20
Lock-in amplifiers http://www.lockin.de/

Lock-in amplifiers . Signals and noise Frequency dependence of noise Low frequency ~ 1 / f –example: temperature (0.1 Hz), pressure

Embed Size (px)

Citation preview

Page 1: Lock-in amplifiers . Signals and noise Frequency dependence of noise Low frequency ~ 1 / f –example: temperature (0.1 Hz), pressure

Lock-in amplifiers

http://www.lockin.de/

Page 2: Lock-in amplifiers . Signals and noise Frequency dependence of noise Low frequency ~ 1 / f –example: temperature (0.1 Hz), pressure

Signals and noiseFrequency dependence of noise• Low frequency ~ 1 / f

– example: temperature (0.1 Hz) , pressure (1 Hz), acoustics (10 -- 100 Hz)

• High frequency ~ constant = white noise– example: shot noise, Johnson noise, spontaneous emission

noise• Total noise depends strongly on signal freq

– worst at DC, best in white noise region• Problem -- most signals at DC

log(Vnoise)

log(f )

Noise amplitude

1/f noise

0

White noise

0.1 1 10 100 1kHz

log(

Vno

ise)

log(f )

Total noise in 10 Hz bandwidth

1/f noise

0

White noise

0.1 1 10 100 1kHz

Signal at DC

log(

Vno

ise)

log(f )

1/f noise

0

White noise

0.1 1 10 100 1kHz

Signal at 1 kHz

10 Hz

10 Hz

Page 3: Lock-in amplifiers . Signals and noise Frequency dependence of noise Low frequency ~ 1 / f –example: temperature (0.1 Hz), pressure

Lock-in amplifiers• Shift signal out to higher frequencies• Approach:• Modulate signal, but not noise, at high freq

– no universal technique -- art– example: optical chopper wheel, freq modulation

• Detect only at modulation frequency– Noise at all other frequencies averages to zero– Use demodulator and low-pass filter

Page 4: Lock-in amplifiers . Signals and noise Frequency dependence of noise Low frequency ~ 1 / f –example: temperature (0.1 Hz), pressure

Demodulation / Mixing• Multiply input signal by sine wave• Sum and difference freq generated• Compare to signal addition -- interference• Signal frequency close to reference freq

– low freq beat– DC for equal freq sine waves– DC output level depends on relative phase

Two sine waves

Product

Sum

Page 5: Lock-in amplifiers . Signals and noise Frequency dependence of noise Low frequency ~ 1 / f –example: temperature (0.1 Hz), pressure

Signal freq approaches ref freq• Beat frequency approaches DC as signal freq approaches ref freq

1

1.05

1.1

1.15

1.2

1.25

Signal freqvs ref freq

Reference

Mix

er o

utpu

ts

Page 6: Lock-in amplifiers . Signals and noise Frequency dependence of noise Low frequency ~ 1 / f –example: temperature (0.1 Hz), pressure

Phase sensitive detection• Signal freq matches reference freq• Reference = sin(2ft) • Signal = sin(2ft + )

– is signal phase shift• Product = cos() - cos(2ft)

Signalphaseshift

0

0.2

0.4

0.6

0.8

Reference wave

Prod

uct w

avef

orm

s--

sig

nal t

imes

ref

eren

ceDC part

Page 7: Lock-in amplifiers . Signals and noise Frequency dependence of noise Low frequency ~ 1 / f –example: temperature (0.1 Hz), pressure

Low pass filterRemoves noise• Example -- modulate above 1/f noise

– noise slow compared to reference freq– noise converted to slowly modulated sine wave– averages out to zero over 1 cycle

• Low pass filter integrates out modulated noise – leaves signal alone

Reference

Input Output Mixer Low pass

filter Buffer

Lock-in amplifier Demodulated signal

After mixer

Vol

tage

time

After mixer & low pass

Page 8: Lock-in amplifiers . Signals and noise Frequency dependence of noise Low frequency ~ 1 / f –example: temperature (0.1 Hz), pressure

Typical LIA low pass filters• For weak signal buried in noise

• Ideal low pass filter blocks all except signal

• Approximate ideal filter with cascaded low pass filters

18 db/oct

12 db/oct

6 db/oct

Ideal

loggain

frequency

Page 9: Lock-in amplifiers . Signals and noise Frequency dependence of noise Low frequency ~ 1 / f –example: temperature (0.1 Hz), pressure

Phase control• Reference has phase control

• Can vary from 0 to 360°

• Arbitrary input signal phase

• Tune reference phase to give maximum DC output

Reference

Phaseshift

Input Output Mixer

Page 10: Lock-in amplifiers . Signals and noise Frequency dependence of noise Low frequency ~ 1 / f –example: temperature (0.1 Hz), pressure

Reference options• Option 1 -- Internal reference

– best performance

– stable reference freq

• Option 2 -- External reference

• System generates reference– ex: chopper wheel

• Lock internal ref to system ref– use phase locked loop (PLL)

– source of name “lock-in amplifier”

