Review - LIGOajw/40m/40m_000516.pdf · Review of 40m upgrade go als The primary goal of the 40 m...

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Transcript of Review - LIGOajw/40m/40m_000516.pdf · Review of 40m upgrade go als The primary goal of the 40 m...

Page 1: Review - LIGOajw/40m/40m_000516.pdf · Review of 40m upgrade go als The primary goal of the 40 m upgrade is to demonstrate a sc heme for using ... Caltec h: RSE mo delling; Twiddle/Finesse!

40m Upgrade Plans

� Review of 40m upgrade goals

� 40m infrastructure upgrade

� RSE con�guration - design considerations

� IFO optical con�guration

� RSE control scheme

� people, money, schedule

� problems and questions

http://www.ligo.caltech.edu/�ajw/40m 000516.pdf

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Page 2: Review - LIGOajw/40m/40m_000516.pdf · Review of 40m upgrade go als The primary goal of the 40 m upgrade is to demonstrate a sc heme for using ... Caltec h: RSE mo delling; Twiddle/Finesse!

Review of 40m upgrade goals

� The primary goal of the 40 m upgrade

is to demonstrate a scheme for using

resonant sideband extraction (RSE),

in either broadband or tuned con�g,

appropriate for an optimal LIGO con�g

� RSE and DR have been demonstrated at

Garching 30m, and at table-top IFOs

� An RSE/DR con�g appropriate for LIGO

will be demonstrated at the Glasgow 10m

� For LIGO, need a full engineering prototype,

using LIGO electronics and control scheme.

This is the primary goal of the 40 m upgrade.

� Complements work at other R&D facilities:

{ 40m will focus on shot (phase, sensing) noise, high-f

{ LASTI: full-scale SEI,SUS prototyping; low-f

{ TNI: thermal noise; middle-f

{ ETF: Sagnac, high powered lasers

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Secondary 40m upgrade goals

Prototype \everything"?

� potentially, multiple pendula SUS

| this may be necessary, to extrapolate experience

gained at 40m to LIGO-II

� potentially, advanced SEI systems

| scaled down, of course. Cannot replace full-scale

testing at LASTI.

� potentially, thermal noise measurements

with maximized beam width (� at mirrors)

| a big, and challenging, diversion.

� LIGO-III: cryogenic TMs, QND, etc..

� physicist training

At the least, must prototype everything that has

large impact on electronics/control system,

for a meaningful full engineering test!

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40m infrastructure upgrade

� LIGO-like upgrade, during next 1-2 years:

{ building modi�cations, control room, electrical;

work to be completed by fall (???)

{ Active seismic isolators on TM stacks?

{ EPICS-based vacuum control system

(to be completed by summer)

{ LIGO-I PSL from Peter King (fall?)

{ 12 meter mode cleaner and MMT

(vacuum envelope, stack, exists)

{ 4" optics for IR running

{ 7th suspended optic (SM)

{ scaled (for 4" optics) suspensions

{ Output chamber for signal mirror

(chamber exists, seismic stack to be built)

{ full CDS control system: ISC, LSC, ASC, GDS

{ control scheme for all optics

{ strawman: frontal mod with M-Z IFO

� Ready to prototype an RSE scheme by 2002.

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Seismic noise

We have measured the seismic noise (V,H; day, night) at

the 40m lab:

100

101

102

10−16

10−14

10−12

10−10

10−8

10−6

10−4

Frequency (Hz)

Dis

plac

emen

t noi

se, m

/ rt

Hz

40m displacement noise

Starting GPS time:Wed Apr 12 02:17:43 2000 (and 0 usec)

Hanford IFO−Seis Floor−X Floor−Y Floor−Z Microphone

100

101

102

10−12

10−11

10−10

10−9

10−8

10−7

10−6

zrmsnite = 0.13 µm

zrmsday = 0.23 µm

nightday

100

101

102

10−10

10−9

10−8

10−7

10−6

10−5

vrmsnite = 1.64 µm/s

vrmsday = 3.13 µm/s

nightday

100

101

102

10−8

10−7

10−6

10−5

10−4

10−3

armsnite = 1929 µm/s2

armsday = 1809.59 µm/s2

nightday

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Stack transfer function

V,H transfer functions of the existing TM stacks:

100

101

102

10−4

10−3

10−2

10−1

100

101

102

Frequency (Hz)

Hor

izon

tal T

rans

fer

func

tion

40m displacement noise 12−Apr−2000 03:17:30 PDT −−− Horizontal

Seismic+Geo Shaker+AccelShaker+Geo Model

100

101

102

10−4

10−3

10−2

10−1

100

101

102

Frequency (Hz)

Ver

tical

Tra

nsfe

r fu

nctio

n

40m displacement noise 12−Apr−2000 03:17:30 PDT −−− Vertical

Seismic+Geo Shaker+AccelShaker+Geo Model

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Active seismic isolation?

