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Red dwarf

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.[1] 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.[2]

Proxima Centauri, the closest star to the Sun, at a distance of 4.2 ly (1.3 pc), is a red dwarf.

The coolest red dwarfs near the Sun have a surface temperature of about 2,000 K and the smallest have radii about 9% that of the Sun, with masses about 7.5% that of the Sun. These red dwarfs have spectral types of L0 to L2. There is some overlap with the properties of brown dwarfs, since the most massive brown dwarfs at lower metallicity can be as hot as 3,600 K and have late M spectral types.

Definitions and usage of the term "red dwarf" vary on how inclusive they are on the hotter and more massive end. One definition is synonymous with stellar M dwarfs (M-type main sequence stars), yielding a maximum temperature of 3,900 K and 0.6 M. One includes all stellar M-type main-sequence and all K-type main-sequence stars (K dwarf), yielding a maximum temperature of 5,200 K and 0.8 M. Some definitions include any stellar M dwarf and part of the K dwarf classification. Other definitions are also in use. Many of the coolest, lowest mass M dwarfs are expected to be brown dwarfs, not true stars, and so those would be excluded from any definition of red dwarf.

Stellar models indicate that red dwarfs less than 0.35 M are fully convective.[3] Hence, the helium produced by the thermonuclear fusion of hydrogen is constantly remixed throughout the star, avoiding helium buildup at the core, thereby prolonging the period of fusion. Low-mass red dwarfs therefore develop very slowly, maintaining a constant luminosity and spectral type for trillions of years, until their fuel is depleted. Because of the comparatively short age of the universe, no red dwarfs yet exist at advanced stages of evolution.

Definition edit

The term "red dwarf" when used to refer to a star does not have a strict definition. One of the earliest uses of the term was in 1915, used simply to contrast "red" dwarf stars from hotter "blue" dwarf stars.[4] It became established use, although the definition remained vague.[5] In terms of which spectral types qualify as red dwarfs, different researchers picked different limits, for example K8–M5[6] or "later than K5".[7] Dwarf M star, abbreviated dM, was also used, but sometimes it also included stars of spectral type K.[8]

In modern usage, the definition of a red dwarf still varies. When explicitly defined, it typically includes late K- and early to mid-M-class stars,[9] but in many cases it is restricted just to M-class stars.[10][11] In some cases all K stars are included as red dwarfs,[12] and occasionally even earlier stars.[13]

The most recent surveys place the coolest true main-sequence stars into spectral types L2 or L3. At the same time, many objects cooler than about M6 or M7 are brown dwarfs, insufficiently massive to sustain hydrogen-1 fusion.[14] This gives a significant overlap in spectral types for red and brown dwarfs. Objects in that spectral range can be difficult to categorize.

Description and characteristics edit

Red dwarfs are very-low-mass stars.[15] As a result, they have relatively low pressures, a low fusion rate, and hence, a low temperature. The energy generated is the product of nuclear fusion of hydrogen into helium by way of the proton–proton (PP) chain mechanism. Hence, these stars emit relatively little light, sometimes as little as 110,000 that of the Sun, although this would still imply a power output on the order of 1022 watts (10 trillion gigawatts or 10 ZW). Even the largest red dwarfs (for example HD 179930, HIP 12961 and Lacaille 8760) have only about 10% of the Sun's luminosity.[16] In general, red dwarfs less than 0.35 M transport energy from the core to the surface by convection. Convection occurs because of opacity of the interior, which has a high density compared to the temperature. As a result, energy transfer by radiation is decreased, and instead convection is the main form of energy transport to the surface of the star. Above this mass, a red dwarf will have a region around its core where convection does not occur.[17]

 
The predicted main-sequence lifetime of a red dwarf plotted against its mass relative to the Sun.[18]

Because low-mass red dwarfs are fully convective, helium does not accumulate at the core, and compared to larger stars such as the Sun, they can burn a larger proportion of their hydrogen before leaving the main sequence. As a result, red dwarfs have estimated lifespans far longer than the present age of the universe, and stars less than 0.8 M have not had time to leave the main sequence. The lower the mass of a red dwarf, the longer the lifespan. It is believed that the lifespan of these stars exceeds the expected 10-billion-year lifespan of the Sun by the third or fourth power of the ratio of the solar mass to their masses; thus, a 0.1 M red dwarf may continue burning for 10 trillion years.[15][19] As the proportion of hydrogen in a red dwarf is consumed, the rate of fusion declines and the core starts to contract. The gravitational energy released by this size reduction is converted into heat, which is carried throughout the star by convection.[20]

Properties of typical M-type main-sequence stars[21][22] [23]
Spectral
type
[24]
Mass (M) Radius (R) Luminosity (L) Effective
temperature

(K)
Color
index

(B − V)
M0V 0.57 0.588 0.069 3,850 1.42
M1V 0.50 0.501 0.041 3,660 1.49
M2V 0.44 0.446 0.029 3,560 1.51
M3V 0.37 0.361 0.016 3,430 1.53
M4V 0.23 0.274 7.2x10−3 3,210 1.65
M5V 0.162 0.196 3.0x10−3 3,060 1.83
M6V 0.102 0.137 1.0x10−3 2,810 2.01
M7V 0.090 0.120 6.5x10−4 2,680 2.12
M8V 0.085 0.114 5.2x10−4 2,570 2.15
M9V 0.079 0.102 3.0x10−4 2,380 2.17

