Cepheids: Why Does Their Luminosity Vary So Regularly?
The bright star of the southern hemisphere RS Puppis (at the center of the image) is wrapped in a cocoon of dust that reflects its light. This Cepheid of about 9 to 10 solar masses is roughly 200 times larger than the Sun and about 15,000 times more luminous.
Its brightness increases and decreases rhythmically over a cycle of about 41.5 days, nearly six weeks.
Image source: NASA, ESA and the Hubble Heritage Team (STScI/AURA) – Hubble/Europe Collaboration (new window). Acknowledgments: H. Bond (STScI and Penn State University).
Scientific summary
The Astronoo article presents Cepheids, evolved pulsating stars whose brightness varies periodically, linked to oscillations in size and temperature. The period-luminosity relation, published in 1912 from the work of Henrietta Swan Leavitt (1868-1921), allows their intrinsic luminosity, and therefore their distance, to be deduced. The article describes the physical mechanism of the helium ionization zone instability (κ mechanism), the contraction-expansion cycle, and then the historical role of Cepheids in proving that spiral nebulae are external galaxies (observations by Edwin Hubble in 1923-1925). It also reviews recent calibrations, with Gaia and the James Webb Space Telescope, and the place of Cepheids in the tension over the Hubble constant. Finally, RS Puppis illustrates these pulsations through Hubble observations.
Why do Cepheids pulsate?
A hidden engine in the star's envelope
Cepheids are variable stars whose brightness increases and decreases at a regular rhythm, from about one day to more than two months. Their pulsation is due to their internal structure. In a layer of the envelope, helium is partially ionized. When the star contracts, this zone becomes more opaque and retains energy, which pushes the envelope outward. As it expands, the star cools, the helium recombines, the opacity decreases, the energy escapes and the star falls back. The cycle begins again with great regularity.
A clock that reveals luminosity
The duration of the period is directly linked to the star's intrinsic luminosity: the longer the period, the more luminous the Cepheid. This period-luminosity relation, published in 1912 from the work of Henrietta Swan Leavitt, transformed Cepheids into standard candles. By comparing their apparent luminosity, observed from Earth, with their true luminosity, astronomers deduce their distance.
A decisive role in the history of cosmology
This method allowed Edwin Hubble to show, between 1923 and 1925, that the "nebula" of Andromeda and other spiral nebulae were indeed far beyond the Milky Way. Cepheids thus constitute the first rung of the cosmic distance ladder based on standard candles, before other indicators such as type Ia supernovae. Even today, their observation with Hubble and the James Webb Space Telescope is at the heart of measuring the expansion of the Universe and the debate over the Hubble tension.
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What is a Cepheid?
Definition and astronomical role
Cepheids are pulsating variable stars whose luminosity varies periodically due to changes in their size and temperature. These stars are essential in astrophysics because they allow astronomical distances to be measured, both in our galaxy and in nearby galaxies, thanks to the period-luminosity relation. This relation was discovered by the American astronomer Henrietta Swan Leavitt at the beginning of the 20th century. The name of these stars comes from δ Cephei (delta Cephei), in the constellation Cepheus, whose variability was discovered in 1784 by the British astronomer John Goodricke (1764-1786).
Two main families
- Classical Cepheids (population I): young, massive and very luminous stars, located mainly in the spiral arms of galaxies. Their periods range from about 1.5 days to more than 50 days. They follow the period-luminosity relation most used to measure distances.
- Type II Cepheids (population II): much older, less massive and less luminous stars (W Virginis and BL Herculis types, among others). They obey a different period-luminosity relation and are less useful as distance indicators.
Some famous Cepheids
- δ Cephei: the prototype of the class, whose variability has been known since 1784.
- Polaris (the North Star): the closest Cepheid to us, at about 430 light-years. Its period is about four days, and its brightness variations are very small.
- RS Puppis: a massive and very luminous Cepheid, surrounded by a dust nebula, presented below.
Characteristics of Cepheids
Variability and period-luminosity relation
- Variability: Cepheids see their luminosity vary regularly over periods ranging from about one day to more than two months. The known record in the Milky Way, identified in 2024, is 78.1 days. This variation is due to oscillations in the star's internal structure.
