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LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory Reported on behalf of LIGO colleagues by Fred Raab, LIGO Hanford Observatory

LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

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Page 1: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO-G030184-00-W

"Colliding Black Holes"

Credit:National Center for Supercomputing Applications (NCSA)

The Laser Interferometer Gravitational-Wave Observatory

Reported on behalf of LIGO colleagues by

Fred Raab,

LIGO Hanford Observatory

Page 2: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 2LIGO-G030184-00-W

The spirit of exploration did not end 200 years

ago. A new age of

discovery is beginning

with LIGO…

Snake River

Corps of Discovery detour

Columbia River

LIGO

Yakima River

Page 3: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 3LIGO-G030184-00-W

LIGO’s Mission is to Open a New Portal on the Universe

In 1609 Galileo viewed the sky through a 20X telescope and gave birth to modern astronomy» The boost from “naked-eye” astronomy revolutionized humanity’s

view of the cosmos» Ever since, astronomers have “looked” into space to uncover the

natural history of our universe

LIGO’s quest is to create a radically new way to perceive the universe, by directly listening to the vibrations of space itself

LIGO consists of large, earth-based, detectors that will act like huge microphones, listening for the most violent events in the universe

Page 4: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 4LIGO-G030184-00-W

LIGO (Washington) LIGO (Louisiana)

The Laser InterferometerGravitational-Wave Observatory

Brought to you by the National Science Foundation; operated by Caltech and MIT; the research focus for more than 400 LIGO Science Collaboration members worldwide.

Page 5: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 5LIGO-G030184-00-W

LIGO Laboratories Are Operated as National Facilities in the US…

Page 6: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 6LIGO-G030184-00-W

Part of Future International Detector Network

LIGO

Simultaneously detect signal (within msec)

detection confidence locate the sources

decompose the polarization of gravitational waves

GEO VirgoTAMA

AIGO

Page 7: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 7LIGO-G030184-00-W

Big Question: What is the universe like now and what is its future?

New and profound questions exist after nearly 400 years of optical astronomy» 1850’s Olber’s Paradox: “Why is the night sky dark?”» 1920’s Milky Way discovered to be just another galaxy» 1930’s Hubble discovers expansion of the universe» mid 20th century “Big Bang” hypothesis becomes a theory, predicting

origin of the elements by nucleosynthesis and existence of relic light (cosmic microwave background) from era of atom formation

» 1960’s First detection of relic light from early universe» 1990’s First images of early universe made with relic light» 2003 High-resolution images imply universe is 13.7 billion years old and

composed of 4% normal matter, 24% dark matter and 72% dark energy; 1st stars formed 200 million years after big bang.

We hope to open a new channel to help study this and other mysteries

Page 8: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 8LIGO-G030184-00-W

A Slight Problem

Regardless of what you see on Star Trek, the vacuum of interstellar space does not transmit conventional

sound waves effectively.

Don’t worry, we’ll work around that!

Page 9: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 9LIGO-G030184-00-W

John Wheeler’s Picture of General Relativity Theory

Page 10: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 10LIGO-G030184-00-W

General Relativity: A Picture Worth a Thousand Words

Page 11: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 11LIGO-G030184-00-W

New Wrinkle on Equivalencebending of light

Not only the path of matter, but even the path of light is affected by gravity from massive objects

First observed during the solar eclipse of 1919 by Sir Arthur Eddington, when the Sun was silhouetted against the Hyades star cluster

Measurements showed that the light from these stars was bent as it grazed the Sun, by the exact amount of Einstein's predictions.

A massive object shifts apparent position of a star

The light never changes course, but merely follows the curvature of space. Astronomers now refer to this displacement of light as gravitational lensing.

Page 12: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 12LIGO-G030184-00-W

Einstein’s Theory of Gravitation…at work

“Einstein Cross”The bending of light rays

gravitational lensing

Quasar image appears around the central glow formed by nearby galaxy. The Einstein Cross is only visible in southern hemisphere.

In modern astronomy, such gravitational lensing images are used to detect a ‘dark matter’ body as the central object

Photo credit: NASA and ESA

Page 13: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 13LIGO-G030184-00-W

Gravitational Waves

Gravitational waves are ripples in space when it is stirred up by rapid motions of large concentrations of matter or energy

Rendering of space stirred by two orbiting black holes:

Page 14: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO-G030184-00-W

What Phenomena Do We Expect to Study With LIGO?

