Habitability of red dwarf systems

Last updated
An artist's impression of a young red dwarf surrounded by three planets. Planets Under a Red Sun.jpg
An artist's impression of a young red dwarf surrounded by three planets.

The theorized habitability of red dwarf systems is determined by a large number of factors. Modern evidence suggests that planets in red dwarf systems are unlikely to be habitable, due to their low stellar flux, high probability of tidal locking, likely lack of magnetospheres and atmospheres, and the high stellar variation such planets would experience. However, the sheer number and longevity of red dwarfs could provide ample opportunity to realize any small possibility of habitability.

Contents

Current arguments concerning the habitability of red dwarf systems are unresolved, and the area remains an open question of study in the fields of climate modeling and the evolution of life on Earth. Observational data and strong statistical arguments suggest that red dwarf systems are uninhabitable for indeterminate reasons [1] . On the other hand, 3D climate models favor habitability [2] and wider habitable zones for slow rotating and tidally locked planets. [3]

A major impediment to the development of life in red dwarf systems is the intense tidal heating caused by the eccentric orbits of planets around their host stars. [4] [5] Other tidal effects reduce the probability of life around red dwarfs, such as the lack of planetary axial tilts and the extreme temperature differences created by one side of planet permanently facing the star and the other perpetually turned away. Still, a planetary atmosphere may redistribute the heat, making temperatures more uniform. [6] [5] However, it is important to bear in mind that most flare stars are red dwarfs, and their flare events could greatly reduce the habitability of their satellites by eroding their atmosphere (though a planetary magnetic field could protect from these flares). [7] Non-tidal factors further reduce the prospects for life in red-dwarf systems, such as spectral energy distributions shifted toward the infrared side of the spectrum relative to the Sun and small circumstellar habitable zones due to low light output. [5]

There are, however, a few factors that could increase the likelihood of life on red dwarf planets. Intense cloud formation on the star-facing side of a tidally locked planet may reduce overall thermal flux and drastically reduce equilibrium temperature differences between the two sides of the planet. [8] In addition, the sheer number of red dwarfs statistically increases the probability that there might exist habitable planets orbiting some of them. Red dwarfs account for about 85% of stars in the Milky Way [9] [10] and constitute the vast majority of stars in spiral and elliptical galaxies. There are expected to be tens of billions of super-Earth planets in the habitable zones of red dwarf stars in the Milky Way. [11] Investigating the habitability of red dwarf star systems could help determine the frequency of life in the universe and aid scientific understanding of the evolution of life.

Background

Red dwarfs [12] are the smallest, coolest, and most common type of star. Estimates of their abundance range from 70% of stars in spiral galaxies to more than 90% of all stars in elliptical galaxies, [13] [14] an often quoted median figure being 72–76% of the stars in the Milky Way (known since the 1990s from radio telescopic observation to be a barred spiral). [15] Red dwarfs are usually defined as being of spectral type M, although some definitions are wider (including also some or all K-type stars). Given their low energy output, red dwarfs are almost never naked-eye visible from Earth: the closest red dwarf to the Sun, Proxima Centauri, is nowhere near visual magnitude. The brightest red dwarf in Earth's night sky, Lacaille 8760 (+6.7) is visible to the naked eye only under ideal viewing conditions.

Longevity and ubiquity

Red dwarfs’ greatest advantage as candidate stars for life is their longevity. It took 4.5 billion years for intelligent life to evolve on Earth, and life as we know it will see suitable conditions for 1 [16] to 2.3 [17] billion years more. Red dwarfs, by contrast, could live for trillions of years because their nuclear reactions are far slower than those of larger stars, [lower-alpha 1] meaning that life would have longer to evolve and survive.

While the likelihood of finding a planet in the habitable zone around any specific red dwarf is slight, the total amount of habitable zone around all red dwarfs combined is equal to the total amount around Sun-like stars, given their ubiquity. [18] Furthermore, this total amount of habitable zone will last longer, because red dwarf stars live for hundreds of billions of years or even longer on the main sequence, [19] potentially allowing for the evolution of microbial or intelligent life in the future.

Luminosity and spectral composition

Relative star sizes and photospheric temperatures. Any planet around a red dwarf, such as the one shown here (Gliese 229A), would have to huddle close to achieve Earth-like temperatures, probably inducing tidal lock. See Aurelia. Credit: MPIA/V. Joergens. BrownDwarfs Comparison 01.png
Relative star sizes and photospheric temperatures. Any planet around a red dwarf, such as the one shown here (Gliese 229A), would have to huddle close to achieve Earth-like temperatures, probably inducing tidal lock. See Aurelia. Credit: MPIA/V. Joergens.

For years, astronomers have been pessimistic about red dwarfs as potential candidates for hosting life. The low masses of red dwarves (from roughly 0.08 to 0.60 solar masses (M)) cause their nuclear fusion reactions to proceed exceedingly slowly, giving them low luminosities ranging from 10% to just 0.0125% that of the Earth's Sun. [20] Consequently, any planet orbiting a red dwarf would need a low semi-major axis in order to maintain an Earth-like surface temperature, from 0.268 astronomical units (AU) for a relatively luminous red dwarf like Lacaille 8760 to 0.032 AU for a smaller star like Proxima Centauri. [21] Such a world would have a year lasting just 3 to 150 Earth days. [22] [23]

