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PionIn particle physics, pion (short for the Greek language ''pi meson'' = 'P middle') is the collective name for three subatomic particles discovered in 1947: π0, π+ and π−. Pions are the lightest mesons. ==Basic properties== Pions have zero spin (physics) and are composed of first generation quarks. In the quark model, an up and an anti-down quark compose a π+, while a down and an anti-up quark compose the π−, its antiparticle. Combinations of up and anti-up, or down and anti-down, would both be neutral, but because they have the same quantum numbers are only found in superpositions. The lowest energy superposition is the π0, which is its own antiparticle. The π± mesons have a mass of 139.6 MeV/''c''2 and a half-life of 2.6 × 10−8 seconds. The main decay mode is into a muon and its neutrino or antineutrino: : : The π0 has as slightly smaller mass of 135.0 MeV/''c''2 and a ''much'' shorter mean life of 8.4 × 10−17 seconds. The main decay mode is into two photons: : ==History== After theoretical work by Hideki Yukawa in 1935 had predicted the existence of mesons as the carrier particles of the strong nuclear force, charged pions were found experimentally in 1947 by a team led by Cecil Powell. The age of particle accelerators had yet to arrive in those days. Instead, the team lifted photographic emulsions by balloon to high altitude, where they were exposed to cosmic rays. After recovery of the balloon, microscopic inspection of the emulsion revealed the tracks of charged particles, among which the pions were discovered. Their achievements earned Yukawa in 1949 and Powell in 1950 the Nobel Prize in Physics. The π0 is more difficult to observe than π±; being electrically neutral it doesn't leave a track in an emulsion. The π0 was finally identified in 1950 by its decay products. The pions are considered to be the pseudo Nambu-Goldstone bosons of a spontaneously broken symmetry. This is also the reason why the pion masses are considerably lighter than the masses of other mesons like the -Meson (547.75 MeV/''c''2). ==Theoretical overview== The pion can be thought of as the particle that mediates the interaction between a pair of nucleons. This interaction is attractive, that is, it pulls the nucleons together. Written in a non-relativistic form, it is called the Yukawa potential. The pion, being a meson, has kinematics described by the Klein-Gordon equation. In the general terms of quantum field theory, the Lagrangian describing the pion-nucleon interaction is called the Yukawa interaction. The nearly identical masses of and imply that there must be a symemtry at play; this symmetry is called the SU(2) flavour symmetry or isospin. The reason that there are three pions, , and is that these are understood to belong to the triplet representation or the adjoint representation of SU(2). By contrast, the up and down quarks transform accodring to the irreducible, semi-simple fundamental representation of SU(2), whereas the the anti-quarks transform according to the conjugate representation. Thus, one has : which is one of the many relationships which lends weight to the quark model of pions and nucleons. With the addition of the strange quark, one can say that the pions participate in an SU(3) symmetry with the strange paritcles, belonging to the octect representation (the adjoint representation of SU(3)). With the addition of the charmed, top, and bottom quarks, one can argue that the full flavour symmetry is SU(6) but the argument is strained because the large masses of these other quarks implies that the masses of the corresponding particles are nowhere near the pion mass. Pions are pseudoscalars under a parity (physics) transformation. Pion currents thus couple to the axial vector current and pions participate in the chiral anomaly. ==See also== *Pionium *List of particles *Quark model ==References== * Gerald Edward Brown and A. D. Jackson, ''The Nucleon-Nucleon Interaction'', (1976) North-Holland Publishing, Amsterdam ISBN 0-7204-0335-9 ==External link== * [http://pdg.lbl.gov/2004/tables/mxxx.pdf Mesons] at the Particle Data Group * [http://hyperphysics.phy-astr.gsu.edu/hbase/particles/hadron.html Mesons] at Hyperphysics Meson Hadron Nuclear physics Quantum chromodynamics Pion==Wikipedia:Welcome, newcomers to the Wikipedia== Welcome, newcomer! Here are some useful tips to ease you into the Wikipedia experience: * First, take a look at the Wikipedia:Tutorial, and perhaps dabble a bit in the Wikipedia:Test area. * When you have some free time, take a look at the Wikipedia:Manual of Style and Wikipedia:Policies and guidelines. They can come in very handy! * Remember to use a Wikipedia:Neutral point of view! * If you need any Wikipedia:Help, feel free to post a question at the