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HBT results from UrQMD

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It includes 55 baryon species (with mass up to 2.25GeV) and 32 meson species ... the density dependent term used for formed baryons is used for 'pre-formed' particles. ... – PowerPoint PPT presentation

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Title: HBT results from UrQMD


1
HBT results from UrQMD
  • by Qingfeng Li
  • (_at_ FIAS/Frankfurt Huzhou)

In cooperation with M. Bleicher and H. Stoecker
2
outline
  • Brief introduction to the UrQMD and potential
    updates.
  • HBT results from UrQMD with cascade and with
    potentials.
  • The effects of the non-Gaussian and the resonance
    decay on HBT radii.
  • Other results from UrQMD with and without
    potentials stopping, elliptic flow.

3
The UrQMD model
  • UrQMD Ultra-relativistic Quantum Molecular
    Dynamics
  • It is a non-equilibrium transport model
  • It includes 55 baryon species (with mass up to
    2.25GeV) and 32 meson species (with mass up to
    1.91GeV)
  • Particles interact via
  • - Mean Field modification -
    Collisions (with measured and calculated cross
    sections)
  • Particles produce via
  • - Formation and decay of resonance
  • - Excitation and fragmentation of string
  • It provides full phase-space dynamics of
    heavy-ion collisions
  • it can be used to study HICs at energies from
    SIS to RHIC
  • The newest version 2.3 has been released.
    (http//th.physik.uni-frankfurt.de/urqmd/)

4
EoS
  • It is well-known that, in low-energy nuclear
    physics, the mean-field effect is essential.
  • Phenomenologically, the mean field includes
  • - bulk term (density dependent)
  • - surface term
  • - Yukawa term
  • - Pauli term
  • - symmetry energy term
  • - momentum dependent term

And, the Coulomb potential for charged particles
5
One example to solve the Flow puzzle at low
energies
At Eblt10 A GeV, the flow can be well reproduced
with a specified potential.
6
Treatment of the pre-formed hadrons
before string fragmentation
  • At high SPS and RHIC energies, particle
    production is dominated by the string mechanism.
  • The formation time of the hadron is determined by
    the yo-yo mode. During this time, the particles
    are taken as pre-formed. The transport of the
    pre-formed particles is treated to be
    free-streaming.
  • The reduced cross sections are only included for
    leading hadrons.

7
Why to consider the potential for pre-formed
hadrons?
  • sQGP tells us that there is a strong coupling
    between particles at early stage.
  • Small elliptic flow at RHIC was predicted by
    UrQMD.
  • The gg?gg interaction is believed not enough by
    Xu and Greiner (PRC71, 064901 (2005) ).
  • There is no free quarks/gluons in UrQMD.
  • Shorter formation time leads to increase the flow
    but also multiplicities drastically.

8
How to consider the pre-formed hadronic
potential?
  • To modify the interactions at early stage, more
    collisions (by considering a shorter formation
    time or larger cross sections for pre-formed
    particles) or a mean-field potential for
    pre-formed hadrons might be taken into account.
    The former idea has been checked in the AMPT and
    the HRM models. Here we would like to consider
    the latter idea.
  • As the first step,
  • the density dependent term used for formed
    baryons is used for pre-formed particles.
  • The pre-formed mesons act like pre-formed
    baryons but with a reduction factor (2/3) due to
    the quark-number difference.
  • The potential interaction between formed and
    pre-formed particles is neglected.
  • The pre-formed particles also contribute to the
    hadronic density (for pre-formed mesons, the
    2/3 factor is considered).

9
Meanwhile, to check Hybrid model HydroUrQMD
  • Ideal (31) D hydrodynamic evolution.
  • Time scales in hydro process from 6 to 12 fm/c
    at SPS energies.
  • Hadron gas equation of state (EoS) (No phase
    transition))
  • Hydrodynamic evolution until e lt 730 MeV/fm³ ( 5
    e0) in all cells
  • After the hydro freeze-out, hadronic cascade
    follows.
  • Typical times before cascade freezeout 20-25
    fm/c
  • Pion production changes slightly total yields
    less momentum distribution flatter at high SPS
    energies.

