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5.11.2013 WPCF Catania, November 5-8, 2013 1
Femtoscopic aspects of FSI, resonances and bound states
In memory of V.L.Lyuboshitz (19.3.1937-4.5.2013)
R. Lednický @ JINR Dubna & IP ASCR Prague
• History• QS correlations• FSI correlations • Coalescence Femtoscopy• Correlation study of strong interaction• Correlation asymmetries• Summary Femtoscopy on marsh in Nantes’94
RL VLL MIP
2
History
Fermi’34: e± Nucleus Coulomb FSI in β-decay modifies the relative momentum (k) distribution → Fermi (correlation) function F(k,Z,R) is sensitive to Nucleus radius R if charge Z » 1
measurement of space-time characteristics R, c ~ fm
Correlation femtoscopy :
of particle production using particle correlations
3
Fermi function(k,Z,R) in β-decay
= |-k(r)|2 ~ (kR)-(Z/137)2
Z=83 (Bi)β-
β+
R=84 2 fm
k MeV/c
4
2xGoldhaber, Lee & Pais GGLP’60: enhanced ++ , -- vs +- at small opening angles – interpreted as BE enhancement depending on fireball radius R0
R0 = 0.75 fm
p p 2+ 2 - n0
5
Modern correlation femtoscopy formulated by Kopylov & Podgoretsky
KP’71-75: settled basics of correlation femtoscopyin > 20 papers
• proposed CF= Ncorr /Nuncorr &
• showed that sufficiently smooth momentum spectrum allows one to neglect space-time coherence at small q*
(for non-interacting identical particles)
mixing techniques to construct Nuncorr
• clarified role of space-time characteristics in various models
|∫d4x1d4x2p1p2(x1,x2)...|2 → ∫d4x1d4x2p1p2(x1,x2)|2...
6
QS symmetrization of production amplitude momentum correlations of identical particles are
sensitive to space-time structure of the source
CF=1+(-1)Scos qx
p1
p2
x1
x2
q = p1- p2 → {0,2k*} x = x1 - x2 → {t*,r*}
nnt , t
, nns , s2
1
0 |q|
1/R0
total pair spin
2R0
KP’71-75
exp(-ip1x1)
CF → |S-k*(r*)|2 = | [ e-ik*r* +(-1)S eik*r*]/√2 |2
PRF
7
Assumptions to derive KP formula
CF - 1 cos qx
- two-particle approximation (small freeze-out PS density f)
- smoothness approximation: Remitter Rsource |p| |q|peak
- incoherent or independent emission
~ OK, <f> 1 ? low pt
~ OK in HIC, Rsource2 0.1 fm2 pt
2-slope of direct particles
2 and 3 CF data approx. consistent with KP formulae:CF3(123) = 1+|F(12)|2+|F(23)|2+|F(31)|2+2Re[F(12)F(23)F(31)]CF2(12) = 1+|F(12)|2 , F(q)| = eiqx
- neglect of FSIOK for photons, ~ OK for pions up to Coulomb repulsion
Resonances as emitters
most of the produced pions come from resonance decays symmetrization accounting for resonance propagator (M2-kr
2-iM)-1
yields (in the limit << M )
CF - 1 = Reexp(-iqx)/(1+iy) 1-½[q(x+l)]2+(q l)2], y=(krq)/M (q l)
• i.e. the width of BE enhancement is determined by the source size enhanced by the resonance decay length l = kr/M
• -meson as a typical resonance decay length in PRF l*~3.3 fm• in contrast with correlation radii ~1 fm measured from qinv CFs in
p, pp or e+e- collisions• explained by a rapid decrease of the slope of the resonance factor
1/(1+y2) with increasing q 8
Grishin, Kopylov, Podgoretsky’71, Grassberger’77, RL’78, RL,Progulova’92
Resonances as emittersNote: the narrow resonance limit resonance as a classical emitter with
exponential decay law ~ exp(-t)
(used in transport codes)
However, at qinv > 0.1 GeV it may lead to a substantial overestimation of the resonance correlation factor (by ~ 15% for )
9
It may be important for the interpretation of CF data from elementary particle collisions,
though much less important for HIC (due to substantial fireball
size)
classical approx.
