Movatterモバイル変換


[0]ホーム

URL:


Jump to content
WikipediaThe Free Encyclopedia
Search

Astrophysical jet

From Wikipedia, the free encyclopedia
Stream of ionized matter flowing away from a rotating astronomical object
Thestarburst galaxyCentaurus A, with its plasma jets extending over a millionlight years, is considered as the closestactiveradio galaxy toEarth. The 870-micronsubmillimetre data, fromLABOCA on APEX, are shown in orange.X-ray data from theChandra X-ray Observatory are shown inblue.Visible light data from theWide Field Imager (WFI) on the MPG/ESO 2.2 m telescope located atLa Silla, Chile, show the backgroundstars and the galaxy's characteristicdust lane in close to "true colour".

Anastrophysical jet is anastronomical phenomenon whereionised matter is expelled at high velocity from an astronomical object, in a pair of narrow streams aligned with the object'saxis of rotation.[1] When the matter in the beam approaches thespeed of light, astrophysical jets becomerelativistic jets as they show effects fromspecial relativity.

Astrophysical jets are associated with many types ofhigh-energy astronomical sources, such asblack holes,neutron stars andpulsars. Their causes are not yet fully understood, but they are believed to arise from dynamic interactions withinaccretion disks. One explanation is that as an accretion disk spins, it generates a rotating, tangledmagnetic field which concentrates material from the disk into the jets and then drives it away from the central object.[2] Jets may also be influenced by ageneral relativity effect known asframe-dragging.[3]

Most of the largest and most active jets are created bysupermassive black holes (SMBH) in the centre ofactive galaxies such asquasars and radio galaxies or within galaxy clusters.[4] Such jets can exceed millions ofparsecs in length.[2] Other astronomical objects that produce, or are caused by, jets includecataclysmic variable stars,X-ray binaries andgamma-ray bursts (GRB). Jets on a much smaller scale (~parsecs) may be found in star forming regions, includingT Tauri stars andHerbig–Haro objects; these objects are partially formed by the interaction of jets with theinterstellar medium.Bipolar outflows may also be associated withprotostars,[5] or with evolvedpost-AGB stars,planetary nebulae andbipolar nebulae.

Relativistic jets

[edit]

Elliptical galaxy M87 emitting a relativistic jet, as seen by theHubble Space Telescope

Relativistic jets are beams of ionised matter accelerated close to the speed of light. Most have been observationally associated with central black holes of someactive galaxies,radio galaxies orquasars, and also by galacticstellar black holes,neutron stars orpulsars. Beam lengths may extend between several thousand,[6] hundreds of thousands[7] or millions of parsecs.[2] Jet velocities when approaching the speed of light show significant effects of thespecial theory of relativity; for example,relativistic beaming that changes the apparent beam brightness.[8]

Massive central black holes in galaxies have the most powerful jets, but their structure and behaviours are similar to those of smaller galacticneutron stars and black holes. These SMBH systems are often calledmicroquasars and show a large range of velocities.SS 433 jet, for example, has a mean velocity of 0.26c.[9] Relativistic jet formation may also explain observed gamma-ray bursts, which have the most relativistic jets known, beingultrarelativistic.[10]

Mechanisms behind the composition of jets remain uncertain,[11] though some studies favour models where jets are composed of an electrically neutral mixture ofnuclei,electrons, andpositrons, while others are consistent with jets composed of positron–electron plasma.[12][13][14] Trace nuclei swept up in a relativistic positron–electron jet would be expected to have extremely high energy, as these heavier nuclei should attain velocity equal to the positron and electron velocity.

Rotation as possible energy source

[edit]

Because of the enormous amount of energy needed to launch a relativistic jet, some jets are possibly powered by spinningblack holes. However, the frequency of high-energy astrophysical sources with jets suggests combinations of different mechanisms indirectly identified with the energy within the associated accretion disk and X-ray emissions from the generating source. Two early theories have been used to explain how energy can be transferred from a black hole into an astrophysical jet:

Relativistic jets from neutron stars

[edit]
The pulsar IGR J11014-6103 with supernova remnant origin, nebula and jet

Jets may also be observed from spinning neutron stars. An example is pulsarIGR J11014-6103, which has the largest jet so far observed in theMilky Way, and whose velocity is estimated at 80% the speed of light (0.8c). X-ray observations have been obtained, but there is no detected radio signature nor accretion disk.[19][20] Initially, this pulsar was presumed to be rapidly spinning, but later measurements indicate the spin rate is only 15.9 Hz.[21][22] Such a slow spin rate and lack of accretion material suggest the jet is neither rotation nor accretion powered, though it appears aligned with the pulsar rotation axis and perpendicular to the pulsar's true motion.

