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Observables and initial conditions from exact rotational hydro solutions. T . Csörgő 1 , I. Barna 1 and M.I . N agy 1, 3 1 MTA Wigner Research Center for Physics , RMKI 3 ELTE University, Budapest, Hungary Continuation: observables Two different family of equations of state - PowerPoint PPT Presentation
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Zimányi Winter School, 2013/12/05 Csörgő, T.1
Observables and initial conditions from exact rotational hydro solutions
T. Csörgő 1 , I. Barna 1 and M.I. Nagy 1,3
1 MTA Wigner Research Center for Physics, RMKI3 ELTE University, Budapest, Hungary
Continuation: observablesTwo different family of equations of state
Single particle spectraElliptic and higher order flows
Oscillations of HBT radiiWhat have we learnt?
Summary
Manuscript in preparationarXiv:1309.4390v2
Zimányi Winter School, 2013/12/05 Csörgő, T.2
Rotated Gaussian solutions
Note: (r’, k’) in fireball frame rotated wrt lab frame (r,k)
Note: in this talk, rotation in the (X,Z) impact parameter plane !
Zimányi Winter School, 2013/12/05 Csörgő, T.3
Role of EoS on acceleration
Lattice QCD type Eos is explosive
Tilt angle q integrates rotation in (X,Z) plane: sensitive to EoS!
Zimányi Winter School, 2013/12/05 Csörgő, T.4
Single particle spectra
In the rest frame of the fireball:
Rotation increases effective temperatures both in the
longitudinal and impact parameter direction
in addition to Hubble flows
Zimányi Winter School, 2013/12/05 Csörgő, T.5
Directed, elliptic and other flows
Note: model is fully analytic
As of now, only X = Z = R(t)spheroidal solutions are found
→ vanishing odd order flows
See next talk for fluctuations
From the single particle spectra→ flow coefficents vn
Zimányi Winter School, 2013/12/05 Csörgő, T.6
Reminder: Universal w scaling of v2
Notes: Rotation does not change thisJust modifiesRadial flow parameters
See +for more details
Zimányi Winter School, 2013/12/05 Csörgő, T.7
HBT radii for rotating spheroids
New terms with blue → Rotation decreases HBT radii similarly to Hubble flow.
Diagonal Gaussians in natural frame
Zimányi Winter School, 2013/12/05 Csörgő, T.8
HBT radii in the lab frameHBT radii without flow
But spheriodal symmetry of the solutionMakes several cross terms vanish → need for ellipsoidal solutions
Zimányi Winter School, 2013/12/05 Csörgő, T.9
HBT radii in the lab frameHBT radii without flow
But spheriodal symmetry of the solutionMakes several cross terms vanish → need for ellipsoidal solutions
Zimányi Winter School, 2013/12/05 Csörgő, T.10
Qualitatively rotation and flow similar
But need more time dependent calculations
and less academic studies(relativistic solutions)
Zimányi Winter School, 2013/12/05 Csörgő, T.11
SummaryObservables calculated
Effects of rotation and flowCombine and have same mass dependence
Spectra: slope increasesv2: universal w scaling remains valid
HBT radii:Decrease with mass intensifies
Even for spherical expansions:v2 from rotation.
Picture: vulcanoHow to detect the rotation?
Next step: penetrating probes
Zimányi Winter School, 2013/12/05 Csörgő, T.12
SummaryObservables calculated
Effects of rotation and flowCombine and have same mass dependence
Spectra: slope increasesv2: universal w scaling remains valid
HBT radii:Decrease with mass intensifies
Even for spherical expansions:v2 from rotation.
Picture: vulcanoHow to detect the rotation?
Next step: penetrating probes