Meff(-0p)
-0+X
-0+X
“General” parameterization at |q| 0
Particles on mass shell & azimuthal symmetry 5 variables:q = {qx , qy , qz} {qout , qside , qlong}, pair velocity v = {vx,0,vz}
Rx2 =½ (x-vxt)2 , Ry
2 =½ (y)2 , Rz2 =½ (z-vzt)2
q0 = qp/p0 qv = qxvx+ qzvz
y side
x out transverse pair velocity vt
z long beam
Podgoretsky’83, Bertsch, Pratt’95; so called out-side-long parameterization
Interferometry or correlation radii:
cos qx=1-½(qx)2+.. exp(-Rx2qx
2 -Ry2qy
2 -Rz
2qz2
-2Rxz2qx qz)
Grassberger’77RL’78
Csorgo, Pratt’91: LCMS vz = 0
11
Probing source shape and emission duration
Static Gaussian model with space and time dispersions
R2, R||
2, 2
Rx2 = R
2 +v22
Ry2 = R
2
Rz2 = R||
2 +v||22
Emission duration2 = (Rx
2- Ry2)/v
2
f (degree)
Rsi
de2 fm
2If elliptic shape also in transverse plane RyRside oscillates with pair azimuth f
Rside (f=90°) small
Rside (f=0°) large
z
A
B
Out-of reaction plane
In reaction plane
In-planeCircular
Out
-of
plan
e
KP (71-75) …
Probing source dynamics - expansionDispersion of emitter velocities & limited emission momenta (T)
x-p correlation: interference dominated by pions from nearby emitters
Interferometry radii decrease with pair velocity
Interference probes only a part of the sourceResonances GKP’71 ..
Strings Bowler’85 ..
Hydro
Pt=160 MeV/c Pt=380 MeV/c
Rout Rside
Rout Rside
Collective transverse flow F RsideR/(1+mt F2/T)½
during proper freeze-out (evolution) time
Rlong (T/mt)½/coshy
Pratt, Csörgö, Zimanyi’90
Makhlin-Sinyukov’87
}
1 in LCMS
…..
Bertch, Gong, Tohyama’88Hama, Padula’88
Mayer, Schnedermann, Heinz’92
Pratt’84,86Kolehmainen, Gyulassy’86
Longitudinal boost invariant expansion
pion
Kaon
Proton
, , Flow & Radiiin Blast Wave model
← Emission points at a given tr. velocitypx = 0.15 GeV/c 0.3 GeV/c
px = 0.53 GeV/c 1.07 GeV/c
px = 1.01 GeV/c 2.02 GeV/c
For a Gaussian density profile with a radius RG and linear flow velocity profile F (r) = 0 r/ RG:
0.73c 0.91c
Rz2 2 (T/mt)
Rx2= x’2-2vxx’t’+vx
2t’2
Rz = evolution time Rx = emission duration
Ry2 = y’2
Ry2 = RG
2 / [1+ 02 mt /T]
Rx , Ry 0 = tr. flow velocity pt–spectra T = temperature
t’2 (-)2 ()2
BW: Retiere@LBL’05
x = RG bx 0 /[02+T/mt]
hierarchy x(p) < x(K) < x(p)
BW fit ofAu-Au 200 GeV
T=106 ± 1 MeV<bInPlane> = 0.571 ± 0.004 c<bOutOfPlane> = 0.540 ± 0.004 cRInPlane = 11.1 ± 0.2 fmROutOfPlane = 12.1 ± 0.2 fmLife time (t) = 8.4 ± 0.2 fm/cEmission duration = 1.9 ± 0.2 fm/cc2/dof = 120 / 86
Retiere@LBL’05
R
βz ≈ z/τβx ≈ β0 (r/R)
15
Final State InteractionSimilar to Coulomb distortion of -decay Fermi’34:
e-ikr -k(r) [ e-ikr +f(k)eikr/r ]
eicAc
F=1+ _______ + …kr+krka
Coulomb
s-wavestrong FSIFSI
fcAc(G0+iF0)
}
}
Bohr radius}
Point-likeCoulomb factor k=|q|/2
CF nnpp
Coulomb only
|1+f/r|2
FSI is sensitive to source size r and scattering amplitude fIt complicates CF analysis but makes possible
Femtoscopy with nonidentical particles K, p, .. &
Study relative space-time asymmetries delays, flow
Study “exotic” scattering , K, KK, , p, , ..Coalescence deuterons, ..
|-k(r)|2Migdal, Watson, Sakharov, … Koonin, GKW, LL, ...
