Title: Dynamics of Hadronization
1Dynamics of Hadronization Interplay of
Fragmentation and Recombination
Steffen A. Bass
Duke University RIKEN-BNL Research Center
- The baryon puzzle at RHIC
- Recombination Fragmentation Model
- Results single particle observables,
correlations entropy
- R.J. Fries, C. Nonaka, B. Mueller S.A. Bass,
PRL 90 202303 (2003) - R.J. Fries, C. Nonaka, B. Mueller S.A. Bass,
PRC 68 044902 (2003) - C. Nonaka, B. Mueller, M. Asakawa, S.A. Bass
R.J. Fries, PRC 69 031902 (2004) - R.J. Fries, S.A. Bass B. Mueller, PRL in print
(nucl-th/0407102) - C. Nonaka, B. Mueller, S.A. Bass M. Asakawa,
nucl-th/0501028
2Standard Model of Hadronization
?
- low pt
- hadron yields ratios fit with a SM
- spectra via Hydro
- high pt
- pQCD is applicable, hadronization via
fragmentation - a fast parton fragments via a color string a ?
hX - hadron spectrum is given by
3The baryon puzzle _at_ RHIC
- where does the large proton over pion ratio at
high pt come from? - why do protons not exhibit the same suppression
as pions? - fragmentation yields Np/Np
- fragmentation starts with a single fast parton
energy loss affects pions and protons in the same
way!
ratio of KKP fragmentation functions for p and p
from u quarks
4Species dependent saturation of elliptic flow
- hyperon v2 saturates later and higher than kaon
v2. - same effect observed for protons and pions.
- at low pT the phenomenology seems better
described in mT m0 than pT , indicating hydro
scaling, yet scaling breaks down for high pT - what drives the different pT scales for KS and ?
v2? - novel mechanism of baryon formation?
5RecombinationFragmentation Model
- basic assumptions
- at low pt, the quarks and antiquark spectrum is
thermal and they recombine into hadrons locally
at an instant - features of the parton spectrum are shifted to
higher pt in the hadron spectrum - at high pt, the parton spectrum is given by a
pQCD power law, partons suffer jet energy loss
and hadrons are formed via fragmentation of
quarks and gluons
6Recombination Pros Cons
- Pros
- for exponential parton spectrum, recombination
is more effective than fragmentation - baryons are shifted to higher pt than mesons,
for same quark distribution - understand behavior of protons!
- Cons
fragmenting parton ph z p, z
recombining partons p1p2ph
- simple recombination may violate entropy
conservation - gluons at hadronization need to be converted
7Recombination new life for an old idea
- High Energy Physics Phenomenology
- K.P. Das R.C. Hwa, Phys. Lett. B68, 459 (1977)
- Quark-Antiquark Recombination in the
Fragmentation Region - description of leading particle effect
- T. Ochiai, Prog. Theo. Phys. 75, 1184 (1986)
- E. Braaten, Y. Jia T. Mehen, Phys. Rev. Lett.
89, 122002 (2002) - R. Rapp E.V. Shuryak, Phys. Rev. D67, 074036
(2003) - Heavy-Ion Phenomenology
- T. S. Biro, P. Levai J. Zimanyi, Phys. Lett.
B347, 6 (1995) - ALCOR a dynamical model for hadronization
- yields and ratios via counting of constituent
quarks - R.C. Hwa C.B. Yang, Phys. Rev. C66, 025205
(2002) - R. Fries, B. Mueller, C. Nonaka S.A. Bass,
Phys. Rev. Lett. 90 - V. Greco, C.M. Ko and P. Levai, Phys. Rev. Lett.
