instrument

interferometer

An interferometer is an instrument that measures physical quantities by analyzing interference patterns of waves.
21 related articles

Description

The interferometer is like a clever detective that investigates the difference in the paths of two beams. Imagine you and your friend running towards each other from opposite ends of a maze; when you meet, you can tell who ran slower by how out of breath you are. The interferometer 'sees' even a difference of a thousandth of the thickness of a hair — by how the light and dark fringes shift, like sand in an hourglass.

History

Interference phenomena were observed by Newton ('Newton's rings'), but systematic study began with Thomas Young in 1801 (double-slit experiment). The first interferometer was built by Albert Michelson in 1881 to test the hypothesis of the luminiferous ether. The famous Michelson-Morley experiment (1887) showed with the highest accuracy the absence of ether wind, which became a decisive argument for the constancy of the speed of light. In the mid-20th century, Joseph Weber built resonant gravitational antennas, but did not achieve decisive success. Modern laser interferometers (LIGO, Virgo) were proposed in the 1970s-80s and in 2015 for the first time directly detected gravitational waves (from the merger of black holes). Robert Hooke in 1665 described the colors of thin films, which was a manifestation of interference. Alain Aspect used interferometers in pioneering experiments on photon entanglement.

How it works

In the Michelson interferometer, light from a laser hits a beam splitter, where half the intensity is reflected into a perpendicular arm, and half passes straight through. At the end of each arm, a mirror reflects the beam back. After returning, both beams partially pass through the beam splitter and reach a photodetector. The phase difference Δφ = 2πΔL/λ determines whether interference is constructive (light) or destructive (dark). The intensity of the detected light is described by the formula I = I₁+I₂+2√(I₁I₂)cos(Δφ). Any slightest change in ΔL (due to gravitational waves, thermal expansion, or vibrations) leads to a change in the signal. To enhance sensitivity, Fabry-Perot cavities are installed in the arms, greatly increasing the effective light path. Maxwell's equations guarantee the constancy of the speed of light, allowing interferometry to be used as a 'ruler' of exceptional precision.

Fun fact

The giant LIGO interferometers can detect a change in the length of their four-kilometer arms of less than one ten-thousandth the size of a proton — about the same as if the distance from Earth to the Sun changed by the thickness of a human hair!

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