Laser Interferometer Gravitational-Wave Observatory (LIGO)
A 4-kilometre ruler that measures the universe shrinking and stretching by less than one-thousandth the width of a proton.
LIGO detects gravitational waves — ripples in spacetime curvature — produced when massive objects accelerate. To date its primary sources have been merging pairs of black holes and neutron stars. Each detection encodes information about the objects' masses, spins, and distance that cannot be obtained by any electromagnetic telescope. LIGO has opened a new observational window on the universe: gravitational-wave astronomy.
Each LIGO interferometer is a power-recycled, signal-recycled Michelson interferometer with 4-km Fabry-Pérot arm cavities. A 200-W infrared laser (1064 nm) is injected into the system; a power-recycling mirror boosts the circulating laser power at the beam splitter, while the Fabry-Pérot cavities build up ~750 kW of optical power in each arm. The 40-kg fused-silica test mass mirrors are suspended on quadruple-pendulum chains that provide seismic isolation exceeding 10¹² above 10 Hz. The entire optical path resides inside a 10,000 m³ vacuum system maintained at 10⁻⁹ Torr, using 1.2-m-diameter beam tubes baked out to remove outgassed molecules. A passing gravitational wave differentially stretches one arm while compressing the other; the resulting differential length change shifts the interference fringe at the output. The fringe is held on the dark fringe by active feedback; the gravitational wave signal appears as the correction signal fed to the mirrors.
In plain terms
Imagine stretching a laser pointer beam to be four kilometres long, then bouncing it back and forth hundreds of times inside a mirror-lined tunnel. When a gravitational wave passes through — a ripple in the very fabric of space — the tunnel stretches by less than a trillionth of a millimetre, and the laser's interference pattern changes. That tiny flicker is the signal.
Also called: LIGO, Advanced LIGO, aLIGO, gravitational wave detector, GW observatory.
Why it matters
- First direct measurement of gravitational waves, confirming a central prediction of Einstein's general theory of relativity 100 years after it was made.
- First observational evidence for binary black hole systems; before GW150914, no direct evidence existed that stellar-mass black holes could pair and merge.
- GW170817, the binary neutron star merger detected alongside a gamma-ray burst, inaugurated multi-messenger astronomy and constrained the neutron star equation of state and the speed of gravitational waves to within 10⁻¹⁵ of the speed of light.
- LIGO and its partners (Virgo, KAGRA) had detected over 300 gravitational-wave candidate events by the end of O4 in November 2025, transforming compact-binary statistics from a handful of known systems to a population with measured mass and spin distributions.
- The 2017 Nobel Prize in Physics was awarded to Rainer Weiss, Barry Barish, and Kip Thorne for decisive contributions to LIGO and the observation of gravitational waves.
Where it lives
- LIGO Hanford Observatory (H1), Richland, Washington, USA — 4-km L-shaped interferometer
- LIGO Livingston Observatory (L1), Livingston, Louisiana, USA — 4-km L-shaped interferometer
- Virgo (V1), Cascina, Italy — 3-km interferometer, joined Advanced-network operations 2017
- KAGRA, Kamioka, Japan — 3-km cryogenic interferometer, joined O3 2020, O4 2023
- LIGO-India — planned 4-km interferometer in Aundha, Maharashtra, India; approvals granted 2023
Key numbers
- Arm length: 4 km (Each of the two perpendicular arms)
- Laser wavelength: 1064 nm (Nd:YAG, infrared)
- Arm cavity circulating power: ~750 kW (Advanced LIGO design at full power; 800 kW in older specs)
- Test mass: 40 kg fused silica (35 cm diameter, polished to sub-nm roughness)
- Vacuum pressure: 10⁻⁹ Torr (In 10,000 m³ volume; 1.2 m dia. beam tubes, 4 km long)
- Peak strain sensitivity: ~4 × 10⁻²⁴ Hz⁻¹/² (Advanced LIGO design goal at ~100 Hz)
- First detection (GW150914): h ≈ 10⁻²¹ (Peak strain, Sept. 14 2015; SNR 24)
- Total detections (O1–O4): ~300 candidates (O4 ended Nov. 2025; GWTC-4 covers O4a (128 new))
Surprising facts
- The strain amplitude of GW150914 peaked at h ≈ 10⁻²¹, meaning the 4-km arm stretched or compressed by roughly 4 × 10⁻¹⁸ m — about 1,000 times smaller than the diameter of a proton.
