2006
DOI: 10.1364/ol.31.001292
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Broadly tunable dual-wavelength light source for coherent anti-Stokes Raman scattering microscopy

Abstract: The signal and idler beams from a picosecond, synchronously pumped optical parametric oscillator (OPO) provide the two colors necessary for coherent anti-Stokes Raman scattering (CARS) microscopy. The OPO provides a continuously tunable frequency difference between the two beams over a broad range of Raman shifts (100-3700 cm(-1)) by varying the temperature of a single nonlinear crystal. The near-infrared output (900-1300 nm) allows for deep penetration into thick samples and reduced nonlinear photodamage. App… Show more

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Cited by 216 publications
(139 citation statements)
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References 24 publications
(16 reference statements)
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“…The near IR lasers avoid two-photon electronic enhancement of the nonresonant background ( 32 ), reduce the photodamage induced by multiphoton absorption ( 33 ), and diminish tissue scattering leading to increased optical penetration depth ( 34 ). As a two-beam modality, CARS microscopy is mostly operated with picosecond (ps) pulses, either from two synchronized Ti:sapphire lasers ( 35 ) or from a synchronously pumped Optical Parametric Oscillator system ( 34 ).…”
Section: Near Ir Laser Excitationmentioning
confidence: 99%
See 1 more Smart Citation
“…The near IR lasers avoid two-photon electronic enhancement of the nonresonant background ( 32 ), reduce the photodamage induced by multiphoton absorption ( 33 ), and diminish tissue scattering leading to increased optical penetration depth ( 34 ). As a two-beam modality, CARS microscopy is mostly operated with picosecond (ps) pulses, either from two synchronized Ti:sapphire lasers ( 35 ) or from a synchronously pumped Optical Parametric Oscillator system ( 34 ).…”
Section: Near Ir Laser Excitationmentioning
confidence: 99%
“…As a two-beam modality, CARS microscopy is mostly operated with picosecond (ps) pulses, either from two synchronized Ti:sapphire lasers ( 35 ) or from a synchronously pumped Optical Parametric Oscillator system ( 34 ). Picosecond pulse excitation not only provides suffi cient spectral resolution ( 36 ) but also increases the ratio of resonant signal to nonresonant background ( 35 ).…”
Section: Near Ir Laser Excitationmentioning
confidence: 99%
“…Stokes) involves the use of the output with only a single oscillator. There are various strategies for this approach: (1) using an optical parametric oscillator (OPO) (Ganikhanov et al 2006); (2) mixing the frequencies from a single high bandwidth pulse (Dudovich et al 2002); (3) generating new spectral components using a photonic crystal fiber (PCF) (Paulsen et al 2003). Figure 3 illustrates simplified configurations of OPO-and PCF-based multimodal CARS systems.…”
Section: Laser Sourcesmentioning
confidence: 99%
“…For this purpose, the pump frequency of the OPO has to be shifted to the visible spectral range, since otherwise the excitation-beam frequencies lie too far in the IR region. [39] For this type of experiment, the range of accessible low-frequency Raman transitions is only limited by the characteristics of the optical filter used to separate the excitation light from the anti-Stokes signal. This is also true for a second type of experiment, in which the signal output of two OPOs pumped in parallel is used as pump/probe and Stokes beams.…”
mentioning
confidence: 99%