At these close distances, the star's gravity would cause tidal locking. One side of the planet would eternally face the star, while the other would always face away from it. The only ways in which potential life could avoid either an inferno or a deep freeze would be if the planet had an atmosphere thick enough to transfer the star's heat from the day side to the night side. Photosynthesis on such a planet would be difficult, as much of the low luminosity falls under the lower energy infrared and red part of the electromagnetic spectrum, and would therefore require additional photons to achieve excitation potentials. [24] Potential plants would likely adapt to a much wider spectrum (and as such appear black in visible light). [24]

In addition, because water strongly absorbs red and infrared light, less energy would be available for aquatic life on red dwarf planets. [25] However, a similar effect of preferential absorption by water ice would increase its temperature relative to an equivalent amount of radiation from a Sun-like star, thereby extending the habitable zone of red dwarfs outward. [26]

The evolution of the red dwarf stars may also inhibit habitability. As red dwarf stars have an extended pre-main sequence phase, their eventual habitable zones would be for around 1 billion years in a zone where water was not liquid but rather in a gaseous state. Thus, terrestrial planets in the actual habitable zones, if provided with abundant surface water in their formation, would have been subject to a runaway greenhouse effect for several hundred million years. During such an early runaway greenhouse phase, photolysis of water vapor would allow hydrogen escape to space and the loss of several Earth oceans of water, leaving a thick abiotic oxygen atmosphere. [27]

Because the lifespan of red dwarf stars exceeds the age of the known universe, the further evolution of red dwarfs is known only by theory and simulations. According to computer simulations, a red dwarf becomes a blue dwarf after exhausting its hydrogen supply. As this kind of star is more luminous than the previous red dwarf, planets orbiting it that were frozen during the former stage could be thawed during the several billions of years this evolutionary stage lasts (5 billion years, for example, for a 0.16  M star), giving life an opportunity to appear and evolve. [28]

Tidal effects

For planets to retain significant amounts of water in the habitable zone of ultra-cool dwarfs, a planet must orbit very near to the star. [29] At these close orbital distances, tidal locking to the host star is likely. Tidal locking makes the planet rotate on its axis once every revolution around the star. As a result, one side of the planet would eternally face the star and another side would perpetually face away, creating great extremes of temperature.

For many years, it was believed that life on such planets would be limited to a ring-like region known as the terminator, where the star would always appear on or close to the horizon. It was also believed that efficient heat transfer between the sides of the planet necessitates atmospheric circulation of an atmosphere so thick as to disallow photosynthesis. Due to differential heating, it was argued, a tidally locked planet would experience fierce winds with permanent torrential rain at the point directly facing the local star, [30] the sub-solar point. In the opinion of one author this makes complex life improbable. [31] Plant life would have to adapt to the constant gale, for example by anchoring securely into the soil and sprouting long flexible leaves that do not snap. Animals would rely on infrared vision, as signaling by calls or scents would be difficult over the din of the planet-wide gale. Underwater life would, however, be protected from fierce winds and flares, and vast blooms of black photosynthetic plankton and algae could support the sea life. [32]

In contrast to the previously bleak picture for life, 1997 studies by NASA's Ames Research Center have shown that a planet's atmosphere (assuming it included greenhouse gases CO2 and H2O) need only be 100 millibar, or 10% of Earth's atmosphere, for the star's heat to be effectively carried to the night side, a figure well within the bounds of photosynthesis. [33] Subsequent research has shown that seawater, too, could effectively circulate without freezing solid if the ocean basins were deep enough to allow free flow beneath the night side's ice cap. Additionally, a 2010 study concluded that Earth-like water worlds tidally locked to their stars would still have temperatures above 240 K (−33 °C) on the night side. [34] Climate models constructed in 2013 indicate that cloud formation on tidally locked planets would minimize the temperature difference between the day and the night side, greatly improving habitability prospects for red dwarf planets. [8] Further research, including a consideration of the amount of photosynthetically active radiation, has suggested that tidally locked planets in red dwarf systems might at least be habitable for higher plants. [35]

The existence of a permanent day side and night side is not the only potential setback for life around red dwarfs. Tidal heating experienced by planets in the habitable zone of red dwarfs less than 30% of the mass of the Sun may cause them to be "baked out" and become "tidal Venuses." [4] The eccentricity of over 150 planets found orbiting M dwarfs was measured, and it was found that two-thirds of these exoplanets are exposed to extreme tidal forces, rendering them uninhabitable due to the intense heat generated by tidal heating. [36]

Combined with the other impediments to red dwarf habitability, [6] this may make the probability of many red dwarfs hosting life as we know it very low compared to other star types. [5] There may not even be enough water for habitable planets around many red dwarfs; [37] what little water found on these planets, in particular Earth-sized ones, may be located on the cold night side of the planet. In contrast to the predictions of earlier studies on tidal Venuses, though, this "trapped water" may help to stave off runaway greenhouse effects and improve the habitability of red dwarf systems. [38]

An artist's impression of GJ 667 Cc, a potentially habitable planet orbiting a red dwarf constituent in a trinary star system. Gliese 667 Cc sunset.jpg
An artist's impression of GJ 667 Cc, a potentially habitable planet orbiting a red dwarf constituent in a trinary star system.

