2-μm high-power multiple-frequency single-mode Q-switched Ho:YLF laser for DIAL application

Abstract We report on the development and the demonstration of a two-wavelength single-frequency laser oscillator based on Ho:YLF crystal. This laser is especially suitable for application as a transmitter in differential absorption lidar (DIAL)/integrated path differential absorption (IPDA) measurements of atmospheric carbon dioxide (CO2) using the R30 CO2 absorption line at 2,050.967 nm. The oscillator consists in a fiber-coupled and free-space solid-state hybrid system and can be used in high-energy middle-rate or moderate-energy high-rate configurations. The latter produced On and Off sequentially single-frequency laser pulses with 13 mJ of energy at a repetition rate of 2 kHz and pulse duration of 42 ns. The pulse energy and frequency stabilities are specially documented in free-running, single-frequency and two-frequency seeding single-mode operations. Standard deviation is 7.7 % for pulse energy and 2 MHz for frequency stability for the two-wavelength seeding operation. Allan variance plot shows that frequency fluctuations are reduced below 70 kHz for 10 s of averaging which is suitable for accurate CO2 DIAL or IPDA measurements.

[1]  M. Schellhorn,et al.  High-power diode-pumped Tm:YLF laser , 2008 .

[2]  Jacques Pelon,et al.  Complementary study of differential absorption lidar optimization in direct and heterodyne detections. , 2006, Applied optics.

[3]  Didier Bruneau,et al.  Laser diode absorption spectroscopy for accurate CO(2) line parameters at 2 microm: consequences for space-based DIAL measurements and potential biases. , 2009, Applied optics.

[4]  M. Ostermeyer,et al.  Frequency stabilization of a Q-switched Nd:YAG laser oscillator with stability better 300 kHz following an rf-sideband scheme , 2009 .

[5]  M. Eichhorn,et al.  High-energy Ho:LLF MOPA laser system using a top-hat pump profile for the amplifier stage , 2012 .

[6]  M. Schellhorn,et al.  A comparison of resonantly pumped Ho:YLF and Ho:LLF lasers in CW and Q-switched operation under identical pump conditions , 2011 .

[7]  J. Caron,et al.  Operating wavelengths optimization for a spaceborne lidar measuring atmospheric CO2. , 2009, Applied optics.

[8]  Atsushi Sato,et al.  Coherent 2 microm differential absorption and wind lidar with conductively cooled laser and two-axis scanning device. , 2010, Applied optics.

[9]  L. Botha,et al.  Ho:YLF pumped HBr laser. , 2009, Optics express.

[10]  Jirong Yu,et al.  Side-line tunable laser transmitter for differential absorption lidar measurements of CO2: design and application to atmospheric measurements. , 2008, Applied optics.

[11]  Norman P. Barnes,et al.  Ho:Ho upconversion: applications to Ho lasers , 2003 .

[12]  V. Wulfmeyer,et al.  2-microm Doppler lidar transmitter with high frequency stability and low chirp. , 2000, Optics letters.

[13]  E. Black An introduction to Pound–Drever–Hall laser frequency stabilization , 2001 .

[14]  C. Kieleck,et al.  Ho:YAG laser intracavity pumped by a diode-pumped Tm:YLF laser. , 2003, Optics letters.

[15]  B. Samson,et al.  Tm-Doped Fiber Lasers: Fundamentals and Power Scaling , 2009, IEEE Journal of Selected Topics in Quantum Electronics.

[16]  Fiber-coupled diode laser modules with wavelengths around 2 &mgr;m , 2007, SPIE LASE.

[17]  Farzin Amzajerdian,et al.  High-energy 2μm Doppler lidar for wind measurements , 2007 .

[18]  S. Lamrini,et al.  Efficient high-power Ho:YAG laser directly in-band pumped by a GaSb-based laser diode stack at 1.9 μm , 2011, Applied Physics B.

[19]  J. Toutain,et al.  Diffuse volcanic emissions of carbon dioxide from Vulcano Island, Italy , 1990, Nature.

[20]  S. Houweling,et al.  Space-borne remote sensing of CO2, CH4, and N2O by integrated path differential absorption lidar: a sensitivity analysis , 2008 .

[21]  Upendra N. Singh,et al.  Can CO2 Turbulent Flux Be Measured by Lidar? A Preliminary Study , 2011 .

[22]  T. Y. Fan,et al.  Spectroscopy and diode laser-pumped operation of Tm,Ho:YAG , 1988 .

[23]  P. Flamant,et al.  Two-micrometer heterodyne differential absorption lidar measurements of the atmospheric CO2 mixing ratio in the boundary layer. , 2006, Applied optics.

[24]  D. C. Hanna,et al.  Energy-transfer upconversion and thermal lensing in high-power end-pumped Nd:YLF laser crystals , 1999 .

[25]  R. A. Fields,et al.  Thermal modeling of continuous‐wave end‐pumped solid‐state lasers , 1990 .

[26]  Jeffrey R. Chen,et al.  Frequency stabilization of distributed-feedback laser diodes at 1572 nm for lidar measurements of atmospheric carbon dioxide. , 2011, Applied optics.

[27]  D. Schrag Preparing to Capture Carbon , 2007, Science.

[28]  D. W. Allan,et al.  Statistics of atomic frequency standards , 1966 .