Understanding the laser brightness calculator — concept and principle
This calculator finds the brightness, or radiance, of a laser beam: its optical power per unit area per unit solid angle. It uses the power, wavelength and beam quality M² on both axes, and also gives the beam parameter product and how close the beam is to the diffraction-limited ideal. It helps compare laser sources for cutting, pumping or long-range applications.
How it is calculated
B = P ÷ (λ² × M²x × M²y), in W/(m²·sr)
Beam parameter product (per axis) = w₀ θ = M² λ ÷ π
Diffraction-limited brightness (M² = 1) = P ÷ λ²
Share of the ideal = 100% ÷ (M²x × M²y)
- P in watts, λ in nm; results in MW/(cm²·sr) and TW/(m²·sr).
The principle
A beam's waist has area πw₀² and its far-field cone has solid angle πθ². Radiance is power divided by both. For a Gaussian-like beam the product w₀θ is fixed by the beam quality, M²λ/π, so the radiance depends only on power, wavelength and M². Lenses can trade a smaller spot for a wider angle, but they cannot increase radiance; it is conserved through ideal optics. That makes brightness the right figure for comparing how well different sources can be focused or sent over long distances.
Worked example
Default inputs: P = 1 W, λ = 532 nm, M²x = M²y = 1.1.
- λ² = (532 × 10⁻⁹)² = 2.830 × 10⁻¹³ m².
- B = 1 ÷ (2.830 × 10⁻¹³ × 1.21) = 2.920 × 10¹² W/(m²·sr) = 2.9201 TW/(m²·sr) = 292.01 MW/(cm²·sr).
- Beam parameter product = 1.1 × 532 × 10⁻⁹ ÷ π = 0.1863 mm·mrad on each axis.
- With M² = 1: 353.33 MW/(cm²·sr); share of ideal = 100 ÷ 1.21 = 82.64%.
| Wavelength (nm) | Radiance (MW per cm² per steradian) |
|---|---|
| 133 | 4,672.09 |
| 266 | 1,168.02 |
| 399 | 519.12 |
| 532 | 292.01 |
| 665 | 186.88 |
| 798 | 129.78 |
| 1,064 | 73 |
How to read the result
Brightness rises with power and falls with the square of the wavelength and with poorer beam quality on either axis. A beam with M² = 2 on both axes has only a quarter of the ideal brightness. Use the figure to compare sources; it is not an eye-safety limit.
Common mistakes
- Treating power alone as a measure of how intense a focused spot can be.
- Forgetting that M² can differ between the two axes, as in many diode lasers.
- Expecting optics to increase brightness.
Frequently asked questions
Can a lens make a beam brighter?
No. Ideal passive optics conserve radiance; they only trade spot size for angle.
Why does a shorter wavelength give higher brightness?
Its diffraction-limited beam parameter product is smaller.
What is the beam parameter product?
Waist radius times far-field half-angle, M²λ/π for each axis.
Why do diode lasers have lower brightness?
Their beams usually have high M², especially along the slow axis.
Sources: R. Paschotta, RP Photonics Encyclopedia, "Brightness" and "M² factor"