Other images

[edit]
  • Illustration of the dynamics of a proplyd, including a jet
    Illustration of the dynamics of aproplyd, including a jet
  • Centaurus A in x-rays showing the relativistic jet
    Centaurus A in x-rays showing the relativistic jet
  • The M87 jet seen by the Very Large Array in radio frequency (the viewing field is larger and rotated with respect to the above image.)
    The M87 jet seen by theVery Large Array inradio frequency (the viewing field is larger and rotated with respect to the above image.)
  • Hubble Legacy Archive Near-UV image of the relativistic jet in 3C 66B
    Hubble Legacy Archive Near-UV image of the relativistic jet in3C 66B
  • Galaxy NGC 3862, an extragalactic jet of material moving at nearly the speed of light can be seen at the three o'clock position.
    GalaxyNGC 3862, an extragalactic jet of material moving at nearly the speed of light can be seen at the three o'clock position.
  • Some of the jets in HH 24-26, which contains the highest concentration of jets known anywhere in the sky
    Some of the jets inHH 24-26, which contains the highest concentration of jets known anywhere in the sky

See also

[edit]

References

[edit]
  1. ^Beall, J. H. (2015)."A Review of Astrophysical Jets"(PDF).Proceedings of Science: 58.Bibcode:2015mbhe.confE..58B.doi:10.22323/1.246.0058. Retrieved19 February 2017.
  2. ^abcKundt, W. (2014)."A Uniform Description of All the Astrophysical Jets"(PDF).Proceedings of Science: 58.Bibcode:2015mbhe.confE..58B.doi:10.22323/1.246.0058. Retrieved19 February 2017.
  3. ^Miller-Jones, James (April 2019)."A rapidly changing jet orientation in the stellar-mass black-hole system V404 Cygni"(PDF).Nature.569 (7756):374–377.arXiv:1906.05400.Bibcode:2019Natur.569..374M.doi:10.1038/s41586-019-1152-0.PMID 31036949.S2CID 139106116.
  4. ^Beall, J. H (2014)."A review of Astrophysical Jets".Acta Polytechnica CTU Proceedings.1 (1):259–264.Bibcode:2014mbhe.conf..259B.doi:10.14311/APP.2014.01.0259.
  5. ^"Star sheds via reverse whirlpool".Astronomy.com. 27 December 2007. Retrieved26 May 2015.
  6. ^Biretta, J. (6 Jan 1999)."Hubble Detects Faster-Than-Light Motion in Galaxy M87".
  7. ^"Evidence for Ultra-Energetic Particles in Jet from Black Hole". Yale University – Office of Public Affairs. 20 June 2006. Archived fromthe original on 2008-05-13.
  8. ^Semenov, V.; Dyadechkin, S.; Punsly, B. (2004)."Simulations of Jets Driven by Black Hole Rotation".Science.305 (5686):978–980.arXiv:astro-ph/0408371.Bibcode:2004Sci...305..978S.doi:10.1126/science.1100638.PMID 15310894.S2CID 1590734.
  9. ^Blundell, Katherine (December 2008)."Jet Velocity in SS 433: Its Anticorrelation with Precession-Cone Angle and Dependence on Orbital Phase".The Astrophysical Journal.622 (2): 129.arXiv:astro-ph/0410457.doi:10.1086/429663. Retrieved15 January 2021.
  10. ^Dereli-Bégué, Hüsne; Pe’er, Asaf; Ryde, Felix; Oates, Samantha R.; Zhang, Bing; Dainotti, Maria G. (2022-09-24)."A wind environment and Lorentz factors of tens explain gamma-ray bursts X-ray plateau".Nature Communications.13 (1): 5611.arXiv:2207.11066.Bibcode:2022NatCo..13.5611D.doi:10.1038/s41467-022-32881-1.ISSN 2041-1723.PMC 9509382.PMID 36153328.
