Femtoscopy in heavy ion collisions: Two decades of progress - PowerPoint PPT Presentation

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Femtoscopy in heavy ion collisions: Two decades of progress

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Title: Femtoscopy in heavy ion collisions: Two decades of progress


1
Femtoscopy in heavy ion collisionsTwo decades
of progress
  • Mike Lisa
  • Ohio State University

An experimentalists view of the situation
B.Q.M.() cf. Bysterský, Chajecki, Chaloupka,
Chung, Kisiel, Kniege, Panitkin...
BQM Before Quark Matter
2
Outline
  • Relevance of femtoscopy to R.H.I.C.
  • Growing activitiies of a (sub)field 2 decades
    of systematics
  • R(vSNN, b, Npart, A, B, mT, y, ?, PID)
  • what information is encoded?
  • what have we mined so far?
  • special attention to size and shape
  • comments

blastwave
comparison to models
experimental details
3
Spacetime - an annoying bump on the road to
Stockholm?
  • Non-trivial space-time - the hallmark of rhic
  • Initial state dominates further dynamics
  • Intermediate state impt element in exciting
    signals
  • Final state
  • Geometric structural scale is THE defining
    feature of QGP

4
Spacetime - an annoying bump on the road to
Stockholm?
  • Non-trivial space-time - the hallmark of rhic
  • Initial state dominates further dynamics
  • Intermediate state impt element in exciting
    signals
  • Final state
  • Geometric structural scale is THE defining
    feature of QGP
  • Temporal scale sensitive to deconfinement
    transition (?)

5
Two decades of systematics
R 5 fm
  • Pion HBT _at_ Bevalac largely confirming nuclear
    dimensions
  • Since 90s increasingly detailed understanding
    and study w/ high stats

6
Two decades of systematics
  • Pion HBT _at_ Bevalac largely confirming nuclear
    dimensions
  • Since 90s increasingly detailed understanding
    and study w/ high stats

7
Repeating most basic sanity check at relativistic
energies...
Forget homogeneity regions or fancy stuff. Do
femtoscopic length scales increase when they
should?
p-p correlations big bump ? small source
  • Also
  • SPS NA44(99),NA49(00)
  • RHIC STAR(05)

8
  • Generalize A1/3 ?Npart1/3
  • not bad _at_ RHIC!
  • connection w/ init. size?

9
  • Generalize A1/3 ?Npart1/3
  • not bad _at_ RHIC!
  • connection w/ init. size?
  • Heavy and light data from AGS, SPS, RHIC
  • ?s-ordering in geometrical Rlong, Rside
  • Mult K(?s)Npart
  • source of residual ?s dep?
  • ...Yes! common scaling
  • final state drives radii, not init. geometry
  • (breaks down ?s lt 5 GeV)

NB not constant density
LPSW nucl-ex/0505014
10
We are not alone...
Entropy determines everything at bulk level
(soft sector) ?
NB scaling violated ?s lt 4 GeV (as with
femtoscopy)
11
Refinement chemical effects
  • different behaviour below/above AGS
  • violates universal scaling
  • baryon ? meson dominance
  • neglect time/dynamics gross F.O. geometry
    appears determined by
  • chemistry
  • universal mean free path 1 fm (!?)

12
Messages from systematics
  • AB, b, Npart systematics
  • sanity check on overall size dependence ?
  • final state multiplicity/chemistry determines
    rough geometry...

...and that geometry is 2x initial size
collective/flow-like expansion? ? probe
anisotropically!
13
Strongly-interacting 6Li released from an
asymmetric trap OHara, et al, Science 298 2179
(2002)
What can we learn?
transverse FO shape collective velocity ?
evolution time estimate check independent of
RL(pT)
Teaney, Lauret, Shuryak nucl-th/0110037
14
  • observe the source from all angles with respect
    to RP
  • expect oscillations in HBT radii

15
  • observe the source from all angles with respect
    to RP
  • expect oscillations in HBT radii (including new
    cross-terms)

R2out-sidelt0 when ?pair135º
16
Measured final source shape
R2out-sidelt0 when ?pair135º
ever see that symmetry at ycm ?
model-dependent, but see Retiere MAL PRC70
044907 2004
17
Measured final source shape
Expected evolution
?
model-dependent, but see Retiere MAL PRC70
044907 2004
18
Evolution of size and shape - the rule of two
1/2 shape reduction
x2 size increase
Initial size/shape estimated by Glauber
calculation Final config according to Retiere
MAL PRC70 044907 2004
19
Anisotropic sanity check
  • non-trivial excitation function
  • does it make sense? Is it related to bulk
    dynamics?
  • YES

20
A simple estimate ?0 from ?init and ?final
  • BW ? ?X, ?Y _at_ F.O. (?X gt ?Y)
  • hydro flow velocity grows t
  • From RL(mT) ?0 9 fm/c
  • consistent picture
  • Longer or shorter evolution times
  • inconsistent
  • toy estimate ?0 ?0(BW) 9 fm/c
  • too short to account for expansion??
  • Need a real model comparison? asHBT workable
    evolutionary clock constraint for models

