The Dilepton Probe from SIS to RHIC

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1 The Dilepton Probe from SIS to RHIC Hendrik van Hees Justus-Liebig Universität Gießen May 13, 2011 Institut für Theoretische Physik JUSTUS-LIEBIG- UNIVERSITÄT GIESSEN Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20

2 Outline 1 Electromagnetic probes in heavy-ion collisions 2 Dileptons at SIS energies 3 Dileptons at SPS and RHIC 4 Conclusions Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20

3 Electromagnetic probes in heavy-ion collisions γ, l ± : no strong interactions reflect whole history of collision: from pre-equilibrium phase from thermalized medium QGP and hot hadron gas from VM decays after thermal freezeout dn/(dy dm) π 0, η Dalitz decays ρ/ω Φ DD J/ Ψ ψ Drell Yan π,... ρ/ω γ e e + Low Intermediate High Mass Region > 10 fm > 1 fm < 0.1 fm M [GeV/c] Fig. by A. Drees Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20

4 Vector Mesons and electromagnetic Probes l + l thermal emission rates em. current-correlation function, Π µν [L. McLerran, T. Toimela 85, H. A. Weldon 90, C. Gale, J.I. Kapusta 91] dn e + e d 4 xd 4 q = α 2 gµν 3q 2 Im Π(ret) π3 µν (q) f B (q 0 ) q 2 =M 2 e + e vector-meson dominance model: Π µν = G ρ γ γ hadronic many-body theory for vector mesons ρ π B *, a 1, K 1,... ρ ρ ρ π N, K, π,... elementary processes cut self-energy diagrams Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20

5 Relation to the QCD-phase diagram at high temperature/density: restoration of chiral symmetry Lattice QCD: Tc χ Tc deconf Mass Mechanism of chiral restoration? Two main theoretical ideas dropping masses : m had ψψ melting resonances : broadening of spectra through medium effects More theoretical question: Realization of chiral symmetry in nature? Spectral Function Spectral Function "ρ" "ρ" Dropping Masses? Melting Resonances? "a 1 " "a 1 " pert. QCD pert. QCD Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20

6 Finite Temperature/Density: Idealized theory picture partition sum: Z(V, T, µ q, Φ) = Tr{exp[ (H[Φ] µ q N)/T ]} Real Time Z[V, T, µ,φ] Imag. Time Dynamical quantities off equilibrium: derivation of BUU,... Thermodyn. potentials bulk properties T, µ 0 vacuum analytic continuation [...,K. Chou, Z. Su, B. Hao, L. Yu 85, N.P. Landsmann, C.G. van Weert 87, E.A. Calzetta, B. Hu 08,...] Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20

7 Dileptons at SIS energies dileptons from heavy-ion collisions at DLS at E = 1A GeV [Porter et al, PRL 79, 1229 (1997)] large enhancement at low invariant masses unexplained DLS puzzle [Bratkovskaya et al (1999)] [Ernst et al (1998)] [Fuchs et al (2003)] Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20

8 Experimental confirmation DLS measurement confirmed by HADES at GSI [Sudol et al, EPJC 62, 81 (2009)] Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20

9 Theoretical HADES Puzzle one-boson-exchange model by Shyam/Mosel Bremsstrahlung in pp and pn collisions Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20

10 Hendrik van Hees readjustment (JLU Gießen) of resonance The channels Dilepton Probenecessary? May 13, / 20 Theoretical HADES Puzzle elementary pp- and pn-cross sections discrepancy between models (KK vs. SM); only difference: pseudo-scalar vs. pseudo-vector couplings (should be on-shell equivalent!) discrepancy of between theory and experiment in pn bremsstrahlung

11 Most recent update [R. Shyam, U. Mosel, PRC 82, (R) (2010)] crucial for pn: nucleon- and π-form factors (50% VMD+50% direct quarks) [G. E. Brown, M. Rho, and W. Weise, Nucl. Phys. A 454, 669 (1986)] Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20

12 Dileptons at SPS and RHIC radiation from thermal sources: Hadronic many-body theory [R. Rapp, J. Wambach 99] baryon effects important n B +n B relevant quantity (not net-baryon density)! ρ π B *, a 1, K 1,... ρ ρ ρ π N, K, π,... Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20