  11. ^Georganopoulos, M.; Kazanas, D.; Perlman, E.; Stecker, F. W. (2005). "Bulk Comptonization of the Cosmic Microwave Background by Extragalactic Jets as a Probe of Their Matter Content".The Astrophysical Journal.625 (2):656–666.arXiv:astro-ph/0502201.Bibcode:2005ApJ...625..656G.doi:10.1086/429558.S2CID 39743397.
  12. ^Hirotani, K.; Iguchi, S.; Kimura, M.; Wajima, K. (2000). "Pair Plasma Dominance in the Parsec-Scale Relativistic Jet of 3C 345".The Astrophysical Journal.545 (1):100–106.arXiv:astro-ph/0005394.Bibcode:2000ApJ...545..100H.doi:10.1086/317769.S2CID 17274015.
  13. ^Electron–positron Jets Associated with Quasar 3C 279
  14. ^Naeye, R.; Gutro, R. (2008-01-09)."Vast Cloud of Antimatter Traced to Binary Stars".NASA.
  15. ^Blandford, R. D.; Znajek, R. L. (1977)."Electromagnetic extraction of energy from Kerr black holes".Monthly Notices of the Royal Astronomical Society.179 (3): 433.arXiv:astro-ph/0506302.Bibcode:1977MNRAS.179..433B.doi:10.1093/mnras/179.3.433.
  16. ^Penrose, R. (1969). "Gravitational Collapse: The Role of General Relativity".Rivista del Nuovo Cimento.1:252–276.Bibcode:1969NCimR...1..252P. Reprinted in:Penrose, R. (2002). ""Golden Oldie": Gravitational Collapse: The Role of General Relativity".General Relativity and Gravitation.34 (7):1141–1165.Bibcode:2002GReGr..34.1141P.doi:10.1023/A:1016578408204.S2CID 117459073.
  17. ^Williams, R. K. (1995). "Extracting X-rays, Ύ-rays, and relativistic ee+ pairs from supermassive Kerr black holes using the Penrose mechanism".Physical Review.51 (10):5387–5427.Bibcode:1995PhRvD..51.5387W.doi:10.1103/PhysRevD.51.5387.PMID 10018300.
  18. ^Williams, R. K. (2004). "Collimated Escaping Vortical Polar e−e+Jets Intrinsically Produced by Rotating Black Holes and Penrose Processes".The Astrophysical Journal.611 (2):952–963.arXiv:astro-ph/0404135.Bibcode:2004ApJ...611..952W.doi:10.1086/422304.S2CID 1350543.
  19. ^"Chandra :: Photo Album :: IGR J11014-6103 :: June 28, 2012".
  20. ^Pavan, L.; et al. (2015). "A closer view of the IGR J11014-6103 outflows".Astronomy & Astrophysics.591: A91.arXiv:1511.01944.Bibcode:2016A&A...591A..91P.doi:10.1051/0004-6361/201527703.S2CID 59522014.
  21. ^Pavan, L.; et al. (2014)."The long helical jet of the Lighthouse nebula, IGR J11014-6103"(PDF).Astronomy & Astrophysics.562 (562): A122.arXiv:1309.6792.Bibcode:2014A&A...562A.122P.doi:10.1051/0004-6361/201322588.S2CID 118845324. Long helical jet of Lighthouse nebula page 7
  22. ^Halpern, J. P.; et al. (2014). "Discovery of X-ray Pulsations from the INTEGRAL Source IGR J11014-6103".The Astrophysical Journal.795 (2): L27.arXiv:1410.2332.Bibcode:2014ApJ...795L..27H.doi:10.1088/2041-8205/795/2/L27.S2CID 118637856.

External links

[edit]
Retrieved from "https://en.wikipedia.org/w/index.php?title=Astrophysical_jet&oldid=1318930268"
Categories:
Hidden categories:

[8]ページ先頭

©2009-2025 Movatter.jp