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The_Cambridge_Handbook_of_Physics_Formulas

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5.6 Fluctuations and noise<br />

117<br />

Noise<br />

Nyquist’s noise<br />

theorem<br />

dw = kT ·βɛ(e βɛ −1) −1 dν (5.138)<br />

= kT N dν (5.139)<br />

≃ kT dν (hν ≪ kT) (5.140)<br />

Johnson<br />

(thermal) noise v rms =(4kT N R∆ν) 1/2 (5.141)<br />

voltage a<br />

Shot noise<br />

(electrical)<br />

I rms =(2eI 0 ∆ν) 1/2 (5.142)<br />

(<br />

Noise figure b f dB =10log 10 1+ T )<br />

N<br />

T 0<br />

Relative power<br />

G =10log 10<br />

(<br />

P2<br />

P 1<br />

)<br />

(5.143)<br />

(5.144)<br />

w<br />

k<br />

T<br />

T N<br />

βɛ<br />

ν<br />

h<br />

v rms<br />

R<br />

∆ν<br />

I rms<br />

−e<br />

I 0<br />

f dB<br />

T 0<br />

a <strong>The</strong>rmal voltage over an open-circuit resistance.<br />

b Noise figure can also be defined as f =1+T N /T 0 , when it is also called “noise factor.”<br />

exchangeable noise power<br />

Boltzmann constant<br />

temperature<br />

noise temperature<br />

= hν/(kT)<br />

frequency<br />

Planck constant<br />

rms noise voltage<br />

resistance<br />

bandwidth<br />

rms noise current<br />

electronic charge<br />

mean current<br />

noise figure (decibels)<br />

ambient temperature (usually<br />

taken as 290 K)<br />

G decibel gain <strong>of</strong> P 2 over P 1<br />

P 1 ,P 2 power levels<br />

5

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