Audited 31 Jul 2026·Last updated 28 Oct 2026·3 citations·Tier 2·0 uses

Laser Beam Spot Size Calculator

Radius of an ideal Gaussian laser beam at any distance from its waist, from the waist radius and vacuum wavelength, using w(z) = w₀√(1 + (z/z_R)²).

Laser Beam Spot Size Calculator

m
m
m
Ideal beam radius
0.0014
The ideal Gaussian beam's 1/e² radius at the chosen distance from the waist, in metres; double it for the spot diameter.
Model scope
Ideal TEM00 Gaussian M² = 1 1/e² radius; real beam quality, astigmatism, lenses, clipping, turbulence, and diameter/FWHM conventions are outside it.

Background.

Point a laser at a wall a few metres away and the dot is bigger than the opening the light came out of. How much bigger depends on three things: how tight the beam was at its narrowest point, the waist; how far the wall is from that waist; and the wavelength. For an ideal Gaussian beam the relationship is exact, and it has a distinctive shape: almost flat at first, then bending into a steady straight-line spread.

The hinge between those two regimes is the Rayleigh range, z_R = πw₀²/λ, the distance over which the beam's cross-sectional area doubles and its radius grows by √2. Inside it the beam is close to parallel, which is why a focused beam holds its small spot only over a short working distance. Several Rayleigh ranges out, the radius grows almost in proportion to distance. For the default 1,064 nm beam with a 0.5 mm waist radius, z_R is about 0.738 m.

The surprising consequence is that a smaller waist does not give a smaller spot far away. The Rayleigh range shrinks with the square of the waist, so a tightly focused beam balloons quickly: at 2 m, a 0.1 mm waist grows to about 6.77 mm, nearly five times the 1.444 mm reached from a 0.5 mm waist. For any target distance there is a best waist, √(λz/π), which puts the target exactly one Rayleigh range away.

The radius reported is the 1/e² radius, where intensity has dropped to about 13.5% of the centre value and inside which about 86.5% of the power travels; double it for the diameter. The model is the ideal TEM₀₀ beam with M² = 1. Real beam quality, astigmatism, lenses, clipping and air turbulence all lie outside it, as the scope note beside the result says.

What is laser beam spot size calculator?

Laser spot size means the radius or diameter of the beam at a given plane. For a Gaussian beam the usual convention is the 1/e² radius, w: the distance from the axis at which intensity falls to e⁻², about 13.5% of the peak. Here w(z) is that radius at a distance z along the axis from the beam waist, the plane where the beam is narrowest, for light of the given vacuum wavelength travelling through free space.

How to use this calculator.

  1. Enter the waist radius w₀ in metres: 0.5 mm is 0.0005. Datasheets often give a beam diameter, so halve it, and check that it is a 1/e² figure rather than a FWHM one.
  2. Enter the distance from the waist, not from the laser housing. The datasheet usually says where the waist lies; for many collimated lasers it is close to the output, and after a lens it is near the focal point.
  3. Enter the vacuum wavelength in metres: 1,064 nm is 0.000001064, 532 nm is 0.000000532 and 632.8 nm is 0.0000006328.
  4. Read the ideal beam radius and double it for the spot diameter. For a real laser with a known M², multiply the wavelength by M² before entering it to estimate the real beam's size.

The formula.

w(z) = w₀ sqrt(1 + (zλ/(πw₀²))²)

w(z) = w₀ × √(1 + (zλ / (πw₀²))²). w₀ is the waist radius, z the distance from the waist and λ the vacuum wavelength, all in metres. The group πw₀²/λ is the Rayleigh range z_R, so the formula can also be read as w(z) = w₀√(1 + (z/z_R)²).

Two limits make it easy to sanity-check. Close to the waist, where z is much smaller than z_R, the square-root term is near 1 and the radius barely changes. Far away, where z is many times z_R, the 1 becomes negligible and w ≈ λz/(πw₀), a straight line whose slope is the far-field divergence half-angle. At exactly z = z_R the radius is √2 × w₀.

Wavelength and distance enter only as their product, so doubling either has the same effect. The waist appears twice, once as the starting size and once, squared, inside z_R, which is why small changes to w₀ swing the far-field result so strongly.

A worked example.

Example

The default beam is a 1,064 nm Nd:YAG laser with a 0.5 mm waist radius, observed 2 m from the waist. First the Rayleigh range: π × (5 × 10⁻⁴)² ÷ (1.064 × 10⁻⁶) ≈ 0.738 m. The target is 2 ÷ 0.738 ≈ 2.709 Rayleigh ranges away; squaring gives 7.341, adding 1 gives 8.341, and the square root is 2.888. Multiplying by the waist, 5 × 10⁻⁴ × 2.888 gives a radius of 1.444 × 10⁻³ m, about 1.444 mm, so the spot is roughly 2.89 mm across. The far-field shortcut, a divergence of 6.774 × 10⁻⁴ rad times 2 m, would give 1.355 mm, about 6% low, because 2 m is still only a few Rayleigh ranges out. At 100 m the shortcut and the exact formula agree to better than 0.01%.

wavelength M0
beam Waist Radius M0.001
propagation Distance M2

Frequently asked questions.

What waist gives the smallest spot at a particular distance?
Make the Rayleigh range equal to the distance, which means w₀ = √(λz/π). For a 1,064 nm beam aimed at a target 2 m away that is about 0.823 mm, and the spot there is √2 times the waist, about 1.164 mm in radius. Any smaller or larger waist gives a bigger spot at that distance.
How do I convert the 1/e² radius to a FWHM diameter?
Multiply the 1/e² radius by about 1.177, because intensity falls to half its peak at 0.589 w from the axis. The 1.444 mm radius in the example corresponds to a full width at half maximum of about 1.70 mm, while its 1/e² diameter is 2.888 mm.
Does the beam widen in a straight line from the start?
Only once it is several Rayleigh ranges from the waist. Before that the growth is gentle and curved, and within one Rayleigh range on either side of the waist the beam is nearly parallel. That stretch of twice z_R is often called the depth of focus or confocal parameter.
How do I allow for a real laser's M² value?
Enter M² × λ in place of the wavelength. That gives a real beam with the same waist that spreads M² times faster, the usual embedded-Gaussian approach. With M² = 1.3 and the default settings, the radius at 2 m becomes about 1.831 mm instead of 1.444 mm; treat it as an estimate rather than an ideal-beam figure.
What if the beam travels through water or glass rather than air?
Inside a medium of refractive index n the beam behaves as if its wavelength were λ/n, so it spreads more slowly there. The page assumes free space, and for air the correction is negligible. For a path through water, with n of about 1.33, divide the vacuum wavelength by n before entering it.
Where is the new waist after a focusing lens?
Close to the lens's focal point. For a collimated beam of radius w entering a lens of focal length f, the focused waist radius is roughly λf/(πw). That focusing step is not calculated here, but once you have the new waist you can enter it to see how quickly the beam spreads beyond the focus.

How this page was produced

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Quanta Calculator
Primary sources
3 cited below
Method
w(z) = w₀ sqrt(1 + (zλ/(πw₀²))²)
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