According to computer simulations, the minimum mass a red dwarf must have to eventually evolve into a red giant is 0.25 M; less massive objects, as they age, would increase their surface temperatures and luminosities becoming blue dwarfs and finally white dwarfs.[18]

The less massive the star, the longer this evolutionary process takes. It has been calculated that a 0.16 M red dwarf (approximately the mass of the nearby Barnard's Star) would stay on the main sequence for 2.5 trillion years, followed by five billion years as a blue dwarf, during which the star would have one third of the Sun's luminosity (L) and a surface temperature of 6,500–8,500 kelvins.[18]

The fact that red dwarfs and other low-mass stars still remain on the main sequence when more massive stars have moved off the main sequence allows the age of star clusters to be estimated by finding the mass at which the stars move off the main sequence. This provides a lower limit to the age of the Universe and also allows formation timescales to be placed upon the structures within the Milky Way, such as the Galactic halo and Galactic disk.

All observed red dwarfs contain "metals", which in astronomy are elements heavier than hydrogen and helium. The Big Bang model predicts that the first generation of stars should have only hydrogen, helium, and trace amounts of lithium, and hence would be of low metallicity. With their extreme lifespans, any red dwarfs that were a part of that first generation (population III stars) should still exist today. Low-metallicity red dwarfs, however, are rare. The accepted model for the chemical evolution of the universe anticipates such a scarcity of metal-poor dwarf stars because only giant stars are thought to have formed in the metal-poor environment of the early universe.[why?] As giant stars end their short lives in supernova explosions, they spew out the heavier elements needed to form smaller stars. Therefore, dwarfs became more common as the universe aged and became enriched in metals. While the basic scarcity of ancient metal-poor red dwarfs is expected, observations have detected even fewer than predicted. The sheer difficulty of detecting objects as dim as red dwarfs was thought to account for this discrepancy, but improved detection methods have only confirmed the discrepancy.[25]

The boundary between the least massive red dwarfs and the most massive brown dwarfs depends strongly on the metallicity. At solar metallicity the boundary occurs at about 0.07 M, while at zero metallicity the boundary is around 0.09 M. At solar metallicity, the least massive red dwarfs theoretically have temperatures around 1,700 K, while measurements of red dwarfs in the solar neighbourhood suggest the coolest stars have temperatures of about 2,075 K and spectral classes of about L2. Theory predicts that the coolest red dwarfs at zero metallicity would have temperatures of about 3,600 K. The least massive red dwarfs have radii of about 0.09 R, while both more massive red dwarfs and less massive brown dwarfs are larger.[14][26]

Spectral standard stars edit

 
Gliese 623 is a pair of red dwarfs, with GJ 623a on the left and the fainter GJ 623b to the right of center.

The spectral standards for M type stars have changed slightly over the years, but settled down somewhat since the early 1990s. Part of this is due to the fact that even the nearest red dwarfs are fairly faint, and their colors do not register well on photographic emulsions used in the early to mid 20th century. The study of mid- to late-M dwarfs has significantly advanced only in the past few decades, primarily due to development of new astrographic and spectroscopic techniques, dispensing with photographic plates and progressing to charged-couple devices (CCDs) and infrared-sensitive arrays.

The revised Yerkes Atlas system (Johnson & Morgan, 1953)[27] listed only two M type spectral standard stars: HD 147379 (M0V) and HD 95735/Lalande 21185 (M2V). While HD 147379 was not considered a standard by expert classifiers in later compendia of standards, Lalande 21185 is still a primary standard for M2V. Robert Garrison[28] does not list any "anchor" standards among the red dwarfs, but Lalande 21185 has survived as a M2V standard through many compendia.[27][29][30] The review on MK classification by Morgan & Keenan (1973) did not contain red dwarf standards. In the mid-1970s, red dwarf standard stars were published by Keenan & McNeil (1976)[31] and Boeshaar (1976),[32] but unfortunately there was little agreement among the standards. As later cooler stars were identified through the 1980s, it was clear that an overhaul of the red dwarf standards was needed. Building primarily upon the Boeshaar standards, a group at Steward Observatory (Kirkpatrick, Henry, & McCarthy, 1991)[30] filled in the spectral sequence from K5V to M9V. It is these M type dwarf standard stars which have largely survived as the main standards to the modern day. There have been negligible changes in the red dwarf spectral sequence since 1991. Additional red dwarf standards were compiled by Henry et al. (2002),[33] and D. Kirkpatrick has recently reviewed the classification of red dwarfs and standard stars in Gray & Corbally's 2009 monograph.[34] The M dwarf primary spectral standards are: GJ 270 (M0V), GJ 229A (M1V), Lalande 21185 (M2V), Gliese 581 (M3V), Gliese 402 (M4V), GJ 51 (M5V), Wolf 359 (M6V), van Biesbroeck 8 (M7V), VB 10 (M8V), LHS 2924 (M9V).

