'Pion' presentation slideshows

Subthreshold particle production

Subthreshold particle production. To produce a pion (mass ~ 140 MeV for charged pions, 135 MeV for neutral pions) in a NN collision, a lab energy of at least ~ 290 ( ~ 280) MeV is required.

752 views • 61 slides

Pion form factors and decays .

Pion form factors and decays. A. E. Dorokhov in collaboration with W . Broniowski and E . Ruiz Arriola. Introduction g-2 Transversity pion form factor: c models vs Lattice Conclusions. Cosmology tell us that 95% of matter is not described in text-books yet. Two search strategies:

626 views • 52 slides

Neutral pion decay in Dense Skyrmion Matter

532 views • 39 slides

Pions in nuclei and tensor force

Pions in nuclei and tensor force. Hiroshi Toki (RCNP, Osaka) in collaboration with Yoko Ogawa (RCNP, Osaka) Jinniu Hu (RCNP, Osaka) Takayuki Myo (Osaka Inst. Tech.) Kiyomi Ikeda (RIKEN). Pion is important !! In Nuclear Physics.

588 views • 30 slides

Hadron Structure at Light Quark Masses

Hadron Structure at Light Quark Masses. DWF Valence on a Asqtad light sea Nucleon Properties: Form Factors g A Momentum and Spin Fraction GPDs Pion Form Factor. David Richards (Jefferson Laboratory) for LHPC. LHP Collaboration. Dru Renner University of Arizona

374 views • 28 slides

Franz Gross - JLab/W&M

Covariant dynamical models of photo-and electro-production of pions JLab N* workshop, October 14, 2008. Goals: Definition of the N* problem (from a 2003 talk) Issues The Covariant Spectator Theory (CST) Light front vs CST Outline of planned CST calculation (with the EBAC group)

353 views • 27 slides

Measurement of the Pion Structure Function

252 views • 25 slides

Quantum Treatment of Multiple Scattering and Collective Flow in HBT

Kromeriz, Czech Republic August 17, 2005. Quantum Treatment of Multiple Scattering and Collective Flow in HBT. The pion environment after the QGP phase transition Why quantum treatment? The path integral method to study multiple collisions and collective flow in HBT Conclusions

342 views • 23 slides

226 views • 22 slides

Next-to-Leading Order Parity-Violating Potential and

n p ? d ?. ?. Next-to-Leading Order Parity-Violating Potential and. Chang Ho Hyun Sungkyunkwan University In collaboration with S. Ando and B. Desplanques PAVI06 Milos, Greece May 19, 2006. Outline. Background : One-meson exchange Effective field theory

325 views • 21 slides

2-particle correlation at RHIC

308 views • 20 slides

WP3.4 Reasoning with Inconsistency

WP3.4 Reasoning with Inconsistency. Milestone 3.4 D3.4.3: Reasoning with Inconsistency (version 2) . P/PU/Month 36 PION : a prototype for P rocessing I nconsistent ON tology. PION website: http://wasp.cs.vu.nl/sekt/pion PION package: new release supports Linux.

366 views • 11 slides

Study of the Number of Constituent Quark Scaling of v 2 at High p T Na Li

Study of the Number of Constituent Quark Scaling of v 2 at High p T Na Li ( for the STAR Collaboration ) Institute of Particle Physics, Wuhan, China Brookhaven National Laboratory, Upton, USA. Outline: Introduction STAR Detector and Dataset

241 views • 11 slides

D0 and D0bar signal from 3 rd Production

D0 and D0bar signal from 3 rd Production. Jaiby Joseph 03/19/2011. D0 Signal -200 < slength < 400 , TrkDca <200, |D0dcaPV|<200 , pK >0.7,pPi>0.7,chargeK<0,chargePi>0, pD0>0.3. # of Events: ~ 7.5 M. * Cut change from 1 st Prod. S/B ~5.128.

155 views • 9 slides

Outline:

Feasibility to detect D * (2010) at SIS100. Yu. Vertogradova, V. Pozdnyakov (JINR). Outline:. method to search for D * (2010) +/- input for the study results conclusion. method to search for D * (2010) +/-.

127 views • 5 slides