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What are gravitational waves, and how do we detect them?

Laser beams and the pulse times of distant stars reveal tiny, traveling changes in space and time.

THE SHORT ANSWER

Gravitational waves are traveling changes in space and time that very slightly stretch and squeeze distances. Laser detectors compare light paths in two long arms to measure them. Astronomers also time pulses from many spinning stellar remnants to look for much slower waves. Agreement across detectors or across pulsar pairs, together with careful noise checks, separates a cosmic signal from disturbances in the measuring system.

  • Gravitational waves can travel through empty space at the speed of light.
  • LIGO measures tiny relative changes in two laser paths.
  • Distant detectors help distinguish a shared cosmic signal from local noise.
  • Pulsar timing searches for a shared pattern of early and late pulse arrivals across many stars.
  • Black-hole chirps are wave measurements converted into sound, sometimes with the pitch changed.
A laser beam splits into two perpendicular four-kilometer arms, reflects from mirrors and recombines at a photodetector; insets show the two U.S. sites and noise curves.
About this picture

Simplified Advanced LIGO detector diagram, not to scale · Insets show site locations and historical noise-sensitivity curves from the first detection’s 2016 paper. The curves are not an event waveform, and the labeled powers are not a statement of current hardware settings.

B. P. Abbott et al. (LIGO Scientific Collaboration and Virgo Collaboration), Physical Review Letters 116, 061102 (2016), Fig. 3 · CC BY 3.0 · Image source ↗

WHERE THE EVIDENCE STANDS

How sure are we?

  • Passing gravitational waves can be measured through tiny changes in light paths.Abbott et al.’s 2016 GW150914 paper reports the measured signal, detector response, calibration and validation checks.
  • Agreement across widely separated detectors helps test whether a signal is local noise.LIGO’s FAQ and the GW150914 paper describe environmental sensors, detector comparisons and estimates of false coincidences.
  • A black-hole chirp is sound that traveled through space from the collision.The Gravitational Wave Open Science Center explains that the wave data are converted into audio; gravitational waves themselves are not sound.
  • Giant black-hole pairs are a leading source of the slow wave background studied through pulsar timing.Agazie et al.’s 2023 paper finds the expected pulsar-pair correlations, consistent with a giant black-hole population, while explicitly leaving other source interpretations open.
What the labels mean

WHAT WE DON’T KNOW YET

The exact mix of sources behind the very slow gravitational-wave background is still being studied. A background signal does not identify each individual black-hole pair.

WHAT WOULD CHANGE THIS ANSWER

A stronger explanation for the same signals would need to match the measured patterns and survive the detector and noise checks. More pulsar data and better models can change what we infer about the slow background’s sources without undoing the established laser detections.

Gravitational waves are small, traveling changes in space and time. As a wave passes, distances can stretch in one direction and shrink in another. Scientists detect these changes with laser beams on Earth and, for much slower waves, with pulses from distant stars. The waves are real; they have been measured.

Picture dots drawn in a circle that briefly becomes a tall oval, then a wide one. That is a sketch of one simple wave pattern, not a picture of material floating through space. Space and time are not a sheet of cloth. The useful part of the sketch is the changing distance between the dots.

LIGO uses two long arms at right angles. Laser light travels along both, reflects from mirrors and comes back together. A passing wave changes the two light paths by tiny, different amounts. The way the returning light combines reveals that change. One detector alone has a harder job telling a cosmic signal from a local disturbance, so scientists compare distant instruments and their noise records.

The famous black-hole “chirp” is this measured pattern turned into sound for our ears. It is not a microphone recording sound crossing empty space. As two black holes spiral together, their wave pattern speeds up. Playing that pattern through a speaker makes the pitch rise.

Other waves change too slowly for that approach. Astronomers instead track the regular radio pulses of many spinning stellar remnants called pulsars. A wave can make those pulses arrive slightly early or late. The test is a shared pattern across stars in different directions, not one late tick. Laser detectors and pulsar timing study different parts of the same physical phenomenon.

THE LONG ANSWER

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Words worth knowing (6)
Spacetime
Space and time considered together; gravity can change their geometry.
Interference
The way overlapping waves combine, adding together or partly canceling.
Strain
A change in distance compared with the original distance; a measure of a gravitational wave’s strength.
Pulsar
A spinning neutron star whose beam sweeps past us, producing repeated pulses.
Pulsar timing array
Many pulsars observed together so their pulse times can be compared for a shared wave pattern.
Gravitational-wave background
A combined wave signal from many unresolved sources, rather than one separately identified event.

Sources & further reading

(10) · Checked Oct 2, 2026
  1. Hubble Gravity Waves ↗NASA ScienceTraveling spacetime changes, light-speed propagation and stretching/squeezing. Used for the basic physical picture, not its speculative early-universe examples.
  2. What is LIGO? ↗LIGO Laboratory, Caltech/MITThe two U.S. sites, about 3,000 km separation, perpendicular four-kilometer arms and vacuum tubes. No current event counts or localization totals used.
  3. LIGO’s Interferometer ↗LIGO Laboratory, Caltech/MITSplit and recombined laser beams, repeated reflections and noise isolation. No simple dark-port idealization presented as an exact current operating description.
  4. Frequently Asked Questions ↗LIGO Laboratory, Caltech/MITInstrumental and environmental noise monitoring, isolated mirrors and separated-detector checks. Historical or outdated detection totals are not used.
  5. Observation of Gravitational Waves from a Binary Black Hole Merger ↗B. P. Abbott et al., LIGO Scientific Collaboration and Virgo Collaboration; Physical Review Letters 116, 061102 (2016)Public full paper, DOI 10.1103/PhysRevLett.116.061102. GW150914 date, detector response (Fig. 3), detector validation and independent searches/time-shift false-coincidence estimates (Secs. III–V).
  6. Audio Files ↗Gravitational Wave Open Science CenterGravitational waves versus sound, processed measured data, model clips and shifted-frequency audio. No claim that speakers reproduce sound traveling from the source.
  7. Pulsars ↗NASA ScienceRotating neutron-star remnants, radiation beams and the lighthouse pulse picture. No current pulsar inventory or rotation record used.
  8. Low-Frequency Gravitational Waves ↗NANOGrav CollaborationPulsar timing probes different frequencies and source scales; wave periods of months to decades. Source populations are not treated as uniquely identified.
  9. Detector Characterization and Noise Budget ↗NANOGrav CollaborationPublic companion-paper summary: radio propagation through ionized gas, pulsar behavior, clocks and solar-system modeling affect pulse arrival times. No pulsar-count or precision figure used.
  10. The NANOGrav 15-year Data Set: Evidence for a Gravitational-Wave Background ↗G. Agazie et al., NANOGrav Collaboration; The Astrophysical Journal Letters 951, L8 (2023)Public full author paper, DOI 10.3847/2041-8213/acdac6. Expected angular correlations, timing/noise models, robustness checks and unresolved source interpretation. This is the specific 2023 result, not a claim to summarize the latest data release.

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