GR-1312-CORE
Abstract: rs232 protocol Fiber raman amplifier raman amplifier Raman GR-1312CORE DB25 coefficient raman gain
Text: Raman Amplifier Description Raman amplifier module, with high power and one or multiple pumps, can be used in digital communication or broadband DWDM systems. Both discrete and distributed Raman applications are available. Compact and high reliable, with stimulated Raman scattering in
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GR-1312-CORE
RS232
rs232 protocol
Fiber raman amplifier
raman amplifier
Raman
GR-1312CORE
DB25
coefficient raman gain
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2066
Abstract: SBS 14 fiber bragg grating dispersion compensation
Text: Application Note AN-2066 Inherent Immunity of Chirp Managed Laser to Stimulated Brillouin Scattering 1. Scope and Overview Stimulated Brillouin Scattering SBS is an optical non-linearity limiting the maximum optical power that can be launched into an optical fiber. This constraint is particularly
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AN-2066
2066
SBS 14
fiber bragg grating dispersion compensation
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Fujikura panda fiber
Abstract: No abstract text available
Text: High-power pulsed fiber lasers and their evolution Yoshihiro Terada,1 Michihiro Nakai,1 and Yasuhiro Oba1 Fujikura has achieved an output power of 30 W from a Q-switched pulsed fiber laser with a pulse width about 100 ns for the first time in the world. Following the achievement, we
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B84p-I
B518aVIII10,
Fujikura panda fiber
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FBG laser
Abstract: Stimulated raman scattering pump laser 14xx
Text: Data Sheet June 2001 269-Type 14xx nm DFB Pump Laser Module Description The 269-type DFB pump laser module represents a family of thermoelectrically cooled, high-power lasers. These devices achieve stable wavelength performance within the 1420 nm to 1510 nm range,
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269-Type
Wide65)
DS01-237OPTO
FBG laser
Stimulated raman scattering
pump laser 14xx
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Untitled
Abstract: No abstract text available
Text: Wavelength Conversion Technology utilizing Linearly-Polarized Fiber Laser and its Applications Shohei Takahashi,1 Keiichi Horimoto,1 Keisuke Shimazu,1 Toru Kaneko,1 Fumihiko Nishimura,1 Kenichi Ishibashi,1 Keiji Kaneda,1 and Tomomi Fukushi2 In recent years the visible and ultraviolet high-power lasers utilizing wavelength conversion
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79170B-1-79170B-12,
340-nm
1180-nm
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tunable lasers
Abstract: 81949A Stimulated raman scattering 8198090A11
Text: Agilent 81980A, 81940A, 81989A, 81949A, and 81950A Compact Tunable Laser Sources Data Sheet Modular Design for Multichannel Platform Introduction The Agilent Series 819xxA of compact tunable lasers enables optical device characterization at high power levels and measurement of nonlinear effects. Each
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1980A,
1940A,
1989A,
1949A,
1950A
819xxA
163A/B,
164A/B,
166A/B
tunable lasers
81949A
Stimulated raman scattering
8198090A11
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Untitled
Abstract: No abstract text available
Text: Agilent 83430A Lightwave Digital Source Product Overview SDH/SONET Compliant DFB laser source for digital, WDM, and analog test up to 2.5 Gb/s • 52 Mb/s STM-0/OC-1 • 155 Mb/s STM-1/OC-3 • 622 Mb/s STM-4/OC-12 • 2488 Mb/s STM-16/OC-48 • User adjustable extinction ratio
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3430A
STM-4/OC-12
STM-16/OC-48
5965-5074E
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Untitled
Abstract: No abstract text available
Text: Agilent 81980A, 81960A, 81940A, 81989A, 81949A, and 81950A Compact Tunable Laser Sources Data Sheet Introduction The Agilent 819xxA Series of compact tunable lasers enables optical device characterization at high power levels and measurement of nonlinear effects.
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1980A,
1960A,
1940A,
1989A,
1949A,
1950A
819xxA
163A/B,
164A/B,
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H10769A
Abstract: H10770A H7422
Text: NEWS 01 2010 SOLID STATE PRODUCTS PAGE 10 New silicon infrared enhanced photodiodes for scientific measurement and YAG laser monitoring SOLID STATE PRODUCTS CCD image sensors S11510 series PAGE 12 ELECTRON TUBE PRODUCTS Side-on PMT R9876, R11540 PAGE 25 SYSTEMS PRODUCTS
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S11510
R9876,
R11540
photomultiD-82211
DE128228814
H10769A
H10770A
H7422
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