Please use this identifier to cite or link to this item:
https://doi.org/10.1109/ARFTGS.2005.1500569
DC Field | Value | |
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dc.title | Three-port RF characterization of MOS transistors | |
dc.contributor.author | Mahalingam, U. | |
dc.contributor.author | Rustagi, S.C. | |
dc.contributor.author | Samudra, G.S. | |
dc.date.accessioned | 2014-10-07T04:51:10Z | |
dc.date.available | 2014-10-07T04:51:10Z | |
dc.date.issued | 2005 | |
dc.identifier.citation | Mahalingam, U.,Rustagi, S.C.,Samudra, G.S. (2005). Three-port RF characterization of MOS transistors. 65th ARFTG Microwave Measurements Conference Digest 2005 : 57-62. ScholarBank@NUS Repository. <a href="https://doi.org/10.1109/ARFTGS.2005.1500569" target="_blank">https://doi.org/10.1109/ARFTGS.2005.1500569</a> | |
dc.identifier.isbn | 0780388585 | |
dc.identifier.uri | http://scholarbank.nus.edu.sg/handle/10635/84307 | |
dc.description.abstract | This paper presents the complete RF characterization of a MOSFET in terms of its 3-port admittance network parameters up to the cut-off frequency. The effect of the non-ideal short presented by the GPG (Ground Power Ground) probe - used at the third port for 2-port RF measurements - on characterized data is discussed. An algorithm is developed to de-embed the non-ideal short by (i) characterizing the GPG probe, (ii) representing the transistor by its general equivalent circuit whose components are extracted from the measured y-parameter data in three different configurations, and, (iii) reconstructing the 3-port parameters after removing the GPG probe impedance from the network. The validity of the method is demonstrated by the close agreement between diagonal elements of the 3-port admittance matrix obtained from two different configurations. Without probe de-embedding, the disagreement is over 70% at higher frequencies in some of the parameters. From the accurate de-embedded admittance parameters, the measured 3-port capacitance coefficients for the MOS transistor at different frequencies and biases are reported for the first time. Interestingly, it is observed that the non-quasi-static channel conduction manifests as the increasing difference in the magnitudes of Gsg (trans-conductance in Common Drain configuration) and Gdg (trams-conductance in Common Source configuration) with frequency. | |
dc.description.uri | http://libproxy1.nus.edu.sg/login?url=http://dx.doi.org/10.1109/ARFTGS.2005.1500569 | |
dc.source | Scopus | |
dc.subject | Admittance matrix | |
dc.subject | Capacitance | |
dc.subject | Impedance | |
dc.subject | Inductance | |
dc.subject | Modeling | |
dc.subject | MOSFETs | |
dc.subject | Scattering parameters measurement | |
dc.type | Conference Paper | |
dc.contributor.department | ELECTRICAL & COMPUTER ENGINEERING | |
dc.description.doi | 10.1109/ARFTGS.2005.1500569 | |
dc.description.sourcetitle | 65th ARFTG Microwave Measurements Conference Digest 2005 | |
dc.description.page | 57-62 | |
dc.identifier.isiut | NOT_IN_WOS | |
Appears in Collections: | Staff Publications |
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