But Ranked “B”

Today we learnedJ-Parc construction goes well (Shoji)

Polarizable (Roser)

Diabolically Designed (Jaffe)

withFascinating Physics Opportunities

(Brodsky)

Our Dream Comes TrueAfter Numatron and Big-hadron passed away

Virtual World → 　 Real World

Real Life Budget

Reviews Manpower

・Fight against the AgencyFight between the fields

BeamDump

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

HadronPhysics

NuclearPhysics

Carrier is indispensable

During the last 10 yearsJapanese hadron lovers were

Jet Quenching

In COMPASS

With Bradamante

In HERMES

With Aschnauer

Deeply bound Deeply bound pion sensingpion sensing

In GSI

Gluon Polarization

in Proton

In RHIC (Tanida)

Vector MesonMass Modification

YokkaichiDeeply BoundKaonic Nuclus

OutaPenta Quark

Nakano

Di-muon experiments

•Sawada, 2x1012 pps

•Dbar/ubar, •Quark Bremss.•Spin, SSA

•Goto, 109 pps 10%target

•ΔG→L, SSA•Add π0/γ detector •Backward with PPT •PPB later, quark Sivers with D•A(LL) 2x1012 pps

•Iwata, for COMPASS+π though

transversity development of PPT for 109 pps π

Geesman; Still at the heart of hadron structure

Koike; Twist3 calculation with predictions,

Stratman; Predictions for γ & π0, K~4. Resum. bigger in higher PT but controllable,

Kawamura; Predictions forQT 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

BUTKumano wants PDT

pQCD applicable ?

Brodsky & Strikman stressed an importance of– Exclusive measurements– Very much skewed GPD– Spin structure (Krish effect)

Experimentalist should considerColor Transparency Type Measurements

Like h+A→h+A+p+X(hard)

So far missing in LoI

Strangeness in NucleonJ-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 gΔΔ、– co-habitable with Δs experiment

Arvieux; PV in ep elastic GZ

E GZM = 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 Exp @ Jparc

Japanese ExoticsNakano’s θ+

HosakaYokkaichi: mass shift at nuclear density

New Exp @ Jparc

MorimatsuKunihiro

Outa; Deeply Bound K Nuclus

AkaishiHatsuda

MibeAslanyan

HyodoNagata

New Exp @ Jparc

Now the time to come backWith your friends together

In COMPASS

With Bradamante

In HERMES

With Aschnauer

Deeply bound Deeply bound pion sensingpion sensing

In GSI

Jet Quenching

Gluon Polarization

in Proton

In RHIC (Tanida)

Vector MesonMass Modification

YokkaichiDeeply BoundKaonic Nuclus

OutaPenta Quark

Nakano

Return of The Judi

To J-Parc at Tokaias QCD Paradise

See you again at INPC2007 June 3rd -8th at Tokyo Forum

We must be patient, not in a hurry

good physics never pass away