peter steinbergbnl/riken flow workshop landau hydrodynamics & rhic phenomenology peter steinberg...
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![Page 1: Peter SteinbergBNL/RIKEN Flow Workshop Landau Hydrodynamics & RHIC Phenomenology Peter Steinberg Brookhaven National Laboratory Workshop on Collective](https://reader034.vdocuments.us/reader034/viewer/2022051415/56649cb85503460f9497f6c0/html5/thumbnails/1.jpg)
Peter Steinberg BNL/RIKEN Flow Workshop
Landau Hydrodynamics &RHIC Phenomenology
Peter SteinbergBrookhaven National Laboratory
Workshop on Collective Flow & QGP PropertiesNovember 17-19, 2003
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Peter Steinberg BNL/RIKEN Flow Workshop
Radial Flow
RHIC Data & Calculations by U. Heinz / P. Kolb
=.6c
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Peter Steinberg BNL/RIKEN Flow Workshop
A different perspective• We’re used to this in the transverse direction
• What about the longitudinal direction? Clearly not isotropic!
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Peter Steinberg BNL/RIKEN Flow Workshop
Landau Physical Picture
Incominghadrons or
nuclei
Full stopping
Longitudinalexplosion
Rapid ThermalizationEntropy productionPressure gradient0VV
R
RapidityDistributions
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Peter Steinberg BNL/RIKEN Flow Workshop
Entropy Production• Fermi’s argument: If we assume the
system is a perfect blackbody but system is Lorentz-contracted
3 3/ 4n T s
4
0
s sT s
V V
1/ 4T s
3/ 4 3/ 43 1/ 4
1/ 2
s sN nV VT s s
s
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Peter Steinberg BNL/RIKEN Flow Workshop
“Landau Hydro”• Source-free 3D hydro equations
• Massless EOS
• No scale in the problem (scale invariance)• Only from boundary conditions (Carruthers)
• Initial geometry, freezeout temperature T~m
0T
0p
Energy-MomentumConservation
Equation ofState (EOS)
3p
LandauBilenkijMilekhinShuryakCooperFryeSchonbergCarruthersAndersson…
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Peter Steinberg BNL/RIKEN Flow Workshop
Entropy from EOS
3/ 4
1/ 4
1/ 4
0
4
3
~
~
~
n Ts p
Ts p
d Tds
s
T
N
20p c
2020
1
1
aN s
ca
c
Cooper, Frye, Schonberg 1975
N(s) depends on EOS
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Peter Steinberg BNL/RIKEN Flow Workshop
The “Landau Solution”• Many authors refined original ideas
• This is how things ended up by early 1980’s
• Universal multiplicity formula
• Gaussian Rapidity Distributions
• Thermal pT spectra
2 / 2
1/ 4 2ln ln22
y L
yp
dN e sKs L
dy mL
1/ 4~chN Ks
exp /TT T
dNp T
p dp
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Peter Steinberg BNL/RIKEN Flow Workshop
Universality in 1981Carruthers 1981
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Peter Steinberg BNL/RIKEN Flow Workshop
Landau vs. Bjorken• Landau is not what we expected for RHIC
• Expected Bjorken to simplify things @ 900
• “very reasonable that for nucleus-nucleus collisions the initial conditions for fluid of quanta produced between the receding pancakes are the same as existed in any other frame”
• For Landau, y=0 not special• Most of the energy goes forward
• Correctness of initial conditions must be based on data• Apparently led to many disagreements in 70’s
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Peter Steinberg BNL/RIKEN Flow Workshop
Bjorken or Landau @ ISR?
• Boost invariant• Pseudorapidty• Near mid-
• Gaussian• Rapidity• Look everywhere
Carruthers & Duong-van 1973
ISR 53 GeVPISA/SUNYSB
1972 (unpub.)
