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                 Transverse modes have a field vector normal to the direction of   propogation and are determined by the geometry of the laser or waveguide cavity   and any limiting apertures. Waveguide modes are characterized as TE (transverse   electric) with the electric vector normal, and TE (transverse magnetic) with the   magnetic vector normal. In general, laser modes that do not have wall boundary   conditions are designated TEM (transvers electric magnetic) with both vectors   normal to the direction of propogation. The lowest order mode is the Gaussian   TEM00. The appearance that higher-order modes take depends upon   whether the limiting apertures are circular or rectancular. The three   lowest-order modes for a circularly symmetric cavity are shown below 
                In most laser applications it is necessary to focus, modify, or   shape the laser beam by using lenses and other optical elements. In general,   laser-beam propagation can be approximated by assuming that the laser beam has   an ideal Gaussian intensity profile, corresponding to the theoretical   TEM00 mode. Coherent Gaussian beams have peculiar transformation   properties that require special consideration. In order to select the best   optics for a particular laser application, it is important to understand the   basic properties of Gaussian beams. Unfortunately, the output from real-life   lasers is not truly Gaussian (although helium neon lasers and argon-ion lasers   are a very close approximation). To accommodate this variance, a quality factor,   M2 (called the “M-square” factor), has been defined to describe the   deviation of the laser beam from a theoretical Gaussian. For a theoretical   Gaussian, M2=1; for a real laser beam, M2>1. Helium   neon lasers typically have an M2 factor that is less than 1.1. For   ion lasers, the M2 factor is typically between 1.1 and 1.3. Collimated   TEM00 diode laser beams usually have an M2 ranging from 1.1 to 1.7.   For high-energy multimode lasers, the M2 factor can be as high as 3 or 4. In all   cases, the M2 factor, which varies significantly, affects the   characteristics of a laser beam and cannot be neglected in optical   designs. 
                In TEM00 mode, the beam emitted from a laser begins as   a perfect plane wave with a Gaussian transverse irradiance profile as shown in   the figure below. The Gaussian shape is truncated at some diameter either by the   internal dimensions of the laser or by some limiting aperture in the optical   train. The commonly adopted definition is the diameter at which the beam   irradiance (intensity) has fallen to 1/e2 (13.5%) of its peak, or   axial, value. 
                
                  
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                      Gaussian beam profile (theoretical TEM00 mode) 
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