But Ranked “B” Today we learned J-Parc construction goes well (Shoji) Polarizable (Roser) Diabolically Designed (Jaffe) with Fascinating Physics Opportunities.

Slides:



Advertisements
Similar presentations
Introduction Glasgow’s NPE research Group uses high precision electromagnetic probes to study the subatomic structure of matter. Alongside this we are.
Advertisements

June 20, Back-to-Back Correlations in p+p, p+A and A+A Reactions 2005 Annual AGS-RHIC User's Meeting June 20, BNL, Upton, NY Ivan Vitev, LANL Ivan.
Mauro Anselmino, Prague, August 1, 2005 Hadron Structure and Hadron Spectroscopy Transversity (transverse spin and transverse motion) Transversity distributions.
Roberto Francisco Pérez Benito On behalf the HERMES Collaboration European Graduate School Lecture Week on Hadron Physics Jyväskylä, Aug 25-29, 2008 HERMES.
Working Group on e-p Physics A. Bruell, E. Sichtermann, W. Vogelsang, C. Weiss Antje Bruell, JLab EIC meeting, Hampton, May Goals of this parallel.
The J-PARC Facility and Ideas for TMD Measurements ECT* Workshop June 15, 2007 Yuji Goto (RIKEN/RBRC)
J-PARC: Where is it? J-PARC (Japan Proton Accelerator Research Complex) Tokai, Japan 50 GeV Synchrotron (15  A) 400 MeV Linac (350m) 3 GeV Synchrotron.
1 Updates on Transversity Experiments and Interpretations Jen-Chieh Peng Transversity Collaboration Meeting, JLab, March 4, 2005 University of Illinois.
Working Group on e-p Physics A. Bruell, E. Sichtermann, W. Vogelsang, C. Weiss Antje Bruell, JLab EIC meeting, Stony Brook, Dec Physics Topics Working.
(Concluding) Remarks Ken Imai (JAEA/J-PARC) KEK Workshop on Hadron Physics with high-momentum beams at J-PARC
Future Opportunities at an Electron-Ion Collider Oleg Eyser Brookhaven National Laboratory.
 Nucleon spin structure and Imaging in the Valence quark region ➥ Inclusive measurements at large x; quark models tests and Lattice QCD tests ➥ Exclusive.
Possibilities to perform DVCS measurement at COMPASS E. Burtin CEA-Saclay Irfu/SPhN On Behalf of the COMPASS Collaboration DIS Madrid - 29 April,
Quark Helicity Distribution at large-x Collaborators: H. Avakian, S. Brodsky, A. Deur, arXiv: [hep-ph] Feng Yuan Lawrence Berkeley National Laboratory.
Parton Model & Parton Dynamics Huan Z Huang Department of Physics and Astronomy University of California, Los Angeles Department of Engineering Physics.
Status Report of HERMES Pasquale Di Nezza (on behalf of HERMES Collaboration) First measurement of transversity Exotic baryons: the pentaquark The spectrometer.
Zhongbo Kang Los Alamos National Laboratory QCD structure of the nucleon and spin physics Lecture 5 & 6: TMD factorization and phenomenology HUGS 2015,
Determining Strangeness Quark Spin in Neutrino-Nucleon Scattering at J-PARC T.-A. Shibata (Tokyo Tech) in collaboration with N. Saito (Kyoto Univ) and.
Jim Stewart DESY Measurement of Quark Polarizations in Transversely and Longitudinally Polarized Nucleons at HERMES for the Hermes collaboration Introduction.
Hadron Spectroscopy with high momentum beam line at J-PARC K. Ozawa (KEK) Contents Charmed baryon spectroscopy New experiment at J-PARC.
Single-Spin Asymmetries at CLAS  Transverse momentum of quarks and spin-azimuthal asymmetries  Target single-spin asymmetries  Beam single-spin asymmetries.
PQCD mechanisms for single (transverse) spin asymmetry in Drell-Yan production PQCD mechanisms for single (transverse) spin asymmetry in Drell-Yan production.
Strangeness and Spin in Fundamental Physics Mauro Anselmino: The transverse spin structure of the nucleon Delia Hasch: The transverse spin structure of.
The Quark Structure of the Nucleon Inti Lehmann & Ralf Kaiser University of Glasgow Cosener’s House Meeting 23/05/2007 Nucleon Structure Generalised Parton.