Note however that how quickly tidal locking occurs can depend upon a planet's oceans and even atmosphere, and it may mean that tidal locking fails to happen even after many billions of years. Additionally, tidal locking is not the only possible end state of tidal dampening. Mercury, for example, has had sufficient time to tidally lock, but is in a 3:2 spin orbit resonance. [39]

Variability

Red dwarfs are far more volatile than their larger, more stable cousins. Often, they are covered in starspots that can dim their emitted light by up to 40% for months at a time. At other times, red dwarfs emit gigantic flares that can double their brightness in a matter of minutes. [40] Indeed, as more and more red dwarfs have been scrutinized for variability, more of them have been classified as flare stars to some degree or other. Such variation in brightness could be very damaging for life. Recent 3D climate models simulate flare events by altering the stellar flux received by any given planet. One study found that, should a tidally locked planet possess a sufficient atmosphere, cloud coverage and albedo increase monotonically with stellar flux, increasing the resilience of the planet to variations in radiation. [8] This caveat has proven difficult, however, since flares produce torrents of charged particles that could strip off sizable portions of the planet's atmosphere. [41] Scientists who subscribe to the Rare Earth hypothesis doubt that red dwarfs could support life amid strong flaring. Tidal locking would probably result in a relatively low planetary magnetic moment. Active red dwarfs that emit coronal mass ejections (CMEs) would bow back the magnetosphere until it contacted the planetary atmosphere. As a result, the atmosphere would undergo strong erosion, possibly leaving the planet uninhabitable. [42] [43] [44] It was found that red dwarfs have a much lower CME rate than expected from their rotation or flare activity, and large CMEs occur rarely. This suggests that atmospheric erosion is caused mainly by radiation rather than CMEs. [45]

Otherwise, it is suggested that if the planet had a magnetic field, it would deflect the particles from the atmosphere (even the slow rotation of a tidally locked M-dwarf planet—it spins once for every time it orbits its star—would be enough to generate a magnetic field as long as part of the planet's interior remained molten). [46] This magnetic field should be much stronger compared to Earth's to give protection against flares of the observed magnitude (10–1000 G compared to the terrestrial 0.5G ), which is unlikely to be generated. [47] But mathematical models conclude that, [48] [49] [50] even under the highest attainable dynamo-generated magnetic field strengths, exoplanets with masses similar to that of Earth lose a significant fraction of their atmospheres by the erosion of the exobase's atmosphere by CME bursts and XUV emissions (even those Earth-like planets closer than 0.8 AU, affecting also G and K stars, are prone to losing their atmospheres). Atmospheric erosion even could trigger the depletion of water oceans. [51] Planets shrouded by a thick haze of hydrocarbons like the one on primordial Earth or Saturn's moon Titan might still survive the flares as floating droplets of hydrocarbon are particularly efficient at absorbing ultraviolet radiation. [52]

Actual measurements reject the presence of relevant atmospheres in two exoplanets orbiting a red dwarf: TRAPPIST-1 b and TRAPPIST-1 c are bare rocks or have as much thinner atmospheres. [53]

Another way that life could initially protect itself from radiation would be remaining underwater until the star had passed through its early flare stage, assuming the planet could retain enough of an atmosphere to sustain liquid oceans. Once life reached land, the low amount of UV produced by a quiet red dwarf means that life could thrive without an ozone layer, and thus never need to produce oxygen. [24]

Flare activity

For a planet around a red dwarf star to support life, it would require a rapidly rotating magnetic field to protect it from the flares. A tidally locked planet rotates only very slowly, and so cannot produce a geodynamo at its core. The violent flaring period of a red dwarf's life cycle is estimated to last for only about the first 1.2 billion years of its existence. If a planet forms far away from a red dwarf so as to avoid tidal locking, and then migrates into the star's habitable zone after this turbulent initial period, it is possible for life to have a chance to develop. [54]

It has been found that the largest flares happen at high latitudes near the stellar poles; so if an exoplanet's orbit is aligned with the stellar rotation then it is less affected by the flares than previously thought. [55] However, observations of the 7 to 12-billion year old Barnard's Star showcase that even old red dwarfs can have significant flare activity. Barnard's Star was long assumed to have little activity, but in 1998 astronomers observed an intense stellar flare, showing that it is a flare star. [56]

Methane habitable zone

If methane-based life is possible (similar to the hypothetical life on Titan), there would be a second habitable zone further out from the star corresponding to the region where methane is liquid. Titan's atmosphere is transparent to red and infrared light, so more of the light from red dwarfs would be expected to reach the surface of a Titan-like planet. [57]

Frequency of Earth-sized worlds around ultra-cool dwarfs

TRAPPIST-1 planetary system (artist's impression) PIA21422 - TRAPPIST-1 Planet Lineup, Figure 1.jpg
TRAPPIST-1 planetary system (artist's impression)

A study of archival Spitzer data gives the first idea and estimate of how frequent Earth-sized worlds are around ultra-cool dwarf stars: 30–45%. [58] A computer simulation finds that planets that form around stars with similar mass to TRAPPIST-1 (c. 0.084 M ) most likely have sizes similar to the Earth's. [59]

In fiction

The following examples of fictional "aliens" existing within Red Dwarf star systems exist:

See also

Wikiversity logo 2017.svg Learning materials from Wikiversity:

Notes

  1. The more massive a star is, the shorter it lives.

Related Research Articles

<span class="mw-page-title-main">Exoplanet</span> Planet outside the Solar System

An exoplanet or extrasolar planet is a planet outside the Solar System. The first possible evidence of an exoplanet was noted in 1917 but was not then recognized as such. The first confirmation of the detection occurred in 1992. A different planet, first detected in 1988, was confirmed in 2003. As of 24 July 2024, there are 7,026 confirmed exoplanets in 4,949 planetary systems, with 1007 systems having more than one planet. The James Webb Space Telescope (JWST) is expected to discover more exoplanets, and to give more insight into their traits, such as their composition, environmental conditions, and potential for life.