Page 15: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 15LIGO-G030184-00-W

Gravitational Collapse and Its Outcomes Present LIGO Opportunities

fGW > few Hz accessible from earth

fGW < several kHz interesting for compact objects

Page 16: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 16LIGO-G030184-00-W

Supernovae

time evolution

The Brilliant Deaths of Stars

Images from NASA High EnergyAstrophysics Research Archive

Page 17: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 17LIGO-G030184-00-W

The “Undead” Corpses of Stars:Neutron Stars and Black Holes

Neutron stars have a mass equivalent to 1.4 suns packed into a ball 10 miles in diameter, enormous magnetic fields and high spin rates

Black holes are even more dense, the extreme edges of the space-time fabric

Artist: Walt Feimer, Space Telescope Science Institute

Page 18: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 18LIGO-G030184-00-W

Catching WavesFrom Black Holes

Sketches courtesy of Kip Thorne

Page 19: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 19LIGO-G030184-00-W

Gravitational Waves the evidence

Neutron Binary System – Hulse & Taylor

PSR 1913 + 16 -- Timing of pulsars

17 / sec

Neutron Binary System• separated by 106 miles• m1 = 1.4m; m2 = 1.36m; = 0.617

Prediction from general relativity• spiral in by 3 mm/orbit• rate of change orbital period

~ 8 hr

Emission of gravitational waves

Page 20: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO-G030184-00-W

How does LIGO detect spacetime vibrations?

Leonardo da Vinci’s Vitruvian man

Page 21: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 21LIGO-G030184-00-W

Basic Signature of Gravitational Waves

Page 22: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 22LIGO-G030184-00-W

Power-Recycled Fabry-Perot-Michelson Interferometer

suspended mirrors markinertial frames

antisymmetric portcarries GW signal

symmetric port carriescommon-mode info, like shifts in laser frequency, intensity

Page 23: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 23LIGO-G030184-00-W

How Small is 10-18 Meter?

Wavelength of light, about 1 micron100

One meter, about a yard

Human hair, about 100 microns000,10

LIGO sensitivity, 10-18 meter000,1

Nuclear diameter, 10-15 meter000,100

Atomic diameter, 10-10 meter000,10

Page 24: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 24LIGO-G030184-00-W

Some of the Technical Challenges

Typical Strains < 10-21 at Earth ~ 1 hair’s width at 4 light years

Understand displacement fluctuations of 4-km arms at the millifermi level (1/1000th of a proton diameter)

Control arm lengths to 10-13 meters RMS Detect optical phase changes of ~ 10-10 radians Hold mirror alignments to 10-8 radians Engineer structures to mitigate recoil from atomic

vibrations in suspended mirrors

Page 25: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 25LIGO-G030184-00-W

What Limits Sensitivityof Interferometers?

• Seismic noise & vibration limit at low frequencies

• Atomic vibrations (Thermal Noise) inside components limit at mid frequencies

• Quantum nature of light (Shot Noise) limits at high frequencies

• Myriad details of the lasers, electronics, etc., can make problems above these levels

Page 26: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 26LIGO-G030184-00-W

Vibration Isolation Systems

» Reduce in-band seismic motion by 4 - 6 orders of magnitude» Little or no attenuation below 10Hz» Large range actuation for initial alignment and drift compensation» Quiet actuation to correct for Earth tides and microseism at 0.15 Hz during

observation

HAM Chamber BSC Chamber

Page 27: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 27LIGO-G030184-00-W

Seismic Isolation – Springs and Masses

damped springcross section

Page 28: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 28LIGO-G030184-00-W

Seismic System Performance

102

100

10-2

10-4

10-6

10-8

10-10

Horizontal

Vertical

10-6

HAM stackin air

BSC stackin vacuum

Page 29: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 29LIGO-G030184-00-W

Core Optics

Substrates: SiO2

» 25 cm Diameter, 10 cm thick

» Homogeneity < 5 x 10-7

» Internal mode Q’s > 2 x 106

Polishing» Surface uniformity < 1 nm rms

» Radii of curvature matched < 3%

Coating» Scatter < 50 ppm

» Absorption < 2 ppm

» Uniformity <10-3

Production involved 6 companies, NIST, and LIGO

Page 30: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 30LIGO-G030184-00-W

Core Optics Suspension and Control

Shadow sensors & voice-coil actuators provide

damping and control forces

Mirror is balanced on 30 microndiameter wire to 1/100th degree of arc

Optics suspended as simple pendulums

Page 31: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 31LIGO-G030184-00-W

Feedback & Control for Mirrors and Light

Damp suspended mirrors to vibration-isolated tables» 14 mirrors (pos, pit, yaw, side) = 56 loops

Damp mirror angles to lab floor using optical levers» 7 mirrors (pit, yaw) = 14 loops

Pre-stabilized laser» (frequency, intensity, pre-mode-cleaner) = 3 loops

Cavity length control» (mode-cleaner, common-mode frequency, common-arm, differential

arm, michelson, power-recycling) = 6 loops

Wave-front sensing/control» 7 mirrors (pit, yaw) = 14 loops

Beam-centering control» 2 arms (pit, yaw) = 4 loops

Page 32: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 32LIGO-G030184-00-W