Planets edit

 
Illustration depicting AU Mic, an M-type (spectral class M1Ve) red dwarf star less than 0.7% the age of the Sun. The dark areas represent huge sunspot-like regions.

Many red dwarfs are orbited by exoplanets, but large Jupiter-sized planets are comparatively rare. Doppler surveys of a wide variety of stars indicate about 1 in 6 stars with twice the mass of the Sun are orbited by one or more of Jupiter-sized planets, versus 1 in 16 for Sun-like stars and the frequency of close-in giant planets (Jupiter size or larger) orbiting red dwarfs is only 1 in 40.[35] On the other hand, microlensing surveys indicate that long-orbital-period Neptune-mass planets are found around one in three red dwarfs.[36] Observations with HARPS further indicate 40% of red dwarfs have a "super-Earth" class planet orbiting in the habitable zone where liquid water can exist on the surface.[37] Computer simulations of the formation of planets around low-mass stars predict that Earth-sized planets are most abundant, but more than 90% of the simulated planets are at least 10% water by mass, suggesting that many Earth-sized planets orbiting red dwarf stars are covered in deep oceans.[38]

At least four and possibly up to six exoplanets were discovered orbiting within the Gliese 581 planetary system between 2005 and 2010. One planet has about the mass of Neptune, or 16 Earth masses (ME). It orbits just 6 million kilometers (0.04 AU) from its star, and is estimated to have a surface temperature of 150°C, despite the dimness of its star. In 2006, an even smaller exoplanet (only 5.5 ME) was found orbiting the red dwarf OGLE-2005-BLG-390L; it lies 390 million km (2.6 AU) from the star and its surface temperature is −220 °C (53 K).

In 2007, a new, potentially habitable exoplanet, Gliese 581c, was found, orbiting Gliese 581. The minimum mass estimated by its discoverers (a team led by Stephane Udry) is 5.36 ME. The discoverers estimate its radius to be 1.5 times that of Earth (R🜨). Since then Gliese 581d, which is also potentially habitable, was discovered.

Gliese 581c and d are within the habitable zone of the host star, and are two of the most likely candidates for habitability of any exoplanets discovered so far.[39] Gliese 581g, detected September 2010,[40] has a near-circular orbit in the middle of the star's habitable zone. However, the planet's existence is contested.[41]

On 23 February 2017 NASA announced the discovery of seven Earth-sized planets orbiting the red dwarf star TRAPPIST-1 approximately 39 light-years away in the constellation Aquarius. The planets were discovered through the transit method, meaning we have mass and radius information for all of them. TRAPPIST-1e, f, and g appear to be within the habitable zone and may have liquid water on the surface.[42]

Habitability edit

 
An artist's impression of a planet with two exomoons orbiting in the habitable zone of a red dwarf.

Modern evidence suggests that planets in red dwarf systems are extremely unlikely to be habitable. In spite of their great numbers and long lifespans, there are several factors which may make life difficult on planets around a red dwarf. First, planets in the habitable zone of a red dwarf would be so close to the parent star that they would likely be tidally locked. For a nearly circular orbit, this would mean that one side would be in perpetual daylight and the other in eternal night. This could create enormous temperature variations from one side of the planet to the other. Such conditions would appear to make it difficult for forms of life similar to those on Earth to evolve. And it appears there is a great problem with the atmosphere of such tidally locked planets: the perpetual night zone would be cold enough to freeze the main gases of their atmospheres, leaving the daylight zone bare and dry. On the other hand, though, a theory proposes that either a thick atmosphere or planetary ocean could potentially circulate heat around such a planet.[43]

Variability in stellar energy output may also have negative impacts on the development of life. Red dwarfs are often flare stars, which can emit gigantic flares, doubling their brightness in minutes. This variability makes it difficult for life to develop and persist near a red dwarf.[44] While it may be possible for a planet orbiting close to a red dwarf to keep its atmosphere even if the star flares, more-recent research suggests that these stars may be the source of constant high-energy flares and very large magnetic fields, diminishing the possibility of life as we know it.[45][46]

See also edit

References edit

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  36. ^ Johnson, J.A. (April 2011). "The stars that host planets". Sky & Telescope. pp. 22–27.
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Sources edit

  • Burrows, Adam; Hubbard, William B.; Saumon, Didier; Lunine, Jonathan I. (1993). "An expanded set of brown dwarf and very low mass star models". Astrophysical Journal. 406 (1): 158–71. Bibcode:1993ApJ...406..158B. doi:10.1086/172427.
  • . European Southern Observatory. November 19, 2002. Archived from the original on January 3, 2007. Retrieved 2007-01-12.
  • Neptune-Size Planet Orbiting Common Star Hints at Many More