Thanks Hannah Pertersen
Jan Steinhimer
Also ask them for details, ?
10
Waiting for the EoS which originates from the
first principle lQCD
  • Although
  • The form of the potentials for the new phase is
    simple and rough (in my version)
  • The EoS with the phase transition is needed (in
    JanHannahs version)
  • However
  • it is quite necessary to study the effect of the
    mean field on the two-particle correlation right
    now!

11
The analyzing program and the Gaussian
parameterization
  • CRAB analyzing program http//www.nscl.msu.edu/p
    ratt/freecodes/crab/home.html
  • Three-dimensional Gaussian parameterization
  • LCMS is employed in normal calculations
  • Coulomb effect in FSI is considered for charged
    two-kaon correlation with a Bowler-Sinyukov
    method
  • non-Gaussian effect is discussed under the
    Edgeworth expansion

The fitting work can be done by the ROOT or the
ORIGIN software (using ?-squared method)
12
Non-Gaussian Effect
Non-Gaussian effect is visible in the
3D-correlation functions Its strongest in
longitudinal direction and weakest in sideward
direction.
13
Effect of resonance decay on HBT radii
Treatments of resonance decay affect HBT radii at
small kT, but not the RO/RS ratio
14
HBT results from UrQMD
In the pion case
15
Improvement to the mT-scaling
Left Plots
  • Without pre-formed hadron potential
  • RL of kaons and Lambdas Large
  • RO of all particles Large
  • RS of Lambdas Large

Right Plots
  • With pre-formed Hadron potential
  • RL of Kaons and Lambda follow
  • RO of all particles follow
  • RS of pions and Kaons follow
  • the mT-scaling

T.Csorgo etc, PRC 54, 1390(1996)
Without the consideration of the FSI in
hydro-dynamics
16
To solve the HBT t-puzzle
In the pion case
17
Not only for the ? source
The inclusion of pre-formed particle
interactions cures the deviations and allows for
a consistent understanding of the data.
The marked area illustrates the
uncertainties from non-Gaussian effect and
corrections on FSI
18
Why so ?
Under the assumptions of thermalization and
Gaussian-source shape, the HBT radii can be
expressed analytically as
RO term can be expanded as
Due to the strong phase-correlation induced by
the potentials, the term -2lt?Txtgt might be
comparable to the term lt?t2t2gt.
An important consensus Due to the strong x-t
correlation, RO/RS?1 does not mean t?0
19
Hydro EoS (Hadron-Gas) contribution
Hydro-process helps to drive down the Ro/Rs
ratio The ratio from hybrid model is still
larger than data since it is cascade after hydro
freeze-out.
In the hybrid model More EoS should be
checked More events and particle pairs Should be
analyzed.
Events4000-6000 Pairs 100M (for all kT bins)
20
stopping at SPS energies
In cascade mode Gaussian-like at all energies In
potential mode Two-bump occurs for p at high SPS
energies
Results are still preliminary
21
Elliptic flow at RHIC
  • The v2 at pt1GeV/c is driven up
  • with the pre-formed hadronic potential
  • The potential effect is strong in central HICs

Of course, the collision of partons is necessary
22
Conclusions
  • To understand the HBT t-puzzle and the mT
    -scaling, one needs to consider more about the
    interactions of particles at the early stage of
    HICs
  • The resonance decay contributes to the
    non-Gaussian phenomenon and the HBT radii but not
    the HBT t-puzzle.
  • A consistently thermal dynamic description of
    high energetic HICs is still awaiting.

23
Thanks
Reference list e-Print
arXiv0808.3457 nucl-th
Phys. Lett. B 663, 395 (2008)
Phys. Lett. B 659, 525 (2008) J. Phys.
G 34, 537 (2007) J. Phys. G
34, 2037 (2007) Phys. Rev. C
74, 064908 (2006) Phys. Rev.
C 73, 064908 (2006)
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