Wikipedia:Help desk * Explore, Wikipedia:Be bold in updating pages, and, most importantly, have fun! Also, here are some odds and ends that I find useful from time to time: *Wikipedia:Policy Library *Wikipedia:Utilities *Wikipedia:Cite your sources *Wikipedia:Verifiability *Wikipedia:Wikiquette *Wikipedia:Civility *Wikipedia:Conflict resolution *Wikipedia:Brilliant prose *Wikipedia:Pages needing attention *Wikipedia:Peer review *Wikipedia:Bad jokes and other deleted nonsense *Wikipedia:Village pump *Wikipedia:Boilerplate text Feel free to ask me anything the links and talk pages don't answer. You can most easily reach me by posting on User_talk:ClockworkTroll. You can sign your name on any page by typing 4 tildes, likes this: ~~~~. Best of luck, and have fun! User:ClockworkTroll 05:45, 11 Nov 2004 (UTC) Pion:zh:User:Pion Pion==ToDo List== The following article enhancements should be dealt with at some point: # pions mediate the strong (nuclear) force, # The Yukawa potential is a non-relativistic description for them, # The relativistic equation for pions is the Klein-Gordon equation # They are pseudoscalars under parity inversion, # They couple to the axial vector current, the couple is the axial coupling constant which is a "fundamental"/"important" parameter of the nucleon. # pion is part of the triplet representation aka adjoint representation of SU(2) flavour symmetry, because the up and down quarks belong doublet rep of SU(2) and a pion is a quark and anti-quark, and su(2) cross su(2)-bar is the adjoint rep. # The SU(2) flavour symmetry allows fun games with chiral symmetry and in particular, since su(2) also describes spatial rottations, one can play games with non-trivial topological mappings of the embedding of pion fields into 3D space. i.e. mappings because of the non-trivial fundamental group. # Skyrme's topological soliton aka skyrmion aka 'cloud of pions' aka 'chiral model' is a decent one-parameter model of the nucleon (proton/neutron), which predicts a variety of nuclear properties fairly accurately with only one free parameter. User:Linas 01:00, 24 May 2005 (UTC) See other meanings of words starting from letter: PPA | PB | PC | PD | PE | PF | PG | PH | PI | PJ | PK | PL | PM | PN | PO | PR | PS | PT | PU | PW | PX | PY | PZ |Words begining with Pion: Pion Pion Pion Pion Pioneer Pioneer,_IA Pioneer,_Iowa Pioneer,_LA Pioneer,_Louisiana Pioneer,_OH Pioneer,_Ohio Pioneer-12 Pioneer-12 Pioneer-12/Archive0000001 Pioneer-12/demos/page_concatenation Pioneering Pioneering_(Bahá'í) Pioneers Pioneers_by_field Pioneers_of_photography Pioneers_of_rail_transport Pioneertown Pioneertown,_CA Pioneertown,_California Pioneer_(company) Pioneer_(military) Pioneer_(military) Pioneer_0 Pioneer_0 Pioneer_1 Pioneer_10 Pioneer_10 Pioneer_11 Pioneer_12 Pioneer_13 Pioneer_2 Pioneer_3 Pioneer_4 Pioneer_5 Pioneer_6 Pioneer_6,_7,_8_and_9 Pioneer_7 Pioneer_8 Pioneer_9 Pioneer_A Pioneer_A,_B,_C,_D_and_E Pioneer_anomaly Pioneer_anomaly Pioneer_Aviation Pioneer_Award Pioneer_B Pioneer_C Pioneer_Camps_of_Canada Pioneer_Chicken Pioneer_Chicken Pioneer_Column Pioneer_Corporation Pioneer_Courthouse_Square Pioneer_D Pioneer_Day Pioneer_E Pioneer_effect Pioneer_F Pioneer_Football_League Pioneer_Fund Pioneer_Fund Pioneer_G Pioneer_HLD-X0 Pioneer_HLD-X0 Pioneer_I Pioneer_II Pioneer_III Pioneer_Institute Pioneer_Island Pioneer_IV Pioneer_IX Pioneer_Jazz Pioneer_League Pioneer_Movement Pioneer_Movement Pioneer_movement Pioneer_P Pioneer_P-2 Pioneer_P-3 Pioneer_P-30 Pioneer_P-31 Pioneer_P-31 Pioneer_Park Pioneer_Peaks_National_Park Pioneer_Plant Pioneer_plant Pioneer_plaque Pioneer_plaque Pioneer_Playhouse Pioneer_Press Pioneer_program Pioneer_program Pioneer_program Pioneer_program Pioneer_Public_Television Pioneer_PureVision_Las_Vegas_Bowl Pioneer_Purevision_Las_Vegas_Bowl Pioneer_Sergeant Pioneer_species Pioneer_species Pioneer_Square Pioneer_Square,_Seattle,_WA Pioneer_Square,_Seattle,_Washington Pioneer_Square_South_and_Pioneer_Square_North_(MAX_stations) Pioneer_Total_Abstinence_Association Pioneer_Total_Abstinence_Association Pioneer_Township,_MI Pioneer_Township,_Michigan Pioneer_USA Pioneer_V Pioneer_Valley Pioneer_Valley Pioneer_Valley_Transit_Authority Pioneer_Venus Pioneer_Venus_1 Pioneer_Venus_2 Pioneer_Venus_Multiprobe Pioneer_Venus_Orbiter Pioneer_Venus_Probe_1 Pioneer_Venus_Probe_2 Pioneer_Venus_Probe_3 Pioneer_Venus_Probe_4 Pioneer_Venus_project Pioneer_VI Pioneer_VII Pioneer_VIII Pioneer_Village Pioneer_Village,_Kentucky Pioneer_Village,_KY Pioneer_Women's_Memorial_Gardens Pioneer_X Pioneer_XI Pioneer_XII Pioneer_XIII Pioneer_Y Pioneer_Z Pioneer_Zephyr Pioneer_Zephyr Pioneer_Zephyr/to_do Pioner Pionerskaya_Pravda Pioniere Pionium Pionium Pionki Pions Pionus Pion_coiffé Pion_coiffé |
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