<span class="mw-page-title-main">Red dwarf</span> Dim, low mass stars on the main sequence

A red dwarf is the smallest kind of star on the main sequence. Red dwarfs are by far the most common type of fusing star in the Milky Way, at least in the neighborhood of the Sun. However, due to their low luminosity, individual red dwarfs cannot be easily observed. From Earth, not one star that fits the stricter definitions of a red dwarf is visible to the naked eye. Proxima Centauri, the star nearest to the Sun, is a red dwarf, as are fifty of the sixty nearest stars. According to some estimates, red dwarfs make up three-quarters of the fusing stars in the Milky Way.

<span class="mw-page-title-main">Ross 128</span> Small star in constellation of Virgo

Ross 128 is a red dwarf in the equatorial zodiac constellation of Virgo, near β Virginis. The apparent magnitude of Ross 128 is 11.13, which is too faint to be seen with the unaided eye. Based upon parallax measurements, the distance of this star from Earth is 11.007 light-years, making it the twelfth closest stellar system to the Solar System. It was first cataloged in 1926 by American astronomer Frank Elmore Ross.

GJ 1061 is a red dwarf star located 12 light-years from Earth in the southern constellation of Horologium. Even though it is a relatively nearby star, it has an apparent visual magnitude of about 13, so it can only be seen with at least a moderately-sized telescope.

<span class="mw-page-title-main">Habitable zone</span> Orbits where planets may have liquid surface water

In astronomy and astrobiology, the habitable zone (HZ), or more precisely the circumstellar habitable zone (CHZ), is the range of orbits around a star within which a planetary surface can support liquid water given sufficient atmospheric pressure. The bounds of the HZ are based on Earth's position in the Solar System and the amount of radiant energy it receives from the Sun. Due to the importance of liquid water to Earth's biosphere, the nature of the HZ and the objects within it may be instrumental in determining the scope and distribution of planets capable of supporting Earth-like extraterrestrial life and intelligence.

<span class="mw-page-title-main">K-type main-sequence star</span> Stellar classification

A K-type main-sequence star, also referred to as a K-type dwarf, or orange dwarf, is a main-sequence (hydrogen-burning) star of spectral type K and luminosity class V. These stars are intermediate in size between red M-type main-sequence stars and yellow/white G-type main-sequence stars. They have masses between 0.6 and 0.9 times the mass of the Sun and surface temperatures between 3,900 and 5,300 K. These stars are of particular interest in the search for extraterrestrial life due to their stability and long lifespan. Many of these stars have not left the main sequence as their low masses mean they stay on the main sequence for up to 70 billion years, a length of time much larger than the time the universe has existed. Well-known examples include Toliman and Epsilon Indi.

<span class="mw-page-title-main">Exomoon</span> Moon beyond the Solar System

An exomoon or extrasolar moon is a natural satellite that orbits an exoplanet or other non-stellar extrasolar body.

<span class="mw-page-title-main">Planetary habitability</span> Known extent to which a planet is suitable for life

Planetary habitability is the measure of a planet's or a natural satellite's potential to develop and maintain environments hospitable to life. Life may be generated directly on a planet or satellite endogenously or be transferred to it from another body, through a hypothetical process known as panspermia. Environments do not need to contain life to be considered habitable nor are accepted habitable zones (HZ) the only areas in which life might arise.

<span class="mw-page-title-main">Habitability of natural satellites</span> Measure of the potential of natural satellites to have environments hospitable to life

The habitability of natural satellites is the potential of moons to provide habitats for life, though it is not an indicator that they harbor it. Natural satellites are expected to outnumber planets by a large margin and the study of their habitability is therefore important to astrobiology and the search for extraterrestrial life. There are, nevertheless, significant environmental variables specific to moons.

<span class="mw-page-title-main">Habitability of K-type main-sequence star systems</span> Overview of the habitability of K-type main-sequence star systems

K-type main-sequence stars, also known as orange dwarfs, may be candidates for supporting extraterrestrial life. These stars are known as "Goldilocks stars" as they emit enough radiation in the non-UV ray spectrum to provide a temperature that allows liquid water to exist on the surface of a planet; they also remain stable in the main sequence longer than the Sun by burning their hydrogen slower, allowing more time for life to form on a planet around a K-type main-sequence star. The planet's habitable zone, ranging from 0.1–0.4 to 0.3–1.3 astronomical units (AU), depending on the size of the star, is often far enough from the star so as not to be tidally locked to the star, and to have a sufficiently low solar flare activity not to be lethal to life. In comparison, red dwarf stars have too much solar activity and quickly tidally lock the planets in their habitable zones, making them less suitable for life. The odds of complex life arising may be better on planets around K-type main-sequence stars than around Sun-like stars, given the suitable temperature and extra time available for it to evolve. Some planets around K-type main-sequence stars are potential candidates for extraterrestrial life.

<span class="mw-page-title-main">Kepler-62f</span> Super-Earth orbiting Kepler-62

Kepler-62f is a super-Earth exoplanet orbiting within the habitable zone of the star Kepler-62, the outermost of five such planets discovered around the star by NASA's Kepler spacecraft. It is located about 980 light-years from Earth in the constellation of Lyra.

