LIGO and Virgo Opening Up a New Window on the Universe Nikhef 12 - - PowerPoint PPT Presentation

ligo and virgo opening up a new window on the universe
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LIGO and Virgo Opening Up a New Window on the Universe Nikhef 12 - - PowerPoint PPT Presentation

LIGO and Virgo Opening Up a New Window on the Universe Nikhef 12 September 2017 David Shoemaker For the LIGO and Virgo Scientific Collaborations Credits Measurement results: LIGO/Virgo Collaborations, PRL 116, 061102 (2016);


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LIGO and Virgo – Opening Up a New Window on the Universe

Nikhef 12 September 2017

David Shoemaker For the LIGO and Virgo Scientific Collaborations

Credits Measurement results: LIGO/Virgo Collaborations, PRL 116, 061102 (2016); http://arxiv.org/abs/1606.04856 Simulations: SXS Collaboration; LIGO Laboratory Localization: S. Fairhurst arXiv:1205.6611v1 Photographs: LIGO Laboratory; MIT; Caltech

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  • 1.3 Billion Years ago…

» Two black holes in a tight orbit » Period shrinking due to loss of energy to gravitational waves » Final coalescence into a single black hole

  • Powerful gravitational waves radiated in last several tenths of a

second – ‘ripples in spacetime’

  • On earth, transition from single-cell to multicellular life forms
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100 years ago

  • Albert Einstein is evaluating and processing patent

applications… » …for transmission of electric signals and electrical-mechanical synchronization of time » Musing on relative motion of radio transmitters and receivers » à Special Relativity, 1905

  • …then dreaming of being in an elevator in space

and asking if it is a pull on the cable or gravity... » à General Relativity, 1915

  • Prediction of gravitational waves (GW) as a

consequence of GR in 1916:

  • Notes that it is of no practical interest as it will not

be possible to detect such a small effect

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A Half-Century ago

  • Several scientists think of using laser interferometry

to detect GWs

  • Rainer Weiss of MIT invents the idea as a homework

problem for students learning General Relativity

  • He does the homework, and spends a summer

fleshing out the idea

  • In 1972, Weiss publishes an internal MIT report

» “Electromagnetically coupled broadband gravitational antenna” » Sets the concept and scale of LIGO » This roadmap contains also noise sources and how to manage them

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Two Decades ago

  • Caltech and MIT propose to the NSF to establish Observatories
  • Proposal states clearly that the initial detectors only have a chance of

detections, and that upgraded detectors must be accommodated and foreseen Proposal cover art à

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LIGO Laboratory – Caltech, MIT –

built observatories in ‘90s, and…

LIGO Livingston

…Observed with the initial detectors 2005-2011, and saw…

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nothing

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Initial Detectors

  • That is to say, we saw no gravitational-wave signals.

» We learned how to build and commission detectors » We learned how to analyze the data » We created new upper limits and significant ‘non- detections’ …but it was clear we needed more sensitive detectors.

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Advanced LIGO Sensitivity: a qualitative difference

  • M. Evans
  • While observing with initial detectors,

parallel R&D led to better concepts

  • Initial LIGO proposal included

certainty of the need for improvements

  • Design for 10x better sensitivity

Initial Reach Advanced Reach

  • We measure amplitude,

so signal falls as 1/r

  • 1000x more candidates
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1.3 Billion years after the Black Holes merged.. (and multicellular life started on earth…) 100 years after Einstein predicted gravitational waves… 50 years after Rai Weiss invented the detectors... 20 years after the NSF, MIT, and Caltech Founded LIGO... 10 years after Advanced LIGO got the ok... 6 months after starting detector tuning...

Two days after we started observing...

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The first signal

On September 14, 2015 at 09:50:45 UTC

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ß 1/10 second à

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h ≈ 8GM R

2ωorb 2

rc

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What are Gravitational Waves?