External links edit

  • Variable stars AAVSO
  • Stellar Flares Publications about Flares by the Stellar Activity Group (UCM)
  • Red Dwarfs Jumk.de
  • Red Star Rising : Small, cool stars may be hot spots for life – Scientific American (November 2005)

dwarf, this, article, about, type, star, british, comedy, franchise, dwarf, dwarf, redirects, here, substellar, objects, brown, dwarf, dwarf, smallest, kind, star, main, sequence, most, common, type, fusing, star, milky, least, neighborhood, however, their, lu. This article is about the type of star For the British comedy franchise see Red Dwarf M dwarf redirects here For substellar objects see brown dwarf 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 1 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 2 Proxima Centauri the closest star to the Sun at a distance of 4 2 ly 1 3 pc is a red dwarf The coolest red dwarfs near the Sun have a surface temperature of about 2 000 K and the smallest have radii about 9 that of the Sun with masses about 7 5 that of the Sun These red dwarfs have spectral types of L0 to L2 There is some overlap with the properties of brown dwarfs since the most massive brown dwarfs at lower metallicity can be as hot as 3 600 K and have late M spectral types Definitions and usage of the term red dwarf vary on how inclusive they are on the hotter and more massive end One definition is synonymous with stellar M dwarfs M type main sequence stars yielding a maximum temperature of 3 900 K and 0 6 M One includes all stellar M type main sequence and all K type main sequence stars K dwarf yielding a maximum temperature of 5 200 K and 0 8 M Some definitions include any stellar M dwarf and part of the K dwarf classification Other definitions are also in use Many of the coolest lowest mass M dwarfs are expected to be brown dwarfs not true stars and so those would be excluded from any definition of red dwarf Stellar models indicate that red dwarfs less than 0 35 M are fully convective 3 Hence the helium produced by the thermonuclear fusion of hydrogen is constantly remixed throughout the star avoiding helium buildup at the core thereby prolonging the period of fusion Low mass red dwarfs therefore develop very slowly maintaining a constant luminosity and spectral type for trillions of years until their fuel is depleted Because of the comparatively short age of the universe no red dwarfs yet exist at advanced stages of evolution Contents 1 Definition 2 Description and characteristics 3 Spectral standard stars 4 Planets 5 Habitability 6 See also 7 References 8 Sources 9 External linksDefinition editThe term red dwarf when used to refer to a star does not have a strict definition One of the earliest uses of the term was in 1915 used simply to contrast red dwarf stars from hotter blue dwarf stars 4 It became established use although the definition remained vague 5 In terms of which spectral types qualify as red dwarfs different researchers picked different limits for example K8 M5 6 or later than K5 7 Dwarf M star abbreviated dM was also used but sometimes it also included stars of spectral type K 8 In modern usage the definition of a red dwarf still varies When explicitly defined it typically includes late K and early to mid M class stars 9 but in many cases it is restricted just to M class stars 10 11 In some cases all K stars are included as red dwarfs 12 and occasionally even earlier stars 13 The most recent surveys place the coolest true main sequence stars into spectral types L2 or L3 At the same time many objects cooler than about M6 or M7 are brown dwarfs insufficiently massive to sustain hydrogen 1 fusion 14 This gives a significant overlap in spectral types for red and brown dwarfs Objects in that spectral range can be difficult to categorize Description and characteristics edit nbsp Hertzsprung Russell diagram Spectral type O B A F G K M L T Brown dwarfs White dwarfs Red dwarfs Subdwarfs Main sequence dwarfs Subgiants Giants Red giants Blue giants Bright giants Supergiants Red supergiant Hypergiants absolutemagni tude MV Red dwarfs are very low mass stars 15 As a result they have relatively low pressures a low fusion rate and hence a low temperature The energy generated is the product of nuclear fusion of hydrogen into helium by way of the proton proton PP chain mechanism Hence these stars emit relatively little light sometimes as little as 1 10 000 that of the Sun although this would still imply a power output on the order of 1022 watts 10 trillion gigawatts or 10 ZW Even the largest red dwarfs for example HD 179930 HIP 12961 and Lacaille 8760 have only about 10 of the Sun s luminosity 16 In general red dwarfs less than 0 35 M transport energy from the core to the surface by convection Convection occurs because of opacity of the interior which has a high density compared to the temperature As a result energy transfer by radiation is decreased and instead convection is the main form of energy transport to the surface of the star Above this mass a red dwarf will have a region around its core where convection does not occur 17 nbsp The predicted main sequence lifetime of a red dwarf plotted against its mass relative to the Sun 18 Because low mass red dwarfs are fully convective helium does not accumulate at the core