Hot QCD Matter Peter Jacobs Lawrence Berkeley National

Hot QCD Matter Peter Jacobs Lawrence Berkeley National Laboratory/CERN Lecture 1: Tools Lecture 2: Initial conditions: partonic structure and global observables Lecture 3: Collective flow and hydrodynamics Lecture 4: Jets and other hard probes 6/14/12 Hot QCD Matter - Lecture 2 1

Nuclear geometry and hard processes: Glauber theory Glauber scaling for hard processes with large momentum transfer • short coherence length successive NN collisions independent • p+A is incoherent superposition of N+N collisions Normalized nuclear density r(b, z): Nuclear thickness function Inelastic cross section for p+A collisions: 6/14/12 Hot QCD Matter - Lecture 1 2

Experimental tests of Glauber scaling: hard cross sections in p(m)+A collisions Glauber scaling expectation: sinel for 7 Ge. V muons on nuclei M. May et al, Phys Rev Lett 35, 407 (1975 ) s. Drell-Yan/A in p+A at SPS A 1. 00 NA 50 Phys Lett B 553, 167 A 6/14/12 Hard cross sections in p+A as A 1. 0 Hot QCD Matter - Lecturescale 1 3

Measuring collision geometry I Nuclei are “macroscopic” characterize collisions by impact parameter Correlate particle yields from ~causally disconnected parts of phase space correlation arises from common dependence on collision impact parameter 6/14/12 Hot QCD Matter - Lecture 1 4

Measuring collision geometry II Forward neutrons • Order events by centrality metric 6/14/12 • Classify into percentile bins of “centrality” HI jargon: “ 0 -5% central” Connect to Glauber theory via particle production model: • Nbin: effective number of binary nucleon collisions (~510% precision) • Npart: number of (inelastically scattered) “participating” nucleons Charged hadrons h~3 Hot QCD Matter - Lecture 1 5

Scaling of cross sections using Glauber theory plays a central role in quantitative analysis of experimental measurements and connection to theory. Let’s test it experimentally in A+A collisions… 6/14/12 Hot QCD Matter - Lecture 1 6

Glauber scaling tests at LHC: Scaling of direct photon, Z, W yields in Pb+Pb vs p+p EW bosons do not interact with Quark-Gluon Plasma – should see perturbative production rates in Pb+Pb collisions 6/14/12 Yields all scale with Nbin: Glauber scaling OK for hard processes Hot QCD Matter - Lecture 1 7

Very simple question: can we understand the total number of particles generated in a heavy ion collision (a. k. a. “multiplicity”)? LHC RHIC STAR 6/14/12 Hot QCD Matter - Lecture 2 8

Let’s start with the “initial state”: what is the role of the partonic structure of the projectiles? Hadrons and nuclei are compound objects with complex partonic structure Multiple interactions drive the collision dynamics we need to understand the initial (incoming) state… 6/14/12 Hot QCD Matter - Lecture 2 9

Perturbative QCD factorization in hadronic collisions Hard process scale Q 2>>L 2 QCD p. QCD factorization: parton distribution fn fa/A + partonic cross section s + fragmentation fn Dh/c x=momentum fraction of hadron carried by parton (infinite momentum frame) 6/14/12 Hot QCD Matter - Lecture 2 10

Q 2 evolution of Parton Distribution and Fragmentation Functions Parton Distribution Fucntions (PDFs) and fragmentation functions are not calculable ab initio in p. QCD Q 2 evolution small Q 2 They are essentially non-perturbative in origin (soft, long distance physics) and must be extracted from data at some scale Q 02 p. QCD then specifies how PDFs and fragmentation functions evolve from Q 02 to any other scale Q 2 (DGLAP evolution equations) 6/14/12 Hot QCD Matter - Lecture 2 large Q 2 0. 1 1. 0 x 11

Precision measurements of proton structure: Deep Inelastic Scattering (DIS) of e+p 6/14/12 Hot QCD Matter - Lecture 2 12