90 - Anisotropic flow
- S. Voloshin, QM2002, Nucl. Phys. A715, 379
(2003) - Z.W. Lin C.M. Ko, Phys. Rev. Lett 89, 202302
(2002) - D. Molnar S. Voloshin, Phys. Rev. Lett 91,
092301 (2003)
8Recombination nonrelativistic formalism
- use thermal quark spectrum given by w(p)
exp(-p/T) - for a Gaussian meson wave function with momentum
width ?M, the meson spectrum is obtained as
9Recombination relativistic formalism
- choose a hypersurface S for hadronization
- use local light cone coordinates (hadron
defining the axis) - wa(r,p) single particle Wigner function for
quarks at hadronization - ?M ?B light-cone wave-functions for the meson
baryon respectively - x, x (1-x) momentum fractions carried by the
quarks - integrating out transverse degrees of freedom
yields
10Recombination vs. Fragmentation
Fragmentation
never competes with recombination for a thermal
(exponential) spectrum
but it wins out at large pT, when the spectrum
is a power law (pT)-b
11Hadron Spectra
12Hadron Ratios vs. pt
13Flavor Dependence of high-pt Suppression
- RF model describes different RAA behavior of
protons and pions - in the fragmentation region all hadron flavors
exhibit jet-quenching
14Elliptic Flow
- anisotropic or elliptic flow is sensitive to
initial geometry
low pt domain
high pt domain
more flow in collision plane than perpendicular
to it
less absorption in collision plane than
perpendicular to it
- total elliptic flow is the sum of both
contributions
r(pt) relative weight of the fragmentation
contribution in spectra
15Parton Number Scaling of v2
- in leading order of v2, recombination predicts
- smoking gun for recombination
- measurement of partonic v2 !
16Resonance v2 scaling violations
- QGP resonances
- hadronizing QGP, no rescattering
- HG resonances
- hadronic phase, h-h rescattering
Key v2 is additive for composite particles
17Two-Particle Correlations a Challenge?
- PHENIX STAR measure associated yields in pT
windows of a few GeV/c. - trigger hadron A, associated hadron B associated
yield as a function of relative azimuthal angle - clear jet-like structure observed at
- intermediate pT
- very similar to pp jet fragmentation?
- analyze as function of integrated yield
- simple recombination of uncorrelated
thermal quarks cannot reproduce two
particle correlations
18Recombination Inclusion of Correlations
- Recombination approach allows for two particle
correlations, provided they are contained in the
parton source distributions - Three distinct types are conceivable F-F, SH-F
and SS-SS - Ansatz for SS-SS for two mesons, use product of
correlated parton distributions - Which results in a correlated two hadron yield
19Correlations Proof of Principle
Meson-trigger
Baryon-trigger
- strong correlations from fragmentation, but
suppressed by soft triggers - combination of hard fragmentation and soft
recombination correlations with a fixed
correlation volume is compatible with data
20Recombination Entropy Puzzle
- Does recombination violate the 2nd law of
thermodynamics ? - particle number decreases drastically in
hadronization via reco - restrict reco approach to intermediate momenta,
ignore bulk - decay of hadronic resonances as possible solution
(Greco et al.) - need estimate of entropy at hadronization
21Entropy in the Hadronic Phase
- 1) resonance gas model
- massless particles
- massive particles
2) final state entropy from data
bosons
Pal Pratt, PLB578,310 (2004)
fermions
STAR PRC68, 044905 (2003)
MeV
- HydroUrQMD calculations indicate a 5 increase
in multiplicity due to rescattering in the
hadronic phase
4.72
5.15
- entropy content is larger than often assumed!
22Entropy in the Deconfined Phase
- Lattice QCD CP-PACS with Nt6 Nf2
- entropy content of the deconfined phase near TC
is strongly reduced due to interactions!
systematic uncertainties include thermodynamic
limit, continuum limit, unphysically large quark
mass
23Entropy Puzzle resolved?
Quark Phase
Hadron Phase
- No direct comparison of the entropy content of
both phases - Volume at hadronization ?
- Number of quarks on the lattice ?
24Summary Outlook
- The Recombination Fragmentation Model
- provides a natural solution to the baryon puzzle
at RHIC - describes the intermediate and high pt range of
- hadron ratios spectra
- jet-quenching phenomena
- elliptic flow
- leading / next-to-leading particle correlations
- issues to be addressed in the future
- treatment of gluons higher Fock states (work
in progress) - realistic space-time dynamics of parton source
- need improved data of identified hadrons at high
pt
25The End
26Connecting the dots
jet production
fragmentation
jet quenching
parton recombination
HBT
radial flow
reco/SM?
shattered color-glas
hydrodynamic evolution
27Parton Number Scaling of Elliptic Flow
- in the recombination regime, meson and baryon v2
can be obtained from the parton v2 in the
following way
- neglecting quadratic and cubic terms, one finds a
simple scaling law