- Period-luminosity relation: Henrietta Leavitt (1868-1921) showed that the longer the period of variation of a Cepheid, the higher its intrinsic luminosity. In other words, the absolute magnitude of a Cepheid is directly linked to the period of its oscillations.
What is observed during a cycle
During a cycle, the star changes in size, temperature and therefore color. It goes from a spectral type F (hotter) at maximum brightness to a type G (cooler, like the Sun) at minimum. These stars are yellow giants or supergiants.
Methods for calculating distances in the Universe
The following table compares the main methods of measuring cosmic distances. It shows why Cepheids occupy the first rung of the extragalactic distance ladder: they extend stellar parallax and serve to calibrate more distant indicators.
| Method | Range of validity | Principle | What is measured | Main limitations | Place in the distance ladder |
|---|---|---|---|---|---|
| Stellar parallax | A few parsecs to a few kiloparsecs | Apparent displacement of a star in the sky during Earth's orbit | Parallax angle | Limited precision beyond the Milky Way | Geometric base that calibrates the first rungs |
| Cepheids | A few kiloparsecs to several tens of megaparsecs | Period-luminosity relation: long period = intrinsically more luminous star | Pulsation period and apparent magnitude | Requires precise calibration; possible confusion with other variables | First extragalactic rung: links parallax to nearby galaxies |
| RR Lyrae | Milky Way and nearby galaxies | Tighter period-luminosity relation, older stars | Period and apparent magnitude | Less luminous than Cepheids | Complementary rung for globular clusters and dwarf galaxies |
| Type Ia supernovae | Up to several hundred megaparsecs | Thermonuclear explosion of a white dwarf, standardizable maximum luminosity | Light curve and apparent magnitude | Rare events; calibration dependent on Cepheids | Distant rung, calibrated by Cepheids |
| Tully-Fisher | Distant spiral galaxies | Correlation between rotation speed and galaxy luminosity | Width of spectral lines and apparent magnitude | Large dispersion; depends on galaxy type | Independent rung for large scales |
| Hubble's law | Very large cosmological distances | Recession velocity proportional to distance | Redshift and Hubble constant | Requires absolute calibration | Final rung, calibrated by the previous ones |
The discovery of Henrietta Swan Leavitt
Photographic plates of the Magellanic Clouds
Henrietta Swan Leavitt worked at the Harvard Observatory, where she examined photographic plates of the Magellanic Clouds, taken in particular from the Arequipa station in Peru. In 1908, she published a catalog of 1,777 variable stars in the two Clouds, including several dozen Cepheids. In 1912, a short article, signed by Edward Pickering but "prepared by Miss Leavitt", gave the periods of 25 Cepheids in the Small Magellanic Cloud. Her fundamental discovery is the period-luminosity relation: stars whose period of variation is longer are intrinsically brighter.
From relative scale to absolute distances
Since the stars of the Small Cloud are at roughly the same distance from us, their apparent brightness reflected their relative luminosities. Leavitt could not determine the absolute distances of these stars, but she provided an extremely precise relative scale. It remained to fix its zero point. As early as 1913, Ejnar Hertzsprung attempted to calibrate it from Cepheids in the Milky Way, and then Harlow Shapley refined this calibration in 1918. This opened the way to estimating the distances of galaxies and to understanding the scale of the Universe.
Physics of Cepheids
Evolved stars in the instability strip
Classical Cepheids are evolved stars of intermediate to high mass (on the order of 4 to 20 solar masses). They have left the main sequence of the Hertzsprung-Russell diagram (a graph that links the intrinsic luminosity of stars to their surface temperature) and cross the instability strip, a narrow region of the diagram where the envelope becomes capable of sustaining radial pulsations. In this type of pulsation, the star remains spherical and swells and contracts as a whole.
