Field Manipulation of Ultrabroadband Optical Pulses

Morita, Ryuji; Toda, Yasunori

doi:10.1007/3-540-27140-6_6

Cited by 3 publications

(3 citation statements)

References 46 publications

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“…In experiment, six different cosine phase patterns were used such that the spectra of soliton pulses covered the wavelength between 850 and 1050 nm uniformly. The cosine phase pattern is given by A cos xT and when this phase pattern was used, the pulse train of an original pulse was created with a period T and the peak amplitude of the central pulse was determined by the Bessel function of zero order J 0 (A) [8].…”

Section: Experimental Methodsmentioning

confidence: 99%

Broadband Coherent Anti-Stokes Raman Scattering Microscopic Spectroscopy Using Variable-Wavelength Soliton Pulses from a Photonic Crystal Fiber

Tada

Karasawa

2009

Molecular Crystals and Liquid Crystals

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The object of this work is to demonstrate broadband Coherent anti-Stokes Raman scattering microscopic spectroscopy using a fundamental soliton pulse from a photonic crystal fiber as a variable-wavelength light source, where the center wavelengths of soliton pulses are controlled by a pulse shaper based on a spatial light modulator. It is demonstrated that the Raman shifts for a single 6-mm-diameter polystyrene bead were obtained for the broad range between 800 and 3100 cm À1 accurately. From the measurements, the three-dimensional shape of the polystyrene bead was plotted and the spatial resolutions were estimated.

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Section: Experimental Methodsmentioning

confidence: 99%

Broadband Coherent Anti-Stokes Raman Scattering Microscopic Spectroscopy Using Variable-Wavelength Soliton Pulses from a Photonic Crystal Fiber

Tada

Karasawa

2009

Molecular Crystals and Liquid Crystals

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“…When the cosine phase pattern was used, the pulse train of an original pulse was created with a period T and the peak amplitude of the central pulse was determined by the Bessel function of zero order J 0 ðAÞ. 15) In Fig. 2, the intensity of the central pulse ½J 0 ðAÞ 2 is shown as a function of A.…”

Section: Experimental Methodsmentioning

confidence: 99%

Broadband Coherent Anti-Stokes Raman Scattering Spectroscopy Using Pulse-Shaper-Controlled Variable-Wavelength Soliton Pulses from a Photonic Crystal Fiber

Tada¹,

Karasawa

2008

jjap

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“…The other was the cosine phase pattern of a form A cos ωT. When the cosine phase pattern was used, the pulse train of an original pulse was created with a period T and the peak amplitude of the central pulse was determined by the Bessel function of zero order J 0 (A) (Morita & Toda, 2005). The period T was set to be 500 fs in experiment such that the timing of only the central pulse in a pulse train matched with a pump pulse.…”

Section: Broadband Cars Spectroscopy Using a Pulse Shapermentioning

confidence: 99%