Suspended Mirror Approximates a Free Mass Above Resonance

Data taken using shadow

sensors & voice coil actuators

Blue: suspended mirror XF

Cyan: free mass XF

Page 33: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 33LIGO-G030184-00-W

IO

Frequency Stabilization of the Light Employs Three Stages

Pre-stabilized laser delivers light to the long mode cleaner

• Start with high-quality, custom-built Nd:YAG laser

• Improve frequency, amplitude and spatial purity of beam

Actuator inputs provide for further laser stabilization

• Wideband• Tidal

10-WattLaser

PSL Interferometer

15m4 km

Page 34: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 34LIGO-G030184-00-W

Pre-stabilized Laser (PSL)

Custom-built10 W Nd:YAG Laser,

joint development with Lightwave Electronics

(now commercial product)

Frequency reference cavity (inside oven)

Cavity for defining beam geometry,

joint development withStanford

Page 35: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 35LIGO-G030184-00-W

Interferometer Length Control System

•Multiple Input / Multiple Output

•Three tightly coupled cavities

•Ill-conditioned (off-diagonal) plant matrix

•Highly nonlinear response over most of phase space

•Transition to stable, linear regime takes plant through singularity

•Employs adaptive control system that evaluates plant evolution and reconfigures feedback paths and gains during lock acquisition

Page 36: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 36LIGO-G030184-00-W

Digital Interferometer Sensing & Control System

Page 37: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 37LIGO-G030184-00-W

Digital Controls screen example A

nal

og

In

An

alo

g O

ut

Digital calibration input

Page 38: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 38LIGO-G030184-00-W

Why is Locking Difficult?

One meter

Human hair, about 100 microns000,10

Wavelength of light, about 1 micron100

LIGO sensitivity, 10-18 meter000,1

Nuclear diameter, 10-15 meter000,100

Atomic diameter, 10-10 meter000,10

Earthtides, about 100 microns

Microseismic motion, about 1 micron

Precision required to lock, about 10-10 meter

Page 39: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 39LIGO-G030184-00-W

Tidal Compensation Data

Tidal evaluation on 21-hour locked section of S1 data

Residual signal on voice coils

Predicted tides

Residual signal on laser

Feedforward

Feedback

Page 40: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 40LIGO-G030184-00-W

Microseism: Effect of Ocean Waves

Trended data (courtesy of Gladstone High School) shows large variability of microseism, on several-day- and annual- cycles

Reduction by feed-forward derived from seismometers

Microseism at 0.12 Hz dominates ground velocity

Page 41: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 41LIGO-G030184-00-W

Commissioning Time Line

Page 42: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 42LIGO-G030184-00-W

Noise Equivalent Strain Spectra for S1

Page 43: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 43LIGO-G030184-00-W

Background Forces in GW Band = Thermal Noise ~ kBT/mode

Strategy: Compress energy into narrow resonance outside band of interest require high mechanical Q, low friction

xrms 10-11 mf < 1 Hz

xrms 210-17 mf ~ 350 Hz

xrms 510-16 mf 10 kHz

Page 44: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 44LIGO-G030184-00-W

Thermal Noise Observed in 1st Violins on H2, L1 During S1

~ 20 millifermi RMS for each

free wire segment

Page 45: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 45LIGO-G030184-00-W

Binary Neutron Stars:S1 Range

Image: R. Powell

Page 46: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 46LIGO-G030184-00-W

LIGO Sensitivity Over TimeLivingston 4km Interferometer

May 01

Jan 03

Page 47: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 47LIGO-G030184-00-W

Binary Neutron Stars:S2 Range

Image: R. Powell

S1 Range

Page 48: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 48LIGO-G030184-00-W

Binary Neutron Stars:Initial LIGO Target Range

Image: R. Powell

S2 Range

Page 49: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 49LIGO-G030184-00-W

What’s next? Advanced LIGO…Major technological differences between LIGO and Advanced LIGO

Initial Interferometers

Advanced Interferometers

Open up wider band

ReshapeNoise

Quadruple pendulum

Sapphire optics

Silica suspension fibers

Advanced interferometry

Signal recycling

Active vibration isolation systems

High power laser (180W)

40kg

Page 50: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 50LIGO-G030184-00-W

Binary Neutron Stars:AdLIGO Range

Image: R. Powell

LIGO Range

Page 51: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 51LIGO-G030184-00-W

…and opening a new channel with a detector in space.

Planning underway for space-based detector, LISA, to open up a lower frequency band ~ 2015

SpaceTerrestrial

Page 52: LIGO-G030184-00-W "Colliding Black Holes" Credit: National Center for Supercomputing Applications (NCSA) The Laser Interferometer Gravitational-Wave Observatory

LIGO 52LIGO-G030184-00-W

Despite a few difficulties, science runs started in 2002.