Coherence Theory
16.1 Temporal Coherence
Temporal coherence describes the correlation of a wave with itself at different times. The coherence time is the time over which the phase relationship is maintained.
For a quasi-monochromatic source with bandwidth :
The coherence length: .
| Source | ||
|---|---|---|
| White light | nm | M |
| Na D line | nm | mm |
| He-Ne laser | nm | cm |
| Stabilised laser | nm | 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:
Where is the source intensity distribution and 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:
Where is the angular diameter and is the aperture separation.
16.3 Degree of Coherence
The complex degree of coherence between fields at points 1 and 2 with time delay :
This satisfies . The visibility of interference fringes is:
Worked Example 16.1: Double-Slit with Extended Source
A double-slit experiment uses an extended source of width at distance from the slits (slit separation ).
By the van Cittert—Zernike theorem, the spatial coherence at the slits is:
The fringe visibility vanishes when I.e., .
For a candle flame ( mm) at m with nm:
Beyond this slit separation, the fringes wash out. For a star ( km, km):
This is the basis of the Michelson stellar interferometer: by measuring The stellar diameter is determined.