<span class="mw-page-title-main">Superhabitable world</span> Hypothetical type of planet or moon that may be better-suited for life than Earth

A superhabitable world is a hypothetical type of planet or moon that is better suited than Earth for the emergence and evolution of life. The concept was introduced in a 2014 paper by René Heller and John Armstrong, in which they criticized the language used in the search for habitable exoplanets and proposed clarifications. The authors argued that knowing whether a world is located within the star's habitable zone is insufficient to determine its habitability, that the principle of mediocrity cannot adequately explain why Earth should represent the archetypal habitable world, and that the prevailing model of characterization was geocentric or anthropocentric in nature. Instead, they proposed a biocentric approach that prioritized astrophysical characteristics affecting the abundance and variety of life on a world's surface.

<span class="mw-page-title-main">Proxima Centauri b</span> Terrestrial planet orbiting Proxima Centauri

Proxima Centauri b, also referred to as Alpha Centauri Cb, is an exoplanet orbiting within the habitable zone of the red dwarf star Proxima Centauri, which is the closest star to the Sun and part of the larger triple star system Alpha Centauri. It is about 4.2 light-years from Earth in the constellation Centaurus, making it and Proxima d, along with the currently disputed Proxima c, the closest known exoplanets to the Solar System.

<span class="mw-page-title-main">TRAPPIST-1f</span> Earth-size exoplanet orbiting TRAPPIST-1

TRAPPIST-1f, also designated as 2MASS J23062928-0502285 f, is an exoplanet, likely rocky, orbiting within the habitable zone around the ultracool dwarf star TRAPPIST-1, located 40.7 light-years away from Earth in the constellation of Aquarius. The exoplanet was found by using the transit method, in which the dimming effect that a planet causes as it crosses in front of its star is measured.

<span class="mw-page-title-main">Ross 128 b</span> Confirmed terrestrial exoplanet orbiting Ross 128

Ross 128 b is a confirmed Earth-sized exoplanet, likely rocky, that is orbiting within the inner habitable zone of the red dwarf star Ross 128, at a distance of around 11 light-years from Earth. The exoplanet was found using a decade's worth of radial velocity data using the European Southern Observatory's HARPS spectrograph at the La Silla Observatory in Chile. Ross 128 b is the nearest exoplanet around a quiet red dwarf, and is considered one of the best candidates for habitability. The planet is only 35% more massive than Earth, receives only 38% more starlight, and is expected to be a temperature suitable for liquid water to exist on the surface, if it has an atmosphere.

TOI-700 is a red dwarf 101.4 light-years away from Earth located in the Dorado constellation that hosts TOI-700 d, the first Earth-sized exoplanet in the habitable zone discovered by the Transiting Exoplanet Survey Satellite (TESS).

<span class="mw-page-title-main">Kepler-1649c</span> Earth-size exoplanet orbiting Kepler-1649

Kepler-1649c is an Earth-sized exoplanet, likely rocky, orbiting within the habitable zone of the red dwarf star Kepler-1649, the outermost planet of the planetary system discovered by Kepler’s space telescope. It is located about 301 light-years (92 pc) away from Earth, in the constellation of Cygnus.

<span class="mw-page-title-main">Habitability of yellow dwarf systems</span> Likelihood of finding extraterrestrial life in yellow dwarf systems

Habitability of G V stars of G V stars systems defines the suitability for life of exoplanets belonging to yellow dwarf stars. These systems are the object of study among the scientific community because they are considered the most suitable for harboring living organisms, together with those belonging to K-type stars.

<span class="mw-page-title-main">Habitable zone for complex life</span>

A Habitable Zone for Complex Life (HZCL) is a range of distances from a star suitable for complex aerobic life. Different types of limitations preventing complex life give rise to different zones. Conventional habitable zones are based on compatibility with water. Most zones start at a distance from the host star and then end at a distance farther from the star. A planet would need to orbit inside the boundaries of this zone. With multiple zonal constraints, the zones would need to overlap for the planet to support complex life. The requirements for bacterial life produce much larger zones than those for complex life, which requires a very narrow zone.

