Spectral shapes in pp collisions

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Presentation transcript:

Spectral shapes in pp collisions Mt-scaling for soft particles Power-law tail from hard scattering Increasing with energy

Scaling of spectra in dA and AA collisions mT scaling in pp and dA, but NOT in AA. Signature of radial flow.

Fitting p,K,p with hydrodynamics model 40-50% 80-92% 0-5%

Blast wave fits: Tfo and flow velocity

Flow velocity vs energy < bT > slowly increasing from AGS to SPS to RHIC

Basics of Hydrodynamics Hydrodynamic Equations Energy-momentum conservation Charge conservations (baryon, strangeness, etc…) Need equation of state (EoS) P(e,nB) to close the system of eqs.  Hydro can be connected directly with lattice QCD For perfect fluids (neglecting viscosity), Energy density Pressure 4-velocity Within ideal hydrodynamics, pressure gradient dP/dx is the driving force of collective flow.  Collective flow is believed to reflect information about EoS!  Phenomenon which connects 1st principle with experiment Caveat: Thermalization, l << (typical system size)

Inputs to Hydrodynamics Final stage: Free streaming particles  Need decoupling prescription t Intermediate stage: Hydrodynamics can be valid if thermalization is achieved.  Need EoS z Initial stage: Particle production and pre-thermalization beyond hydrodynamics Instead, initial conditions for hydro simulations Need modeling (1) EoS, (2) Initial cond., and (3) Decoupling