  • GWs propagate at the speed of light (according to GR)
  • Emitted from rapidly accelerating mass distributions
  • Creates a strain h in space
  • Space is very stiff; h is ~10-21 for say Neutron Stars in Virgo Cluster
  • …or two ~30-solar-mass Black Holes at 1.2 billion light years...
  • Measurable GWs can only be expected from Stars or Black Holes

undergoing incredibly violent accelerations

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r = distance from the source to the observer

h = ΔL L ≈ 1 r G c4 !! I

worb

R M

Rotating Dumbbell:

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What is our measurement technique?

  • Enhanced Michelson

interferometers

  • Passing GWs modulate the

distance between the end test mass and the beam splitter

  • Arms are short compared

to our GW wavelengths, so longer arms make bigger signals à multi-km installations

  • Sensitivity limited by quantum

noise, thermal noise, seismic noise

  • Einstein’s contributions

throughout our measurement science!

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L L h D »

Magnitude of h at Earth: Largest signals h ~ 10-21 (1 hair / Alpha Centauri) For L = 1 m, ΔL= 10-21 m For L = 4km, ΔL= 4x10-18 m

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LIGO Sensitivity for first Observing run

Initial LIGO O1 aLIGO Design aLIGO

Broadband, Factor ~3 improvement At ~40 Hz, Factor ~100 improvement

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FI FI PSL

Input Mode Cleaner Output Mode Cleaner Signal Recycling Cavity Power Recycling Cavity

PRM SRM ITMY PR2 PR3 SR2 SR3 BS DC PD

Differential Arm Length Readout

MC2 MC3 MC1 HAM2 HAM3 HAM4 HAM5 HAM6 HAM1

  • L. Barsotti - March 9, 2012

Adapted from G1200071-v1

ETMX ITMX TRANSMON ALS ETMY

The real instrument is also more complex than a simple Michelson…

photodiode

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Kai Staats

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Infrastructure: 4km Beam Tubes

  • Light must travel in an excellent vacuum

» Just a few molecules traversing the optical path makes a detectable change in path length, masking GWs! » 1.2 m diameter – avoid scattering against walls

  • Cover over the tube – stops hunters’ bullets and the stray car
  • Tube is straight to a fraction of a cm…not like the earth’s curved surface
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LIGO Vacuum Equipment –

designed for several generations of instruments

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200W CW Nd:YAG laser

Designed and contributed by Max Planck Albert Einstein Institute

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  • Stabilized in power and frequency – using

techniques developed for time references

  • Uses a monolithic master oscillator followed

by injection-locked rod amplifier

  • Delivers the required shot-noise limited

fringe resolution

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  • Both the physical test mass – a free point in

space-time – and a crucial optical element

  • Mechanical requirements: bulk and coating

thermal noise, high resonant frequency

  • Optical requirements: figure, scatter,

homogeneity, bulk and coating absorption

Test Masses

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  • Requires the state of the art

in substrates and polishing

  • Pushes the art for coating!
  • Sum-nm flatness over 300mm

Test Masses: 34cm f x 20cm 40 kg 40 kg BS: 37cm f x 6cm ITM T = 1.4% Round-trip optical loss: 75 ppm max Compensation plates: 34cm f x 10cm

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Optics Table Interface (Seismic Isolation System) Damping Controls Electrostatic Actuation Hierarchical Global Controls

Test Mass Quadruple Pendulum suspension

designed jointly by the UK (led by Glasgow) and LIGO lab, with capital contribution funded by PPARC/STFC

  • Quadruple pendulum suspensions for the main optics;

second ‘reaction’ mass to give quiet point from which to push

  • Create quasi-monolithic pendulums using

GPB star-tracking telescope techniques; Fused silica fibers to suspend 40 kg test mass » VERY Low thermal noise!

22 Final elements All Fused silica

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So, that’s the LIGO instrument. How about the detection? What did we learn from our record of h(t)?