MAL ISMD03
21
Messages from systematics
  • AB, b, Npart systematics
  • sanity check on overall size dependence ?
  • final state multiplicity/chemistry determines
    rough geometry...
  • ?, b, ?s systematics
  • sanity check on shape evolution ?
  • geometric evolution consistent with collective
    bulk dynamics (flow)

look for dynamic signatures substructure
  • more than T versus mass
  • more than spectral shapes
  • more than v2
  • ...
  • flow is defined by space-momentum correlations
  • only femtoscopy can probe substructure
  • of dynamic bulk behaviour

22
Flow-dominated Blast-wave model PRC70 044907
(2004)
23
  • Decreasing R(pT)
  • usually attributed to collective flow
  • flow integral to our understanding of R.H.I.C.
    taken for granted
  • femtoscopy the only way to confirm x-p
    correlations impt check

Kolb Heinz, QGP3 nucl-th/0305084
24
  • Decreasing R(pT)
  • usually attributed to collective flow
  • flow integral to our understanding of R.H.I.C.
    taken for granted
  • femtoscopy the only way to confirm x-p
    correlations impt check
  • Non-flow possibilities
  • cooling, thermally (not collectively) expanding
    source
  • combo of x-t and t-p correlations

early times small, hot source
late times large, cool source
25
  • Decreasing R(pT)
  • usually attributed to collective flow
  • flow integral to our understanding of R.H.I.C.
    taken for granted
  • femtoscopy the only way to confirm x-p
    correlations impt check
  • Non-flow possibilities
  • cooling, thermally (not collectively) expanding
    source
  • combo of x-t and t-p correlations

26
  • Decreasing R(pT)
  • usually attributed to collective flow
  • flow integral to our understanding of R.H.I.C.
    taken for granted
  • femtoscopy the only way to confirm x-p
    correlations impt check
  • Non-flow possibilities
  • cooling, thermally (not collectively) expanding
    source
  • combo of x-t and t-p correlations
  • hot core surrounded by cool shell
  • important ingredient of Buda-Lund hydro
    picturee.g. Csörgo LörstadPRC54 1390 (1996)

27
Each scenario generates x-p correlations
  • Decreasing R(pT)
  • usually attributed to collective flow
  • flow integral to our understanding of R.H.I.C.
    taken for granted
  • femtoscopy the only way to confirm x-p
    correlations impt check

but
?x2?-p correlation yes ?x?-p correlation yes
  • Non-flow possibilities
  • cooling, thermally (not collectively) expanding
    source
  • combo of x-t and t-p correlations
  • hot core surrounded by cool shell
  • important ingredient of Buda-Lund hydro
    picturee.g. Csörgo LörstadPRC54 1390 (1996)

?x2?-p correlation yes ?x?-p correlation no
t
?x2?-p correlation yes ?x?-p correlation no
28
  • flow-dominated models can reproduce soft-sector
    x-space observables
  • imply short timescales
  • however, are we on the right track? flow
  • puzzles? ? check your assumptions!
  • look for flows special signature ?x?-p
    correlation
  • In flow pictures, low-pT particles emitted closer
    to sources center (along out)
  • non-identical particle correlations(FSI at low
    ?v) probe
  • ?(x1-x2)2? (as does HBT)
  • ?x1-x2?

?
K
p
click for more details on non-id correlations
Csanád, Csörgo, Lörstad nucl-th/0311102 and
nucl-th/0310040
F. Retiere MAL, nucl-th/0312024
29
  • extracted shift in emission point ?x1-x2?
    consistent w/ flow-dominated blastwave
  • In flow pictures, low-pT particles emitted closer
    to sources center (along out)
  • non-identical particle correlations(FSI at low
    ?v) probe
  • ?(x1-x2)2? (as does HBT)
  • ?x1-x2?

30
RHIC femtoscopy with wide variety of particle
species
R(vSNN, b, Npart, A, B, mT, y, ?, PID1, PID2)
? ?- K K- K0S p ?p ? ?? ? ??
? ? ? ? ? ? ? ? ?
? ? ? ? ? ? ? ?-
? - ? ? K
? ? ? K-
? - - K0S
? ? ? ? p
? ? ? ?p
?
??
?
??
? prelim or final result available
31
Strong flow confirmed by all expts...
32
Strong flow confirmed by all expts...
Central (10) AuAu (PbPb) collisions at y0
33
Another implication of strong flow mT scaling
34
Some longitudinal systematics
consistent with boost-invariance
35
Dynamic BI without Chemical BI ? Only
femtoscopy can tell!
36
Dynamic BI without Chemical BI ? Only
femtoscopy can tell!
37
Greater detail - ?-p correlations _at_ AGS
38
Comments
  • massive systematic program provides tremendous
    geometric detail
  • each element reasonable by itself not really
    puzzling.
  • critical mass in the femtoscopy community
  • Related, but not in my talk important new
    directions talks _at_ WPCF
  • moments analysis
  • imaging
  • continued emphasis on non-identical particle
    correlations
  • connection to elementary systems -
    communication across lines
  • Important puzzles beyond central AuAu at top
    energy
  • Ignoring femtoscopy to pursue perfection is
    unjustified
  • Space-time is the defining feature of R.H.I.C.
  • Femtoscopy does measure space-time
  • The measurements are sensitive to underlying
    physics
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