Formula & Calculator
Coherence Length
Calculates the maximum path length difference over which light waves maintain a consistent phase relationship, key to interference visibility.
Interpretation
Lc = λ²/Δλ. The distance over which a wave maintains a constant phase relationship. Used in interferometry and optical communications.
Variables
| Symbol | Quantity | Unit |
|---|---|---|
| Lc | Coherence length | m |
| λ | Central wavelength | m |
| Δλ | Spectral bandwidth | m |
What it means
Coherence length is a measure of the temporal coherence of a light source. It is inversely proportional to the spectral width (Δλ). A longer coherence length allows more interference fringes and is needed for high‑precision interferometry. Lasers have long coherence lengths; LEDs have short. Understanding this is essential for designing interferometers, holography systems, and in fibre optic communications where phase coherence matters.
Worked example
Coherence Length – Two Detailed Examples
Real‑World| Parameter | Value |
|---|---|
| λ (nm) | 632.8 |
| Δλ (nm) | 0.002 |
| Parameter | Value |
|---|---|
| λ | 850 |
| Δλ | 10 |
Common mistakes
- Coherence length: L_c = λ² / Δλ – where Δλ is the spectral width of the source.
- Units: λ and Δλ in the same units (e.g., nm) – L_c in the same unit.
- Interpretation: The distance over which the light remains coherent – for a laser, L_c can be long; for an LED, short.
- Assumes: Gaussian or rectangular spectrum – this is an approximation.
- Coherence time: τ_c = L_c / c – the corresponding time.
Applications
Coherence length, L_c = λ²/Δλ, is the distance over which a light wave maintains a predictable phase relationship, limited by the spectral width Δλ. This is important in interferometry, holography, and optical communications. Engineers use it to select light sources for coherence‑dependent applications. For example, laser sources have long coherence lengths, suitable for interferometry, while LEDs have short coherence lengths, reducing speckle. By understanding coherence length, they can design systems for optical coherence tomography (OCT), fibre sensors, and metrology. This concept is fundamental to understanding the temporal coherence of light.
- Design of interferometers and holographic systems
- Optical coherence tomography (OCT) for medical imaging
- Selection of light sources for coherence‑sensitive applications
- Speckle reduction in imaging and display systems
- Understanding of laser and light source characteristics
Frequently Asked Questions
It calculates the maximum path length difference over which light waves maintain a consistent phase relationship: Lc = λ² / Δλ.
Lc = coherence length.
λ = central wavelength.
Δλ = spectral bandwidth (linewidth).
It determines the visibility of interference fringes; fringes are visible only when the path difference is less than Lc.
From the Fourier transform of the spectrum; a narrow spectral width corresponds to a long coherence length.
Temporal coherence is related to the spectral purity (Lc); spatial coherence relates to the uniformity of phase across a wavefront.
A laser with λ = 633 nm and Δλ = 0.01 nm has Lc = (633×10⁻⁹)² / (0.01×10⁻⁹) = 4.0×10⁻¹⁴ / 1.0×10⁻¹¹ = 0.04 m = 4 cm.
- Confusing coherence length with coherence time.
- Forgetting that Δλ must be in the same units as λ.
- Assuming a laser has infinite coherence length (real lasers have finite linewidth).
For an interferometer to produce fringes, the path difference must be less than the coherence length of the source.
Sunlight has a broad spectrum, so Lc is very short, on the order of microns, which is why white‑light interferometry requires careful path matching.
OCT uses low‑coherence light; the coherence length determines the axial resolution of the imaging.