status of high-power laser development at stanford shally saraf*, supriyo sinha, arun kumar...

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Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford University LIGO Science Collaboration Meeting Hanford Site, August 19 – 22, 2002 *[email protected] LIGO-G020356-00-Z

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Page 1: Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford

Status of High-Power Laser Development at Stanford

Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan

and Robert L. Byer

E. L. Ginzton Laboratory, Stanford University

LIGO Science Collaboration Meeting

Hanford Site, August 19 – 22, 2002

*[email protected]

LIGO-G020356-00-Z

Page 2: Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford

Outline

• Review of slab lasers.

• Progress since Livingston LSC.

• 100W demonstration results.

• 200W amplifier design and status.

• (Near) future work.

Page 3: Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford

Rod vs Slab

• 1st order thermal lens • Spatially dependent

birefringence (depolarization)

• 2nd order thermal distortions

• Slightly reduced mode-fill

zig-zag slabrod

Page 4: Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford

Face-pumping vs Edge-pumping

Pumping

Cooling

zig-zagplane

Pumping

Cooling

zig-zagplaneFace-

pumping

Edge-pumping

zig-zag slab

Page 5: Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford

Nd:YAG Laser Head

3.8 cm

Page 6: Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford

Amplification Goal: 100 W

• Two zig-zag edge-pumped slab amplifiers.– Brewster ends.– 3:1 aspect ratio (width/thickness).

• About 900 W total pump power.• 10W LIGO laser followed by an external

amplifier provides 20W to drive slab amplifiers.

Page 7: Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford

Experimental Setup for 100W demonstration

10W LIGO

LASER ISOL

20W

AMP

DUMP

2 2

2

Power

Meter

PBS

PBS

PBS

Edge Pumped Slab #1

Edge Pumped Slab #2

Beam Waist ~ 300m

Beam Waist ~ 300m

DUMP

DUMP

Page 8: Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford

100W experimental setup

Page 9: Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford

10W Amplifier

Page 10: Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford

• Increased NPRO power from 235mW to 418mW by turning up drive current from 1.89A to 2.4A.

• Realigned optical train.

• Output power increased to 10.4W back to original specs.

• Set diode temperature to 24.1oC and pump current to 23A for the double passed amplifier.

10W Amplifier upgrade

Page 11: Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford

20W Amplifier

• Replaced Faraday Isolator following 10W LIGO Laser.• Replaced faulty power supply for external 20W amplifier.• Mode matched beam into 20W amplifier (waist ~ 245m)

Page 12: Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford

Beam quality after 20 W amplifier

Beam diameter versus Propagation Distance after 20W amplifier

0

200

400

600

800

1000

1200

1400

1600

1800

2000

0 50 100 150 200 250 300 350

Distance (mm)

Bea

m D

iam

eter

(u

m)

Hor. beam diameter

M2X = 1.09

Ver. beam diameter

M2Y = 1.02

Measured output power ~ 24.4W.

Page 13: Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford

Edge pumped slab head assembly

Page 14: Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford

Slab 2 power amplifier set up

Page 15: Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford

Complication ---- Slab #1 cracked

Page 16: Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford

Results for slab amplifier # 1

Extracted Power versus Input PowerSlab 1 single pass

0

2

4

6

8

0 5 10 15 20 25

Input Power (W)

Ext

ract

ed

Pow

er (W

)

180W Pump goL = 0.412150W Pump goL = 0.357120W Pump goL = 0.22790W Pump goL = 0.184

Output Power = Input Power + Extracted Power

Page 17: Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford

Power and M2 measurement after slab #1

Beam diameter vs propagation distance

0

500

1000

1500

390 490 590

Propagation distance (mm)

Beam

dia

met

er

(um

)

Horizontal diameter

M2x = 1.01

Vertical Diameter

M2y = 1.02

Output Power from triple passed slab #1 = 39W

Page 18: Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford

Slab #2 single pass power output

Output Power versus Pump Power for Power Amplifier (single pass)

30

35

40

45

50

55

0 100 200 300 400 500

Pump Power (W)

Ou

tpu

t P

ow

er (

W)

Page 19: Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford

Slab #2 triple pass power output

Triple Pass Output Power versus Pump Power

30

40

50

60

70

80

0 100 200 300 400 500

Pump Power (W)

Ou

tpu

t P

ow

er

(W)

Power out of MOPA ~ 71.8W

Page 20: Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford

Thermal lens measurements

Thermal Lens Power versus Pump

0

2

4

6

8

100 200 300 400 500

Pump Power (W)

Dio

pte

rs (

1/m

)

Pumping

Cooling

zig-zagplane

Page 21: Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford

Future work on 100W MOPA

• Compensate for thermal lens in second slab by using cylindrical lenses in triple pass.

• Faster beam quality measurements using holographic beam sampler to eliminate need for multiple wedges for attenuating power.

• M2 measurement of MOPA output.

• Redo theoretical calculation of thermal lens.

Page 22: Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford

End pumping topology for 200W design

Motivation -> Higher efficiency

• Near total absorption of pump light.

• Confinement of pump radiation leads to better mode overlap

signal IN

Pump

0.6% Nd:YAG

undoped end

undoped endsignal OUT

Page 23: Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford

Pre-amplifier Design : End-pumping

20 W 160 W

2-slab end-pumped double passed

amplifier

Crystal Dimensions Width = 1.11 mm,

Length = 6.6 cm, Thickness = 0.9 mm

Slab Design Issues1. Parasitic suppression2. Pump light coupling and absorption

Courtesy, Hagop Injeyan, TRW

Page 24: Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford

Expected MOPA System Performance

Amplifier Input

Power

Multi-mode

Output

Output TEM00

End-pumped

(Ppump = 130W)16W 60W 48W

End-pumped

(Ppump = 435W)48W 200W 160W

Edge-pumped

(Ppump = 1400W)160W 500W 400W

• Edge pumped design chosen for final stage because of heat extraction requirement and simpler engineering design without sacrificing much pump absorption.

Page 25: Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford

Status of 200W design

• Received 8mm x 8mm Nd:YAG composites with undoped ends from Onyx.

• Diced up one composite in the Stanford Crystal shop. On one plate undoped end broke off cleanly from the doped portion. (possibly defective bonding from Onyx?)

Page 26: Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford

Status of 200W design (contd….)

• Second composite being diced up by Crystal River Optics.

Page 27: Status of High-Power Laser Development at Stanford Shally Saraf*, Supriyo Sinha, Arun Kumar Sridharan and Robert L. Byer E. L. Ginzton Laboratory, Stanford

Future Work on 200W MOPA

• Get coated plates from MLD, inspect and dice up into slabs with final dimensions.

• Install Laser Line pump diodes with total pump power of 500W.

• Fabricate laser head with microchannel coolers.

• Integrate and start amplifier experiments.