Title: Slajd%201
1Raport z konferencji EPS2003 w Akwizgranie
Jan Pawel Nassalski Instytut Problemów Jadrowych
im. A.Soltana
2- 17-23 lipca 2003
- 500 uczestników
- 9 z Polski
- Prezentacje B.Badelek, J.Ukleja, M.Krawczyk,
M.Rózanska, - F.Zarnecki, A.Trzupek
- Konwenerzy B.Wosiek High energy nuclear
physics - M.Turala Detectors
and data handling - JPN CP
violation
- High Energy Particle Physics Prize of EPS to
- David Gross, David Politzer, and Frank
Wilczek - Gribov Medal to Nima Arkani-Hamed, Harvard
- Young Particle Physicist Award to Guillaume
Unal - Outreach Prize to Rolf Landua, and Nicholas
Tracas
3SESJE
prezentacji
- Hard QCD . 51
- Hadronic physics . 35
- Heavy flavour physics .. 31
- Physics beyond the Standard Model .. 30
- Tests of the Standard Model 30
- Physics beyond the Standard Model .. 30
- Detectors and data handling 24
- Neutrino Properties and oscillations 21
- CP violation . . 19
- High energy nuclear physics 17
- Particle astrophysics dark matter .10
- Accelerator RD .. 10
- Particle astrophysics cosmic rays 9
- String theory and extra dimensions . 8
- Non perturbative field theory 7
41
5(No Transcript)
6(No Transcript)
7(No Transcript)
8(No Transcript)
9(No Transcript)
10(No Transcript)
11(No Transcript)
12(No Transcript)
13(No Transcript)
14(No Transcript)
15(No Transcript)
16(No Transcript)
17(No Transcript)
18(No Transcript)
19(No Transcript)
20(No Transcript)
21(No Transcript)
22(No Transcript)
232
24(No Transcript)
25(No Transcript)
26(No Transcript)
27(No Transcript)
28(No Transcript)
29(No Transcript)
30(No Transcript)
31(Laser-Electron Photon facility at SPring-8 ?
12C ?K- K X)
(ITEP 0.85 GeV K Xe ? K0 p Xe)
32(S1)
(JLAB 3-5.25 GeV ?)
33(F.Wilczek)
34SAPHIR Collaboration 1.7-2.7 GeV ? p -gt n
K K0s
35(No Transcript)
36(of Frank Wilczek presentation)
37Relativistic Heavy Ion Physics An Experimental
Review
3
Saskia Mioduszewski
22 July 2003
38Summary
- Physics highlights
- Strong collective expansion at SPS and RHIC
- Evidence for early equilibration at RHIC
- SPS Anomalous J/? suppression
- Enhancement of low-mass
dileptons - RHIC Suppression of high pT particles
- and disappearance of away-side
jet - Very intriguing results. All consistent with QGP
formation
39Nuclear Modification Factor RAA
Nuclear Modification Factor
ltNbinarygt/sinelpp
NN cross section
- in absence of nuclear effects
- RAA lt 1 at low pT (soft physics regime)
- RAA 1 at high pT (hard scattering regime)
- suppression (enhancement, e.g. Cronin effect)
- RAA lt 1 (gt 1) at high pT
40RAA for p0
- By definition, processes that scale with Nbinary
will produce RAA1. - RAA is what we measure divided by what we expect.
Nbinary-scaling
RAA is lt 1 at RHIC, but gt 1 at SPS SPS Cronin
effect dominates RHIC suppression dominates
A.L.S.Angelis PLB 185, 213 (1987) WA98, EPJ C 23,
225 (2002) PHENIX, PRL 88 022301 (2002) PHENIX
submitted to PRL, nucl-ex/0304022
41Jet Quenching ?
- high pT suppression reproduced by models with
parton energy loss - other explanations not ruled out, need to measure
initial-state effects
Wang X.N. Wang, Phys. Rev. C61, 064910
(2000). Levai P.Levai, Nuclear Physics A698
(2002) 631. Vitev I. Vitev and M. Gyulassy,
hep-ph/0208108 Gyulassy, Levai, Vitev, Nucl.
Phys. B 594, p. 371 (2001).
