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Sketch of a competitive experiment on dense nuclear matter in the (future) Nuclotron energy range (2-5 AGeV). Helmholtz Summer School 2006, Dubna, Student Seminar Peter Senger, GSI. 1. The physics case:  Nuclear equation of state at high baryon densities

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Sketch of a competitive experiment on dense nuclear matter

Sketch of a competitive experiment on dense nuclear matter

in the (future) Nuclotron energy range (2-5 AGeV)

Helmholtz Summer School 2006, Dubna, Student Seminar

Peter Senger, GSI

1. The physics case:

 Nuclear equation of state at high baryon densities

 Search for a first order phase transition between

hadronic matter and quark matter

2. Observables:

 Yield, spectra and collective flow of hadrons

incl. (multi-) strange particles

 Event-by-event fluctuations of particle yields and

mean transverse momenta

 Excitation functions (1-5 AGeV),

system size and centrality dependence

3. Estimation of feasibility

 Particle production cross sections in heavy ion collisions

 Reaction rates

4. Experimental conditions and requirements

 Beam energy and intensity

 Detectors (tracking, momentum determination, particle identification)

 Efficiencies, signal-to background


Sketch of a competitive experiment on dense nuclear matter

Transport calculations: energy densities

Baryon density in central cell (Au+Au, b=0 fm):

HSD: mean field, hadrons + resonances + strings

QGSM: Cascade, hadrons + resonances + strings

C. Fuchs, E. Bratkovskaya, W. Cassing


Sketch of a competitive experiment on dense nuclear matter

Ch. Fuchs, Tübingen


Sketch of a competitive experiment on dense nuclear matter

“Trajectories” from UrQMD

L. Bravina, M. Bleicher et al., PRC 1998


Sketch of a competitive experiment on dense nuclear matter

Event-by-event analysis by NA49: 5% most central Pb+Pb collisions at 158 AGeV

liquid

gas

coexistence

Below Tc: 1. order phase transition

above Tc: no phase boundary

At the critical point:

Large density fluctuations,

critical opalescence

The critical point


Sketch of a competitive experiment on dense nuclear matter

Strangeness production in central Pb+Pb collisions

C. Blume et al., nucl-ex/0409008 (CERN NA49)


Sketch of a competitive experiment on dense nuclear matter

Multistrange hyperons

from p+Be, p+Pb and Pb+Pb at 158 AGeV/c

Strangeness enhancement:

F. Antinori et al, Nucl. Phys. A 661 (1999) 130c


Sketch of a competitive experiment on dense nuclear matter

Thermal production of multistrange hyperons ?


Sketch of a competitive experiment on dense nuclear matter

Production processes of multistrange hyperons

Production processes and thresholds

pp  K+0p ( Ep 1.6 GeV )

pp  K+K-pp(Ep  2.5 GeV)

pp K+K+-p ( Ep  3.7 GeV )

pp K+K+K+-p ( Ep  7.0 GeV )

0(s d u) m =1116 MeV

- (s s d) m =1321 MeV

- (s s s) m =1672 MeV

pp 0 0pp ( Ep  7.1 GeV )

pp + -pp ( Ep  9.0 GeV )

pp + -pp ( Ep  12.7 GeV )

In heavy ion collisions: “cooking” of multistrange hyperons ?

Strangeness exchange reactions:

2) 0 K-  -00 K+  +0

3) -K-  -- +K+  ++

Enhanced yield at high densities


Hyperon properties

Hyperon properties


Particle multiplicities for central au au collisions from urqmd calculations

Particle multiplicities for central Au+Au collisionsfrom UrQMD calculations

Au+Au 5 AGeV

central minimum bias

8.2 2

0.06 0.015

0.0002 0.00005


Sketch of a competitive experiment on dense nuclear matter

Reaction rate:R = NB · · NT/F·

  • R = reactions/sec

  • NB = beam particles/sec

  • = cross section [barn = 10-24cm2]

    NT /F= target atoms/cm2 = NA ··d/A

    with Avogadros Number NA = 6.02·1023· mol-1,

    material density  [g/cm3],

    target thickness d [cm]

    atomic number A

     = efficiency


Sketch of a competitive experiment on dense nuclear matter

Determination of target thickness

Reaction cross section:

R = · (2 ·R)2 = 4 ·(r0·A1/3)2 with r0=1.2 fm

Au+Au collisions:

A=197  R = 6.1 barn, 1 barn = 10-24 cm2

Reaction probability for Au+Au collisions:

