HIM 2006-09 SHLee 1 1.Introduction for Exotics 2.Hadron production in HIC 3.Exotics from RHIC Hadron Physics at RHIC Su Houng Lee Yonsei Univ., Korea Thanks.

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Presentation transcript:

HIM SHLee 1 1.Introduction for Exotics 2.Hadron production in HIC 3.Exotics from RHIC Hadron Physics at RHIC Su Houng Lee Yonsei Univ., Korea Thanks to: Former collegues and students Present students: Y. Park, Y. Sarac, Y. Heo, K. Kim Post doc: K. Ohnishi

HIM SHLee 2 Introduction for Exotics

HIM SHLee 3 1.Hadrons that can not be explained by quark- antiquark, or 3 quarks 2.That are bound by strong interaction 3.Reasons for its search are similar to that for superheavy Element in low energy nuclear Physics  Understand QCD  sQGP Definition of Exotics

HIM SHLee 4 Mass= 1.54 GeV, width <25 MeV, quark content= uudds 1. LEPS coll., Nakano et.al. PRL (2003) Experiment - First claim

HIM SHLee 5 In Carbon target, but Experiment - Recent claim

HIM SHLee 6 Positive resultsNegative results Recent CLAS experiments find no  + in  +d or  +p  Give up, more experiment or theoretical guideline?

HIM SHLee 7 1. SU(3) soliton 2. Quantizing the 8 angles, the Hamiltonian becomes I=J Hedghog Theory : prediction (Diakanov, Petrov, Polyakov 97)

HIM SHLee 8 4. Diakanov Petrov Polyakov applied it to Anti-decuplet which predicted M  = 1540,   =30 MeV 1. only SU(3) representations containing Y=1 are allowed  moreover, the number of states 2I+1 at S=0 or Y= N c /3 must determine the spin of the representation through 2J+1 because I=J in the SU(2) soliton  one spin state for given representation 3. With constraint coming from WZ term

HIM SHLee 9 1. Soliton picture is valid at large N c : Semi-classical quantization is valid for slow rotation: ie. Valid for describing excitations of order 1/N_c, so that it does not mix and breakdown with vibrational modes of order 1 2. Lowest representation SU(3) f (p,q) at large N c Quantization constraint requires 1.Octet 2.Decuplet 3.Anti decuplet (lowest representation containing s=1) Theory: why it can be wrong (T. Cohen)

HIM SHLee Mass splitting in large N c : Anit decuplet octet mass splitting is mixes with vibrational mode and inconsistent with original assumption and has undetermined correction of same order  Rotation is too fast and may couple to vibrational modes, which might be important to excite q qbar mode, hence describing anti decuplet state with naive soliton quantization might be wrong

HIM SHLee 11 diquark: C=3,F=3,S=0 triquark: C=3,F=6,S=1/2 Jaffe, Wilczek model Karlinear, Lipkin model Theory: Quark model of a pentaquark u d s u d 2 diquark: C=3,F=3,S=0 relative p wave Strong diquark correlation u d s u d

HIM SHLee In QCD q-q are also attractive if in color anti-triplet channel. Color Spin Interaction in QCD In perturbative QCD, 2 C B =C M This term is called color spin interaction

HIM SHLee 13 Color spin interaction explains hadron spectrum Works very well with 3 C B =C M = constant Nucleon uud Baryon Mass differenceMeson Mass difference

HIM SHLee 14 Why there should be a heavy pentaquark 1. For a Pentaquark s u d d u 2. If recombined into a Kaon and a Nucleon s u d d u 3. If recombined into a D-meson and a Nucleon c c 1. For a charmed Pentaquark

HIM SHLee 15 Other possible states - Tetraquark 1. For a Tetraquark A u d B 2. For the meson and meson B ud A ABE tetraquark -E 2meson u u663 MeV u s530 s s374 u c397 s c218 c c39 b b-88 DD - BB -

HIM SHLee 16 Where to search: Baryonic decay mode of B + decay in hadronic language Larger By N c

HIM SHLee 17 Pentaquark decay mode of B + cc Weak decay Branching ratio is Using pevious fit, we find the branching ratio to be 14.4x10 -7 g Dp  x g Kp  /g Kp  lower limit in B-factory Can search for it in Belle S.H.Lee. Y. Kown. Y. Kwon, PRL (06)