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Time trace from Hanford, high- and low-pass filtered to make signal more evident. Signal in-band for ~0.2 secs. Amplitude ~1x10-21

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Time trace from Hanford and Livingston; Hanford inverted (observatory orientation is 180), and shifted by 7.1 msec (the observatories are separated by 10 msec time of flight). Source is in an annulus in the Southern hemisphere.

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Numerical Relativity waveform, putting in the same high/low pass filtering (so no long sinusoidal precursor). Same fit matches both

  • bservatories.
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Real time-series data, minus waveform

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Spectrogram of high/low pass filtered data shows characteristic ‘chirp’ form.

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One event…was it real?

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Our second signal, 26 December 2015 – the SNR we thought we would be working with

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A nice way to look at the signals from O1

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And then there were 3! (+1) 4 January 2017

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Then…. Virgo joins O2

  • The EGO Observatory in Cascina, Italy, near Pisa
  • Advanced Virgo joined the O2 Observing run on 1 August 2017

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Virgo Commissioning and Running

Very rapid progress to a good sensitivity Very high uptime

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Virgo-LIGO O2 Run now complete

  • Triple-interferometer observing from 1 August to 25 August
  • Some promising gravitational-wave candidates have been identified in

data from both LIGO and Virgo during our preliminary analysis » We have shared what we currently know with astronomical

  • bserving partners.
  • We are working hard to assure that the candidates are valid

gravitational-wave events » It will require time to establish the level of confidence needed to bring any results to the scientific community and the greater public

  • We will let you know as soon we have information ready to share

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Working toward multi-messenger astronomy with gravitational waves

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Sw ift

LIGO Livingston Virgo

t1 t2 t3

X-ray, g-ray follow-up Optical follow-up

Coherent Detector Network

Image: http://earthobservatory.nasa.gov/

Swift

Palomar Transient Factory

  • About 95 Partners

from 19 countries

  • ~150 instruments

covering the full spectrum from radio to very high-energy gamma-rays

  • No EM anticipated for

black holes

  • Really profits from 3rd

detector….

Abadie, et al, (LSC & Virgo Collaborations)

  • Astron. Astrophys. 541 (2012) A155.

Nissanke, Kalsiwal, Georgieva, Astrophysical J. 767 (2013) 124. Singer, Price, et al., Astrophysical J., 795 (2014) 105.

LIGO Hanford

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The advanced GW detector network

Advanced LIGO Hanford, Livingston 2015 Advanced Virgo 2017 LIGO-India 2024 KAGRA 2019

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Contrast of Electromagnetic vs. Gravitational Waves

  • Visible, IR, Xray

» High spatial resolution » Relatively small masses radiating (atoms!) » Exterior surface of astronomical objects » Masked and scattered by intervening matter » 1/r2 fall-off

  • Gravitational waves:

» Low spatial resolution » Coherent motion of Huge masses » Deep interior of objects – where the mass is » No masking or scattering » 1/r fall-off

Wonderfully complementary information

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What does the near-term future hold?

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First Detection Sensitivity/configuration: 2 detectors, 1/3 goal sensitivity ~3 signals in 4 months of observation

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2017 Sensitivity/configuration: 3 detectors (Virgo joined 1 August), predict ~1-2 signals per month of observation

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And then a year break between O2 and O3 to bring the instruments to better sensitivity

Virgo:

  • Monolithic suspensions
  • Vacuum upgrade for dust protection
  • High power laser
  • Squeezing
  • Newtonian noise test installation
  • à ~Factor 2 network sensitivity

improvement

  • à ~Factor 8 greater signal rate

LIGO:

  • Scattered light mitigation
  • High power laser
  • Optics replacements
  • Squeezing

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Possible improvements in

  • ne of the LIGO detectors
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2018-19 Sensitivity/configuration: 3 detectors, ~2-3 signals per week

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2024 Sensitivity/configuration: 5 detectors (add India and Japan) far improved source localization

~60% in 10 sq deg 2022

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…and this is just the beginning!