Reference

Signal Mixer

Lock-in amplifier System

Reference

Signal Mixer

Lock-in amplifier System

VCO

Integrate

PLL

Page 11: Lock-in amplifiers . Signals and noise Frequency dependence of noise Low frequency ~ 1 / f –example: temperature (0.1 Hz), pressure

Analog mixer• Direct multiplication

– accurate

– not enough dynamic range

– weak signal buried in noise

• Switching mixer– big dynamic range

– but also demodulates harmonics

Multiplying mixer

Switching mixer

Harmonic content of square wave

1

1/31/5 1/7 1/9

Page 12: Lock-in amplifiers . Signals and noise Frequency dependence of noise Low frequency ~ 1 / f –example: temperature (0.1 Hz), pressure

Switching mixer design• Sample switching mixer• Back-to-back FETs

– example: 1 n-channel & 1 p-channel– feed signal to one FET, inverted signal to second FET

• Apply square wave to gates– upper FET conducts on positive part of square wave– lower FET conducts on negative part

Switching mixer circuit

p

n

Signal voltage

source draingate

bias

n-channel FET

Page 13: Lock-in amplifiers . Signals and noise Frequency dependence of noise Low frequency ~ 1 / f –example: temperature (0.1 Hz), pressure

Signals with harmonic content• Option 1: Use multi-switch mixer

– approximate sine wave

– cancel out first few harmonic signals

• Option 2: Filter harmonic content from signal– bandpass filter at input

– Q > 100

Lock-in amp with input filter

Page 14: Lock-in amplifiers . Signals and noise Frequency dependence of noise Low frequency ~ 1 / f –example: temperature (0.1 Hz), pressure

Digital mixers

• Digitize input with DAC• Multiply in processor• Advantages:

– Accurate sine wave multiplication– No DC drift in low pass filters– Digital signal enhancement

• Problems:– Need 32 bit DAC for signals buried in noise– Cannot digitize 32 bits at 100 kHz rates

• Should be excellent for slow servos– Ex: tele-medicine, temperature controllers– Digital processing can compensate for certain system time delays ?

Page 15: Lock-in amplifiers . Signals and noise Frequency dependence of noise Low frequency ~ 1 / f –example: temperature (0.1 Hz), pressure

Lock-in amps in servos• Lock to resonance peak

– Servos only lock to zero– Need to turn peak into zero

• Take derivative of lineshape– modulate x-voltage– F(x)-voltage amplitude like derivative

• Use lock-in amp to extract amplitude of F(x)– “DC” part of mixer output– filter with integrator, not low-pass

x

F(x)

Take derivative with lock-in

No fundamental• only 2 f signal

Page 16: Lock-in amplifiers . Signals and noise Frequency dependence of noise Low frequency ~ 1 / f –example: temperature (0.1 Hz), pressure

Lock-in amps for derivative• Lock-in turns sine wave signal into DC voltage

• At peak of resonance– no signal at modulation freq

– lock-in output crosses zero

• Discriminant– use to lock

x

F(x)

Input signal

Lock-inoutput

(derivative)

Zero crossingat resonance

Page 17: Lock-in amplifiers . Signals and noise Frequency dependence of noise Low frequency ~ 1 / f –example: temperature (0.1 Hz), pressure

Effect of modulation on lineshape• Start with resonance lineshape• Intensity vs PZT voltage: I = I0 exp( -V2)

• Modulate voltage: V= V0 sin (2 f t)

• Modified lineshape

• Analog to numerical derivatives• Derivative is: I’ = I(V+ V) - I(V) / V

– Set V = 1

• Modulation replaces V= V0 sin (2 f t)• Derivative is sine wave part

– Assumes is V0 small

V

I

t

t

V

I

Page 18: Lock-in amplifiers . Signals and noise Frequency dependence of noise Low frequency ~ 1 / f –example: temperature (0.1 Hz), pressure

Modulation amplitude

0.05 linewidth

0.1

0.2

0.5 linewidth

1

2

Effect of modulation amplitude• For large modulation amps

– Distortion and broadening• Modulation like a noise source

– Always use minimum necessary

Expanded scan

Page 19: Lock-in amplifiers . Signals and noise Frequency dependence of noise Low frequency ~ 1 / f –example: temperature (0.1 Hz), pressure

Modulation amplitude

0.1 linewidth

0.2

0.5 linewidth

1

2

Mixer outputs• Maximum mixer output

– modulation ~ 1 linewidth– saturates and broadens

Mixer out0.1 linewidth

0.2

0.5

1

2

Page 20: Lock-in amplifiers . Signals and noise Frequency dependence of noise Low frequency ~ 1 / f –example: temperature (0.1 Hz), pressure

Fabry-Perot servo• Lock to peak transmission of high Q Fabry-Perot etalon• Use lock-in amp to give discriminant

– No input bandpass -- or low Q < 2• Bandpass rolloff usually 2-pole or greater

– No low pass filter -- replace with integrator• Low pass filter removes noise• Need noise to produce correction

• Design tips– reference freq must exceed servo bandwidth by factor of ~ 10– but PZT bandwidth is servo limiter– use PZT resonance for modulation

Acoustic noise

Laser

Fabry-Perot

PD LIA

Sum& HV

reference