12
Studies of Thermal Loading in Pre-Modecleaners for Advanced LIGO Amber Bullington Stanford University LSC/Virgo March 2007 Meeting Optics Working Group G070084-00-Z

Studies of Thermal Loading in Pre-Modecleaners for Advanced LIGO Amber Bullington Stanford University LSC/Virgo March 2007 Meeting Optics Working Group

Embed Size (px)

Citation preview

Page 1: Studies of Thermal Loading in Pre-Modecleaners for Advanced LIGO Amber Bullington Stanford University LSC/Virgo March 2007 Meeting Optics Working Group

Studies of Thermal Loading in Pre-Modecleaners for Advanced LIGO

Amber BullingtonStanford University

LSC/Virgo March 2007 MeetingOptics Working Group

G070084-00-Z

Page 2: Studies of Thermal Loading in Pre-Modecleaners for Advanced LIGO Amber Bullington Stanford University LSC/Virgo March 2007 Meeting Optics Working Group

2

Outline

Thermal Loading Experiment» Ring cavity known as pre-modecleaner (PMC)

– Same geometry as cavity used in the PSL

» Goal: Achieve resonant thermal load akin to Advanced LIGO

– Use calibrated absorption loss– Reach absorption comparable to Advanced

LIGO ~12 mW per suspended MC optic for

0.5 ppm coating absorption – Compare results to models

Results» Onset of thermal loading» Thermal limits

For the future» Further tests» Suggestions

A Pre-Modecleaner

Page 3: Studies of Thermal Loading in Pre-Modecleaners for Advanced LIGO Amber Bullington Stanford University LSC/Virgo March 2007 Meeting Optics Working Group

3

Experimental Setup

NPRO4-rod

amplifier

LIGO 10 W MOPA

4-rod amplifier

External Amplifier

Mode-matching lenses

Low FinessePre-Modecleaner

Pre-Modecleaner under test

Beam Analysis-Transmission Monitor-Data Acquisition-CCD

Reflection locking electronics

Reflection locking electronics

Mode-matching lensesPhotodiode

Modal Analysis-’Mode Analyzer’ - Scanning modecleaner

Page 4: Studies of Thermal Loading in Pre-Modecleaners for Advanced LIGO Amber Bullington Stanford University LSC/Virgo March 2007 Meeting Optics Working Group

4

Pre-Modecleaner Properties

Dominant thermal load in coatings» Low-loss coatings coated by Research Electro-Optics» Absorption loss measured by PCI

– Flat I/O optics: 1.4 ppm

– Curved optic: 0.4 ppm

‘Lossy’ pre-modecleaner» Low-loss fused silica input/output optics» Rear optic: low-loss coating on absorptive substrate

– IR absorbing glass: KG5

– KG5 optic coating transmission: 81 ppm

‘Low-loss’ pre-modecleaner» REO coatings on BK7 substrates

Resonances of different polarizations do not overlap

– Low Finesse (p-pol) ~ 330

– High Finesse (s-pol) ~ 5000

Fused Silica

BK7

BK7

KG5

‘Lossy’ Pre-modecleaner

‘Low-loss’ Pre-modecleaner

Page 5: Studies of Thermal Loading in Pre-Modecleaners for Advanced LIGO Amber Bullington Stanford University LSC/Virgo March 2007 Meeting Optics Working Group

5

‘Lossy’ Pre-Modecleaner – Low Finesse

Increase input power in steps» Analyze transmitted TEM00

content

Higher order mode overlap with TEM00

» Occasional overlap seen as power is increased

» Roll-off in TEM00 content at high absorbed power

Transmitted CCD Image – ‘Lossy’ PMCCCD Image – Mode Analyzer PMC

Transmitted TEM00 Mode Content

0.8

0.85

0.9

0.95

1

1.05

0 10 20 30 40 50

Absorbed Power, mW

Fra

ctio

n T

EM

00

Page 6: Studies of Thermal Loading in Pre-Modecleaners for Advanced LIGO Amber Bullington Stanford University LSC/Virgo March 2007 Meeting Optics Working Group

6

‘Lossy’ PMC Thermal Limit

Thermal Limit» Transmission linear up to 5 W

input power (Pabsorbed = 40 mW)

» For Pabsorbed > 40 mW, higher order modal content degrades transmitted beam quality

» For Pabsorbed > 47 mW, constant locked transmitted power not achieved

Transmitted Beam Reflected Beam Mode Analyzer Transmission‘Lossy’ PMC Images

Input Power = 6 W, Pabsorbed = 47 mW

'Lossy' PMC Transmission

0

1

2

3

4

5

0 1 2 3 4 5 6 7

Input Power, W

Tra

nsm

itte

d P

ow

er, W

Page 7: Studies of Thermal Loading in Pre-Modecleaners for Advanced LIGO Amber Bullington Stanford University LSC/Virgo March 2007 Meeting Optics Working Group

