Analyze beam waist, spot size, and propagation with confidence. Review lens focusing and divergence instantly. Built for optics students, engineers, experiments, and fast checks.
Choose a solving path, enter the known beam data, and submit. The result appears above this form and directly below the header section.
This sample table shows typical optical inputs and approximate outputs produced by the calculator.
| Mode | Inputs | Approximate waist radius | Approximate Rayleigh range | Approximate full divergence |
|---|---|---|---|---|
| Divergence | 632.8 nm, M² 1.0, θ = 0.50 mrad | 402.8530 µm | 805.7060 mm | 1.000000 mrad |
| Rayleigh range | 1064 nm, M² 1.2, zR = 35 mm | 119.2671 µm | 35.0000 mm | 6.815261 mrad |
| Lens focus | 532 nm, M² 1.1, f = 100 mm, D = 2.5 mm | 14.9020 µm | 1.1922 mm | 25.000000 mrad |
The calculator follows standard Gaussian beam relations with the 1/e² radius definition.
w0 = (M²λ) / (πθ) for solving waist from far-field half-angle divergence.w0 = √(M²λzR / π) for solving waist from Rayleigh range.w0 ≈ (2M²λf) / (πD) for a collimated beam focused by a thin lens.zR = πw0² / (M²λ) for Rayleigh range.w(z) = w0√(1 + (z/zR)²) for beam radius at distance z.θfull = 2M²λ / (πw0) for full-angle divergence.I0 ≈ 2P / (πw0²) for approximate on-axis peak intensity of a TEM00 beam.R(z) = z[1 + (zR/z)²] for wavefront curvature away from the waist.The beam waist is the location where a Gaussian beam reaches its minimum 1/e² radius. That radius is written as w0 and controls divergence, Rayleigh range, spot area, and focusing behavior.
M² adjusts ideal Gaussian formulas for real beams. A perfect TEM00 beam has M² = 1. Higher values mean poorer focusability, larger beam parameter product, and stronger divergence for the same waist size.
The divergence input in this page is the far-field half-angle, measured from the optical axis to the 1/e² beam envelope. The result table reports both half-angle and full-angle divergence values.
Rayleigh range is the distance from the waist to the point where the beam radius grows by √2. It describes how quickly a beam spreads and defines the confocal parameter as 2zR.
Use lens mode when a collimated beam is focused by a lens and you know wavelength, focal length, input beam diameter, and beam quality. It estimates the diffraction-limited waist near focus.
No. Power does not change the geometric waist calculation. It is only used to estimate the approximate on-axis peak intensity at the waist, assuming a Gaussian beam profile.
Beam parameter product combines waist radius and half-angle divergence into one quality metric. Lower values indicate tighter focusing and better spatial quality, while real beams increase with larger M².
Yes, for quick engineering estimates and educational optics work. Final laboratory design should still confirm conventions, actual beam profiles, lens aberrations, truncation effects, and manufacturer data.
Important Note: All the Calculators listed in this site are for educational purpose only and we do not guarentee the accuracy of results. Please do consult with other sources as well.