2014
DOI: 10.1088/2040-8978/17/1/015604
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Implementation of a spatial light modulator for intracavity beam shaping

Abstract: In this paper we outline the steps necessary to create a laser with an intra-cavity spatial light modulator (SLM) for transverse mode control. We employ a commercial SLM as the back reflector in an otherwise conventional diode-pumped solid state laser. We show that the geometry of the liquid crystal (LC) arrangement strongly influences the operating regime of the laser, from nominally amplitude-only mode control for twisted nematic LCs to nominally phaseonly mode control for parallel-aligned LCs. We demonstrat… Show more

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Cited by 31 publications
(16 citation statements)
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References 23 publications
(25 reference statements)
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“…But the feedback loop and wavefront sensing made the solution impractical for most applications. A major advance was the demonstration of conventional SLMs inside a laser cavity . Using a commercial SLM device, it was shown that the SLM could form the back reflector of a laser cavity, acting as a rewritable “holographic mirror.” Since the SLM requires only a new image to implement a new phase, the laser could output any structured light pattern without any changes to the cavity geometric and without any realignment of optical elements.…”
Section: Structured Light Lasersmentioning
confidence: 99%
“…But the feedback loop and wavefront sensing made the solution impractical for most applications. A major advance was the demonstration of conventional SLMs inside a laser cavity . Using a commercial SLM device, it was shown that the SLM could form the back reflector of a laser cavity, acting as a rewritable “holographic mirror.” Since the SLM requires only a new image to implement a new phase, the laser could output any structured light pattern without any changes to the cavity geometric and without any realignment of optical elements.…”
Section: Structured Light Lasersmentioning
confidence: 99%
“…One recent advance that eliminates the need for custom designed and fabricated optics is the so-called digital laser [45,46]. A typical configuration is shown in figure 6, comprising a Nd:YAG gain medium in a Fabry-Perot resonator.…”
Section: Oam Mode Generation (A) Scalar Modesmentioning
confidence: 99%
“…Non-homogeneous intensities are all the more critical in experiments involving non-linear light-matter interactions. For such systems exhibiting optical non-linearities (like two-photon absorption [8]), saturated optical responses (lasers [17], light-sentitive membrane channels [18]) or optical processes sensitive to temperature (photo-polymerization [19]), speckled patterns generated by regular CGH with phase-only modulation are thus detrimental and may result in experimental artifacts. Moreover, in applications using linear photo-excitation processes, the speckle pattern may also be problematic.…”
Section: Introductionmentioning
confidence: 99%