400 w cryo cooled yb yag laser with 56 efficiency authors
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400-W Cryo-cooled Yb:YAG Laser with 56% Efficiency Authors: Bhabana Pati and Kevin F. Wall Q-Peak, Inc., 135 South Road, Bedford, MA 01730 www.qpeak.com Acknowledgments: AFRL/DELO Phase II SBIR Contract # FA9451-04-C-0151 Outline 1 .


  1. 400-W Cryo-cooled Yb:YAG Laser with 56% Efficiency Authors: Bhabana Pati and Kevin F. Wall Q-Peak, Inc., 135 South Road, Bedford, MA 01730 www.qpeak.com Acknowledgments: AFRL/DELO Phase II SBIR Contract # FA9451-04-C-0151

  2. Outline 1 . Objective 2. Laser performance in a prism-pump design 3. Conclusions and improvements

  3. Objectives  Build a highly efficient, cryogenically-cooled, Yb:YAG laser at 1030 nm.  Produce >250 W, Q-switched, TEM 00 output power from an side-pumped slab laser.

  4. Show MPS design

  5. Specific Yb:YAG design Crystal is 2% doped  and 28 x 10 x 4 mm in size.  Two pump diode lasers are off set on the opposite sides of the slab. Heat is removed from  the two large faces of the crystal.

  6. Nuvonyx lensed diode laser arrays are pump sources

  7. Pump Focusing Design Side view Top view

  8. Measured pump beam at the crystal Imaged at the plane of  crystal surface  Intensity of the beam was reduced by operating the laser in pulse mode Beam size 10 X 2 mm   CCD camera and Spiricon beam analyzer.

  9. Calculated slope efficiency is 61% Parameter Symbol Value η t Transfer efficiency 0.98 η a Absorption efficiency 0.98 η qe Quantum efficiency 1.00 η qd Quantum defect 0.91 η o Overlap efficiency 0.80 η st Storage efficiency 0.71 η oc Output coupling efficiency 0.87 η sl Slope Efficiency 0.61 • Output coupling efficiency assumes 3% round-trip losses and R = 80% OC

  10. Multimode laser performance 500  Maximum output power Output power (W) was 400 W with a total 400 pump power of 720 W. 300  98% of pump power was 200 incident on the crystal and 100 98% was absorbed. 0 0 200 400 600 800  With 80%-reflective output Pump power (W) coupler, the slope efficiency was 62%. The laser was multi-mode  in the horizontal plane and Yb:YAG Flat OC nearly diffraction limited 50 cm cc HR in the vertical plane.

  11. Measured temperatures - crystal base and clamp plates Non-lasing condition Lasing condition 130 110 Base plate Temperature (K) Base plate Temperature (K) 120 Clamp plate Clamp plate 100 110 100 90 90 80 80 70 70 0 200 400 600 800 0 200 400 600 800 Pump power (W) Pump power (W)  Compared with the lasing condition, in the non-lasing condition, the temperatures of the clamp and base plates were 26 ° K and 11 ° K higher respectively.

  12. Sectional view of modeled temperature distribution Assumptions:  Uniform heat deposition of 360 W in the crystal. Perfect contact between  the crystal and heat sinks. Also, perfect contact between the base and clamp plates.  Heat removal from the crystal mount is only from the base plate. Temperature of the center  of the crystal is ~ 129 ° K .  Crystal surface- temperatures at the interfaces of the base and clamp plates are 90 ° K and 101 ° K respectively.

  13. Measured probe-beam deflection in the crystal Thermal wedging due  to the temperature 1.5 Horizontal difference between the Beam deflection (mm) Vertical 1 top and bottom of the crystal. 0.5  Camera was 1 m away 0 from the crystal. -0.5 0 200 400 600 800 Beam deflection is  Pump power (W) prominent in the vertical plane

  14. Conclusion  We demonstrated a 400 W, cryogenically cooled Yb:YAG laser. We obtained a slope efficiency of 62% and optical-to-optical  efficiency of 56% in a side-pumped slab geometry, in good agreement with our estimates.  The laser is multi mode in the horizontal plane and nearly diffraction limited in the vertical plane. Beam quality will be improved by multi passing the laser in the  crystal – experiments underway, along with Q-switching.

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