and compared to larger stars such as the Sun they can burn a larger proportion of their hydrogen before leaving the main sequence As a result red dwarfs have estimated lifespans far longer than the present age of the universe and stars less than 0 8 M have not had time to leave the main sequence The lower the mass of a red dwarf the longer the lifespan It is believed that the lifespan of these stars exceeds the expected 10 billion year lifespan of the Sun by the third or fourth power of the ratio of the solar mass to their masses thus a 0 1 M red dwarf may continue burning for 10 trillion years 15 19 As the proportion of hydrogen in a red dwarf is consumed the rate of fusion declines and the core starts to contract The gravitational energy released by this size reduction is converted into heat which is carried throughout the star by convection 20 Properties of typical M type main sequence stars 21 22 23 Spectraltype 24 Mass M Radius R Luminosity L Effectivetemperature K Colorindex B V M0V 0 57 0 588 0 069 3 850 1 42 M1V 0 50 0 501 0 041 3 660 1 49 M2V 0 44 0 446 0 029 3 560 1 51 M3V 0 37 0 361 0 016 3 430 1 53 M4V 0 23 0 274 7 2x10 3 3 210 1 65 M5V 0 162 0 196 3 0x10 3 3 060 1 83 M6V 0 102 0 137 1 0x10 3 2 810 2 01 M7V 0 090 0 120 6 5x10 4 2 680 2 12 M8V 0 085 0 114 5 2x10 4 2 570 2 15 M9V 0 079 0 102 3 0x10 4 2 380 2 17 According to computer simulations the minimum mass a red dwarf must have to eventually evolve into a red giant is 0 25 M less massive objects as they age would increase their surface temperatures and luminosities becoming blue dwarfs and finally white dwarfs 18 The less massive the star the longer this evolutionary process takes It has been calculated that a 0 16 M red dwarf approximately the mass of the nearby Barnard s Star would stay on the main sequence for 2 5 trillion years followed by five billion years as a blue dwarf during which the star would have one third of the Sun s luminosity L and a surface temperature of 6 500 8 500 kelvins 18 The fact that red dwarfs and other low mass stars still remain on the main sequence when more massive stars have moved off the main sequence allows the age of star clusters to be estimated by finding the mass at which the stars move off the main sequence This provides a lower limit to the age of the Universe and also allows formation timescales to be placed upon the structures within the Milky Way such as the Galactic halo and Galactic disk All observed red dwarfs contain metals which in astronomy are elements heavier than hydrogen and helium The Big Bang model predicts that the first generation of stars should have only hydrogen helium and trace amounts of lithium and hence would be of low metallicity With their extreme lifespans any red dwarfs that were a part of that first generation population III stars should still exist today Low metallicity red dwarfs however are rare The accepted model for the chemical evolution of the universe anticipates such a scarcity of metal poor dwarf stars because only giant stars are thought to have formed in the metal poor environment of the early universe why As giant stars end their short lives in supernova explosions they spew out the heavier elements needed to form smaller stars Therefore dwarfs became more common as the universe aged and became enriched in metals While the basic scarcity of ancient metal poor red dwarfs is expected observations have detected even fewer than predicted The sheer difficulty of detecting objects as dim as red dwarfs was thought to account for this discrepancy but improved detection methods have only confirmed the discrepancy 25 The boundary between the least massive red dwarfs and the most massive brown dwarfs depends strongly on the metallicity At solar metallicity the boundary occurs at about 0 07 M while at zero metallicity the boundary is around 0 09 M At solar metallicity the least massive red dwarfs theoretically have temperatures around 1 700 K while measurements of red dwarfs in the solar neighbourhood suggest the coolest stars have temperatures of about 2 075 K and spectral classes of about L2 Theory predicts that the coolest red dwarfs at zero metallicity would have temperatures of about 3 600 K The least massive red dwarfs have radii of about 0 09 R while both more massive red dwarfs and less massive brown dwarfs are larger 14 26 Spectral standard stars edit nbsp Gliese 623 is a pair of red dwarfs with GJ 623a on the left and the fainter GJ 623b to the right of center The spectral standards for M type stars have changed slightly over the years but settled down somewhat since the early 1990s Part of this is due to the fact that even the nearest red dwarfs are fairly faint and their colors do not register well on photographic emulsions used in the early to mid 20th century The study of mid to late M dwarfs has significantly advanced only in the past few decades primarily due to development of new astrographic and spectroscopic techniques dispensing with photographic plates and progressing to charged couple devices CCDs and infrared sensitive arrays The revised Yerkes Atlas system Johnson amp Morgan 1953 27 listed only two M type spectral standard stars HD 147379 M0V and HD 95735 Lalande 21185 M2V While HD 147379 was not considered a standard by expert