CHEM 524 -- Course Outline (Part 10)

VII. Signal to noise considerations (Text - Chap. 5)

A. Noise definitions:

1. Types

  1. evaluate by understanding noise power spectrum
  2. use to design modulation or detection scheme

2. Amplitude transfer function (book: Table 5-1, Fig. 5-4)

B. Quantum/shot noise -- square root dependence on signal level

due to random photon field and random probability of emission of at interface

a - multiplier add on noise [vary 0.1-0.5, good PMT ~ (d-1)-1, d - gain per dynode]

C. Others

  1. Flicker, due to sample or blank vary (eg. source fluct.) ~ light signal:
  2. Dark current (e.g. field emission dynode or amplifier output level) -- excess noise
  3. Quantization noise (finite digital resolution) -- sq = q/2 , q- quantization level
  4. Thermal (Johnson) noise - (thermal fluctuation of e- in resistor) sJ = (4kTRDf)1/2 -- cooling, narrowing band pass help, lowering R also, but usually costs signal (in volts)
  5. Uncorrelated sources, sum the noise: (read Section 5.4, 5.5)

D. Bottom line -- understand Figures relating S/N and E (fig. 5.6), A/sA vs A (fig. 5.7)

E. Enhance S/N

  1. Filtering ---time domain (avg or use time constant, eg. multiplex -- time avg idea, integrate signals in each channel) - multiple (n) scan average, increase S/N = n1/2
  2. Filter -- frequency domain ( select signal) -- best: fully digitize signal, FT to frequencies, multiply by H(f), back transform
  3. Adjust levels - shot (raise to flicker limit), dark (cool detector), flicker (adjust instrument, eg. Double beam -- counter drift -- signal and blank simultaneous)
  4. Photon counting -- best for low light level -- (S/N)PC/(S/N)i = [fd(1+a)]1/2, fd discriminator coeff., (1+a) term gives 5-25% improvement
  5. Modulation -- demodulate with lock in, boxcar, or correlation -- all discriminate against noise which is broad band and no time correlation to signal (except flicker) - (Fig. 5-9)