References

  1. Waltham, David (January 2017). "Star Masses and Star-Planet Distances for Earth-like Habitability". Astrobiology. 17 (1): 61–77. doi:10.1089/ast.2016.1518 . Retrieved 30 July 2024.
  2. Yang, Jun; Cowan, Nicolas B.; Abbot, Dorian S. (27 June 2013). "STABILIZING CLOUD FEEDBACK DRAMATICALLY EXPANDS THE HABITABLE ZONE OF TIDALLY LOCKED PLANETS". The Astrophysical Journal. 771 (2): L45. doi:10.1088/2041-8205/771/2/L45 . Retrieved 30 July 2024.
  3. Yang, Jun; Boué, Gwenaël; Fabrycky, Daniel C.; Abbot, Dorian S. (25 April 2014). "STRONG DEPENDENCE OF THE INNER EDGE OF THE HABITABLE ZONE ON PLANETARY ROTATION RATE". The Astrophysical Journal. 787 (1): L2. doi:10.1088/2041-8205/787/1/L2 . Retrieved 30 July 2024.
  4. 1 2 Barnes, Rory; Mullins, Kristina; Goldblatt, Colin; Meadows, Victoria S.; Kasting, James F.; Heller, René (March 2013). "Tidal Venuses: Triggering a Climate Catastrophe via Tidal Heating". Astrobiology. 13 (3): 225–250. arXiv: 1203.5104 . Bibcode:2013AsBio..13..225B. doi:10.1089/ast.2012.0851. PMC   3612283 . PMID   23537135.
  5. 1 2 3 4 Major, Jason (23 December 2015). ""Tidal Venuses" May Have Been Wrung Out To Dry". Universetoday.com. Archived from the original on 26 March 2023. Retrieved 9 April 2012.
  6. 1 2 Wilkins, Alasdair (2012-01-16). "Life might not be possible around red dwarf stars". Io9.com. Archived from the original on 2015-10-03. Retrieved 2013-01-19.
  7. "Habitable Exoplanet Observatory (HabEx)". www.jpl.nasa.gov. Archived from the original on 2019-10-08. Retrieved 2020-03-31.
  8. 1 2 3 Yang, J.; Cowan, N. B.; Abbot, D. S. (2013). "Stabilizing Cloud Feedback Dramatically Expands the Habitable Zone of Tidally Locked Planets". The Astrophysical Journal. 771 (2): L45. arXiv: 1307.0515 . Bibcode:2013ApJ...771L..45Y. doi:10.1088/2041-8205/771/2/L45. S2CID   14119086.
  9. Than, Ker (2006-01-30). "Astronomers Had it Wrong: Most Stars are Single". Space.com. TechMediaNetwork. Archived from the original on 2019-09-24. Retrieved 2013-07-04.
  10. Staff (2013-01-02). "100 Billion Alien Planets Fill Our Milky Way Galaxy: Study". Space.com. Archived from the original on 2020-05-09. Retrieved 2013-01-03.
  11. Gilster, Paul (2012-03-29). "ESO: Habitable Red Dwarf Planets Abundant". Centauri-dreams.org. Archived from the original on 2017-01-18. Retrieved 2013-01-19.
  12. The term dwarf applies to all stars in the main sequence, including the Sun.
  13. van Dokkum, Pieter G.; Conroy, Charlie (1 December 2010). "A substantial population of low-mass stars in luminous elliptical galaxies". Nature . 468 (7326): 940–942. arXiv: 1009.5992 . Bibcode:2010Natur.468..940V. doi:10.1038/nature09578. PMID   21124316. S2CID   205222998.
  14. Yale University (December 1, 2010). "Discovery Triples Number of Stars in Universe". ScienceDaily. Archived from the original on January 4, 2019. Retrieved December 17, 2010.
  15. Dole, Stephen H. Habitable Planets for Man 1965 Rand Corporation report, published in book form--A figure of 73% is given for the percentage of red dwarfs in the Milky Way.
  16. Hines, Sandra (13 January 2003). "'The end of the world' has already begun, UW scientists say" (Press release). University of Washington. Archived from the original on 11 January 2008. Retrieved 5 June 2007.
  17. Li, King-Fai; Pahlevan, Kaveh; Kirschvink, Joseph L.; Yung, Yuk L. (2009). "Atmospheric pressure as a natural climate regulator for a terrestrial planet with a biosphere" (PDF). Proceedings of the National Academy of Sciences. 106 (24): 9576–9579. Bibcode:2009PNAS..106.9576L. doi: 10.1073/pnas.0809436106 . PMC   2701016 . PMID   19487662. Archived (PDF) from the original on 4 July 2009. Retrieved 19 July 2009.
  18. "M Dwarfs: The Search for Life is On, Interview with Todd Henry". Astrobiology Magazine. 29 August 2005. Archived from the original on 2011-06-03. Retrieved 5 August 2007.{{cite web}}: CS1 maint: unfit URL (link)
  19. Cain, Fraser (4 February 2009). "Red Dwarf Stars". Universe Today. Archived from the original on 5 October 2023. Retrieved 26 November 2023.
  20. Chabrier, G.; Baraffe, I.; Plez, B. (1996). "Mass-Luminosity Relationship and Lithium Depletion for Very Low Mass Stars". Astrophysical Journal Letters. 459 (2): L91–L94. Bibcode:1996ApJ...459L..91C. doi: 10.1086/309951 .
  21. "Habitable zones of stars". NASA Specialized Center of Research and Training in Exobiology. University of Southern California, San Diego. Archived from the original on 2000-11-21. Retrieved 2007-05-11.
  22. Ségransan, Damien; Kervella, Pierre; Forveille, Thierry; Queloz, Didier (2003). "First radius measurements of very low mass stars with the VLTI". Astronomy and Astrophysics. 397 (3): L5–L8. arXiv: astro-ph/0211647 . Bibcode:2003A&A...397L...5S. doi:10.1051/0004-6361:20021714. S2CID   10748478.