Probing the structure of the proton with DIS Define a new quantity F 2: parton density for flavor i Sum over quark flavors charge for flavor i If a proton were made up of 3 quarks, each carrying 1/3 of proton’s momentum: F 2 with some smearing x • If partons are point-like and incoherent then Q 2 shouldn’t matter 6/14/12 Hot QCD - Lecture 2 13 • Bjorken scaling: F 2 has no Q 2 Matter dependence

Measurement of proton F 2 Tour de force for perturbative QCD: Q 2 does matter! • Partons are not point-like and incoherent. • Hadronic structure depends on the scale at which you probe it! Spectacular agreement with DGLAP evolution 6/14/12 Hot QCD Matter - Lecture 2 14

Parton Distribution Function in the proton Low Q 2: valence structure Soft gluons 6/14/12 Q 2 evolution (gluons) Valence quarks (p = uud) Hot QCD Matter - Lecture 2 15 Q 2 Gluon density decreases towards lower x ~ 1/3

Gluon saturation at low x Fix Q 2 and consider what happens as x is decreased… Problem: low x gluon density cannot increase without limit (unitarity bound) Solution: • gluons carry color charge • if packed at high enough density they will recombine gluon density is self-limiting 6/14/12 Hot QCD Matter - Lecture 2 gluon saturation ! 16

Gluon recombination in nuclei Uncertainty principle: wave fn. for very low momentum (low x) gluons extends over entire depth of nucleus Define gluon density per unit area in nucleus of mass A: Gluon recombination cross section: Recombination occurs if: Saturation momentum scale Qsat 2 satisfies self-consistent condition: 6/14/12 Gluon recombination Q 22 < Qsat 2 Hot QCD Matter for - Lecture Nuclear enhancement of Qsat 17

Saturation scale vs nuclear mass What’s that? 6/14/12 LHC RHIC Heavy ions Hot QCD Matter - Lecture 2 18

Color Glass Condensate (CGC) in n Semi-classical effective theory of saturation e e s s e l c er i t b r a m p u n ed o t g r l a a h n io )c t e r t o a s t i p s o h r l c a p i n is wh (fi n , f ) o i o 1 s r i ~ ll K be o ( c m n u n o i lis n: y l o v o i a t c e a e l h √s d n Trans ctor in a early in th fects a y t i l e a f t d r e e t e en c the d ns scatter aturation n o i is l o o u o l t c g e u ith of d w d g e s n li es a r c p s p c u i s if c e p s cts i d e r P 6/14/12 Hot QCD Matter - Lecture 2 19

Can we see Saturation experimentally? Asymmetric deuteron+Au collisions at RHIC: • Look at forward 2 -particle correlations • Back-scatter off Au-nucleus: low x in Au p 0 Ep qp d xg p N xq p N Triggered hadron Au Associated hadron Saturation picture: “mono-jets” Dilute parton system (deuteron) Monojet Perturbative picture: Back-to-back jets PT is balanced by many gluons Dense gluonfield (Au) 6/14/12 Hot QCD Matter - Lecture 2 20

What are we plotting? 2 -particle correlations in azimuthal angle qp d xq p N xg p N Au Associated hadron Transverse plane Trigger trigger 21 6/14/12 p 0 Ep Hot QCD Matter - Lecture 2 Triggered hadron

STAR: d+Au forward azimuthal correlations p+p Centrality Averaged Peripheral d+Au perturbative Central Mono-jet/saturation CGC Model : Albacete+Marquet (ar. Xiv: 1005. 4065) 6/14/12 Hot QCD Matter - Lecture 2 22

J. Albacete, Hard Probes 2012 But maybe not: Conventional p. QCD mechanisms plus conventional nuclear effects work as well… 6/14/12 Hot QCD Matter - Lecture 2 23

Next step: p+A at LHC (November 2012 run) C. Salgado, Hard Probes 2012 Region of greatest interest: low x and low Q 2 6/14/12 Hot QCD Matter - Lecture 2 24

