Sometimes, manufacturers provide Gaussian beam data as Full Width Half Maximum (FWHM) measurements, but OpticStudio uses the 1/e^{2} measure of beam width. This article describes how to convert FWHM measurements to 1/e^{2} halfwidth measurements.

**Authored By Dan Hill**

## Introduction

For Gaussian beam size measurements, OpticStudio uses the 1/e^{2} half-width point, which means the intensity has fallen to about 13.5% of the peak. However, often times manufacturer’s data sheets provide only Full Width Half Maximum (FWHM) measurements and not 1/e^{2} half-widths.

The relationship between the FWHM and 1/e^{2} halfwidth of a gaussian beam

For a truly TEM00, rotationally symmetric & normalized Gaussian beam, there is a linear relationship between the FWHM and 1/e^{2} values.

The intensity of a Gaussian beam goes as:

where w is the half width of the beam to the 1/e^{2} intensity point at some distance from the waist along the propagation axis, and r is the radial distance from the center of the beam. The width, w, at some z position is given by:

where w_{0} is the waist radius at the 1/e^{2} point. For a normalized Gaussian beam, we know that the FWHM is the point at which the beam reaches half of the peak intensity. As a result, our equation simplifies to:

The FWHM is the full width of the beam at half of the maximum intensity, so we need to divide this value by 2 so that we can replace it with r, the radial size.

Simplifying, we get:

Taking the natural log of both sides, and bringing the constant to the other side of the equation yields:

Solving for w, the relationship between the FWHM and the 1/e^{2} intensity point becomes:

KA-01545

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