- The two black holes that produced GW150914 were each roughly 30 solar masses, merged at a distance of ~410 Mpc (~1.3 billion light-years), and radiated 3 solar masses of energy as gravitational waves in a fraction of a second.
- LIGO's 4-km beam tubes hold a vacuum at 10⁻⁹ Torr — one trillion times lower pressure than sea-level atmosphere — making them among the largest sustained ultra-high-vacuum volumes in the world at 10,000 cubic metres.
- During O4, the LIGO–Virgo–KAGRA network detected its 200th candidate gravitational-wave event in March 2025; the total by the end of O4 in November 2025 was on the order of 300 detections, most from binary black hole mergers.
Open questions
- Correlated noise between the two LIGO sites: Studies of the O2 and O3 data found low-level correlated noise power between the Hanford and Livingston detectors at frequencies below ~20 Hz. Some of this correlation is attributed to global magnetic field noise (Schumann resonances) and possibly correlated seismic fields, but its full characterisation remains incomplete. Unmodelled correlated noise can bias parameter estimation for long-duration or low-frequency signals and is one of the open engineering challenges for future detector generations.
A short history
Rainer Weiss at MIT outlined the laser interferometric gravitational wave detector concept in a 1972 Quarterly Progress Report, identifying the dominant noise sources and the path to sensitivity at 10⁻²¹ strain. Parallel prototype work by Ronald Drever's group at Glasgow and Caltech and by groups in Germany (Garching) and France/Italy (Virgo precursor) refined the cavity optics and seismic isolation through the 1980s. The formal LIGO proposal to NSF was submitted in 1989 by Drever, Raab, Thorne, Vogt, and Weiss; Congress approved funding in 1991. Construction of the Hanford site began in 1994 and Livingston in 1995. Initial LIGO (iLIGO) ran science operations from 2002 to 2010 without a detection. Advanced LIGO installation was completed in 2014, and on September 14, 2015 — during a pre-official engineering run of O1 — the two detectors recorded GW150914, the first gravitational wave detection, from a binary black hole merger at ~410 Mpc. The result was published in Physical Review Letters on February 11, 2016, and Weiss, Barish, and Thorne shared the 2017 Nobel Prize in Physics.
Sources
- Abbott et al. (LIGO Scientific Collaboration, Virgo Collaboration), Phys. Rev. Lett. 116, 061102 (2016) — GW150914 (https://journals.aps.org/prl/abstract/10.1103/PhysRevLett.116.061102)
- GWTC-3: Third Gravitational-Wave Transient Catalog, Phys. Rev. X 13, 041039 (2023) — 90 events through O3 (https://link.aps.org/doi/10.1103/PhysRevX.13.041039)
- LIGO Instrument Science White Paper 2022–2023, LIGO DCC T2200384 (https://dcc.ligo.org/public/0185/T2200384/002/Instrument_Science_White_Paper_2022.pdf)
- LIGO ultra-high vacuum system overview, Caltech LIGO Lab (https://www.ligo.caltech.edu/page/vacuum)
- Nobel Prize in Physics 2017 press release — Weiss, Barish, Thorne (https://www.nobelprize.org/prizes/physics/2017/press-release/)
- EGO / Virgo: 200th GW detection in O4 announced March 2025 (https://www.ego-gw.it/blog/2025/03/20/record-detection-of-200-gravitational-waves-in-the-current-run-of-ligo-virgo-and-kagra/)