  23. Williams, David R. (2004-09-01). "Earth Fact Sheet". NASA. Archived from the original on 2013-05-08. Retrieved 2010-08-09.
  24. 1 2 3 Kiang, Nancy Y. (April 2008). "The color of plants on other worlds". Scientific American. 298 (4): 48–55. Bibcode:2008SciAm.298d..48K. doi:10.1038/scientificamerican0408-48. PMID   18380141. S2CID   12329051.
  25. Hoejerslev, N. K. (1986). "3.3.2.1 Optical properties of pure water and pure sea water". Subvolume A. Landolt-Börnstein - Group V Geophysics. Vol. 3a. pp. 395–398. doi:10.1007/10201933_90. ISBN   978-3-540-15092-3.
  26. Joshi, M.; Haberle, R. (2012). "Suppression of the water ice and snow albedo feedback on planets orbiting red dwarf stars and the subsequent widening of the habitable zone". Astrobiology. 12 (1): 3–8. arXiv: 1110.4525 . Bibcode:2012AsBio..12....3J. doi:10.1089/ast.2011.0668. PMID   22181553. S2CID   18065288.
  27. Luger, R.; Barnes, R. (2014). "Extreme Water Loss and Abiotic O2 Buildup on Planets Throughout the Habitable Zones of M Dwarfs". Astrobiology. 15 (2): 119–143. arXiv: 1411.7412 . Bibcode:2015AsBio..15..119L. doi:10.1089/ast.2014.1231. PMC   4323125 . PMID   25629240.
  28. Adams, Fred C.; Laughlin, Gregory; Graves, Genevieve J. M. "Red Dwarfs and the End of the Main Sequence". Gravitational Collapse: From Massive Stars to Planets. Revista Mexicana de Astronomía y Astrofísica. pp. 46–49. Bibcode:2004RMxAC..22...46A.
  29. Bolmont, E.; Selsis, F.; Owen, J. E.; Ribas, I.; Raymond, S. N.; Leconte, J.; Gillon, M. (21 January 2017). "Water loss from terrestrial planets orbiting ultracool dwarfs: implications for the planets of TRAPPIST-1". Monthly Notices of the Royal Astronomical Society. 464 (3): 3728–3741. arXiv: 1605.00616 . Bibcode:2017MNRAS.464.3728B. doi: 10.1093/mnras/stw2578 .
  30. Joshi, M. (2003). "Climate model studies of synchronously rotating planets". Astrobiology. 3 (2): 415–427. Bibcode:2003AsBio...3..415J. doi:10.1089/153110703769016488. PMID   14577888.
  31. "Gliese 581d". Astroprof’s Page. 16 June 2007. Archived from the original on 29 October 2013.
  32. Dartnell, Lewis (April 2010). "Meet the Alien Neighbours: Red Dwarf World". Focus: 45. Archived from the original on 2010-03-31. Retrieved 2010-03-29.
  33. Joshi, M. M.; Haberle, R. M.; Reynolds, R. T. (October 1997). "Simulations of the Atmospheres of Synchronously Rotating Terrestrial Planets Orbiting M Dwarfs: Conditions for Atmospheric Collapse and the Implications for Habitability" (PDF). Icarus. 129 (2): 450–465. Bibcode:1997Icar..129..450J. doi:10.1006/icar.1997.5793. Archived from the original (PDF) on 2014-07-15. Retrieved 2007-08-11.
  34. Merlis, T. M.; Schneider, T. (2010). "Atmospheric dynamics of Earth-like tidally locked aquaplanets". Journal of Advances in Modeling Earth Systems. 2 (4): n/a. arXiv: 1001.5117 . Bibcode:2010JAMES...2...13M. doi:10.3894/JAMES.2010.2.13. S2CID   37824988.
  35. Heath, Martin J.; Doyle, Laurance R.; Joshi, Manoj M.; Haberle, Robert M. (1999). "Habitability of Planets Around Red Dwarf Stars" (PDF). Origins of Life and Evolution of the Biosphere. 29 (4): 405–424. Bibcode:1999OLEB...29..405H. doi:10.1023/A:1006596718708. PMID   10472629. S2CID   12329736. Archived (PDF) from the original on 2010-10-08. Retrieved 2007-08-11.
  36. Sagear, Sheila; Ballards, Sarah (2023). "The Orbital Eccentricity Distribution of Planets Orbiting M dwarfs". PNAS . XXX (XX): e2217398120. arXiv: 2305.17157 . Bibcode:2023PNAS..12017398S. doi:10.1073/pnas.2217398120. PMC   10265968 . PMID   37252955. S2CID   258960478.
  37. Lissauer, Jack J. (2007). "Planets formed in habitable zones of M dwarf stars probably are deficient in volatiles". The Astrophysical Journal . 660 (2): 149–152. arXiv: astro-ph/0703576 . Bibcode:2007ApJ...660L.149L. doi:10.1086/518121. S2CID   12312927.
  38. Menou, Kristen (16 August 2013). "Water-Trapped Worlds". The Astrophysical Journal. 774 (1): 51. arXiv: 1304.6472 . Bibcode:2013ApJ...774...51M. doi:10.1088/0004-637X/774/1/51. S2CID   118363386.
  39. Kasting, James F.; Whitmire, Daniel P.; Reynolds, Ray T. (1993). "Habitable Zones around Main Sequence Stars" (PDF). Icarus. 101 (1): 108–128. Bibcode:1993Icar..101..108K. doi:10.1006/icar.1993.1010. PMID   11536936. Archived (PDF) from the original on 2023-04-26. Retrieved 2017-08-03.
  40. Croswell, Ken (27 January 2001). "Red, willing and able". New Scientist. Archived from the original on 2008-04-30. Retrieved 2007-08-05.
  41. Guinan, Edward F.; Engle, S. G.: "Future Interstellar Travel Destinations: Assessing the Suitability of Nearby Red Dwarf Stars as Hosts to Habitable Life-bearing Planets"; American Astronomical Society, AAS Meeting #221, #333.02 Publication Date:01/2013 Bibcode : 2013AAS...22133302G