classifiers in later compendia of standards Lalande 21185 is still a primary standard for M2V Robert Garrison 28 does not list any anchor standards among the red dwarfs but Lalande 21185 has survived as a M2V standard through many compendia 27 29 30 The review on MK classification by Morgan amp Keenan 1973 did not contain red dwarf standards In the mid 1970s red dwarf standard stars were published by Keenan amp McNeil 1976 31 and Boeshaar 1976 32 but unfortunately there was little agreement among the standards As later cooler stars were identified through the 1980s it was clear that an overhaul of the red dwarf standards was needed Building primarily upon the Boeshaar standards a group at Steward Observatory Kirkpatrick Henry amp McCarthy 1991 30 filled in the spectral sequence from K5V to M9V It is these M type dwarf standard stars which have largely survived as the main standards to the modern day There have been negligible changes in the red dwarf spectral sequence since 1991 Additional red dwarf standards were compiled by Henry et al 2002 33 and D Kirkpatrick has recently reviewed the classification of red dwarfs and standard stars in Gray amp Corbally s 2009 monograph 34 The M dwarf primary spectral standards are GJ 270 M0V GJ 229A M1V Lalande 21185 M2V Gliese 581 M3V Gliese 402 M4V GJ 51 M5V Wolf 359 M6V van Biesbroeck 8 M7V VB 10 M8V LHS 2924 M9V Planets edit nbsp Illustration depicting AU Mic an M type spectral class M1Ve red dwarf star less than 0 7 the age of the Sun The dark areas represent huge sunspot like regions Many red dwarfs are orbited by exoplanets but large Jupiter sized planets are comparatively rare Doppler surveys of a wide variety of stars indicate about 1 in 6 stars with twice the mass of the Sun are orbited by one or more of Jupiter sized planets versus 1 in 16 for Sun like stars and the frequency of close in giant planets Jupiter size or larger orbiting red dwarfs is only 1 in 40 35 On the other hand microlensing surveys indicate that long orbital period Neptune mass planets are found around one in three red dwarfs 36 Observations with HARPS further indicate 40 of red dwarfs have a super Earth class planet orbiting in the habitable zone where liquid water can exist on the surface 37 Computer simulations of the formation of planets around low mass stars predict that Earth sized planets are most abundant but more than 90 of the simulated planets are at least 10 water by mass suggesting that many Earth sized planets orbiting red dwarf stars are covered in deep oceans 38 At least four and possibly up to six exoplanets were discovered orbiting within the Gliese 581 planetary system between 2005 and 2010 One planet has about the mass of Neptune or 16 Earth masses ME It orbits just 6 million kilometers 0 04 AU from its star and is estimated to have a surface temperature of 150 C despite the dimness of its star In 2006 an even smaller exoplanet only 5 5 ME was found orbiting the red dwarf OGLE 2005 BLG 390L it lies 390 million km 2 6 AU from the star and its surface temperature is 220 C 53 K In 2007 a new potentially habitable exoplanet Gliese 581c was found orbiting Gliese 581 The minimum mass estimated by its discoverers a team led by Stephane Udry is 5 36 ME The discoverers estimate its radius to be 1 5 times that of Earth R Since then Gliese 581d which is also potentially habitable was discovered Gliese 581c and d are within the habitable zone of the host star and are two of the most likely candidates for habitability of any exoplanets discovered so far 39 Gliese 581g detected September 2010 40 has a near circular orbit in the middle of the star s habitable zone However the planet s existence is contested 41 On 23 February 2017 NASA announced the discovery of seven Earth sized planets orbiting the red dwarf star TRAPPIST 1 approximately 39 light years away in the constellation Aquarius The planets were discovered through the transit method meaning we have mass and radius information for all of them TRAPPIST 1e f and g appear to be within the habitable zone and may have liquid water on the surface 42 Habitability editMain article Habitability of red dwarf systems nbsp An artist s impression of a planet with two exomoons orbiting in the habitable zone of a red dwarf Modern evidence suggests that planets in red dwarf systems are extremely unlikely to be habitable In spite of their great numbers and long lifespans there are several factors which may make life difficult on planets around a red dwarf First planets in the habitable zone of a red dwarf would be so close to the parent star that they would likely be tidally locked For a nearly circular orbit this would mean that one side would be in perpetual daylight and the other in eternal night This could create enormous temperature variations from one side of the planet to the other Such conditions would appear to make it difficult for forms of life similar to those on Earth to evolve And it appears there is a great problem with the atmosphere of such tidally locked planets the perpetual night zone would be cold enough to freeze the main gases of their atmospheres leaving the daylight zone bare and dry On the other hand though a theory proposes that either a thick atmosphere or planetary ocean could potentially circulate