“duck orrabbit”
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Peter Steinberg BNL/RIKEN Flow Workshop
Connections vs. Coincidences
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Peter Steinberg BNL/RIKEN Flow Workshop
dN
/d
19.6 GeV 130 GeV 200 GeV
Npart
PHOBOS dN/dh
• These plots are interpreted as the emergence of the central plateau with increasing collision energy
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Peter Steinberg BNL/RIKEN Flow Workshop
Coincidence #1: BRAHMS dN/dy
BRAHMS Preliminary 2003
~ 2.3
ln 100 2.15
BRAHMSy
Landauy
BRAHMS showsno plateau
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Peter Steinberg BNL/RIKEN Flow Workshop
= - ybeam
PHOBOS Au+Au
19.6 GeV
130 GeV
200 GeV
Limiting Fragmentation
' ~ ln ln /beam T py x p M
2part
dNdN
Seen generically in manysystems (AA, pp…)
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Peter Steinberg BNL/RIKEN Flow Workshop
Coincidence #2Limiting fragmentation (x scaling) somehow “built-in”
20s GeV
60s GeV
130s GeV
200s GeV
Cooper & Schonberg 1973
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Peter Steinberg BNL/RIKEN Flow Workshop
CGC Calculations• KLN: Final state from 21 gluon scattering
• Overall scale
• Jacobian
• Quark counting
gN cN
~dN dN
d dy
41 x
(LPHD)
Energy, Rapidity, Centrality
Kharzeev, Levin, Nardi (2001)
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Peter Steinberg BNL/RIKEN Flow Workshop
Coincidence #3
KLN, =.3Landau Hydro
30s GeV
60GeV
200GeV
Normalized here
“Default” KLN parameters(normalize @ 200 GeV peak)
Scale in similar fashionboth height & width
Compare dN/dy
This was a surprise.
Of course different KLNparameters can make the
agreement worse
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Peter Steinberg BNL/RIKEN Flow Workshop
Landau & The QGP• Landau’s physics is still
used in relevant physics arguments
• Gazdzicki et al (NA49)• Massless EOS• Chemical potential = 0• “Entropy” pions ~ s1/4
• Lots of features vs. pp• Pion suppression• Crossover• Enhancement!
• Is this evidence of a phase transition?
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Peter Steinberg BNL/RIKEN Flow Workshop
Some Issues• Landau left out B (
= 0 is OK)
OK for pp, not AA
• All particles contribute to the entropy• Thermal models
determine all species given T, B
• Landau & Bilenkij
~ 4
S N
Ts p Bn
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Peter Steinberg BNL/RIKEN Flow Workshop
Comparison with e+e-
(Mueller 1983)
)/exp( sAsch BN
Relative to p+p, NA49 featuresRelative to e+e-, different story
PHOBOS
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Peter Steinberg BNL/RIKEN Flow Workshop
Baryon Density & Entropy
PAS, Cleymans, et al
AGS SPS RHIC
Fix pp vs. AA by removingenergy of leading particles
Can use thermal modelapproach to “fix” A+A:Predictable decrease
in entropy densityfrom baryon number
conservation
PAS, Work in progress
No more features
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Peter Steinberg BNL/RIKEN Flow Workshop
Historical Interlude• Landau (1953) considered pp, pA, AA• Cooper & Frye (1973) tried e+e-
• More compact initial state (R~1/s)• Initial expectations 3+1D, jets 1+1D!
• In this context, similar multiplicities given similar energies not crazy
• However, many competing models on the market. • Parton model / QCD eventually achieved
descriptive power in many details.
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Peter Steinberg BNL/RIKEN Flow Workshop
Coincidence #4: Landau vs. Mueller
Landau “better” atlow energies
MLLA QCD better athigher energies
(esp. including pp@s/2)
Difference increasesdramatically athigher energies
(LHC day-1 important)
Oddity: slower increasefrom pQCD is like
2 1/ 3sc
Landau
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Peter Steinberg BNL/RIKEN Flow Workshop
Does this make sense?• These comparisons ask more questions than
they answer• Is e+e- “thermal”?• Why is pQCD ~ blackbody formula?• Are leading particles relevant?
• A+A looks “local” (Npart scaling)
• Little work on this for 30 years
• Coincidence #4: Is there a deep theoretical connection between pQCD and hydro?• Hard processes should be immune…
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Peter Steinberg BNL/RIKEN Flow Workshop
Transverse Expansion?• Carruthers & Minh
• Noticed that spectrum of high-pT 0 described by
• Coincidence #5, is the transverse spectrum also gaussian in rapidity?• Carruthers conjecture
• Let’s look at higher energy, higher pT
2exp / 2TT T
dNC y L
p dp
1ln2
T TT
T T
m py
m p
~ .51L
Carruthers & Duong-van (PRL 1973)
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Peter Steinberg BNL/RIKEN Flow Workshop
Coincidence #5: RHIC pp Data• One parameter fit to STAR
& PHENIX pp data• L = 0.570±.001 (STAR)• L = 0.541±.001 (PHENIX)
• Power-law has two:
• Not sure if or how this formula works with A+A• Mass dependence of yT
PHENIX d 0
STAR dN h+h-
0
1n
Tp
p
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Peter Steinberg BNL/RIKEN Flow Workshop
Conclusions• Landau’s concepts & results appear to be relevant to
RHIC phenomena• Why do we hold on to boost invariance?