Assumptions to derive “Fermi-like” formula
CF = |-k*(r*)|2
tFSI (s-wave) = µf0/k* |k*| = ½|q*| hundreds MeV/c
- same as for KP formula in case of pure QS &
- equal time approximation in PRF
» typical momentum transfer in production
RL, Lyuboshitz’82 eq. time condition |t*| r*2
OK (usually, to several % even for pions) fig.
RL, Lyuboshitz ..’98
same isomultiplet only: + 00, -p 0n, K+K K0K0, ...
& account for coupledchannels within the
- tFSI = d /d dE > tprod
∫d3r {WP(r,k) + WP(r,-kn) |-k(r)|2
+ 2[WP(r,k)WP(r,-kn)]1/2 Re[exp(ikr)-k(r)]}
where -k(r) = exp(-ikr)+-k(r) and n = r/r
The usual moothness approximation: WP(r,-kn) WP(r,k) is valid if one can neglect the k-dependence of WP(r,k), e.g.
for k << 1/r0
Caution: Smoothness approximation is justified for small k << 1/r0
It should be generalized in the region k > ~100 MeV/c
CF(p1,p2) ∫d3r WP(r,k) |-k(r)|2
18
Effect of nonequal times in pair cmsRL, Lyuboshitz SJNP 35 (82) 770; RL nucl-th/0501065
Applicability condition of equal-time approximation: |t*| m1,2r*2 r0=2 fm 0=2 fm/c r0=2 fm v=0.1
OK for heavy
particles & small k*
OK within 5%even for pions if0 ~r0 or lower
→
|k*t*| m1,2r*
Using spherical wave in the outer region (r>) & inner region (r<) correction analytical dependence on scatt. amplitudes fL and source radius r0 LL’81
19
Inner region: W(r) W(0) & integral relation (single channel and no Coulomb) with the phase shifts L and momentum derivative L :
∫d3r[|-k(r)|2 -1]= (2/k3)L(2L+1){kL-½[sin2(k+L)-sin2(k)]+..}
Þ FSI contribution to the CF of nonidentical particles, assuming Gaussian source function W(r)=exp(-r2/4r0
2)/(2 r0) :
for kr0 << 1: CFFSI = ½|f0/r0|2[1-d0/(2r0)]+2f0/(r0) ~ r0-1 or r0
-2
f0 and d0 are the s-wave scatt. length and eff. radius entering in the (L=0) amplitude fL(k) = sinLexp(iL)/k (1/fL+½dLk2 - ik)-1
for kr0 >> 1: CFFSI = (2/k2)W(0)L(2L+1)L ~ r0-3
L=[(2L+1)/2k]sin(2 L) - (dL/k2L)sin2L
L-wave saturated by a resonance:
L= /2, dL= 2k2L+1()-1 L(k=k0) = 2k0()-1
20
Þ for kr0 >> 1: CFr,L(k=k0)= 4W(0)(2L+1) (k0)-1
& resonance yield in the narrow width limit L(k) = (k-k0)
rd3Nr,L/d3pr = (2)3W(0)(2L+1)(12/1*2
*)d6N0/(d3p1 d3p2)
® a problem with π+- * no room for direct production !