heat around such a planet 43 Variability in stellar energy output may also have negative impacts on the development of life Red dwarfs are often flare stars which can emit gigantic flares doubling their brightness in minutes This variability makes it difficult for life to develop and persist near a red dwarf 44 While it may be possible for a planet orbiting close to a red dwarf to keep its atmosphere even if the star flares more recent research suggests that these stars may be the source of constant high energy flares and very large magnetic fields diminishing the possibility of life as we know it 45 46 See also editList of red dwarfs Aurelia and Blue Moon Hypothetical examples of a planet and a moon supporting extraterrestrial life Cataclysmic variable star Stars with irregular large fluctuations in brightness Nemesis hypothetical star Hypothetical star orbiting the Sun supposedly responsible for extinction events Star count bookkeeping survey of starsPages displaying wikidata descriptions as a fallback Stellar evolution Changes to stars over their lifespans Kapteyn s Star Subdwarf star in the constellation Pictor Yerkes luminosity classification Classification of stars based on spectral propertiesPages displaying short descriptions of redirect targetsReferences edit Ken Croswell The Brightest Red Dwarf Retrieved 2019 07 10 Jason Palmer 6 February 2013 Exoplanets near red dwarfs suggest another Earth nearer BBC Retrieved 2019 07 10 Reiners Ansgar Basri Gibor March 2009 On the magnetic topology of partially and fully convective stars Astronomy and Astrophysics 496 3 787 790 arXiv 0901 1659 Bibcode 2009A amp A 496 787R doi 10 1051 0004 6361 200811450 S2CID 15159121 Lindemann F A 1915 The age of the Earth The Observatory 38 299 Bibcode 1915Obs 38 299L Edgeworth K E 1946 Red Dwarf Stars Nature 157 3989 481 Bibcode 1946Natur 157 481E doi 10 1038 157481d0 S2CID 4106298 Dyer Edward R 1956 An analysis of the space motions of red dwarf stars Astronomical Journal 61 228 Bibcode 1956AJ 61 228D doi 10 1086 107332 Mumford George S 1956 The motions and distribution of dwarf M stars Astronomical Journal 61 224 Bibcode 1956AJ 61 224M doi 10 1086 107331 Vyssotsky A N 1956 Dwarf M stars found spectrophotometrically Astronomical Journal 61 201 Bibcode 1956AJ 61 201V doi 10 1086 107328 Engle S G Guinan E F 2011 Red Dwarf Stars Ages Rotation Magnetic Dynamo Activity and the Habitability of Hosted Planets 9th Pacific Rim Conference on Stellar Astrophysics Proceedings of a Conference Held at Lijiang 451 285 arXiv 1111 2872 Bibcode 2011ASPC 451 285E Heath Martin J Doyle Laurance R Joshi Manoj M Haberle Robert M 1999 Habitability of planets around red dwarf stars Origins of Life and Evolution of the Biosphere 29 4 405 24 Bibcode 1999OLEB 29 405H doi 10 1023 A 1006596718708 PMID 10472629 S2CID 12329736 Farihi J Hoard D W Wachter S 2006 White Dwarf Red Dwarf Systems Resolved with the Hubble Space Telescope I First Results The Astrophysical Journal 646 1 480 492 arXiv astro ph 0603747 Bibcode 2006ApJ 646 480F doi 10 1086 504683 S2CID 16750158 Pettersen B R Hawley S L 1989 A spectroscopic survey of red dwarf flare stars Astronomy and Astrophysics 217 187 Bibcode 1989A amp A 217 187P Alekseev I Yu Kozlova O V 2002 Starspots and active regions on the emission red dwarf star LQ Hydrae Astronomy and Astrophysics 396 203 211 Bibcode 2002A amp A 396 203A doi 10 1051 0004 6361 20021424 a b Dieterich Sergio B Henry Todd J Jao Wei Chun Winters Jennifer G Hosey Altonio D Riedel Adric R Subasavage John P 2014 The Solar Neighborhood XXXII The Hydrogen Burning Limit The Astronomical Journal 147 5 94 arXiv 1312 1736 Bibcode 2014AJ 147 94D doi 10 1088 0004 6256 147 5 94 S2CID 21036959 a b Richmond Michael November 10 2004 Late stages of evolution for low mass stars Rochester Institute of Technology Retrieved 2019 07 10 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 Padmanabhan Thanu 2001 Theoretical Astrophysics Cambridge University Press pp 96 99 ISBN 0 521 56241 4 a b c Adams Fred C Laughlin Gregory Graves Genevieve J M 2004 Red Dwarfs and the End of the Main Sequence PDF Gravitational Collapse From Massive Stars to Planets Revista Mexicana de Astronomia y Astrofisica pp 46 49 Bibcode 2004RMxAC 22 46A Fred C Adams amp Gregory Laughlin 1997 A Dying Universe The Long Term Fate and Evolution of Astrophysical Objects Reviews of Modern Physics 69 2 337 372 arXiv astro ph 9701131 Bibcode 1997RvMP 69 337A doi 10 1103 RevModPhys 69 337 S2CID 12173790 Koupelis Theo 2007 In Quest of the Universe Jones amp Bartlett Publishers ISBN 978 0 7637 4387 1 Pecaut Mark J Mamajek Eric E 1 September 2013 Intrinsic Colors Temperatures and Bolometric Corrections of Pre main sequence Stars The Astrophysical Journal Supplement Series 208 1 9 arXiv 1307 2657 Bibcode 2013ApJS 208 9P doi 10 1088 0067 0049 208 1 9 ISSN 0067 0049 S2CID 119308564 Mamajek Eric 2 March 2021 A Modern Mean Dwarf Stellar Color and Effective Temperature Sequence University of Rochester Department of Physics and Astronomy Retrieved 5 July 2021 Cifuentes C Caballero J A Cortes Contreras M Montes D Abellan F J Dorda R Holgado G 2020 CARMENES input catalogue of M dwarfs V Luminosities colours and spectral energy distributions Astronomy and Astrophysics 642 October 2020 32 arXiv 