STACIS isolator pedestals (roughly $120K)

For robust IFO lock, need mirror horizontal vrms � �=s

�lock ��=2

vthrP (v < vthr); vthr ' 1�=s

100

101

102

10−16

10−14

10−12

10−10

10−8

10−6

10−4

vrmsfloor = 1.64 µm/s

vrmsmirr = 0.43 µm/s

vrmsSTACIS = 0.27 µm/s

Frequency (Hz)

velo

city

noi

se p

ower

spe

ctru

m, µ

m/s

/ rt

Hz

40m displacement noise 12−Apr−2000 03:17:30 PDT

vrms

, floor v

rms, mirror

vrms

, STACIS

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Resonant Sideband Extraction(RSE) Config

South

East Arm

ArmL1

l 3

l 2l 1

PSL

RM

L2

RF 12m MC

APD PPDSPD

BS

SM

A power-recycled Michelson IFO with Fabry-Perot arms,

with a signal recycling mirror (SM) for resonant sideband

extraction (RSE).

� LSC/AIC group is evaluating di�erent control schemes.

� Key parameters depend on what is chosen:

{ TITM , TSM , LSRC , LPRC

{ Method for applying sidebands to beam

� Hope to have a workable scheme by fall

� May have to fold SRC!!

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Will it fit?

150

cm

Output chamber

Beam splitter

25 cm

Recycling mirror

Signal mirror

For broadband operation (�cs = 0, worst case),

need � 178 cm. Have only � 150 cm!

May be limited in available tune,

or may have to fold the SRC optical path.

More careful optimizations and drawings are in the works

(Mike Smith).

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Fundamental noise at 40m

101

102

103

104

10−22

10−21

10−20

10−19

10−18

10−17

10−16

40m strain sensitivity

stra

in s

ensi

tivity

(1/

rtH

z)

Frequency (Hz)

TITM

TPRM

TSRM

Gprc

Garm

fpol

0.030 0.000 0.176 10 131 9516

Seismic

FSilica Thermal

Suspension

RSE, tuned

Radiation pressure

40m RSE total

� Thermoelastic, photothermal noise are negligible

� Suspension noise may be trouble with 3" optics

� Q (F-Si) = 2� 106. Dominates from 100{3KHz!

� May need to turn laser power down

to expose shot noise over thermal;

� Alternatively, live with thermal noise;

don't bother to expose shot noise;

focus on controls problem

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People

� Currently: Two physicists (Weinstein, Ugolini),

one master tech (Vass)

� MUST make heavy use of LIGO engineers:

{ building modi�cations: Fred Asiri

{ Output chamber stack: Fred Asiri

{ active isolators?: Larry Jones

{ PSL-I: Peter King, Rich Abbott

{ optics: Garilynn Billingsley

{ single ! multiple pendula: Janeen Romie

{ optical layout, ba�ing: Mike Smith

{ CDS (ISC, LSC, ASC): Jay Heefner, Rolf Bork,

new hire

� Expect to hire another controls engineer/postdoc

� MUST involve more postdocs, grad students,

undergrads

� MUST involve LSC personnel

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Summer REU's

� Lisa Goggin, University College, Cork:

12 meter mode cleaner

� Jitesh Chauhan, Leicester U:

Global Diagnostics System

� Brian Kappus, Harvey Mudd:

Wavefront sensing

� Ted Jou, Caltech:

RSE modelling; Twiddle/Finesse ! E2E

� Ivica Stevanovic, Belgrade U:

multiple pendulum modelling

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Schedule, Milestone Fantasy

� 3q2000

{ lab building repairs and mods

{ LIGO IR PSL

{ Construction of new Output chamber, stack

{ Bakeout? Active isolators?

� 4q2000

{ Review of optical design consistent with RSE/DR

{ Development of control system

� 2q2001

{ LIGO-like suspensions, controllers, optics in place

{ LIGO-like CDS: ISC, LSC, ASC, WFS systems

{ LIGO-like diagnostics, DAQS software

{ Review of SM control scheme

(broad-band and detuned)

� 2002

{ Prototype installation complete.

{ Initial shakedown complete.

{ Ready to prototype an RSE scheme.

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Problems and questions

� Do we need to bake out the vacuum envelope?

� Should we rebuild the seismic stacks,

replacing sti�-but-well-damped viton

(contaminating the vacuum at a low level?)

with soft but-poorly-damped metal springs?

� Should we consider employing

advanced (scaled down) SEI systems?

� should we consider prototyping advanced SUS systems

(multiple pendula, electrostatic control)?

� Is the \simple" control scheme developed by Mason

adequate for LIGO-II?

� How can we implement it? M-Z? fRF2 = 100 MHz?

� Modulation in vacuum or air? Before/after MC?

� where will we get the physicists and eng. support?

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