1999
DOI: 10.1103/physrevlett.82.1434
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Pattern Formation in the Transverse Section of a Laser with a Large Fresnel Number

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Cited by 124 publications
(84 citation statements)
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“…The predicted laser TW patterns have been observed in experiments with large-Fresnel-number cavities [126][127][128]. The TW solutions are also found in passive resonators described by the same order parameter equation, such as nondegenerate optical parametric oscillators (OPOs) [35,129].…”
Section: Extended Patternsmentioning
confidence: 64%
“…The predicted laser TW patterns have been observed in experiments with large-Fresnel-number cavities [126][127][128]. The TW solutions are also found in passive resonators described by the same order parameter equation, such as nondegenerate optical parametric oscillators (OPOs) [35,129].…”
Section: Extended Patternsmentioning
confidence: 64%
“…We interpret these intriguing observations by taking into account that reflections of waves at the side aperture and DBRs couple the polarization orientation of wave vectors already in linear order. Therefore, the 90 rule reported in [1] is valid only in a tiny range of transverse wave vectors parallel to one of the boundaries. Our argument shows also that single-wave number solutions are not possible, which provides justification for the phenomenological construction of superposition states to explain the scared structures in [4].…”
mentioning
confidence: 99%
“…The main mechanism determining the length scale of spatial structures for broad-area devices is provided by the alignment of the cavity resonance and the gain maximum [1,2]. If the cavity resonance is redshifted versus the gain maximum (positive detuning >0) tilted waves are favored to on-axis emission, which leads to pattern formation.…”
mentioning
confidence: 99%
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