2007 15077 Bibcode 2020A amp A 642A 115C doi 10 1051 0004 6361 202038295 Younger brown dwarfs may also exhibit spectra similar to late M type stars Elisabeth Newton Feb 15 2012 And now there s a problem with M dwarfs too Astrobites Retrieved 2019 07 10 Burrows Adam Hubbard William B Lunine Jonathan I Liebert James 2001 The theory of brown dwarfs and extrasolar giant planets Reviews of Modern Physics 73 3 719 765 arXiv astro ph 0103383 Bibcode 2001RvMP 73 719B doi 10 1103 RevModPhys 73 719 S2CID 204927572 a b Johnson H L Morgan W W 1953 Fundamental stellar photometry for standards of spectral type on the revised system of the Yerkes spectral atlas Astrophysical Journal 117 313 Bibcode 1953ApJ 117 313J doi 10 1086 145697 Garrison Robert F MK anchor point standards table Department of Astronomy amp Astrophysics astro utoronto ca University of Toronto Archived from the original on 2019 06 25 Retrieved 2011 12 18 Keenan Philip C McNeil Raymond C 1989 The Perkins catalog of revised MK types for the cooler stars Astrophysical Journal Supplement Series 71 245 Bibcode 1989ApJS 71 245K doi 10 1086 191373 S2CID 123149047 a b Kirkpatrick J D Henry Todd J McCarthy Donald W 1991 A standard stellar spectral sequence in the red near infrared Classes K5 to M9 Astrophysical Journal Supplement Series 77 417 Bibcode 1991ApJS 77 417K doi 10 1086 191611 Keenan Philip Childs McNeil Raymond C 1976 An atlas of spectra of the cooler stars Types G K M S and C Part 1 Introduction and tables Columbus OH Ohio State University Press Bibcode 1976aasc book K Boeshaar P C 1976 The spectral classification of M dwarf stars Ph D thesis Columbus OH Ohio State University Bibcode 1976PhDT 14B Henry Todd J Walkowicz Lucianne M Barto Todd C Golimowski David A 2002 The Solar neighborhood VI New southern nearby stars identified by optical spectroscopy The Astronomical Journal 123 4 2002 arXiv astro ph 0112496 Bibcode 2002AJ 123 2002H doi 10 1086 339315 S2CID 17735847 Gray Richard O Corbally Christopher 2009 Stellar Spectral Classification Princeton University Press Bibcode 2009ssc book G Mawet Dimitri Jovanovic Nemanja Delorme Jacques Robert et al 2018 07 10 Keck Planet Imager and Characterizer KPIC status update PDF In Schmidt Dirk Schreiber Laura Close Laird M eds Adaptive Optics Systems VI SPIE p 6 doi 10 1117 12 2314037 ISBN 9781510619593 Close separations lt 1 AU have been extensively probed by Doppler and transit surveys with the following results the frequency of close in giant planets 1 10 M Jup is only 2 5 0 9 consistent with core accretion plus migration models Johnson J A April 2011 The stars that host planets Sky amp Telescope pp 22 27 Billions of rocky planets in habitable zones around red dwarfs European Southern Observatory 28 March 2012 Retrieved 10 July 2019 permanent dead link Alibert Yann 2017 Formation and composition of planets around very low mass stars Astronomy and Astrophysics 539 12 October 2016 8 arXiv 1610 03460 Bibcode 2017A amp A 598L 5A doi 10 1051 0004 6361 201629671 S2CID 54002704 Than Ker 24 April 2007 Major discovery New planet could harbor water and life SPACE com Retrieved 2019 07 10 Scientists find potentially habitable planet near Earth Physorg com Retrieved 2013 03 26 Tuomi Mikko 2011 Bayesian re analysis of the radial velocities of Gliese 581 Evidence in favour of only four planetary companions Astronomy amp Astrophysics 528 L5 arXiv 1102 3314 Bibcode 2011A amp A 528L 5T doi 10 1051 0004 6361 201015995 S2CID 11439465 NASA telescope reveals record breaking exoplanet discovery www nasa gov 22 February 2017 Charles Q Choi 9 February 2015 Planets Orbiting Red Dwarfs May Stay Wet Enough for Life Astrobiology Archived from the original on 2015 09 21 Retrieved 15 January 2017 a href Template Cite web html title Template Cite web cite web a CS1 maint unfit URL link Vida K Kovari Zs Pal A Olah K Kriskovics L et al 2017 Frequent Flaring in the TRAPPIST 1 System Unsuited for Life The Astrophysical Journal 841 2 2 arXiv 1703 10130 Bibcode 2017ApJ 841 124V doi 10 3847 1538 4357 aa6f05 S2CID 118827117 Alpert Mark 1 November 2005 Red Star Rising Scientific American George Dvorsky 2015 11 19 This Stormy Star Means Alien Life May Be Rarer Than We Thought Gizmodo Retrieved 2019 07 10 Sources editBurrows Adam Hubbard William B Saumon Didier Lunine Jonathan I 1993 An expanded set of brown dwarf and very low mass star models Astrophysical Journal 406 1 158 71 Bibcode 1993ApJ 406 158B doi 10 1086 172427 VLT Interferometer Measures the Size of Proxima Centauri and Other Nearby Stars European Southern Observatory November 19 2002 Archived from the original on January 3 2007 Retrieved 2007 01 12 Neptune Size Planet Orbiting Common Star Hints at Many MoreExternal links edit nbsp Look up red dwarf in Wiktionary the free dictionary nbsp Wikimedia Commons has media related to Red dwarfs Variable stars AAVSO Stellar Flares Publications about Flares by the Stellar Activity Group UCM Red Dwarfs Jumk de Red Star Rising Small cool stars may be hot spots for life Scientific American November 2005 Portals nbsp Astronomy nbsp Stars nbsp Outer space Retrieved from https en wikipedia org w index php title Red dwarf amp oldid 1222099917, wikipedia, wiki, book, books, library,

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