Laser Beam Divergence Calculator
Find Gaussian beam spread, Rayleigh range, and radius at distance.
Gaussian beam parameters
Enter vacuum wavelength, waist radius, and propagation distance from the waist.
About laser beam divergence
Laser beam divergence describes how a beam expands as it propagates away from its narrowest point. This calculator uses the ideal fundamental Gaussian beam model, in which the intensity profile is smooth and the beam radius is measured where intensity falls to one over e squared of its axial value. The waist radius is that radius at the minimum spot. For wavelength lambda and waist radius w0, the far-field half-angle divergence is lambda divided by pi times w0. A smaller waist therefore creates a larger angular spread, while a larger waist produces a more collimated beam.
The Rayleigh range is the distance from the waist at which the beam radius grows by a factor of the square root of two. It equals pi times waist radius squared divided by wavelength. Within roughly one Rayleigh range, the beam remains comparatively narrow; farther away, its radius increasingly follows the far-field divergence angle. The radius at axial distance z is w0 multiplied by the square root of one plus the square of z divided by the Rayleigh range.
This page accepts wavelength in nanometres, waist radius in millimetres, and distance in metres. It converts those values to SI units before calculation. The displayed divergence is a half-angle in milliradians. Some specifications quote full-angle divergence, which is twice the half-angle, so always check the convention before comparing values. The displayed beam size is a radius, not a diameter; double it when a full beam diameter is required.
Real beams depart from the diffraction-limited Gaussian model. Their divergence is often represented by multiplying the ideal result by a beam-quality factor called M squared. Astigmatism may also require separate horizontal and vertical waist measurements. Optical clipping, lens aberration, multimode structure, thermal lensing, and imperfect alignment can further alter propagation. Even with these limitations, the ideal calculation is valuable for selecting optics, estimating aperture clearance, checking focusing tradeoffs, and establishing a best-case baseline. For safety or hardware decisions, include tolerances, the measured beam-quality factor, and an appropriate margin.
Laser divergence examples
| Wavelength, waist, distance | Divergence, range, radius |
|---|---|
| 1064 nm, 1 mm, 10 m | 0.338682 mrad, 2.952625 m, 3.531402 mm |
| 632.8 nm, 0.5 mm, 0 m | 0.402853 mrad, 1.241147 m, 0.5 mm |
| 532 nm, 1 mm, 0 m | 0.169341 mrad, 5.905249 m, 1 mm |
How to calculate beam divergence
- Enter the laser wavelength in nanometres.
- Enter the one-over-e-squared beam waist radius in millimetres.
- Enter the propagation distance measured from the waist.
- Calculate the divergence, Rayleigh range, and beam radius.
Frequently asked questions
Is the divergence a half-angle or full angle?
The result is the Gaussian far-field half-angle. Double it when a specification requires full-angle divergence.
What is the beam waist?
The waist is the location of minimum beam radius. In the ideal Gaussian model, wavefront curvature is infinite there.
What does Rayleigh range represent?
It is the distance from the waist where radius becomes the square root of two times larger. It provides a useful measure of the beam's collimated region.
Does this account for beam quality?
No, the equations assume a diffraction-limited Gaussian beam with M squared equal to one. A real beam's measured quality factor generally increases divergence.
Is beam radius the same as diameter?
No, radius extends from the axis to the stated intensity boundary. Beam diameter is twice the reported radius.