See also the talk by Petr Chaloupka on Wednesday
Likely due to violation of eq. time approx. for a part of the coalescence contribution (|k*t*| m1,2r* is valid for m2=m only)
Resonance contribution to CF vs r-k correl. b
Rpeak(STAR)
----------- 0.025
Rpeak(NA49)
---------- 0.10 0.14
Smoothness assumption:
WP(r,-kn) WP(r,k) Exact
WP(r,k) ~ exp[-r2/4r02 + bkrcos]; = angle between r and k
CF suppressed by a factor WP(0,k) ~ exp[-b2r02k2]
To leave a room for a direct production b > 0.3 is required for π+- system; however, BW b ~ 0.2; likely eq.-time approx. not valid for π+- at k*~ 150 MeV/c
*(k=146 MeV/c), r0=5 fm (k=126 MeV/c), r0=5 fm-----------
r-k correl. b 0.2 for K+K- CF indicates ~ ½ direct -meson yield – in qualitative agreement with the difference between the measured
rapidity width in central Pb+Pb collisions at SPS and expected from coalescence: -2 = K+-2 + K--2
-
K+
anti-
p+p
K-K+K- coalescence
23
Bound state production
Migdal, Watson, Sakharov, .. hadronic processes
Dominated by FSI provided a small binding energy b
Closely related to production of free particles at k* 0
FSI theory: Fermi -decay
Continuum:d6N/(d3p1 d3p2)= d6N0/(d3p1 d3p2)|-k*(r*)|2
d3N/d3pb= (2)3bd6N0/(d3p1 d3p2)|b(r*)|2 Discrete spectrum:
+x1
x2
x2
x1
p1
p2
p1
p2
pb
r*= x1*- x2
*= distance between particle emitters in pair cms
p1/m1≈ p2/m2 pb/mb
Basis of bound state coalescence femtoscopy
Universal relation between production of free and bound ’s is used to determine pionium lifetime in DIRAC exp. at CERN :
Assume only two types of pion sources Nemenov ‘85Short-Lived Emitters SLE (, , ..) r* |a| = 387 fm both ’s from SLE
Long-Lived Emitters LLE (, Ks, , ..) r* |a| one or both ’s from LLE
Then, neglecting strong FSI
|-k*(r*)|2 = |c-k*(0)|2 + (1- ) |c
-k*()|2
|A(r*)|2 = |cA(0)|2 + (1- ) |c
A()|2
1Ac(Q)
01/(|na|3)
A={n,L=0}
Þ d6N/(d3p1 d3p2)= d6N0/(d3p1 d3p2) [ Ac(Q) + (1- )]
d3N/d3pA= d6N0/(d3p1 d3p2) (2)3A/(|na|3), p1 ≈ p2 ≈ ½pA
= SLE pair fraction
Coalescence: deuterons ..
Edd3N/d3pd = B2 Epd3N/d3pp End3N/d3pn pp pn ½pd
Here is realized the opposite limit compared with r*<<|a| for +- atom: r* > deuteron radius = -1 = (2b)-1/2 |b(r*)|2 W(0) ~ r0
-3
Coalescence factor: B2 = (2)3(mpmn/md)-1t|b(r*)|2 ~ r0-3
Triplet fraction = ¾ unpolarized Ns
Assuming Gaussian r* distribution and accounting for
a boost from LCMS to PRF:
B2 33/2/(2mptr03)
r0(pp) ~ 4 fm from AGS to RHIC
Lyuboshitz’88 ..
B2 d,d-bar at pt=1.3 GeV/c
in central HICs
d d-bar PHENIX
B2 at RHIC energies with pt and centrality
in agreement with B2 ~ R-3
+fragmentation ?
coalescence
Is there double counting in thermal model with FSI ?Global thermal equilibrium in nonrelativistic limit; T,i<<E ~ mi
d3Ni/d3p = Vgi(2)-3exp[-(E-i)/T] gi=2Si+1 = spin factor, i= chemical potential, T = temperature
In the limit kV1/3 >> 1 and simultaneous emission: Jennings, Boal, Shillcock’86
the L-wave resonance contribution due to FSI of spin-0 particles d3Nr,L/(d3pr) = (2)3V-1(2L+1)d3N1/d3p1 d3N2d3p2
= Vgr,L(2)-3exp[-(Er-r)/T] gr.L=2L+1, r= 1+ 2, Er=E1+E2
resonances due to FSI are also in thermal equilibrium in this limit
Similarly, in the limit V1/3 >> 1 and simultaneous emission: d3Nb/d3pb= (2)3V-1d3N1/d3p1 d3N2d3p2
= V(2)-3exp[-(Eb-b)/T] i.e., the (s-wave) coalescence bound state is also in thermal equilibrium
Is there double counting in thermal model with FSI ?
