EE539: Analog Integrated Circuit Design; Lecture 15
Nagendra Krishnapura ([email protected]) 06 Feb. 2006
Input Referred noise
Noisy
Components Sv
out
Components Svout
Svin
Vin=0
Noiseless
Figure 1: Input Referred noise
Consider a network whose output noise power spectral density isSvout. Now, if we make all the components in the network noiseless, then the noise that should be present at the input of the network in order to get the sameSvout at the output is called the ”input referred noise”.
PSD of the input referred noise (Svin) is given by Svin = Svout
|H(f)|2 where|H(f)|is the transfer function from input to output.
Input referred noise is useful when we need to compare the noise and input signal level.
For e.g.Let us calculate the input referred noise for a MOSFET.(Fig. 2)
Svin = SID+SIR
gm2 =
4kT
R +8kTgm 3
gm2 = 4kT gm
1 gmR +2
3
Dynamic Range
Let us calculate the Dynamic Range of a MOSFET amplifier.
Let the input signal have a peak amplitudeVp.Neglecting noise due to load resistance and assuming a band- width of B,
1
2
Vdd
R
SID=(8/3)KTgm SIR=4KT/R
Figure 2: MOSFET noise
S N
i
= V
√p
2
q8kT B
3gm
For an SNR of 0dB,
Vpmin = s
16kT B 3gm
For a max Harmonic Distortion of x%,
Vpmax Vpmin
= 4(VGS−VT)x q16kT B
3gm
= 4x q16kT B
3
rµCoxW
L (VGS−VT)32
= Vpmax Vpmin
= 4x q16kT B
3
1 µCoxW
L
14(2ID)34
Dynamic Range= 20∗logV
pmax
Vpmin
From these equations, we see that the dynamic range can be increased by
• increasing the overdrive for the same aspect ratio
• decreasing the aspect ratio while keeping the bias current constant. (But it is a weak function of aspect ratio)
3
Common Drain Amplifier(Source Follower) Vdd
V
inV
outI
0Figure 3: Source Follower Consider the source follower (Fig. 3)
Vout =Vin +VGS=Vin +VT +
s 2I0
„
µCoxW
L
«
Small signal gain = 1 (if there is no body effect)