1 Probing Spin and Flavor Structures of the Nucleon with Hadron Beams Flavor and spin structures of the nucleons –Overview and recent results Future prospects.
Measurements with Polarized Hadrons T.-A. Shibata Tokyo Institute of Technology Aug 15, 2003 Lepton-Photon 2003.
POLARISATION IN QCD -  anomalous magn. moment, g-2 - Spin structure of the nucleon  q,  G, GPD,  t q.
JPARC DY Workshop, April 7 Ralf Seidl (RBRC) R.Seidl: Transverse Spin 1RIKEN, April 7 In JPARC Drell Yan accessible with: UU(unpolarized beam, unpolarized.
Thomas Jefferson National Accelerator Facility PAC-25, January 17, 2004, 1 Baldin Sum Rule Hall C: E Q 2 -evolution of GDH integral Hall A: E94-010,
CEBAF - Continuous Electron Beam Accelerator Facility.
International Workshop on Transversity: New Developments in Nucleon Spin Structure June 2004 Color Gauge Invariance in Hard Processes Vrije Universiteit.
Thomas Jefferson National Accelerator Facility Operated by the Southeastern Universities Research Association for the U.S. Department of Energy Anthony.
TMD flavor decomposition at CLAS12 Patrizia Rossi - Laboratori Nazionali di Frascati, INFN  Introduction  Spin-orbit correlations in kaon production.
1 Quarkonium Production at J-PARC Quarkonium Production at J-PARC with Unpolarized Proton Beam Quarkonium Production at J-PARC with Polarized Beam and.
Structure of Nucleons and Nuclei Como June 14, 2013 CONCLUDING REMARKS F. Bradamante University of Trieste, Italy.
October 22, 2004 Single Spin Asymmetries at RHIC 1 F.Videbaek Physics Department, Brookhaven National.
The transverse structure of the nucleon (resolving the quark motion inside a nucleon) Mauro Anselmino, Torino University and INFN, JLab, December 15, 2006.
Relativistic Nuclear Collisions (RNC) Group Nuclear Science Division (NSD), Lawrence Berkeley National Lab Large Hadron Collider (LHC) Spin physics program.
Forward/p+A Update June 2005 Carl Gagliardi, Mike Leitch, Kirill Tuchin.
— Seminar, CERN, Dec. 15, 2005 — Opportunities in nucleon spin physics Xiangdong Ji University of Maryland.
1 Small x and Forward Physics in pp/pA at RHIC STAR Forward Physics FMS Steve Heppelmann Steve Heppelmann Penn State University STAR.
High-t Exclusive Reactions With Real Photons Gerald A. Miller, UW.
The goal of the COMPASS" workshop at CERN on 4 March 2010 at CERN on 4 March 2010 is to better define the key measurements and their outcomes with.
1 Transversity Experiments Experimental probes for transversity Current experimental status on transversity and other related distribution and fragmentation.
Transversity (transverse spin and transverse motion)
Nucleon spin decomposition
Transversity: New Developments in Nucleon Spin Structure
Long-range plan of nuclear physics in Japan
Future lepton scattering facilities
Physics of the EIC Cyrille Marquet Theory Division - CERN.
Theory : phenomenology support 12 GeV
Measurements of quark transversity and orbital motion in hard scattering Yoshiyuki Miyachi Tokyo Institute of Technology.
The Spin of the Nucleon --- The View from HERMES ---
Wide Angle Compton Scattering
Plans for nucleon structure studies at PANDA
Strangeness and Spin in Fundamental Physics
August 29, Riken Tokyo Office, Tokyo, Japan
Semi-inclusive DIS at 12 GeV
Can We Learn Quark Orbital Motion from SSAs?
Generalized Parton Distributions at
Selected Physics Topics at the Electron-Ion-Collider
Study of Strange Quark in the Nucleon with Neutrino Scattering
Spin WG Summary - spin experiments -
Single Spin Asymmetries: from JLab12 to EIC
The transverse spin structure of the nucleon
Quark and Gluon Sivers Functions
Single Spin Asymmetry with a Transversely Polarized
On behalf of the HERMES collaboration
Overview on hard exclusive production at HERMES
Spin effects and partonic intrinsic k┴
Presentation transcript:

