ISMD 2007
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Transcript of ISMD 2007
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ISMD 2007
Berkeley, August 5-9 2007
Chairman: Nu Xu
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Seria ISMD
• Początek: Paryż 1970 (Lestienne,Salmeron, Sosnowski, Krzywicki + Wróblewski itd.), Helsinki 71, Zakopane 72 (Kraków-Warszawa), Pawia 73..., Tihany 2000, Datong 01, Alushta 02, Kraków 2003, Sonoma 04, Kromeriz 05, Parati 06
• Nazwy zmienne, ale zawsze „multiparticle” (w latach 70’ mały margines fizyki cząstek)
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Program
1.Jet physics (Salgado, Takai) 7 referatów2.Fluctuations and Correlations (Padula, Strickland,
Soltz, Roland) 133.Small x and Diffraction (Kovchegov, Staśto) 104.Soft Interactions (Cebra, Soldner-Rembold) 105.Astroparticle Physics (Drescher, Huentemeyer) 66.Particle Propagating in Dense Matter (Casalderrey-
Solana, Dremin, Jia, Fuqian Wang) 157.Heavy Quark Production (Bauer, Gary, Huang) 11
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Statystyka
• Uczestnicy: 85, afiliacje: 44 USA, 11 RFN, 4 Brazylia, Rosja, 3 Polska, Włochy, 2 Czechy, Francja, Węgry, 1 Chiny, Holandia, Indie, Izrael, Japonia, Kanada, Słowacja, Szwajcaria, Szwecja, Ukraina.
• Uwaga: afiliacje, nie narodowości!
• Referaty: 73: 7+13+10+10+6+15+11+1.
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Polscy uczestnicy i referaty
• D.Antończyk (Frankfurt), Z.Chajecki (Ohio), P.Danielewicz (Michigan), KF (UJ), A.Galas (IFJ), A.Kisiel (Ohio), R.Maj (AŚ), A.Staśto (Penn), M.Szuba (LBL)+B.Jacak,?
• P.Danielewicz-imaging review (MSU)• A.Kisiel-STAR and Therminator (OSU)• A.Galas-production in DIS, p from ep• KF-HERMES and absorption
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Co naprawdę nowego?
• Astrocząstki: ograniczenie GZK działa, korelacje - źródła?
• Asymetria eliptyczna: przyczynek korelacji
• Korelacje cząstkowe
• Odkrycie b, b‘,b
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Ograniczenie GZK, klastry
• Kai Martens (HiRes, U. of Utah)
• Glennys Farrar (New York U.)
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Results from HiResand Observation of the GZK
Suppression
Kai Martens
High Energy Astrophysics Institute
Department of Physics, University of Utah
for the HiRes Collaboration
HR1HR2
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HiRes Monocular Spectra
flux x E3
HR1: longer exposure high energy
HR2: larger elevation coverage low energy
energy scale uncertainties:
- missing energy 5%- energy loss rate 10%- fluorescence yield 6%- atmospheric conditions 4%- photometric calibration10%
total (energy): 17%
flux uncertainty: 30% (@ =2.8)
data:HR1: 5/97-6/05HR2: 12/99-8/04
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Old plots:AGASAAGASA (E–20%)
avoid double counting:remove HR1 events that also
are in the HR2 data set
Broken power-law fits:a.) one vs. two breakpoints:
2 reduced by 23.4 4.5
b.) compare measured data to red line extrapolation:expect: 39.9observe: 13 4.8 (P=7x10-7)
Quacks like duck, don’t
it?
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ee
eepn
HiRes Composition Guided Fits flux
source model:all sources inject with E
= 2.42uniform with redshiftevolution (1+z)m
m = 2.46
future: astronomy inspired redshift evolution
composition as measured !
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Rescaling energies to dip=> consistency!
• Left: published spectra x E3 from different expts
• Right: spectra after shifting energies by factors
AG = 0.9; HR = 1.2; Yk = 0.75; Auger = 1.2
• Shift => consistent normalizations of all spectra, for Auger = 1.4.
(HR = 1.2 + difference in AF yield assumptions => Auger ~ 1.35)
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UHECR multiplets• Cluster candidate in published AGASA-HiRes data:
– 5 events, chance probability 2 10-3
– Energies (15), 38, 53, 55, 78 EeV (1 EeV = 1018 eV)– (b, l) = (55o,145o) (“Ursa Major Cluster”)
• Projecting from AGASA-HiRes suggests with a dataset like Auger~ 1 multiplet with 8-10 UHECRs 1 multiplet with ~ 6 UHECRs~ 5 multiplets with ~ 4 UHECRs
• Need good analysis tools to avoid using false multiplets. Maximum Likelihood method has been developed (GRF)
• If (when!) such multiplets are found, they will give a powerful constraint on GMF and sources.
