Continuous-wave Optical Parametric Oscillators

Continuous-wave Optical Parametric Oscillators PDF Author: S. Schiller
Publisher:
ISBN:
Category :
Languages : en
Pages : 104

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Continuous-wave Optical Parametric Oscillators

Continuous-wave Optical Parametric Oscillators PDF Author: S. Schiller
Publisher:
ISBN:
Category :
Languages : en
Pages : 104

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High-power, Continuous-wave Optical Parametric Oscillators from Visible to Near-infrared

High-power, Continuous-wave Optical Parametric Oscillators from Visible to Near-infrared PDF Author: Goutam Kumar Samanta
Publisher:
ISBN:
Category :
Languages : en
Pages :

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An Analysis of the Performance Characteristics of Continuous Wave Optical Parametric Oscillators

An Analysis of the Performance Characteristics of Continuous Wave Optical Parametric Oscillators PDF Author: Finlay G. Colville
Publisher:
ISBN:
Category :
Languages : en
Pages : 342

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Special Issue "Continuous Wave Optical Parametric Oscillators: Materials, Devices, and Applications"

Special Issue Author: Stephan Schiller
Publisher:
ISBN:
Category :
Languages : en
Pages : 101

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Continuous-wave, Intracavity Optical Parametric Oscillators

Continuous-wave, Intracavity Optical Parametric Oscillators PDF Author: Graham Alexander Turnbull
Publisher:
ISBN:
Category :
Languages : en
Pages : 172

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Continuous-wave Optical Parametric Oscillators Pumped by External Cavity Diode Lasers

Continuous-wave Optical Parametric Oscillators Pumped by External Cavity Diode Lasers PDF Author: Constantinos Petridis
Publisher:
ISBN:
Category : Optical parametric oscillators
Languages : en
Pages : 0

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Continuous Wave Singly Resonant Intracavity Optical Parametric Oscillators Using Periodically Poled LiNbO3

Continuous Wave Singly Resonant Intracavity Optical Parametric Oscillators Using Periodically Poled LiNbO3 PDF Author: Leonel Pastor Gonzalez
Publisher:
ISBN:
Category : Continuous wave radar
Languages : en
Pages : 0

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The use of continuous wave singly resonant optical parametric oscillators (CW SROs) has been limited in the past mainly because of the high threshold powers necessary. Thresholds of SROs are orders of magnitude greater than doubly resonant oscillators. While lithium niobate has long been in use as a nonlinear material, periodically poled lithium niobate (PPLN) recently emerged as an excellent source for CW SROs. Quasi-phase matching with PPLN has allowed access to the higher nonlinear coefficients of lithium niobate permitting construction of CW SROs. By placing the OPO within the laser resonator, threshold should be significantly reduced. We have designed, built, and investigated an optical parametric oscillator within a laser cavity to access the high circulating fields within the resonator. The intracavity OPO acted as the output coupler for the laser and ideally the total down converted power from the OPO should approach the maximum output power available from th pump laser under optimal output coupling. PPLN OPOs were built within the resonators of a lamp-pumped Nd:YAG laser and a diode-pumped Nd:YVO4 laser. Combined idler output at 3.3 microns from both ends of an intracavity 30-mm PPLN OPO was 1.15 W. Output of the Nd:YVO4 laser optimized for 1.064-micron output with the same resonator was 5 W. The entire device, except for power supply and cooler, fit on a 1' x 2' breadboard.

Continuous Wave Singly Resonant Optical Parametric Oscillator

Continuous Wave Singly Resonant Optical Parametric Oscillator PDF Author: Steven Tsung-Lin Yang
Publisher:
ISBN:
Category :
Languages : en
Pages : 276

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Continuous Wave Singly Resonant Intracavity Optical Parametric Oscillators Using Periodically Poled LiNbO3

Continuous Wave Singly Resonant Intracavity Optical Parametric Oscillators Using Periodically Poled LiNbO3 PDF Author: Leonel Pastor Gonzalez
Publisher:
ISBN:
Category : Continuous wave radar
Languages : en
Pages : 216

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Book Description
The use of continuous wave singly resonant optical parametric oscillators (CW SROs) has been limited in the past mainly because of the high threshold powers necessary. Thresholds of SROs are orders of magnitude greater than doubly resonant oscillators. While lithium niobate has long been in use as a nonlinear material, periodically poled lithium niobate (PPLN) recently emerged as an excellent source for CW SROs. Quasi-phase matching with PPLN has allowed access to the higher nonlinear coefficients of lithium niobate permitting construction of CW SROs. By placing the OPO within the laser resonator, threshold should be significantly reduced. We have designed, built, and investigated an optical parametric oscillator within a laser cavity to access the high circulating fields within the resonator. The intracavity OPO acted as the output coupler for the laser and ideally the total down converted power from the OPO should approach the maximum output power available from th pump laser under optimal output coupling. PPLN OPOs were built within the resonators of a lamp-pumped Nd:YAG laser and a diode-pumped Nd:YVO4 laser. Combined idler output at 3.3 microns from both ends of an intracavity 30-mm PPLN OPO was 1.15 W. Output of the Nd:YVO4 laser optimized for 1.064-micron output with the same resonator was 5 W. The entire device, except for power supply and cooler, fit on a 1' x 2' breadboard.

Continuous-wave terahertz light from optical parametric oscillators

Continuous-wave terahertz light from optical parametric oscillators PDF Author: Rosita Sowade
Publisher: Sudwestdeutscher Verlag Fur Hochschulschriften AG
ISBN: 9783838126951
Category :
Languages : de
Pages : 104

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Book Description
Continuous-wave (cw) optical parametric oscillators (OPOs) are working horses for spectroscopy for near and mid infrared wavelengths. However, in the terahertz frequency range (0.1 to 10 THz), the pump threshold for oscillation is larger than 100 W due to high absorptions and thus exceeds the power of standard cw single-frequency pump sources. In this thesis, the first cw OPO capable of generating terahertz radiation is demonstrated. To overcome thethreshold, the signal wave of a primary infrared process is resonantly enhanced to serve as a pump wave for a cascaded parametric process with one wave being at the terahertz frequency level. Such a device inhibits high potential for applications in areas like astronomy, telecommunications or high-resolution spectroscopy.