But Ranked “B” Today we learned J-Parc construction goes well (Shoji) Polarizable (Roser) Diabolically Designed (Jaffe) with Fascinating Physics Opportunities (Brodsky)

Our Dream Comes True After Numatron and Big-hadron passed away Virtual World → Real World Real Life Budget Reviews Manpower ・ Fight against the Agency Fight between the fields

Beam Dump A-Line Hadron Experimental Hall (Phase 1) Experimental Area Test Beam (on the guide rail for Phase 2) Hadron Experimental Hall (Phase 2)

Flag Ship Needed Hadron Physics Nuclear Physics Carrier is indispensable

During the last 10 years Japanese hadron lovers were Jet Quenching In COMPASS With Bradamante In HERMES With Aschnauer Deeply bound pion sensing In GSI Gluon Polarization in Proton In RHIC (Tanida) Vector Meson Mass Modification Yokkaichi Deeply Bound Kaonic Nuclus Outa Penta Quark Nakano

Di-muon experiments Sawada, 2x10 12 pps Dbar/ubar, Quark Bremss. Spin, SSA Goto, 10 9 pps 10%target ΔG → L, SSA Add π 0 /γ detector Backward with PPT PPB later, quark Sivers with D A(LL) 2x10 12 pps Iwata, for COMPASS+π though transversity development of PPT for 10 9 pps π Geesman ; Still at the heart of hadron structure Koike; Twist3 calculation with predictions, Stratman; Predictions for γ & π 0, K~4. Resum. bigger in higher PT but controllable, Kawamura; Predictions for QT spectrum, to resolve soft part Yokoya ; K=3~10, NNL converges well. Burkardt, B(T) to relate L to GPD Ji; Measure SSA in DY !! Theorists will figure out What to do with it BUT Kumano wants PDT

pQCD applicable ? Brodsky & Strikman stressed an importance of –Exclusive measurements –Very much skewed GPD –Spin structure (Krish effect) Experimentalist should consider Color Transparency Type Measurements Like h+A→h+A+p+X(hard) So far missing in LoI

Strangeness in Nucleon J-Parc is ~1GeV Neutrino Factory Miyachi – HERMES ΔS~0 but x coverage limited – ν p ( E734) → -0.21< ⊿ s<0 – δΔs = 0.03 Sakemi –Coherent pion production for g ΔΔ 、 –co-habitable with Δs experiment Arvieux; PV in ep elastic G Z E G Z M = Non zero Pate; Combined analysis eP experiment HAPPEx E734,G0 Δs< 0 Sakuta; νA for νphysics Sudo & Forte; for High blow neutrino factory FINeSSE => JParc Experimental Collaboration should be formed soon

Conclusive Jparc Japanese Exotics Nakano’s θ+ Hosaka Yokkaichi: mass shift at nuclear density New Jparc Morimatsu Kunihiro Outa; Deeply Bound K Nuclus Akaishi Hatsuda Mibe Aslanyan Hyodo Nagata New Jparc

Now the time to come back With your friends together In COMPASS With Bradamante In HERMES With Aschnauer Deeply bound pion sensing In GSI Jet Quenching Gluon Polarization in Proton In RHIC (Tanida) Vector Meson Mass Modification Yokkaichi Deeply Bound Kaonic Nuclus Outa Penta Quark Nakano

Return of The Judi To J-Parc at Tokai as QCD Paradise See you again at INPC2007 June 3 rd -8 th at Tokyo Forum

We must be patient, not in a hurry good physics never pass away