The Spectator-Induced Electromagnetic Effect on Meson Production
... Processes occurring in nucleus-nucleus collisions include the participant zone and the highly charged nuclear remnant (spectator system). Interesting information about dynamics of the nuclear collision is brought by the analysis of electromagnetic interaction between produced particles and spectator ...
... Processes occurring in nucleus-nucleus collisions include the participant zone and the highly charged nuclear remnant (spectator system). Interesting information about dynamics of the nuclear collision is brought by the analysis of electromagnetic interaction between produced particles and spectator ...
Effects of color superconductivity on the nucleation of quark matter in
... matter has a lower energy per baryon (Bodmer-Witten-Terazawa hypothesis). However, quantum fluctuations can form the so called Q*phase bubbles, in which the flavor content of the quark phase is equal to that of the β-stable hadronic system at the same pressure. Since no flavor conversion is involved ...
... matter has a lower energy per baryon (Bodmer-Witten-Terazawa hypothesis). However, quantum fluctuations can form the so called Q*phase bubbles, in which the flavor content of the quark phase is equal to that of the β-stable hadronic system at the same pressure. Since no flavor conversion is involved ...
Infrastructure Clouds for Science and Education: ATLAS
... The ATLAS Experiment One of the particle physics experiments at the Large Hadron Collider (LHC) in Geneva ...
... The ATLAS Experiment One of the particle physics experiments at the Large Hadron Collider (LHC) in Geneva ...
Local Parity Violation in Strong Interactions
... transitions can be classified by their winding number and all vacuum configurations can be classified by the Chern-Simons number, NC S[2]. It is pointed out by Kharzeev et al.[1] that all non-zero NC S states lead to a non-conservation of the axial current which in turn leads to parity violation of ...
... transitions can be classified by their winding number and all vacuum configurations can be classified by the Chern-Simons number, NC S[2]. It is pointed out by Kharzeev et al.[1] that all non-zero NC S states lead to a non-conservation of the axial current which in turn leads to parity violation of ...
Higher order corrections to Color superconducting gaps
... the Cooper pair gap, paying special attention to the Ward-Takahashi identity. This way of calculating higher order corrections in the SD analysis has been proved extremely useful in dynamical mass generation of (2+1)-dimensional quantum electrodynamics and in others, since the higher order correctio ...
... the Cooper pair gap, paying special attention to the Ward-Takahashi identity. This way of calculating higher order corrections in the SD analysis has been proved extremely useful in dynamical mass generation of (2+1)-dimensional quantum electrodynamics and in others, since the higher order correctio ...
ng - CAPCA
... 3-D electromagnetic, relativistic, particle-in-cell code. originally written under NASA grant to study interaction of the solar wind and Earth’s magnetosphere used by A. Spitkovsky for magnetosphere physics of neutron stars (mid- 1990’s onward). K. Nishikawa reported initial TRISTAN simulati ...
... 3-D electromagnetic, relativistic, particle-in-cell code. originally written under NASA grant to study interaction of the solar wind and Earth’s magnetosphere used by A. Spitkovsky for magnetosphere physics of neutron stars (mid- 1990’s onward). K. Nishikawa reported initial TRISTAN simulati ...
Lecture 1 - Institute for Nuclear Theory
... Are all particle species produced at the right relative abundances? Energetic sconsistent with common temperature plus flow velocity? ...
... Are all particle species produced at the right relative abundances? Energetic sconsistent with common temperature plus flow velocity? ...
Plasma Dark Current in Self-ionized Plasma Wake Field
... rush back to the beam axis, approximately one half plasma period after being expelled. This creates an on axis negative charge spike that can accelerate the electrons in the back of the bunch or trap the electrons from the plasma. An energy gain of about 4 GeV, the largest to date in any plasma acce ...
... rush back to the beam axis, approximately one half plasma period after being expelled. This creates an on axis negative charge spike that can accelerate the electrons in the back of the bunch or trap the electrons from the plasma. An energy gain of about 4 GeV, the largest to date in any plasma acce ...
Working Group Talks Gobinda Majumdar Issues In The Construction
... • In SUSY we need gaugino mass nonuniversality: M2/M1~4 at the weak scale • We found a good benchmark point with this property by “deforming” the SPS1a. • Substantial rate of dilepton cascade decays at this point will allow for a precise determination of the spectrum at the LHC • A more general scan ...
... • In SUSY we need gaugino mass nonuniversality: M2/M1~4 at the weak scale • We found a good benchmark point with this property by “deforming” the SPS1a. • Substantial rate of dilepton cascade decays at this point will allow for a precise determination of the spectrum at the LHC • A more general scan ...
Central exclusive production of heavy quarkonia and charmonium
... Hopefully, LHCb one day if/when RPs are installed. ...
... Hopefully, LHCb one day if/when RPs are installed. ...
Constraining decaying dark matter with neutron stars
... lifetime, but also in the previous late stages of the progenitor star where the dense nuclear ash central core allows the build-up of a χ -distribution, nχ (r ), over time. In previous works we have considered the effect of a self-annihilating DM particle on the internal NS dynamics [12–15] but here ...
... lifetime, but also in the previous late stages of the progenitor star where the dense nuclear ash central core allows the build-up of a χ -distribution, nχ (r ), over time. In previous works we have considered the effect of a self-annihilating DM particle on the internal NS dynamics [12–15] but here ...
33 PARTICLE PHYSICS - Wright State University
... Although these four forces are distinct and differ greatly from one another under all but the most extreme circumstances, we can see similarities among them. (In GUTs: the Unification of Forces, we will discuss how the four forces may be different manifestations of a single unified force.) Perhaps t ...
... Although these four forces are distinct and differ greatly from one another under all but the most extreme circumstances, we can see similarities among them. (In GUTs: the Unification of Forces, we will discuss how the four forces may be different manifestations of a single unified force.) Perhaps t ...
Strangeness production
Strangeness production is a signature and a diagnostic tool of quark–gluon plasma (or QGP) formation and properties. Unlike up and down quarks, from which everyday matter is made, strange quarks are formed in pair-production processes in collisions between constituents of the plasma. The dominant mechanism of production involves gluons only present when matter has become a quark–gluon plasma. When quark–gluon plasma disassembles into hadrons in a breakup process, the high availability of strange antiquarks helps to produce antimatter containing multiple strange quarks, which is otherwise rarely made. Similar considerations are at present made for the heavier charm flavor, which is made at the beginning of the collision process in the first interactions and is only abundant in the high-energy environments of CERN's Large Hadron Collider.