No double counting with respect to direct thermal production since the latter is characterized by local thermal equilibrium (not reproduced by the coalescence states – as revealed e.g. by -meson rapidity width)
besides the coalescence FSI contribution, one may expect essential direct contribution of resonances (with sufficiently long lifetime) and bound states (with sufficiently large binding energy)
28
Correlation femtoscopy with nonid. particles p CFs at AGS & SPS & STAR
Fit using RL-Lyuboshitz’82 with
consistent with estimated impurityr0~ 3-4 fm consistent with the radius from pp CF & mt scaling
Goal: No Coulomb suppression as in pp CF &Wang-Pratt’99 Stronger sensitivity to r0
=0.50.2r0=4.50.7 fm
Scattering lengths, fm: 2.31 1.78Effective radii, fm: 3.04 3.22
singlet triplet
AGS SPS STAR
r0=3.10.30.2 fm
Pair purity problem for p CF @ STARÞ PairPurity ~ 15%Assuming no correlation for misidentified particles and particles from weak decays
Fit using RL-Lyuboshitz’82 (for np)
¬ but, there can be residualcorrelations for particles fromweak decays requiring knowledgeof , p, , , p, , correlations
30
Correlation study of strong interaction
-
+& & p scattering lengths f0 from NA49 and STAR
NA49 CF(+) vs RQMD with SI scale: f0 sisca f0 (=0.232fm)
sisca = 0.60.1 compare ~0.8 fromSPT & BNL data E765 K e
Fits using RL-Lyuboshitz’82
NA49 CF() data prefer
|f0()| f0(NN) ~ 20 fm
STAR CF(p) data point to
Ref0(p) < Ref0(pp) 0
Imf0(p) ~ Imf0(pp) ~ 1 fm
But r0(p) < r0(p) ? Residual correlations
pp
Correlation study of strong interaction
-
-
scattering lengths f0 from NA49 correlation data
Fit using RL-Lyuboshitz (82) with fixed Pair Purity =0.16 from feed-down and PID
Data prefer |f0| « f0(NN) ~ 20 fm
-
CF=1+[CFFSI+SS(-1)Sexp(-r0
2Q2)]
0= ¼(1-P2) 1= ¼(3+P2) P=Polar.=0
CFFSI = 20[½|f0(k)/r0|2(1-d00/(2r0))
+2Re(f0(k)/(r0))F1(r0Q)
- 2Im(f0(k)/r0)F2(r0Q)]
fS(k)=(1/f0S+½d0
Sk2 - ik)-1 k=Q/2
F1(z)=0z dx exp(x2-z2)/z F2(z)=[1-exp(-z2)]/z
CF=N{1+[CFFSI -½exp(-r02Q2)]}
N r0 f0
0
d00
fmfmfm
B
33
Correlation asymmetries
CF of identical particles sensitive to terms even in k*r* (e.g. through cos 2k*r*) measures only
dispersion of the components of relative separation r* = r1
*- r2* in pair cms
CF of nonidentical particles sensitive also to terms odd in k*r* ® measures also relative space-time asymmetries - shifts r*
RL, Lyuboshitz, Erazmus, Nouais PLB 373 (1996) 30
Construct CF+x and CF-x with positive and negative k*-projection
k*x on a given direction x and study CF-ratio CF+x/CFx
34
CF-asymmetry for charged particlesAsymmetry arises mainly from Coulomb FSI
CF Ac() |F(-i,1,i)|2 =(k*a)-1, =k*r*+k*r*
F 1+ = 1+r*/a+k*r*/(k*a)r*|a|
k*1/r* Bohr radius
}
±226 fm for ±p±388 fm for +±
CF+x/CFx 1+2 x* /ak* 0
x* = x1*-x2* rx* Projection of the relative separation r* in pair cms on the direction x
In LCMS (vz=0) or x || v: x* = t(x - vtt)
CF asymmetry is determined by space and time asymmetries
35
Usually: x and t comparable
RQMD Pb+Pb p +X central 158 AGeV : x = -5.2 fmt = 2.9 fm/cx* = -8.5 fm+p-asymmetry effect 2x*/a -8%
Shift x in out direction is due to collective transverse flow
RL’99-01 xp > xK > x > 0
& higher thermal velocity of lighter particles
rt
y
x
F
tT
t
F = flow velocity tT = transverse thermal velocity
t = F + tT = observed transverse velocity
x rx = rt cos = rt (t2+F2- t
T2)/(2tF) y ry = rt sin = 0 mass dependence
z rz sinh = 0 in LCMS & Bjorken long. exp.
out
side
measures edge effect at yCMS 0
NA49 & STAR out-asymmetriesPb+Pb central 158 AGeV not corrected for ~ 25% impurityr* RQMD scaled by 0.8
Au+Au central sNN=130 GeV corrected for impurity
Mirror symmetry (~ same mechanism for and mesons) RQMD, BW ~ OK points to strong transverse flow
pp K
(t yields ~ ¼ of CF asymmetry)
37
Summary
• Assumptions behind femtoscopy theory in HIC seem OK at k 0. At k > ~ 100 MeV/c, the usual smoothness and equal-time approximations may not be valid.
