Flicker noise

Flicker noise

Flicker noise is a type of electronic noise with a 1/f, or pink spectrum. It is therefore often referred to as 1/f noise or pink noise, though these terms have wider definitions. It occurs in almost all electronic devices, and results from a variety of effects, such as impurities in a conductive channel, generation and recombination noise in a transistor due to base current, and so on. It is always related to a direct current.

In electronic devices, it is a low-frequency phenomenon, as the higher frequencies are overshadowed by white noise from other sources. In oscillators, however, the low-frequency noise is mixed up to frequencies close to the carrier which results in oscillator phase noise.

Flicker noise is often characterized by the corner frequency f_mathrm{c} between the regions dominated by each type. MOSFETs have a higher f_mathrm{c} than JFETs or bipolar transistors which is usually below 2 kHz for the latter.

The flicker noise voltage power in MOSFET can be expressed by K/(Cox*W*L*f), where K is the process-dependent constant, W and L are channel width and length respectively [Behzad Razavi, Design of Analog CMOS Integrated Circuits, McGraw-Hill, 2000, Chapter 7: Noise.] .

Flicker noise is found in carbon composition resistors, where it is referred to as "excess noise", since it increases the overall noise level above the thermal noise level, which is present in all resistors. In contrast, wire-wound resistors have the least amount of flicker noise. Since flicker noise is related to the level of DC, if the current is kept low, thermal noise will be the predominant effect in the resistor, and the type of resistor used will not affect noise levels.

For measurements the interest is in the "drift" of a variable with respect to a measurement at a previous time. This is calculated by applying the signal time differencing:

1-e^{-Tdcdot s}

tofrac{a}{f}

Where Td is the time between measurements, s=icdot2pi f, anda includes thecontribution of both positive and negative frequency terms.

After some manipulation, the variance of the voltage difference is:

2aint_{0}^{f_{hfrac{1-cos(Tdcdot2pi f)}{f}df=-2acdot Cin(Tdcdot2pi f_{h})

[Milton Abramowitz and Irene A. Stegun, eds. "Handbook of Mathematical Functions with Formulas, Graphs, and Mathematical Tables." New York: Dover, 1972. " [http://www.math.sfu.ca/~cbm/aands/page_228.htm (See Chapter 5)] "
* " [http://www.math.sfu.ca/~cbm/aands/page_231.htm (Section 5.2, Sine and Cosine Integrals)] "
] Where f_{h} is a brick wall filter limiting the upper bandwidth during measurement.

Real measurements involve more complicated calculations.

See also

* Aldert van der Ziel
* Noise (physics)
* Electronic noise

References

* cite journal
author = Johnson, J. B.
date= 1925
title = The Schottky effect in low frequency circuits
journal = Physical Review
volume = 26
pages = 71–85
doi = 10.1103/PhysRev.26.71

* cite journal
author = Schottky, W.
date= 1918
title = Über spontane Stromschwankungen in verschiedenen Elektrizitätsleitern
journal = Annalen der Physik
volume = 362
pages = 541–567
doi = 10.1002/andp.19183622304

* cite journal
author = Schottky, W.
date= 1922
title = Zur Berechnung und Beurteilung des Schroteffektes
journal = Annalen der Physik
volume = 373
pages = 157–176
doi = 10.1002/andp.19223731007

* [http://www.rane.com/par-f.html#flicker_noise Rane Pro Audio Reference definition of "flicker noise"]
* [http://www.odyseus.nildram.co.uk/RFIC_Theory_Files/Noise_Tutorial.pdf#search=%22flicker%20noise%20tutorial%22 Noise Tutorial]


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