7

Thermally Induced Power Fluctuation

Power fluctuation from thermal effects

» Lossy PMC: Thermal cycling induces periodic fluctuation of transmitted power

Transmitted mode images1: near maximum power

2: during power decline

3: near minimum power

1 2 3

Transmitted Power Fluctuation

0

1

2

3

4

5

6

0 0.02 0.04 0.06 0.08 0.1 0.12 0.14 0.16

Time, s

Po

wer

, W

29 Hz

41%

Page 8: Studies of Thermal Loading in Pre-Modecleaners for Advanced LIGO Amber Bullington Stanford University LSC/Virgo March 2007 Meeting Optics Working Group

8

Modal Analysis

Higher order mode overlap with TEM00

» Change in cavity g-factor: g = 1 - L/R» Change in Radius of Curvature (ROC)

of KG5 optic New g factor gives thermally

distorted radius of curvature, Rhot

» Cold cavity g factor = 0.79– Rcold = 1 m

» Example: TEM00/TEM11,0 overlap– Hot cavity g factor = 0.83– Rhot = 1.2 m

Calculate absorbed power from Rhot, compare with expected absorption

» Pabsorbed = (4s)/

Input Power

Calculated Absorbed Power

Expected Absorbed Power

Observed Mode

1 W 13 mW 9 mW LG23

4 W 23 mW 30 mW TEM11,0

> 4.5 W 39 mW 40 mW LG12

TEM11,0

TEM00

Cold g

Page 9: Studies of Thermal Loading in Pre-Modecleaners for Advanced LIGO Amber Bullington Stanford University LSC/Virgo March 2007 Meeting Optics Working Group

9

‘Lossy’ Pre-Modecleaner – High Finesse

Strong higher order mode coupling

» First observation at 4.25 mW absorbed power

– Several TEMmn, large m+n, modes

– 96 % TEM00 output

Degradation of TEM00 output» Increased absorbed power

– Multiple higher order mode coupling

– Sometimes one dominant higher order mode

» Lowest TEM00 transmission 57% at 12 mW absorbed power

Transmitted Beam, Pabs ~ 4 mW Mode Analyzer

Mode Analyzer, Pabs ~ 10 mW

PZT drive

TEM00

Higher order modes

Page 10: Studies of Thermal Loading in Pre-Modecleaners for Advanced LIGO Amber Bullington Stanford University LSC/Virgo March 2007 Meeting Optics Working Group

10

‘Low-loss’ Pre-Modecleaner

REO coatings on BK7 substrates

High finesse» Higher order modes at a few

absorbed powers, starting at Pabs = 5.1 mW

» Rollover in transmission > 20 mW absorbed power

Low Finesse» First higher order mode coupling

noted near max available input power, Pabs = 5.1 mW

Transmitted TEM00 Content, High Finesse

0.920.930.940.950.960.970.980.99

11.01

0 5 10 15 20 25

Absorbed Power, mW

Fra

ctio

n T

EM

00

'Low-Loss' PMC Transmission, High Finesse

0

0.5

1

1.5

2

2.5

3

3.5

0 2 4 6 8 10 12

Input Power, W

Tra

nsm

itte

d P

ow

er, W

Page 11: Studies of Thermal Loading in Pre-Modecleaners for Advanced LIGO Amber Bullington Stanford University LSC/Virgo March 2007 Meeting Optics Working Group

11

Other Issues

Reduced transmission in high finesse for both pre-modecleaners» 30% coupling, expect closer to 80%

» Scatter loss from curved optic

» Response to thermal load agrees with expected absorption

Melody» Mode-based interferometer thermal modeling tool

» Limited agreement with data– Thermal loading of ‘Lossy’ PMC in low finesse– Differing behavior for thermal loading in high finesse

Melody shows sharp coupling decline without higher order mode coupling

Page 12: Studies of Thermal Loading in Pre-Modecleaners for Advanced LIGO Amber Bullington Stanford University LSC/Virgo March 2007 Meeting Optics Working Group

12

Summary

Transmission degradation from higher order mode coupling» Stronger coupling in high finesse case» Large thermal load may induce power fluctuations

Recommendations based on observations» Coating absorption <= 1ppm» Higher finesse -> lower absorption

– From experiment, < 4 mW– Scale results to other substrate materials

» Aperture to suppress large order modes– Suspended modecleaner

» Consider alternative geometry– 4-bounce pre-modecleaner?

Advantage: reduce mode overlap possibility Disadvantage: not polarization sensitive

For the future … » Test pre-modecleaners with sapphire and undoped YAG optical substrates» Design an all-reflective modecleaner using gratings

– Expand substrate possibilities (e.g. silicon)