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J/ψ
(J/psi) meson is a subatomic particle,a flavor-neutral meson consisting of a charm quark and a charm antiquark. Mesons formed by a bound state of a charm quark and a charm anti-quark are generally known as "charmonium" or psions. The
J/ψ
is the most common form of charmonium,due to its spin of 1 and its low rest mass. The
J/ψ
has a rest mass of 3.0969 GeV/c2,just above that of the
η
c,and a mean lifetime of 7.2×10−21 s. This lifetime was about a thousand times longer than expected.
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References
- 1 2 "Larry McLerran | Department of Physics | University of Washington". phys.washington.edu.
- 1 2 "Larry D. McLerran". scholar.google.com.
- 1 2 3 "Prize Recipient". www.aps.org.
- 1 2 "News and Announcements | Institute for Nuclear Theory (INT)". www.int.washington.edu.
- ↑ "Ulkomaiset jäsenet".
- 1 2 "Symposium on Contemporary QCD Physics and Relativistic Nuclear Collisions". Indico.
- ↑ "From BNL: "New Matter, Mathematical Models & Larry McLerran"". November 18, 2014.
- ↑ Freedman, Barry A.; McLerran, Larry D. (August 15, 1977). "Fermions and gauge vector mesons at finite temperature and density. III. The ground-state energy of a relativistic quark gas". Physical Review D. 16 (4): 1169–1185. doi:10.1103/PhysRevD.16.1169 – via APS.
- ↑ Freedman, Barry; McLerran, Larry (February 15, 1978). "Quark star phenomenology". Physical Review D. 17 (4): 1109–1122. doi:10.1103/PhysRevD.17.1109 – via APS.
- ↑ McLerran, Larry D.; Svetitsky, Benjamin (January 8, 1981). "A Monte Carlo study of SU(2) Yang-Mills theory at finite temperature". Physics Letters B. 98 (3): 195–198. doi:10.1016/0370-2693(81)90986-2 – via ScienceDirect.
- ↑ McLerran, Larry D.; Svetitsky, Benjamin (July 15, 1981). "Quark liberation at high temperature: A Monte Carlo study of SU(2) gauge theory". Physical Review D. 24 (2): 450–460. doi:10.1103/PhysRevD.24.450 – via APS.
- ↑ Anishetty, R.; Koehler, P.; McLerran, L. (December 1, 1980). "Central collisions between heavy nuclei at extremely high energies: The fragmentation region". Physical Review D. 22 (11): 2793–2804. doi:10.1103/PhysRevD.22.2793 – via APS.
- ↑ McLerran, L. D.; Toimela, T. (February 1, 1985). "Photon and dilepton emission from the quark-gluon plasma: Some general considerations". Physical Review D. 31 (3): 545–563. doi:10.1103/PhysRevD.31.545 – via APS.
- ↑ "Electron-Ion Collider (EIC)". www.bnl.gov.
- ↑ McLerran, Larry; Venugopalan, Raju (March 1, 1994). "Computing quark and gluon distribution functions for very large nuclei". Physical Review D. 49 (5): 2233–2241. doi:10.1103/PhysRevD.49.2233 – via APS.
- ↑ McLerran, Larry; Venugopalan, Raju (April 1, 1994). "Gluon distribution functions for very large nuclei at small transverse momentum". Physical Review D. 49 (7): 3352–3355. doi:10.1103/PhysRevD.49.3352 – via APS.
- ↑ Iancu, Edmond; Leonidov, Andrei; McLerran, Larry (September 11, 2001). "Nonlinear Gluon Evolution in the Color Glass Condensate: I". Nuclear Physics A. 692 (3–4): 583–645. arXiv: hep-ph/0011241 . doi:10.1016/S0375-9474(01)00642-X – via arXiv.org.
- ↑ Ferreiro, Elena; Iancu, Edmond; Leonidov, Andrei; McLerran, Larry (May 11, 2002). "Nonlinear Gluon Evolution in the Color Glass Condensate: II". Nuclear Physics A. 703 (1–2): 489–538. arXiv: hep-ph/0109115 . doi:10.1016/S0375-9474(01)01329-X – via arXiv.org.
- ↑ Kovner, Alex; McLerran, Larry; Weigert, Heribert (December 1, 1995). "Gluon production from non-Abelian Weizs\"acker-Williams fields in nucleus-nucleus collisions". Physical Review D. 52 (11): 6231–6237. doi:10.1103/PhysRevD.52.6231 – via APS.
- ↑ Kovner, Alex; McLerran, Larry; Weigert, Heribert (October 1, 1995). "Gluon production at high transverse momentum in the McLerran-Venugopalan model of nuclear structure functions". Physical Review D. 52 (7): 3809–3814. doi:10.1103/PhysRevD.52.3809 – via APS.
- ↑ Arnold, Peter; McLerran, Larry (July 15, 1987). "Sphalerons, small fluctuations, and baryon-number violation in electroweak theory". Physical Review D. 36 (2): 581–595. doi:10.1103/PhysRevD.36.581 – via APS.
- ↑ Arnold, Peter; McLerran, Larry (February 15, 1988). "The sphaleron strikes back: A response to objections to the sphaleron approximation". Physical Review D. 37 (4): 1020–1029. doi:10.1103/PhysRevD.37.1020 – via APS.
- ↑ Kharzeev, Dmitri E.; McLerran, Larry D.; Warringa, Harmen J. (May 11, 2008). "The effects of topological charge change in heavy ion collisions: "Event by event P and CP violation"". Nuclear Physics A. 803 (3–4): 227–253. arXiv: 0711.0950 . doi:10.1016/j.nuclphysa.2008.02.298 – via arXiv.org.
- ↑ McLerran, Larry; Pisarski, Robert D. (November 11, 2007). "Phases of Dense Quarks at Large N_c". Nuclear Physics A. 796 (1–4): 83–100. arXiv: 0706.2191 . doi:10.1016/j.nuclphysa.2007.08.013 – via arXiv.org.
- ↑ McLerran, Larry; Reddy, Sanjay (March 26, 2019). "Quarkyonic Matter and Neutron Stars". Physical Review Letters. 122 (12): 122701. doi:10.1103/PhysRevLett.122.122701 – via APS.
- ↑ "Profile". www.humboldt-foundation.de.
- 1 2 "Larry McLerran, Ph.D., Ph.D." Brookhaven National Laboratory.
- ↑ "people, Theoretical Physics, Heidelberg". www.thphys.uni-heidelberg.de.
- ↑ "Honorary Doctorate – Jagiellonian University – Jagiellonian University". en.uj.edu.pl.