AuAu?p0X at ?sNN 200 GeV
42RAA vs. RdA for charged hadrons and p0
Initial State Effects Only
PHENIX (dAu) hep-ex/0306021 submitted to PRL
Initial Final State Effects
- No Suppression in dAu, instead small enhancement
observed (Cronin effect)!! - d-Au results rule out initial-state effects as
the explanation for Suppression at Central
Rapidity and high pT
43Azimuthal distributions in AuAu
Near-side peripheral and central AuAu similar
to pp
Strong suppression of back-to-back correlations
in central AuAu collisions
44Azimuthal distributions
Near-side pp, dAu, AuAu similar Back-to-back
AuAu strongly suppressed relative to pp and dAu
Suppression of the back-to-back correlation in
central AuAu is a final-state effect
45S. StoneSyracuse Univ.July 2003
4
- Experimental Results in Heavy Flavor Physics
Far too much interesting Material to include in
45 min. Apologies in advance.
Many references not properly cited here.
Apologies in advance.
46Conclusions
- There have been lots of surprises in Heavy Quark
Physics, including - Long b Lifetime
- Bo Bo mixing
- Narrow Ds states
- Now finding the effects of New Physics in b c
decays would not be a surprise - we expect to do
it!
47Some basics b Lifetimes
- Note ratio tB/tBo
- 1.0730.014, a
- 5.2s difference
- Also tL ? tBo
- According to
- proponents of the
- Heavy Quark Expansion model, there should be
at most a 10 difference between b-bayron Bo
lifetimes
b
48Some basics Charm lifetimes
(charm photoproduction at FERMILAB)
- New precise lifetimes from FOCUS, a challenge to
QCD (from Pedrini)
49Narrow Ds States
- Ds (c s in l1 states) predicted Jp 0, 1,
1 2. One 1 2 previously seen, these decay
into D()K, are relatively narrow. Others are
also predicted to be above D()K threshold and
have large 200 MeV widths - BaBar Narrow peak in Dspo
- mass distribution. Mass is
- 2316.80.43.0 MeV, width
- consistent with mass resolution
- 9 MeV
- Lighter than most potential
- model predictions. Mass is
- 40 MeV below DK threshold
BABAR 91 fb-1
50CLEO Sees Two States
2.32 GeV
2.11 GeV
Ds p0
- Confirms the BaBar observation of Ds(2317) (13.5
fb-1) - s MeV
- Detector resolution 6.00.3 MeV
- 16520 events in peak
51CLEO finds new state near 2460 MeV
2.46 GeV
- See 2nd state decaying
- into Dspo, at 2460 MeV
- s 6.11.0 MeV
- Detector res 6.60.5 MeV
- 5510 events in peak
Ds p0
52Belle Confirms Both States
Ds sidebands
M(Ds p0 )-M(Ds)
M(Ds p0 )-M(Ds)
(See Seusters talk)
53Other Charge States Not Seen
- CLEO Ds p- or Ds p not seen at level more than
factor of 10 lower than Ds p- speaks against
molecule. Also
CLEO
2317
CDF
54(No Transcript)
55(No Transcript)
56Possible Explanations
- DK molecule Barnes, Close Lipkin hep-ph/0305025
- Ordinary excited cs states Ds, narrow
because isospin is violated in the decay (is only
way for hadronic decay to occur since its below
DK threshold - see Cho Wise). Use HQET chiral
symmetry to explain. Bardeen, Eichten Hill
hep-ph/0305049. Also Nowak, Rho Zahed
hep-ph/0307102 (cs states are all I0, p is I1) - Colangelo De Fazio hep-ph/0305140 Godfrey
hep-ph/0305122 ask us to look for radiative
decays such transitions support cs - Van Beveran Rupp explain in terms of unitarized
meson model hep-ph/0305049 - Bali says lattice cannot accommodate these as cs
states hep-ph/0305049, however this claim is
disputed, Dougall et al hep-ph/0307001 - Dai, Huang Zhu hep-ph/0306274 show that the
masses can be obtained using QCD sum rules - Browder et. al, mixture with 4-quark state above
DK threshold hep-ph/0307054
575
58(No Transcript)
59(No Transcript)
60(No Transcript)
61(No Transcript)
62(No Transcript)
63(No Transcript)
64(No Transcript)
65(No Transcript)
66(No Transcript)
67(No Transcript)
68(No Transcript)
69(No Transcript)
70(No Transcript)
71(No Transcript)
72(No Transcript)
73(No Transcript)
74(No Transcript)
75(No Transcript)
76Struktura nukleonu
77Z Podsumowania, D.Treille
78Komplet prezentacji konferencyjnych mozna znalezc
pod adresem
http//eps2003.physik.rwth-aachen.de/transparencie
s/index.php