  42. Khodachenko, Maxim L.; et al. (2007). "Coronal Mass Ejection (CME) Activity of Low Mass M Stars as An Important Factor for The Habitability of Terrestrial Exoplanets. I. CME Impact on Expected Magnetospheres of Earth-Like Exoplanets in Close-In Habitable Zones". Astrobiology. 7 (1): 167–184. Bibcode:2007AsBio...7..167K. doi:10.1089/ast.2006.0127. PMID   17407406.
  43. Kay, C.; et al. (2016). "Probability of Cme Impact on Exoplanets Orbiting M Dwarfs and Solar-Like Stars". The Astrophysical Journal. 826 (2): 195. arXiv: 1605.02683 . Bibcode:2016ApJ...826..195K. doi: 10.3847/0004-637X/826/2/195 . S2CID   118669187.
  44. Garcia-Sage, K.; et al. (2017). "On the Magnetic Protection of the Atmosphere of Proxima Centauri b". The Astrophysical Journal Letters. 844 (1): L13. Bibcode:2017ApJ...844L..13G. doi: 10.3847/2041-8213/aa7eca . S2CID   126391408.
  45. K., Vida (2019). "The quest for stellar coronal mass ejections in late-type stars. I. Investigating Balmer-line asymmetries of single stars in Virtual Observatory data". Astronomy & Astrophysics. 623 (14): A49. arXiv: 1901.04229 . Bibcode:2019A&A...623A..49V. doi:10.1051/0004-6361/201834264. S2CID   119095055.
  46. Alpert, Mark (November 1, 2005). "Red Star Rising: Small, cool stars may be hot spots for life". Scientific American. 293 (5): 28. Bibcode:2005SciAm.293e..28A. doi:10.1038/scientificamerican1105-28. PMID   16318021. Archived from the original on 2022-02-12. Retrieved 2013-01-19.
  47. K., Vida (2017). "Frequent flaring in the TRAPPIST-1 system - unsuited for life?". The Astrophysical Journal. 841 (2): 124. arXiv: 1703.10130 . Bibcode:2017ApJ...841..124V. doi: 10.3847/1538-4357/aa6f05 . S2CID   118827117.
  48. Zuluaga, J. I.; Cuartas, P. A.; Hoyos, J. H. (2012). "Evolution of magnetic protection in potentially habitable terrestrial planets". arXiv: 1204.0275 [astro-ph.EP].
  49. See, V.; Jardine, M.; Vidotto, A. A.; Petit, P.; Marsden, S. C.; Jeffers, S. V.; do Nascimento, J. D. (30 October 2014). "The effects of stellar winds on the magnetospheres and potential habitability of exoplanets". Astronomy & Astrophysics. 570: A99. arXiv: 1409.1237 . Bibcode:2014A&A...570A..99S. doi:10.1051/0004-6361/201424323. S2CID   16146794.
  50. Dong, Chuanfei; Lingam, Manasvi; Ma, Yingjuan; Cohen, Ofer (10 March 2017). "Is Proxima Centauri b Habitable? A Study of Atmospheric Loss". The Astrophysical Journal Letters. 837:L26 (2): L26. arXiv: 1702.04089 . Bibcode:2017ApJ...837L..26D. doi: 10.3847/2041-8213/aa6438 . S2CID   118927765.
  51. Dong, Chuanfei; et al. (2017). "The dehydration of water worlds via atmospheric losses". The Astrophysical Journal Letters. 847 (L4): L4. arXiv: 1709.01219 . Bibcode:2017ApJ...847L...4D. doi: 10.3847/2041-8213/aa8a60 . S2CID   119424858.
  52. Tilley, Matt A; et al. (22 Nov 2017). "Modeling Repeated M-dwarf Flaring at an Earth-like Planet in the Habitable Zone: I. Atmospheric Effects for an Unmagnetized Planet". Astrobiology. 19 (1): 64–86. arXiv: 1711.08484 . doi:10.1089/ast.2017.1794. PMC   6340793 . PMID   30070900.
  53. Zleba, Sebastian; Kreldberg, Laura (19 June 2023). "No thick carbon dioxide atmosphere on the rocky exoplanet TRAPPIST-1 c". Nature . 620 (7975): 746–749. arXiv: 2306.10150 . Bibcode:2023Natur.620..746Z. doi:10.1038/s41586-023-06232-z. PMC   10447244 . PMID   37337068. S2CID   259200424.
  54. Cain, Fraser; Gay, Pamela (2007). "AstronomyCast episode 40: American Astronomical Society Meeting, May 2007". Universe Today. Archived from the original on 2012-03-12. Retrieved 2018-09-06.
  55. Ilin, Ekaterina; Poppenhaeger, Katja; et al. (5 August 2021). "Giant white-light flares on fully convective stars occur at high latitudes". Monthly Notices of the Royal Astronomical Society . 507 (2): 1723–1745. arXiv: 2108.01917 . doi: 10.1093/mnras/stab2159 .
  56. Croswell, Ken (November 2005). "A Flare for Barnard's Star". Astronomy Magazine. Kalmbach Publishing Co. Archived from the original on 2015-02-24. Retrieved 2006-08-10.
  57. Cooper, Keith (10 November 2011). "The Methane Habitable Zone". Astrobiology Magazine. Archived from the original on 2021-05-09. Retrieved 25 February 2019.{{cite web}}: CS1 maint: unfit URL (link)
  58. He, Matthias Y.; Triaud, Amaury H. M. J.; Gillon, Michaël (2017). "First limits on the occurrence rate of short-period planets orbiting brown dwarfs". Monthly Notices of the Royal Astronomical Society . 464 (3): 2687–2697. arXiv: 1609.05053 . Bibcode:2017MNRAS.464.2687H. doi: 10.1093/mnras/stw2391 .
  59. Alibert, Yann; Benz, Willy (26 January 2017). "Formation and composition of planets around very low mass stars". Astronomy & Astrophysics . 598: L5. arXiv: 1610.03460 . Bibcode:2017A&A...598L...5A. doi:10.1051/0004-6361/201629671. S2CID   54002704.
  60. Stapledon, Olaf Star Maker 1937 Chapter 7 "More Worlds" Part 3 "Plant Men and Others"

Further reading