2003
DOI: 10.1364/ol.28.002497
|View full text |Cite
|
Sign up to set email alerts
|

Continuous-wave operation of a single-frequency optical parametric oscillator at 4–5 μm based on periodically poled LiNbO_3

Abstract: We present a cw, Nd:YAG-pumped singly resonant single-frequency narrow-linewidth high-power optical parametric oscillator with idler tuning from 3.7 to 4.7 microm. In this spectral range the absorption of the idler wave in the LiNbO3 crystal is significant, causing the oscillation threshold to increase with a subsequent decrease in output power from 1.2 W at 3.9 microm to 120 mW at 4.7 microm. The optical parametric oscillator's cavity was stabilized and mode-hop tuned with a rotatable solid etalon but with a … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3

Citation Types

0
22
0

Year Published

2007
2007
2020
2020

Publication Types

Select...
6
2

Relationship

0
8

Authors

Journals

citations
Cited by 52 publications
(22 citation statements)
references
References 13 publications
0
22
0
Order By: Relevance
“…Also, the absorption of idler wave inside the nonlinear crystal causes the thermal loading 12,13 of the nonlinear crystal and results in a decrease in the conversion e±ciency. [14][15][16] There are some other OPO con¯gurations to suppress the back conversion, for example, using a two-crystal OPO with four dichroic mirrors. 17 But such con¯gurations have some limitations, such as longer build-up time due to the use of ring cavity and more signal loss due to the use of four mirrors.…”
Section: Introductionmentioning
confidence: 99%
“…Also, the absorption of idler wave inside the nonlinear crystal causes the thermal loading 12,13 of the nonlinear crystal and results in a decrease in the conversion e±ciency. [14][15][16] There are some other OPO con¯gurations to suppress the back conversion, for example, using a two-crystal OPO with four dichroic mirrors. 17 But such con¯gurations have some limitations, such as longer build-up time due to the use of ring cavity and more signal loss due to the use of four mirrors.…”
Section: Introductionmentioning
confidence: 99%
“…The strength of continuous wave, mid-infrared, optical parametric oscillators (OPOs) lies in their ability to cover a broad spectral range, while offering high power and exceptional beam characteristics in terms of beam profile, linewidth and stability [1][2][3][4][5][6]. This makes the OPO an excellent light source for spectroscopic purposes, especially when it is operated in the 3-5 µm wavelength range where many molecules important for life science have strong characteristic absorptions.…”
Section: Introductionmentioning
confidence: 99%
“…In contrast to conventional photoacoustic detection with microphones, QEPAS makes use of a quartz tuning fork (developed as a frequency reference for clocks and watches) as both a detector and high-Q resonator for the acoustic signal. Although the sensitivities that can be reached are comparable to those of conventional photoacoustic spectroscopy, QEPAS has the advantage of a small gas sampling volume (∼ 1 mm 3 ). This volume is ultimately determined by the space between the two prongs of the tuning fork.…”
Section: Introductionmentioning
confidence: 99%
“…The system and crystal performance at high pump powers have been studied. , with wavelengths up to 5 μm also obtained at the mW power level [7]. However, the intrinsic onset of absorption in MgO:PPLN and other oxide-based ferroelectric materials beyond ∼4 μm presents a fundamental barrier to wavelength generation at practical powers further into the mid-IR.…”
mentioning
confidence: 99%
“…As such, for practical generation of widely tunable cw radiation in the mid-IR, nonlinear optical techniques based on difference-frequency generation (DFG) [2] and optical parametric oscillators (OPOs) [5] still represent a highly effective approach. The cw OPOs based on MgO-doped periodically poled LiNbO 3 (MgO:PPLN) are now firmly established as the most effective approach for the generation of tunable high-power radiation up to ∼4 μm [6], with wavelengths up to 5 μm also obtained at the mW power level [7]. However, the intrinsic onset of absorption in MgO:PPLN and other oxide-based ferroelectric materials beyond ∼4 μm presents a fundamental barrier to wavelength generation at practical powers further into the mid-IR.…”
mentioning
confidence: 99%