A REVIEW OF 1/f NOISE IN TERMS OF MOBILITY FLUCTUATIONS AND WHITE NOISE IN MODERN SUBMICRON BIPOLAR TRANSISTORS — BJTs AND HBTs

2001 ◽  
Vol 01 (04) ◽  
pp. R175-R199 ◽  
Author(s):  
L. K. J. VANDAMME ◽  
GY. TREFÁN

Experimental studies on low frequency noise in bipolar junction transistors (BJT) including polysilicon emitter, hetero-junction bipolar transistors (HBTs) and silicon-germanium hetero-junction transistors (SiGe HBTs) are reviewed. The 1/f noise is treated in terms of mobility fluctuations. The validity of a new empirical relation between the 1/f noise corner frequency fc (the frequency where the 1/f noise and shot noise are equal) and the peak cutoff frequency frpeak is investigated. The experimental procedure to investigate the most dominant low-frequency noise source in the equivalent circuit is described. At medium frequencies, the white noise becomes dominant and the noise figure is calculated taking into account the emitter and base series resistance.

2007 ◽  
Vol 07 (03) ◽  
pp. L321-L339 ◽  
Author(s):  
L. K. J. VANDAMME

Often the 1/f noise in MOSFETs is stated to be an ensemble of many RTS with different time constants. The majority of literature on 1/f noise is overlooking the contribution due to mobility fluctuations that are uncorrelated with number fluctuations. Here, we demonstrate that the so-called proofs for Δ N can also be obtained from the empirical relation. The following misunderstandings and controversial topics on the surface and bulk contributions to the low-frequency noise will be addressed: 1) 1/f and RTS noise can have different physical origins. An analysis in time domain shows that the low-frequency noise with RTS is nothing else than a superposition of a two level noise with a Lorentzian spectrum and a Gaussian noise with a pure 1/f spectrum and different bias dependency. 2) It is very unlikely that in a spectrum consisting of one strong two level RTS and a pure 1/f noise, the 1/f noise is a superposition of many RTS with different time constants. 3) The spreading in WLS I /I2 below a critical WL is not a proof for the Δ N origin. 4) The typical shape in the double log plot from sub threshold to strong inversion of S I/ I 2 versus I , is also not a proof for the Δ N origin.


1999 ◽  
Vol 43 (5) ◽  
pp. 931-936 ◽  
Author(s):  
Jean-Marc Routoure ◽  
Jacques Lepaisant ◽  
Daniel Bloyet ◽  
Serge Bardy ◽  
Jacques Lebailly

2011 ◽  
Vol 324 ◽  
pp. 441-444 ◽  
Author(s):  
Jalal Jomaah ◽  
Majida Fadlallah ◽  
Gerard Ghibaudo

A review of recent results concerning the low frequency noise in modern CMOS devices is given. The approaches such as the carrier number and the Hooge mobility fluctuations used for the analysis of the noise sources are illustrated through experimental data obtained on advanced CMOS generations. Furthermore, the impact on the electrical noise of the shrinking of CMOS devices in the deep submicron range is also shown.


2000 ◽  
Vol 76 (23) ◽  
pp. 3442-3444 ◽  
Author(s):  
J. A. Garrido ◽  
B. E. Foutz ◽  
J. A. Smart ◽  
J. R. Shealy ◽  
M. J. Murphy ◽  
...  

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