Hostname: page-component-8448b6f56d-tj2md Total loading time: 0 Render date: 2024-04-20T05:52:29.893Z Has data issue: false hasContentIssue false

A proposed simulation technique to study the series resistance and related millimeter-wave properties of Ka-band Si IMPATTs from the electric field snapshots

Published online by Cambridge University Press:  23 January 2013

Aritra Acharyya*
Affiliation:
Institute of Radio Physics and Electronics, University of Calcutta, 92, APC Road, Kolkata 700009, India. Phone: +91 9432979721
Suranjana Banerjee
Affiliation:
Institute of Radio Physics and Electronics, University of Calcutta, 92, APC Road, Kolkata 700009, India. Phone: +91 9432979721 Academy of Technology, West Bengal University of Technology, Adisaptagram, Hooghly 712121, West Bengal, India
J. P. Banerjee
Affiliation:
Institute of Radio Physics and Electronics, University of Calcutta, 92, APC Road, Kolkata 700009, India. Phone: +91 9432979721 Academy of Technology, West Bengal University of Technology, Adisaptagram, Hooghly 712121, West Bengal, India
*
Corresponding author: A. Acharyya Email: ari_besu@yahoo.co.in

Abstract

A large-signal model and a simulation technique based on non-sinusoidal voltage excitation are used to obtain the electric field snapshots from which the series resistance and related high-frequency properties of a 35 GHz Silicon Single-Drift Region (SDR) Impact Avalanche Transit Time (IMPATT) device have been estimated for different bias current densities. A novel method is proposed in this paper to determine the parasitic series resistance of a millimeter-wave IMPATT device from large-signal electric field snapshots at different phase angles of a full cycle of steady-state oscillation. The method is based on the depletion width modulation of the device under a large-signal condition. The series resistance of the device is also obtained from the large-signal admittance characteristics at threshold frequency. The values of series resistance of a 35 GHz SDR IMPATT diode obtained from the proposed method and the large-signal admittance method are compared with experimentally reported values. The results show that the proposed method provides better and closer agreement with the experimental value.

Type
Research Paper
Copyright
Copyright © Cambridge University Press and the European Microwave Association 2013

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

REFERENCES

[1]Midford, T.A.; Bernick, R.L.: Millimeter wave CW IMPATT diodes and oscillators. IEEE Trans. Microw. Theory Tech, 27 (1979), 483492.Google Scholar
[2]Chang, Y.; Hellum, J.M.; Paul, J.A.; Weller, K.P.: Millimeter-wave IMPATT sources for communication applications. IEEE MTT-S Int. Microwave Symp. Digest, 1977, 216219.Google Scholar
[3]Gray, W.W.; Kikushima, L.; Morentc, N.P.; Wagner, R.J.: Applying IMPATT power sources to modern microwave systems. IEEE J. Solid-State Circuits, 4 (1969), 409413.Google Scholar
[4]Ray, U.C.; Gupta, A.K.: Measurement of electrical series resistance of W-band Si IMPATT diode. in Second Asia Pacific Microwave Conf. Proc., China, 1988, 434437.Google Scholar
[5]Misawa, T.: Multiple uniform layer approximation in analysis of negative resistance in p-n junction in breakdown. IEEE Trans. Electron Devices, 14 (1967), 795808.Google Scholar
[6]Adlerstein, M.G.; Holway, L.H.; Chu, S.L.G.: Measurement of series resistance in IMPATT diodes. IEEE Trans. Electron Devices, 30 (1983), 179182.Google Scholar
[7]Mitra, M.; Das, M.; Kar, S.; Roy, S.K.: A study of the electrical series resistance of Si IMPATT diodes. IEEE Trans. Electron Devices, 40 (1993), 18901893.Google Scholar
[8]Pal, T.K.: Series resistance of silicon millimeter wave (Ka-band) IMPATT diodes. Def. Sci. J., 59 (2009), 189193.Google Scholar
[9]Acharyya, A.; Banerjee, S.; Banerjee, J.P.: Effect of junction temperature on the large-signal properties of a 94 GHz silicon based double-drift region impact avalanche transit time device. J. Semicond., 34 (2013), 024001–12.Google Scholar
[10]Acharyya, A.; Banerjee, S.; Banerjee, J. P.: Large-signal simulation of 94 GHz pulsed DDR silicon IMPATTs including the temperature transient effect. Radioengineering, 21 (2012), 12181225.Google Scholar
[11]Acharyya, A.; Banerjee, S.; Banerjee, J.P.: Temperature transient effect on the large-signal properties and frequency chirping in pulsed silicon DDR IMPATTs at 94 GHz, in IEEE Conf. CODEC 2012, Kolkata, India, 2012, 13.Google Scholar
[12]Pal, T.K.; Banerjee, J.P.: Design, fabrication and RF characterization of Ka-band silicon IMPATT diode. Int. J. Eng. Sci. Technol., 2 (2010), 47754790.Google Scholar
[13]Grant, W.N.: Electron and hole ionization rates in epitaxial silicon. Solid State Electron, 16 (1973), 11891203.Google Scholar
[14]Canali, C.; Ottaviani, G.; Quaranta, A.A.: Drift velocity of electrons and holes and associated anisotropic effects in silicon. J. Phys. Chem. Solids, 32 (1971), 1707.Google Scholar
[15]Zeghbroeck, B.V.: Principles of Semiconductor Devices, Colorado Press, USA, 2011.Google Scholar
[16]Electronic Archive: New Semiconductor Materials, Characteristics and Properties: http://www.ioffe.ru/SVA/NSM/Semicond/Si/index.htmlGoogle Scholar
[17]Resistivity, conductivity and temperature coefficients for some common materials: http://www.engineeringtoolbox.com/resistivity-conductivity-d_418.htmlGoogle Scholar
[18]Kurokawa, K.: Some basic characteristics to broadband negative resistance oscillators. Bell. Syst. Tech. J., 48 (1969), 19371955.Google Scholar
[19]Sridharan, M.; Roy, S.K.: Computer studies on the widening of the avalanche zone and decrease on efficiency in silicon X-band sym. DDR. Electron Lett., 14 (1978), 635637.Google Scholar
[20]Sridharan, M.; Roy, S.K.: Effect of mobile space charge on the small signal admittance of silicon DDR. Solid State Electron, 23 (1980), 10011003.Google Scholar