Helium zone instability (κ mechanism)
The variability of Cepheids is due to a process called "helium zone instability". In certain layers of these stars, helium is partially ionized (He+ and He2+ coexist), which affects the transparency to heat (opacity). This is also called the κ mechanism, from the Greek letter that designates opacity. The idea that these stars pulsate, rather than being binary stars, became established in the 1910s with the work of Shapley and Eddington. The identification of the helium ionization zone as the driving engine of the pulsation dates from the 1950s-1960s.
Contraction-expansion cycle
- Contraction phase: when the star contracts, the temperature increases and helium becomes more ionized. The layer becomes more opaque and retains energy instead of letting it pass. This accumulation of energy raises the pressure and makes the star swell.
- Expansion phase: when the star expands, it cools and helium recombines into a less ionized state. The opacity decreases, which allows energy to escape. The pressure drops, gravity takes over again, the star contracts once more and the cycle begins again.
Regularity of pulsations
This pulsation cycle is very regular, which allows the precise relation between period and luminosity. As with the note of a musical instrument, the period depends on the size of the star: it varies as the inverse of the square root of its mean density (P ∝ ρ−1/2).
Why does the period give the luminosity?
The instability strip covers a narrow temperature interval. The luminosity of a Cepheid therefore depends mainly on its radius, itself linked to its mass by stellar evolution. A more luminous star is larger, therefore less dense on average, therefore slower to pulsate. This is what links the period to the luminosity.
Importance of the discovery
Hubble and external galaxies
At the Mount Wilson Observatory, with the 2.5 m telescope, Edwin Hubble (1889-1953) spotted in October 1923 a Cepheid (named V1) on a photographic plate of the "nebula" of Andromeda. Thanks to the period-luminosity relation, he obtained a distance of about 900,000 light-years, far greater than the dimensions then accepted for the Milky Way. Cepheids observed in M33 and NGC 6822 confirmed the result. His conclusions, presented to the American Astronomical Society on January 1, 1925 and published the same year, demonstrated that certain spiral nebulae are in reality galaxies external to the Milky Way. This discovery changed our understanding of the Universe, showing that it is much vaster than had been thought.
Baade and the doubling of distances
In 1952, the astronomer Walter Baade showed that there are two populations of Cepheids, which obey different period-luminosity relations. This correction multiplied the distances to external galaxies by about two. Andromeda is today at about 2.5 million light-years.
Calibrating Cepheids: from Gaia to the James Webb Space Telescope
Gaia and the zero point
For the period-luminosity relation to give absolute distances, the true luminosity of nearby Cepheids must be known, and therefore their geometric distances. The parallaxes of ESA's Gaia satellite serve this calibration in the Milky Way. The third data release (Gaia DR3, June 2022) contains light curves for 15,006 Cepheids of all types: 5,221 in the field of the Milky Way and its small satellites, 4,663 in the Large Magellanic Cloud, 4,616 in the Small Magellanic Cloud, 321 in the Andromeda galaxy (M31) and 185 in the Triangulum galaxy (M33). Among them, 474 are probably new Cepheids discovered by Gaia.
Three geometric anchors
To fix the zero point, the SH0ES team combines three geometric references: Gaia parallaxes for Milky Way Cepheids, the masers of the galaxy NGC 4258, and the eclipsing binaries of the Large Magellanic Cloud.
Mapping the Milky Way
Classical Cepheids, young and very luminous, also allow the Milky Way to be mapped. The OGLE survey has placed about 2,400 of them on a map of our Galaxy. It also identified in 2024 the known galactic Cepheid with the longest period, OGLE-GD-CEP-1884, with 78.14 days, at about 4.5 kiloparsecs. It exceeds by about ten days the previous record, held by S Vulpeculae.
The James Webb Telescope tests crowding
In distant galaxies, the image of a Cepheid blends with that of neighboring stars. This crowding phenomenon could distort its luminosity, and therefore its distance. In the near infrared, where absorption by dust is low, the resolution of the James Webb Space Telescope is about 2.5 times better than that of Hubble. Over more than 1,000 Cepheids observed in NGC 4258 and five supernova host galaxies, the mean difference between Hubble and Webb measurements is −0.01 ± 0.03 magnitude (Riess et al. 2024). This result rules out crowding as an explanation of the Hubble tension, at about 8 σ. In 2025, the observation of a host galaxy almost devoid of background stars (NGC 3447) confirmed the absence of bias. Webb also reduces the dispersion of the period-luminosity relation.