• Coincidences or Connections?• #1 Gaussian dN/dy, widths • #2 Limiting fragmentation built-in• #3 Similar evolution in Landau & KLN• #4 Universal multiplicity formula & QCD• #5 Gaussian dN/dyT spectra in pp
• Serious issue: connection to QCD?• What are the relevant degrees of freedom that thermalize?
• Still: with few input ingredients, unified description of many facts
~ ln / 2y s
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Peter Steinberg BNL/RIKEN Flow Workshop
Comments• “A true heresy should arise in the context of an established faith.”
(Carruthers 1973)• Does collective-variable approach contrast with QCD?
• Does Landau hydro conflict with Bjorken hydro?
• Interesting issues in 1973 still sound interesting!• Real solution to 3+1D. What are the “right” initial conditions?• Angular momentum for non-zero impact parameter? Spectators and
leading particles?• Incorporating conserved quantities (baryon, charge)• How do we understand hydro microscopically?• “Criteria for the replacement of a field theory by its classical
hydrodynamical analogue”• Turbulence, viscosity, heat conduction, surface tension…• “Relation of Gaussian dN/dy to central limit theorem or the random
walk problem”
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Peter Steinberg BNL/RIKEN Flow Workshop
“Proceedings”:Landau Hydrodynamics &
RHIC Phenomenology
Peter SteinbergBrookhaven National Laboratory
Workshop on Collective Flow & QGP PropertiesNovember 17-19, 2003
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Peter Steinberg BNL/RIKEN Flow Workshop
The “Landau Solution”• Many authors refined
original ideas• This is how things ended up
by early 1980’s
• Universal Entropy
• Gaussian Rapidity Distributions
• Thermal pT spectra
2 / 2
1/ 4 2ln ln22
y L
yp
dN e sKs L
dy mL
1/ 4~chN Ks
exp /TT T
dNp T
p dp
R
Incominghadrons or
nuclei
Full stopping
Longitudinalexplosion
0VV
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Peter Steinberg BNL/RIKEN Flow Workshop
Coincidence #1: BRAHMS dN/dy
BRAHMS Preliminary 2003
~ 2.3
ln 100 2.15
BRAHMSy
Landauy
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Peter Steinberg BNL/RIKEN Flow Workshop
Coincidence #2: ScalingLimiting fragmentation (x scaling) somehow “built-in”
20s GeV
60s GeV
130s GeV
200s GeV
Cooper & Schonberg 1973
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Peter Steinberg BNL/RIKEN Flow Workshop
Coincidence #3: KLN
KLN, =.3Landau Hydro
30s GeV
60GeV
200GeV
Normalized here
“Default” KLN parameters(normalize @ 200 GeV peak)
Scale in similar fashionboth height & width
Compare dN/dy
This was a surprise.
Of course different KLNparameters can make the
agreement worse
![Page 35: Peter SteinbergBNL/RIKEN Flow Workshop Landau Hydrodynamics & RHIC Phenomenology Peter Steinberg Brookhaven National Laboratory Workshop on Collective](https://reader034.vdocuments.us/reader034/viewer/2022051415/56649cb85503460f9497f6c0/html5/thumbnails/35.jpg)
Peter Steinberg BNL/RIKEN Flow Workshop
Coincidence #4: Landau vs. Mueller
Landau “better” atlow energies
MLLA QCD better athigher energies
(esp. including pp@s/2)
Difference increasesdramatically athigher energies
(LHC day-1 important)
Oddity: slower increasefrom pQCD is like
2 1/ 3sc
Landau
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Peter Steinberg BNL/RIKEN Flow Workshop
Coincidence #5: RHIC pp Data• One parameter fit to STAR
& PHENIX pp data• L = 0.570±.001 (STAR)• L = 0.541±.001 (PHENIX)
• Power-law has two:
• Not sure if or how this formula works with A+A• Mass dependence of yT
PHENIX d 0
STAR dN h+h-
0
1n
Tp
p
2exp / 2TT T
dNC y L
p dp
1ln2
T TT
T T
m py
m p