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Coherence Theory

16.1 Temporal Coherence

Temporal coherence describes the correlation of a wave with itself at different times. The coherence time τc\tau_c is the time over which the phase relationship is maintained.

For a quasi-monochromatic source with bandwidth Δω\Delta\omega:

τc2πΔω=1Δν\tau_c \sim \frac{2\pi}{\Delta\omega} = \frac{1}{\Delta\nu}

The coherence length: lc=cτc=λ2/Δλl_c = c\tau_c = \lambda^2/\Delta\lambda.

SourceΔλ\Delta\lambdalcl_c
White light300\sim 300 nm1.5μ\sim 1.5\,\muM
Na D line0.6\sim 0.6 nm0.5\sim 0.5 mm
He-Ne laser0.002\sim 0.002 nm20\sim 20 cm
Stabilised laser106\sim 10^{-6} nm400\sim 400 km

16.2 Spatial Coherence

Spatial coherence describes the correlation of a wave at different points in space at the same time. The van Cittert—Zernike theorem states that the spatial coherence of light from an extended incoherent source is given by the Fourier transform of the source intensity distribution:

γ(Δx)=I(ξ,η)eik(ξΔx)/(R)dξdηI(ξ,η)dξdη\gamma(\Delta x) = \frac{\iint I(\xi, \eta)\,e^{-ik(\xi\Delta x)/(R)}\,d\xi\,d\eta}{\iint I(\xi, \eta)\,d\xi\,d\eta}

Where I(ξ,η)I(\xi, \eta) is the source intensity distribution and RR is the distance to the source.

Michelson stellar interferometer: Uses two separated apertures to measure the spatial coherence of starlight, from which the angular diameter of the star can be determined. The first fringe visibility minimum occurs at:

d=0.61λαd = \frac{0.61\lambda}{\alpha}

Where α\alpha is the angular diameter and dd is the aperture separation.

16.3 Degree of Coherence

The complex degree of coherence γ12(τ)\gamma_{12}(\tau) between fields at points 1 and 2 with time delay τ\tau:

γ12(τ)=E1(t)E2(t+τ)E12E22\gamma_{12}(\tau) = \frac{\langle E_1^*(t)E_2(t+\tau)\rangle}{\sqrt{\langle|E_1|^2\rangle\langle|E_2|^2\rangle}}

This satisfies 0γ1210 \leq |\gamma_{12}| \leq 1. The visibility of interference fringes is:

V=ImaxIminImax+Imin=γ12V = \frac{I_{\max} - I_{\min}}{I_{\max} + I_{\min}} = |\gamma_{12}|

Worked Example 16.1: Double-Slit with Extended Source

A double-slit experiment uses an extended source of width ww at distance DD from the slits (slit separation dd).

By the van Cittert—Zernike theorem, the spatial coherence at the slits is:

γ=sin(πwd/(λD))πwd/(λD)|\gamma| = \left|\frac{\sin(\pi wd/(\lambda D))}{\pi wd/(\lambda D)}\right|

The fringe visibility vanishes when πwd/(λD)=π\pi wd/(\lambda D) = \piI.e., d=λD/wd = \lambda D/w.

For a candle flame (w1w \approx 1 mm) at D=1D = 1 m with λ=550\lambda = 550 nm:

dmax=550×109×1103=5.5×104m=0.55mmd_{\text{max} = \frac{550 \times 10^{-9} \times 1}{10^{-3}} = 5.5 \times 10^{-4}\,\text{m} = 0.55\,\text{mm}}

Beyond this slit separation, the fringes wash out. For a star (w108w \sim 10^8 km, D1014D \sim 10^{14} km):

dmax=550×109×10171011=550md_{\text{max} = \frac{550 \times 10^{-9} \times 10^{17}}{10^{11}} = 550\,\text{m}}

This is the basis of the Michelson stellar interferometer: by measuring dmaxd_{\text{max}}The stellar diameter is determined.