13 Dilepton rates: Hadron gas QGP in-medium hadron gas matches with QGP similar results also for γ rates quark-hadron duality!? consistent with chiral-symmetry restoration resonance melting rather than dropping masses Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20

14 Sources of dilepton emission in heavy-ion collisions 1 initial hard processes: Drell Yan 2 core emission from thermal source [McLerran, Toimela 1985] 1 dn (thermal) = q T dmdq T d 4 x dy Mdϕ dn (thermal) d 4 xd 4 Acc(M, q T, y) q use cylindrical thermal fireball with QGP, mixed and hadronic phase 3 corona emission from primordial mesons (jet-quenching) 4 after thermal freeze-out emission from freeze-out mesons [Cooper, Frye 1975] d N (fo) 3 q = q 0 q µ dσ µ f B (u µ q µ /T ) Γ meson l + l Acc Γ meson Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20

15 CERES/NA45 dielectron spectra (dn ee /dm) / <N ch > [100 MeV/c 2 ] good agreement also for dielectron spectra in 158 GeV Pb-Au low-mass tail from baryon effects Pb(158 AGeV)+Au (7% central) <N ch >=335 CERES 00 in-med ρ+ω+φ 4π mix QGP DY total total (no bar ρ) p t >0.2GeV 2.1<η<2.65 Θ ee >35mrad M ee [GeV] (d 2 N ee /dηdm) / (dn ch /dη) [100MeV] % Central Pb(158AGeV)+Au <N ch >=250 Cocktail QGP CERES free ρ in-med ρ+ω+φ+qgp+4π p t >0.2GeV 2.1<η<2.65 Θ ee >35mrad 4π M ee [GeV] Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20

16 M spectra (in p T slices) norm corrected by 3% due to centrality correction (min-bias data: N ch = 120, calculation N ch = 140) (1/N ch ) d 2 N µµ /(dm dη) (20 MeV) T c =T ch =175 MeV, a t =0.1 c 2 /fm all q T NA60 in-med ρ QGP prim ρ FO ρ 4π mix DY ω φ ω-t ex total +ω-t ex M (GeV) Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20

17 M spectra (in p T slices) norm corrected by 3% due to centrality correction (min-bias data: N ch = 120, calculation N ch = 140) (1/N ch ) d 2 N µµ /(dm dη) (20 MeV) T c =T ch =175 MeV, a t =0.1 c 2 /fm 0<q t <0.2 GeV NA60 in-med ρ QGP prim ρ FO ρ 4π mix DY ω φ ω-t ex total +ω-t ex M (GeV) Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20

18 M spectra (in p T slices) norm corrected by 3% due to centrality correction (min-bias data: N ch = 120, calculation N ch = 140) (1/N ch ) d 2 N µµ /(dm dη) (20 MeV) T c =T ch =175 MeV, a t =0.1 c 2 /fm 0.2 GeV<q t <0.4 GeV NA60 in-med ρ QGP prim ρ FO ρ 4π mix DY ω φ ω-t ex total +ω-t ex M (GeV) Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20

19 M spectra (in p T slices) norm corrected by 3% due to centrality correction (min-bias data: N ch = 120, calculation N ch = 140) (1/N ch ) d 2 N µµ /(dm dη) (20 MeV) T c =T ch =175 MeV, a t =0.1 c 2 /fm 0.4 GeV<q t <0.6 GeV NA60 in-med ρ QGP prim ρ FO ρ 4π mix DY ω φ ω-t ex total +ω-t ex M (GeV) Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20

20 M spectra (in p T slices) norm corrected by 3% due to centrality correction (min-bias data: N ch = 120, calculation N ch = 140) (1/N ch ) d 2 N µµ /(dm dη) (20 MeV) T c =T ch =175 MeV, a t =0.1 c 2 /fm 0.6 GeV<q t <0.8 GeV NA60 in-med ρ QGP prim ρ FO ρ 4π mix DY ω φ ω-t ex total +ω-t ex M (GeV) Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20