Cepheids and the tension over the Hubble constant
Two values that do not agree
The Hubble constant, denoted H0, measures the current expansion rate of the Universe. Calibrated with Cepheids and then type Ia supernovae, the SH0ES team obtains H0 = 73.04 ± 1.04 km s−1 Mpc−1 (Riess et al. 2022). The cosmic microwave background observed by the Planck satellite, interpreted with the ΛCDM model, gives H0 = 67.4 ± 0.5. The discrepancy, of about 8%, reaches nearly 5 σ: this is the Hubble tension.
Recent results with James Webb (space telescope)
The SH0ES team published new results in 2025. With Cepheids observed by Webb in 19 host galaxies of 24 type Ia supernovae, it finds H0 = 73.49 ± 0.93. Adding calibrations by the tip of the red giant branch (TRGB), it obtains 73.18 ± 0.88.
Wendy Freedman's Chicago-Carnegie Hubble Program (CCHP) arrives at other values. With the tip of the red giant branch (TRGB) method alone and 24 calibrating supernovae, it obtains H0 = 70.39 ± 1.22 (statistical) ± 1.33 (systematic) ± 0.70 (supernovae). With Webb data alone, the TRGB method gives 68.81 ± 1.79 ± 1.32, and that of carbon stars of the asymptotic giant branch (JAGB) gives 67.80 ± 2.17 ± 1.64. Its authors consider these results compatible with the ΛCDM model, without new physics. They also note that the TRGB and JAGB distances agree to better than 1%, and with the Cepheid distances of SH0ES to a little more than 1%.
Sources of uncertainty to watch
- Crowding: tested with Webb, it does not seem to explain the tension.
- Absorption by dust: it reddens and weakens Cepheids, hence the interest of the infrared.
- Metallicity: the content of heavy elements can slightly modify the period-luminosity relation.
- The zero point: it depends on the parallaxes of Gaia, NGC 4258 and the Large Magellanic Cloud.
- The choice of galaxies and supernovae: small samples can shift the final value of H0.
N.B.:
This field is evolving very quickly. The values above are those published at the date of update of this article and the debate is not settled.
RS Puppis, a Cepheid surrounded by light echoes
A montage from Hubble observations
This video montage was made from observations of the Hubble Space Telescope. It shows the pulsations of the variable star RS Puppis and its environment of thick dark dust clouds. RS Puppis is a Cepheid in the constellation Puppis. The Hubble observations were taken over a period of five weeks in 2010, in order to capture the star at different stages of its 41.4-day cycle. Its brightness varies by a factor of nearly five. The short video is repeated several times to show the light echo mechanism more clearly.
The pulsations of RS Puppis are a striking example of a phenomenon called a light echo, where light seems to resonate through the misty environment around the star.
Image source: NASA, ESA, and the Hubble Heritage Team (STScI/AURA)-Hubble/Europe Collaboration (new window).
What is a light echo?
The dust surrounding RS Puppis allows a phenomenon known as a light echo to be observed with astonishing clarity. At each maximum of brightness, a wave of light propagates through the nebula. The light reflected by more distant dust layers travels a longer path and arrives later on Earth. This echo creates the illusion of clouds of gas expanding from RS Puppis, whereas no matter is moving in this way. It is somewhat the luminous equivalent of a sound echo.
A distance measured by the echo, then reconsidered
In 2008, Pierre Kervella and his colleagues used light echoes, observed with ESO's NTT telescope, to propose a purely geometric distance of 6,500 ± 90 light-years, presented as the most precise ever obtained for a Cepheid. In 2009, Howard Bond and William Sparks challenged this value. It assumed that the dust zones were located near the plane of the sky, whereas scattering favors light emitted forward and places most of the observed dust in front of the star. Hubble polarimetric images, taken in 2010 and analyzed in 2014, led to a distance of 1,910 ± 80 parsecs, or about 6,200 light-years. This value is compatible with other methods.