Summary thus far QCD is remarkably successful in describing the partonic stucture of the proton over a vast kinematic range There are good reasons to expect signficant modification of this structure in heavy nuclei saturation • Some experimental evidence in favor of saturation in forward d+Au correlations at RHIC • LHC p+A run this November will provide a wealth of new data to address the issue in more detail (crucially: much smaller x) Does any of this play a role in high energy nuclear collisions? Let’s go back to our original question: what generates all the particles? 6/14/12 Hot QCD Matter - Lecture 2 25

Multiplicity measurements Count the number of charged particles per unit pseudo-rapidity Simplest “bulk” observable that characterizes the collision RHIC LHC STAR 6/14/12 Hot QCD Matter - Lecture 2 26

Charged particle multiplicity ALICE PRL, 105, 252301 (2010), ar. Xiv: 1011. 3916 t n a p i √s. NN=2. 76 Te. V Pb+Pb, 0 -5% central, |η|<0. 5 c i t r f pa o r i a p r “pe e p z i + l p a o m t r e o r N pa m o c o t ” nucleons odeling) m r e b u a l (G 6/14/12 LHC: 2 d. Nch/dη / <Npart> = 8. 3 ± 0. 4 (sys. ) Hot QCD Matter - Lecture 2 27

d. Nch/dη: model comparisons PRL, 105, 252301 (2010), ar. Xiv: 1011. 3916 √s. NN=2. 76 Te. V Pb+Pb, 0 -5% central, |η|<0. 5 d. Nch/dη = 1584 ± 76 (sys. ) p. QCD-based MC Saturation WAGs pp extrapolation Energy density estimate (Bjorken): 6/14/12 Hot QCD Matter - Lecture 2 28

d. Nch/dη: Centrality dependence PRL, 106, 032301 (2011), ar. Xiv: 1012. 1657 2. 5% bins ALICE RHIC scale LHC scale |η|<0. 5 Pb+Pb, √s. NN=2. 76 Te. V Interpolation between 2. 36 and 7 Te. V pp peripheral 6/14/12 central Striking centrality-independent scaling RHIC LHC Hot QCD Matter - Lecture 2 29

Does saturation play a role? peripheral central RHIC Expectation from saturation models: factorization of centrality and energy dependence: 6/14/12 Hot QCD Matter - Lecture 2 LHC 30

d. Nch/dη vs. centrality: models PRL, 106, 032301 (2011), ar. Xiv: 1012. 1657 Pb+Pb, √s. NN=2. 76 Te. V Two-component perturbative models Soft (~Npart) and hard (~Nbin) processes Saturation-type models Parametrization of the saturation scale with centrality Albacete and Dumitru (ar. Xi. V: 1011. 5161): • Most sophisticated saturation model: evolution, running coupling • Captures full centrality dependence…? 6/14/12 Hot QCD Matter - Lecture 2 31

Summary of Lecture 2 Initial state: approaching quantitative control Final charged multiplicity closely related to initial gluon multiplicity: Good evidence that gluon saturation in nuclei plays a role Smooth evolution of multiplicity with collision energy and system size 6/14/12 Hot QCD Matter - Lecture 2 32

Why is any of this surprising? How could it be different? Thermalized system: massive reinteractions, generation of large numbers of particles and softening of momentum spectra expect stronger dependence on energy and system size…? ? Apparently not the case Next lecture: additional news about equilibration. 6/14/12 Hot QCD Matter - Lecture 2 33

Backup 6/14/12 Hot QCD Matter - Lecture 2 34

Simpler case: deep inelastic scattering (DIS) of e+p 6/14/12 Hot QCD Matter - Lecture 2 35

Glauber Theory for A+B Collisions Nuclear overlap function: Average number of binary NN collisions for B nucleon at coordinate s. B: Average number of binary NN collisions for A+B collision with impact parameter b: 6/14/12 Hot QCD Matter - Lecture 1 36