21 M spectra (in p T slices) norm corrected by 3% due to centrality correction (min-bias data: N ch = 120, calculation N ch = 140) (1/N ch ) d 2 N µµ /(dm dη) (20 MeV) T c =T ch =175 MeV, a t =0.1 c 2 /fm 0.8 GeV<q t <1.0 GeV NA60 in-med ρ QGP prim ρ FO ρ 4π mix DY ω φ ω-t ex total +ω-t ex M (GeV) Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20

22 M spectra (in p T slices) norm corrected by 3% due to centrality correction (min-bias data: N ch = 120, calculation N ch = 140) (1/N ch ) d 2 N µµ /(dm dη) (20 MeV) T c =T ch =175 MeV, a t =0.1 c 2 /fm 1.0 GeV<q t <1.2 GeV NA60 in-med ρ QGP prim ρ FO ρ 4π mix DY ω φ ω-t ex total +ω-t ex M (GeV) Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20

23 M spectra (in p T slices) norm corrected by 3% due to centrality correction (min-bias data: N ch = 120, calculation N ch = 140) (1/N ch ) d 2 N µµ /(dm dη) (20 MeV) T c =T ch =175 MeV, a t =0.1 c 2 /fm 2.0 GeV<q t <2.2 GeV NA60 in-med ρ QGP prim ρ FO ρ 4π mix DY ω φ ω-t ex total +ω-t ex M (GeV) Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20

24 M spectra (in p T slices) norm corrected by 3% due to centrality correction (min-bias data: N ch = 120, calculation N ch = 140) (1/N ch ) d 2 N µµ /(dm dη) (20 MeV) T c =T ch =175 MeV, a t =0.1 c 2 /fm 2.2 GeV<q t <2.4 GeV NA60 in-med ρ QGP prim ρ FO ρ 4π mix DY ω φ ω-t ex total +ω-t ex M (GeV) Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20

25 Importance of baryon effects baryonic interactions important! in-medium broadening low-mass tail! (1/N ch ) d 2 N µµ /(dm dη) (20 MeV) NA60 no baryons full model all q T T 10-9 c =T ch =175 MeV, a t =0.1 c 2 /fm M (GeV) Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20

26 IMR: QGP vs. multi-pion radiation dn µµ /dm (counts) semicentral In-In all p T QGP (EoS-A) QGP (EoS-B) QGP (EoS-C) 4π (EoS-A) 4π (EoS-B) 4π (EoS-C) M (GeV) different critical and freeze-out temperatures T c = MeV, T chem = MeV M- and p T spectra comparably well described! reason: T vs. volume maximal l + l emission for T = T max = M/5.5 hadronic and partonic radiation dual for T T c compatible with chiral-symmetry restoration! inconclusive whether hadronic or partonic emission in IMR! Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20

27 (Another) new Puzzle? huge enhancement in the LMR unexplained yet! /GeV) IN PHENIX ACCEPTANCE 2 (c dn/dm ee 10-1 min. bias Au+Au s = 200 GeV NN DATA y < 0.35 e p > 0.2 GeV/c cc ee (PYTHIA) cc ee (random correlation) R.Rapp & H.vanHees cocktail T sum w/ ρ vacuum sum w/ ρ broadening sum/ ρ dropping) partonic yield (PY) model: Rapp, HvH [A. Adare et al (PHENIX), PRC 81, (2010)] (GeV/c ) m ee Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20

28 (Another) new Puzzle? huge enhancement in the LMR unexplained yet! model: PHSD [O. Linnyk, W. Cassing, E.L. Bratkovskaya, J. Manninen, NPA 855, 273 (2011)] Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20

29 Conclusions and Outlook dilepton spectra in-medium em. current correlator SIS energies dominated by bremsstrahlung and Dalitz decays puzzle in OBE models (pp vs. pn)? nucleon/π form factors important bremsstrahlung SPS and RHIC energies excess yield dominated by radiation from thermal sources baryons essential for in-medium properties of vector mesons melting vector mesons with little mass shift IMR well described by scenarios with radiation dominated either by QGP or multi-pion processes (depending on EoS) quark-hadron duality of l + l rates around T c compatible with chiral symmetry restoration! new RHIC?!? recent review: R. Rapp, J. Wambach, HvH, Landolt-Börnstein, 1-23A arxiv: [hep-ph] Hendrik van Hees (JLU Gießen) The Dilepton Probe May 13, / 20