N.B.:
The value of 6,500 ± 90 light-years, often cited, should therefore be handled with caution: it claimed a precision of 1.4%, whereas the 2014 polarimetric measurement announces an uncertainty of about 4%.
From brightness to distance: the example of RS Puppis
The distance d (in parsecs) is deduced from the apparent magnitude m, corrected for interstellar absorption A, and the absolute magnitude M: m − A − M = 5 log10(d) − 5. For RS Puppis, the mean apparent magnitude in the visible is 7.12. The interstellar absorption is about 1.4 magnitude and the absolute visual magnitude is about −5.70. We obtain a distance modulus of 11.40, i.e. d ≈ 1,900 parsecs.
N.B.:
Here, the absolute magnitude is itself deduced from the geometric distance measured thanks to light echoes. The exercise illustrates the logic of the calculation. Above all, it shows that RS Puppis falls, to within about 1 σ, on the period-luminosity relation established with other Cepheids.
A massive Cepheid, but ephemeral in its nebula
RS Puppis is one of the most luminous Cepheids in the Milky Way, with a period of 41.5 days. It is the only known galactic Cepheid to be immersed in a large reflection nebula. This dust was not ejected by the star: it is an interstellar cloud that the Cepheid is traversing. Its strong luminosity could, within a few million years, dissipate the neighboring dust and make the light echoes disappear.
Knowing the distance of such a star with accuracy is important, because Cepheids serve as a marker (standard candle) for distances within our galaxy and nearby galaxies.
References
- Encyclopædia Britannica - Cepheid variable (new window)
- ESA/Hubble - RS Puppis (image heic1323a) (new window)
- ESA/Hubble - RS Puppis and the light echo (press release heic1323, 2013) (new window)
- NASA - Hubble watches RS Puppis (new window)
- ESO - Light echoes whisper the distance to a star (eso0805, 2008) (new window)
- NASA - Hubble and Gaia Measure Cepheid Variable Stars (new window)
- ESA - Comparison of Hubble and Webb views of a Cepheid variable star (new window)
FAQ: Everything you need to know about Cepheids
What is a Cepheid?
A Cepheid is a pulsating variable star whose luminosity varies regularly. Its period of variation is directly linked to its intrinsic luminosity, which makes it a tool for measuring cosmic distances.
Why do Cepheids pulsate?
Their pulsations come from the helium zone instability. When the star contracts, the partially ionized helium increases the opacity, retains energy and makes the star swell. When it expands, it cools, the opacity drops and the cycle begins again.
Why is the period linked to luminosity?
The period depends on the mean density of the star. A more luminous Cepheid is larger, therefore less dense, therefore slower to pulsate. Its period is then longer.
How does the period-luminosity relation measure distances?
By observing the period of a Cepheid, its absolute magnitude is deduced. By comparing this true luminosity with its apparent luminosity, its distance is calculated. The relation is calibrated using geometric measurements, such as Gaia parallaxes. This method is one of the first rungs of the cosmic distance ladder.
Who discovered the period-luminosity relation?
The relation was brought to light by the American astronomer Henrietta Swan Leavitt and published in 1912, thanks to the study of variable stars in the Magellanic Clouds.
What is the difference between a classical Cepheid and a type II Cepheid?
Classical Cepheids are young, massive and very luminous stars. Type II Cepheids are older, less massive and less luminous. They follow a different period-luminosity relation.
What is the closest Cepheid to us?
It is the North Star (Polaris), at about 430 light-years. Its period is about four days and its brightness variations are very small.
Are Cepheids still used today?
Yes. They remain essential for calibrating distances in the Milky Way and nearby galaxies, and for verifying measurements of the expansion rate of the Universe with the Hubble and James Webb space telescopes, as well as other observatories.
What is the Hubble tension?
It is the disagreement between the value of the Hubble constant measured in the nearby Universe with Cepheids and supernovae (about 73 km/s/Mpc) and that deduced from the cosmic microwave background with the ΛCDM model (about 67 km/s/Mpc). Other methods, such as that of the Chicago-Carnegie program, give intermediate values. The debate remains open.
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