General · EdgepediaOctober 15, 20267 min read

Epsilon Canis Majoris

Epsilon Canis Majoris (ε Canis Majoris, abbreviated ε CMa), commonly called Adhara, is a binary star system in the constellation Canis Major and the second-brightest star of that constellation despite carrying the fifth letter of the Greek alphabet, with an apparent visual magnitude of 1.50¹^•². Its primary is a hot blue-white bright giant of spectral type B2 II, and the system is the brightest known extrasolar source of extreme ultraviolet radiation between 504 Å and 760 Å¹. Because much of its output falls in the invisible ultraviolet, its visual brightness understates its total energy output³.

Key fact	Detail
Spectral type	B2 II, a blue bright giant between the giants and supergiants¹^•⁴
Apparent magnitude	1.50; second-brightest star in Canis Major¹
Distance	124 ± 2 pc by parallax (about 404 light-years); older catalogs list about 430 light-years⁵^•⁶
Physical parameters	Radius 10.7 ± 0.7 R☉, mass 13.1 ± 2.3 M☉, effective temperature about 21,000 K, luminosity about 20,000 L☉⁵
EUV status	Brightest extrasolar source of extreme ultraviolet radiation between 504 Å and 760 Å⁷
Proper name	Adhara, approved by the IAU on 21 August 2016²

Name

The name Adhara comes from the Arabic al-ʿAdhārā (العذاري), "the Virgins", later latinized to "Adhara"⁸. In the star catalog of Al Achsasi al Mouakket, Adhara, Wezen (Delta Canis Majoris), Aludra (Eta Canis Majoris), and Omicron² Canis Majoris were collectively known as Al ʽAdhārā, "the Virgins"¹. The International Astronomical Union's Working Group on Star Names approved the name Adhara for ε Canis Majoris A on 21 August 2016, and it now appears in the List of IAU-approved Star Names². The name formally applies only to the primary component, though it is commonly used for the whole system¹.

The Bayer letter ε does not reflect a strict brightness ranking: Adhara is among the brightest stars of Canis Major even though Sirius (α CMa) and Mirzam (β CMa) carry earlier letters³.

Physical properties

The primary, ε Canis Majoris A, is an evolved B-type bright giant. A 2024 analysis by J. Michael Shull, an astrophysicist at the University of Colorado Boulder, and colleagues combined the Gaia parallax distance of 124 ± 2 parsecs with a measured integrated flux of (41.5 ± 3.3) × 10⁻⁶ erg cm⁻² s⁻¹ and an angular diameter of 0.80 ± 0.05 milliarcseconds to derive a consistent parameter set: radius 10.7 ± 0.7 solar radii, mass 13.1 ± 2.3 solar masses, surface gravity log g = 3.50 ± 0.05, effective temperature about 21,000 K, and luminosity about 20,000 times that of the Sun⁵. At this closer parallax distance the star's absolute visual magnitude is M_V = −3.97 ± 0.04, about 0.9 magnitudes fainter than values based on earlier distance estimates⁵.

Published figures vary with the distance adopted. Widely used reference pages list a surface temperature of 22,900 K, a luminosity of 38,700 L☉, and an absolute magnitude of −4.8¹, and the French observing site Astrosud estimates the diameter at about 11 times the Sun's⁴. The 2024 parallax-based values are smaller because the star turned out to be nearer than previously thought⁵.

The derived parameters place ε CMa outside the β Cephei instability strip, consistent with its observed lack of pulsations⁵.

The brightest extreme ultraviolet source

One of the surprising discoveries of NASA's Extreme Ultraviolet Explorer (EUVE) satellite was that ε CMa is the brightest extrasolar source of radiation between 504 Å and 760 Å⁹. EUVE spectroscopy from 70 to 730 Å, taken during the mission's first cycle of pointed observations, produced the first EUV spectrum of an early-type star and made ε CMa the most comprehensively observed B star from the X-ray to the infrared⁷.

The star's EUV flux is extraordinarily hard to reproduce with models. Observed flux levels are 30 times higher than the appropriate LTE Kurucz model atmosphere and 100 times higher than a non-LTE, line-blanketed TLUSTY model⁹. The Lyman continuum and He I continuum radiation shortward of 504 Å both exceed model predictions, and the star's mid-infrared excess points to outer atmospheric layers warmer than the models indicate⁷. Proposed explanations include additional line-blanketing and non-planar effects, mechanical heating, X-ray irradiation from the stellar wind, and non-LTE effects caused by Doppler shifts in the subsonic outer atmosphere⁹.

Two circumstances make ε CMa unusually observable in the EUV. Its sight line has an extremely small interstellar neutral hydrogen column density, N_H below 10¹⁸ cm⁻², so little radiation is absorbed on the way to Earth⁹. It is also one of only two early-type stars for which high-quality EUV spectra can be obtained⁹. During the ORFEUS-SPAS II mission of November and December 1996, the Berkeley EUV spectrometer observed the star five times for a total useful integration of 9,447 seconds, resolving individual EUVE features into multiple components at a spectral resolution of λ/Δλ ≈ 1250 and revealing wind-broadened O V and Si IV lines with blue-edge velocities up to 800 km/s¹⁰.

Ionizing the local interstellar cloud

ε CMa dominates the hydrogen photoionization of the local interstellar cloud (LIC), the wisp of gas the Sun is currently traveling through. Its Lyman continuum radiation sets a lower limit to the ionization of hydrogen in the Local Cloud, and the EUVE spectrum yields a local hydrogen photoionization rate Γ_HI of about 10⁻¹⁵ s⁻¹ at Earth⁵^•¹¹. After correcting for an interstellar H I column density of (6 ± 1) × 10¹⁷ cm⁻², the star's Lyman-continuum photon flux at Earth is about 3,000 photons cm⁻² s⁻¹, and its ionizing luminosity is Q_LyC = 10^(45.7±0.3) photons s⁻¹⁵.

The star's influence was far greater in the recent past. With a heliocentric radial velocity of 27.3 ± 0.4 km/s and a small proper motion, ε CMa passed within 9.3 ± 0.5 parsecs of the Sun about 4.4 million years ago, when its photoionization rate was 180 times higher⁵. A companion 2025 study found that β CMa, at 151 ± 5 parsecs, passed within 10 ± 1 parsecs of the Sun at about the same time with a similarly enhanced flux, and that the EUV radiation of both stars photoionized and heated the tunnel of low-density gas in the local interstellar medium associated with past supernova explosions in the Scorpius-Centaurus OB association¹². A team led by Shull reported in The Astrophysical Journal in November 2025 that this close pass helps explain why the space around the solar system is more energized than models predict, including a surplus of ionized helium; about 4.5 million years ago, β and ε CMa would have been the two brightest stars in Earth's sky, outshining Sirius¹³.

The companion

ε CMa is a binary system. The companion, ε Canis Majoris B, is much fainter than the primary, and its spectral type has been estimated by comparing its Gaia temperature with a standard dwarf stellar color and effective temperature sequence¹⁴.

Observing

At magnitude 1.50, Adhara is easily visible to the naked eye⁴. It lies at coordinates RA 06h 58m 38s, Dec −28° 58′ 20″ (2000.0), in Canis Major⁴^•⁶. Amateur references note its professional significance as one of the strongest ultraviolet sources in the sky¹⁵.

References

Topic: Encyclopedia › Physical world and mathematics › Astronomy › Stars and galaxies

Initially written Oct 15, 2026 · Edited: Oct 25, 2026

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