HIM SHLee 18 Hadron Production in HIC

HIM SHLee 19 Success of statistical model P. Braun-Munzinger, J. Stachel (95 …)

HIM SHLee 20 Recent Star data - I

HIM SHLee 21 Theoretical Explanation – Muller, Kanada-En’yo Quark Coalescence model = Statitical model + overlap integral s u d d u QGP s u d s

HIM SHLee 22 Statistical model = quark coalescence + overlap Explicit example Exotic production in HIC will follow statistical model modified only by the wave function overlap integral and hadronic phase

HIM SHLee 23 Exotic particle production: elementary vs HIC Exotic particle production from elementary processes s u d d u QGP s u d d u ++ Exotic particle production from Heavy Ion collision

HIM SHLee 24 Example  +(1540) production in Au+Au at RHIC in central rapidity region Statistical model J. Randrup, PRC 68 (2003) , N  =1 Coalescence model Chen, Greco, Ko, Lee, Liu, PLB 601 (2004) 34, N  =0.2 Hadronic regeneration or dissociation is not so large

HIM SHLee 25 Exotics from RHIC 1.RHIC (STAR) FAIR (GSI)

HIM SHLee 26 Possible Decay mode of charmed Pentaquark c u d d u ++ L=1 exoticDecay modeFinal statesBranching ratio udusc uds(  ) +uc(D 0 )  + k 0  0 ( k +  -)  + k 0  -  % (3.8 % ) 5.97 % uud(p) +sc (Ds-) P + k 0  - P + k +  -  % 9.2 % ududc udu (p)+dc (D-) P + k 0  - P + k +  -  % 9.2 % udd (n)+uc (D 0 ) n + k 0  0 ( k +  -) n + k 0  -  % (3.8 % ) 5.97 %

HIM SHLee 27 Rough estimate of events at RHIC c u d d u ++ Central collision (0-10%) dN cc /dy = 2.2 (phenix) Final stateDecay modeFinal statesBranching ratio ududc udu (p)+dc (D-) p + k 0  - P + k +  -  % 9.2 % udd (n)+uc (D 0 ) n + k 0  0 ( k +  -) n + k 0  -  % (3.8 % ) 5.97 %

HIM SHLee 28 Possible Decay mode of Tetra-quark c ud c exoticDecay modeFinal statesBranching ratio usccuc (D 0 )+sc (Ds-) D 0 (k 0  0, k +  - k 0  -  + ) Ds-(k 0 k -, k - k +  - ) 3.6 % ( 4.4 %) udcc dc (D-)+uc (D 0 ) D- (k 0  -l k +  -  - ) + D 0 (k 0  0, k +  - k 0  -  + )

HIM SHLee 29 Who can do it : STAR collaboration?

HIM SHLee 30 Who can do it : FAIR ?

HIM SHLee 31 Summary 1.While controvery exist over light pentaquark, Many Theories consistently predict bound heavy pentaquark 2. Quark model also predict metastable tetraquark 3.RHIC can be a very useful exotic factory  If found the first exotic ever, will tell us about QCD and dense matter  color superconductivity

HIM SHLee 32 References Experiments T. Nakano, Phys. Rev. Lett. 91 (03) K.~H.~Hicks, Prog. Part. Nucl. Phys. 55 (05) 647. Skyrme model controversy T.D.Cohen, Phys. Lett. B 581 (04) 175 H. Walliser and H. Weigel, Eur. Phys. J. A 26 (05) 361. D.Diakonov, V.Petrov and M.V.Polyakov, Z. Phys.A 359 (97) 305 Theory H. J. Lipkin, Phys. Lett. B 195 (87) 484. Fl. Stancu, Phys. Rev. D 58 (98) D. O. Riska, N. N. Scoccola, Phys. Lett. B 299 (93) 338. Y.Oh, B.Y. Park, D.P. Min, Phys. Lett. B 331 (94) 362. Phys. Rev. D 50 (94) R.L.Jaffe, F.Wilczek, Phys. Rev.Lett. 91(2003) present work H. Kim, Y. Oh, S.H.Lee, PLB 595 (04) 293: Y. Sarac, H.Kim, S.H.Lee, PRD 73 (06) S.H.Lee, Y. Kown, Y. Kown, PRL 96 (06)