R/NB = R· NT/F

= 6.1 b ·6.02·1023··d/A

= 6.1 ·10-24 cm2·6.02·1023·19.3 g/cm3·d/197 = 1%

target thickness d = 0.027 cm


Sketch of a competitive experiment on dense nuclear matter

Production cross sections for min. bias Au+Au collisions at 5 AGeV:

(Λ) = M(Λ) x R = 2 x 6.1 b = 12.2 b

(Ξ) = M(Ξ) x R = 0.015 x 6.1 b = 0.09 b

(Ω) = M(Ω) x R = 0.00005 x 6.1 b = 0.0003 b

Particle production probabilities for min. bias Au+Au at 5 AGeV:

R(Λ)/NB = (Λ)·NA··d/A = (Λ) [b]·1.6·10-3 = 2·10-2

R(Ξ)/NB = (Ξ)·NA··d/A = (Ξ) [b]·1.6·10-3 = 1.4·10-4

R(Ω)/NB =(Ω)·NA··d/A = (Ω) [b]·1.6·10-3 = 4.8·10-7

R(Λ)/NB = (Λ)·NA··d/A· = ?


Sketch of a competitive experiment on dense nuclear matter

  • Acceptances and Efficiencies

  • = · p ·Det · Trigg · DAQ · analysis

    with

  •  = angular acceptance

  • p = momentum acceptance

  • Det = detector efficiencies

  • Trigg = trigger efficiencies

  • DAQ= deadtime correction of DAQ

  • analysis = efficiency of analysis

  • (track finding, cuts for background suppression , ...)

Typical values:

 0.5, p 0.8, Det 0.9, Trigg  0.9,DAQ  0.5,analysis  0.3,

 0.05


Sketch of a competitive experiment on dense nuclear matter

Typical particle detection probabilities in Au+Au at 5 AGeV:

R(Λ)/NB = (Λ)·NA··d/A· = 2·10-2·0.05=1·10-3

R(Ξ)/NB = (Ξ)·NA··d/A· = 1.4·10-4·0.05 = 7·10-6

R(Ω)/NB =(Ω)·NA··d/A· = 4.8·10-7·0.05 = 2.4·10-8

Required particle yield for a competitive physics analysis:

(differential values like v2 as function of pT): 1 Mio particles

Required number of beam particles (integrated luminosity):

for Λ: NB x sec = 106/ 1·10-3 = 1·109

for Ξ : NB x sec = 106/ 7·10-6 = 1.4·1011

for Ω: NB x sec = 106/ 2.4·10-8 = 4.2·1013

Required beam time for a Au-beam intensity of NB = 106/sec:

for Λ: t = 1·103 sec = 17 min

for Ξ : t = 1.4·105 sec = 1.6 d

for Ω: t = 4.2·107 sec = 500 d

These numbers refer to one

collision system and one

beam energy only.

Systematic studies require

excitation functions

(several beam energies)

with different

collision systems !


Sketch of a competitive experiment on dense nuclear matter

Possible experiment layout

TOF wall measures

Time-of-flight for

mass determination.

needed:

fast detectors

tracking

chambers

Dipole

magnet

Time-of-flight wall

(RPC)

Silicon

tracker

Tracking chambers

are needed to match

tracks in Silicon detector

to hits in TOF wall

Silicon tracker in magnetic

dipole field measures tracks

(particle numbers) and curvature

(particle momentum).

6 m


Hyperons at ags au au 6 agev

Ξ - Hyperons at AGS: Au+Au 6 AGeV

  • Threshold production of Xi measured

  • Main detector: TPC with PID capabilities

  • Measured in 4 centrality bins

  • ~ 250 Xi measured

  • Results consistent with UrQMD

  • Neural network algorithm used for the bgd suppression


Invariant mass distributions

Invariant mass distributions Ξ-

After impact parameter cut

Before cuts

  • Invariant mass resolution is improved with the dca cut

  • σ = 1.7 MeV

  • Signal yield: 264

After dca cut

All cuts


Invariant mass distributions1

Invariant mass distributions Ω-

After impact parameter cut

Before cuts

  • Invariant mass resolution is improved with the dca cut

  • σ = 2.2 MeV

  • Signal yield: 486

After dca cut

All cuts


Results on without pid

Results on Ω- without PID

Statistics: 1.4 108 events


Invariant mass distributions with perfect pid

Invariant mass distributions Ω- with perfect PID

After impact parameter cut

Before cuts

After dca cut

All cuts


Results on with perfect pid

Results on Ω- with perfect PID

Statistics: 1.4 108 events


Conclusions

Conclusions

  • Multistrange hyperon measurements seem feasible in Au+Au collision at 5 AGeV

  • Track reconstruction, momentum determination and particle identification is required

  • Beam intensities of better than NB = 106/sec are needed


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