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Wnioski z astrofizyki
• Ograniczenie GZK (strata energii w produkcji na fotonach tła) jednak chyba działa, więc dziesiątki modeli zbędne.
• Być może są klastry kierunkowe dla najwyższej energii (niezaburzone przez pole magnetyczne); Auger?
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Published by AAAS
The Pierre Auger Collaboration et al., Science 318, 938 -943 (2007)
Fig. 1. Layout of the Pierre Auger Southern Observatory
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Published by AAAS
The Pierre Auger Collaboration et al., Science 318, 938 -943 (2007)
Fig. 2. Aitoff projection of the celestial sphere in galactic coordinates with circles of radius 3.1{degrees} centered at the arrival directions of the 27 cosmic rays with
highest energy detected by the Pierre Auger Observatory
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Azimuthal asymmetry – czy to naprawdę „elliptic flow”?
• Rudy Hwa (Oregon U.)
• Gunther Roland (STAR, MIT)
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Conclusion
• Azimuthal anisotropy is mainly a ridge effect. No fast thermalization or hydrodynamical flow are needed.
• Hydrodynamics may still be applicable after some time, but it is not needed for v2, for which the relevant physics at <1 fm/c is crucial --- semi-hard scattering at qT<3.
• For pT<1.5 GeV/c, the analysis is simple, and the result can be expressed in analytic form that agrees with data.
• For pT>1.5 GeV/c, shower partons must be considered. Jet dominance (>3GeV/c) will saturate v2.
• No part of the study suggests that the medium behaves like a perfect fluid.
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STAR analysis
• Znane efekty korelacyjne (clusters, minijets...) dają przyczynki do asymetrii azymutalnej niezwiązane z przepływem
• Należy je odjąć przed porównaniem danych z modelami hydrodynamicznymi
• STAR, PHOBOS (Krzysztof Woźniak)
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Nowe dane o korelacjach
• Stefan Kniege (Frankfurt U., CERES)
• Jason Ulery (Purdue U., STAR):
• 3-particle correlations to discriminate between the models of „back” jet emission
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Summary• Non gaussian shape on the away side of
2 particle correlation function
• Shape of the correlation function for different charge combinations indicate
charge ordering in the fragmentation process
•Shape of the 3 particle correlations indicate cone like structure on the away side of the jet
Further investigations are needed to draw final conclusions
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Summary and Conclusions• Three 3-particle analyses at RHIC.• PHENIX Analysis
– Shape consistent with conical emission simulation.
• STAR Cumulant Analysis– Non-zero 3-particle correlations.
• STAR 2-Component Analysis– Consistent with conical emission at about 1.45
radians in central Au+Au.– PT independent angle suggests Mach-cone
emission.
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Odkrycie nowych pięknych barionów
• W tablicach z 2006 roku tylko b
• Teraz identyfikowane: b, b*, b, b
• Tania Moulik (U. of Kansas, CDF+D0): przewidywania i wyniki doświadczalne
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b Results
Likelihood Fit Results : M (DØ) = 5774 11 (stat.) 15 (syst.) MeV -- [1]
M (CDF)= 5792.9 2.4 (stat.) 1.7 (syst.) GeV ) – [2] (Theory : 5.793 - 5.814)
Likelihood Fit Results : M (DØ) = 5774 11 (stat.) 15 (syst.) MeV -- [1]
M (CDF)= 5792.9 2.4 (stat.) 1.7 (syst.) GeV ) – [2] (Theory : 5.793 - 5.814)
15.2 4.4
17.5 4.3
[1] PRL 99, 1052001 (2007)[2] arXiv:0707.0589
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Podsumowanie nowych barionów
• Masy i rozpady +/- jak oczekiwano.
• Dlaczego model kwarków działa tu tak dobrze?
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Zalecenia i perspektywy
• Warto oglądnąć strony dostępne pod „Program” na stronie ISMD 2007 http://www-rnc.lbl.gov/ISMD/index.html
• Następne ISMD w Hamburgu (DESY) w dniach 16-20.09.2008 (Hannes Jung + Gösta Gustafson), a przedtem
• WPCF (Workshop on Particle Correlations and Femtoscopy) w Krakowie 10-14.09.08 (Andrzej Białas + KF, G.Miśkowiec etc. w OC, J.Pluta, K.Zalewski wśród conveners...)