si0.925Ge0.075, Si0.998C0.002, and Si0.99C0.01 base layers of bipolar transistors. We show that a conventional transit time analysis for extracting the minority carrier mobilities fails for doping profiles containing a low doped emitter region. The contribution of locally compensated charge storage, called neutral charge storage, in the emitter-base depletion region must not be neglected. To overcome drawbacks of the simple transit time analysis, we use 2D device simulations to obtain an improved understanding of the measured high-frequency parameters. Taking into account the real doping profiles and device structures, and using a calibrated parameter set for strained SiGe, the simulation results for the Si, Si1-xGex, and Si1-yCy(y≤0.2%) base layer transistors reproduce very well the measured transit times (assuming the Si data for the electron mobility μn) in the heteroepiaxial base layers. In the case of higher carbon concentration (y = 1%), the electron mobility is reduced by a factor of two.

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Cite this

Comparative analysis of minority carrier transport in npn bipolar transistors with Si, Si1-xGex, and Si1-yCy base layers. / Heinemann, B.; Knoll, D.; Fischer, G. G. et al.
In: THIN SOLID FILMS, Vol. 369, No. 1, 03.07.2000, p. 347-351.

Research output: Contribution to journalConference articleResearchpeer review

Heinemann B, Knoll D, Fischer GG, Schley P, Osten HJ. Comparative analysis of minority carrier transport in npn bipolar transistors with Si, Si1-xGex, and Si1-yCy base layers. THIN SOLID FILMS. 2000 Jul 3;369(1):347-351. doi: 10.1016/S0040-6090(00)00867-1
Heinemann, B. ; Knoll, D. ; Fischer, G. G. et al. / Comparative analysis of minority carrier transport in npn bipolar transistors with Si, Si1-xGex, and Si1-yCy base layers. In: THIN SOLID FILMS. 2000 ; Vol. 369, No. 1. pp. 347-351.
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abstract = "Here we present a comparative analysis of vertical minority carrier transport in Si, Si0.925Ge0.075, Si0.998C0.002, and Si0.99C0.01 base layers of bipolar transistors. We show that a conventional transit time analysis for extracting the minority carrier mobilities fails for doping profiles containing a low doped emitter region. The contribution of locally compensated charge storage, called neutral charge storage, in the emitter-base depletion region must not be neglected. To overcome drawbacks of the simple transit time analysis, we use 2D device simulations to obtain an improved understanding of the measured high-frequency parameters. Taking into account the real doping profiles and device structures, and using a calibrated parameter set for strained SiGe, the simulation results for the Si, Si1-xGex, and Si1-yCy(y≤0.2%) base layer transistors reproduce very well the measured transit times (assuming the Si data for the electron mobility μn) in the heteroepiaxial base layers. In the case of higher carbon concentration (y = 1%), the electron mobility is reduced by a factor of two.",
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T1 - Comparative analysis of minority carrier transport in npn bipolar transistors with Si, Si1-xGex, and Si1-yCy base layers

AU - Heinemann, B.

AU - Knoll, D.

AU - Fischer, G. G.

AU - Schley, P.

AU - Osten, H. J.

PY - 2000/7/3

Y1 - 2000/7/3

N2 - Here we present a comparative analysis of vertical minority carrier transport in Si, Si0.925Ge0.075, Si0.998C0.002, and Si0.99C0.01 base layers of bipolar transistors. We show that a conventional transit time analysis for extracting the minority carrier mobilities fails for doping profiles containing a low doped emitter region. The contribution of locally compensated charge storage, called neutral charge storage, in the emitter-base depletion region must not be neglected. To overcome drawbacks of the simple transit time analysis, we use 2D device simulations to obtain an improved understanding of the measured high-frequency parameters. Taking into account the real doping profiles and device structures, and using a calibrated parameter set for strained SiGe, the simulation results for the Si, Si1-xGex, and Si1-yCy(y≤0.2%) base layer transistors reproduce very well the measured transit times (assuming the Si data for the electron mobility μn) in the heteroepiaxial base layers. In the case of higher carbon concentration (y = 1%), the electron mobility is reduced by a factor of two.

AB - Here we present a comparative analysis of vertical minority carrier transport in Si, Si0.925Ge0.075, Si0.998C0.002, and Si0.99C0.01 base layers of bipolar transistors. We show that a conventional transit time analysis for extracting the minority carrier mobilities fails for doping profiles containing a low doped emitter region. The contribution of locally compensated charge storage, called neutral charge storage, in the emitter-base depletion region must not be neglected. To overcome drawbacks of the simple transit time analysis, we use 2D device simulations to obtain an improved understanding of the measured high-frequency parameters. Taking into account the real doping profiles and device structures, and using a calibrated parameter set for strained SiGe, the simulation results for the Si, Si1-xGex, and Si1-yCy(y≤0.2%) base layer transistors reproduce very well the measured transit times (assuming the Si data for the electron mobility μn) in the heteroepiaxial base layers. In the case of higher carbon concentration (y = 1%), the electron mobility is reduced by a factor of two.

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