• Wealth of data on correlations of various particles (,K0,p,,), yields of resonances and bound states is available & gives unique space-time info on production characteristics including collective flows
• Rather direct evidence for strong transverse flow in HIC at SPS & RHIC comes from nonidentical particle correlations
• Info on two-particle strong interaction: & & p scattering lengths from HIC at SPS and RHIC. Good perspective at RHIC & LHC (a problem of residual correlations is to be solved).
38
Phase space density from CFs and spectra
Bertsch’94
May be high phase space density at low pt ?
? Pion condensate or laser
? Multiboson effects on CFsspectra & multiplicities
<f> rises up to SPSLisa ..’05
39
Examples of NA49 & STAR data
3-dim fit: CF=1+exp(-Rx2qx
2 –Ry2qy
2 -Rz
2qz2
-2Rxz2qx qz)
z x y
Correlation strength (purity, chaoticity, ..)
NA49
Interferometry or correlation radii
KK STAR
Coulomb corrected
AGSSPSRHIC: radii
STAR Au+Au at 200 AGeV 0-5% central Pb+Pb or Au+Au Clear centrality & mt dependence
Weak energy dependence
R ↑ with centrality & with mt only Rlong slightly ↑ with energy
Rside R/(1+mt F2/T)½
Rlong (T/mt)½
tr. collective flow velocity F Evolution (freeze-out) time
41
hadronization
initial state
pre-equilibrium
QGP andhydrodynamic expansion
hadronic phaseand freeze-out
PCM & clust. hadronization
NFD
NFD & hadronic TM
PCM & hadronic TM
CYM & LGT
string & hadronic TM
Expected evolution of HI collision vs RHIC data
dN/dt
1 fm/c 5 fm/c 10 fm/c 50 fm/c time
Kinetic freeze out
Chemical freeze out
RHIC side & out radii: 2 fm/c
Rlong & radii vs reaction plane: 10 fm/c
Bass’02
Femto-puzzle I
Contradiction with transport and simple hydro calcul.
- small space-time scales
- their weak energy dep.
- Rout/Rside ~ 1
Basically solved due to the initial flow increasing with energy (likely related to the increase of the initial energy density and partonic energy
fraction)
43
Femtoscopy Puzzle I basically solved due to initial flow appearing in realistic IC
Femtoscopic signature of QGP onset3D 1-fluid Hydrodynamics
Rischke & Gyulassy, NPA 608, 479 (1996)
With 1st order
Phase transition
Initial energy density 0
Long-standing signature of QGP onset:
• increase in , ROUT/RSIDE due to the Phase transition
• hoped-for “turn on” as QGP threshold in 0 is reached
• decreases with decreasing Latent heat & increasing tr. Flow
(high 0 or initial tr. Flow)
Femto-puzzle II
No signal of a bump in Rout near
the QGP threshold (expected at AGS-SPS energies) !?
likely solved due to a dramatic decrease of
partonic phase with decreasing
energye.g. in PHSD, Cassing,
Bratkovkaya
46
Cassing – Bratkovskaya: Parton-Hadron-String-Dynamics
Perspectives at FAIR/NICA energies
Femtoscopy of Pb+Pb at LHC ALICE arXiv:1012.4035All radii increase with
Nch from RHIC to LHC (not from SPS to RHIC)!
Multiplicity scaling of the correlation volume universal freeze-out density
Freezeout time f from Rlong=f (T/mt)1/2
The LHC fireball:
- hotter
- lives longer &
- expands to a larger size
Ridge effect
Dense matter (collective flows)
also in pp collisions at LHC (for high Nch) ?
- pt increases with nch and particle mass
- BE CF vs nch and pt points to expansion at high nch
- Ridge effect observed in angular correlations at high nch
R(kt) at large Nch expansion
CMS
Caution: the strong FSI is enhanced by a logarithmic singularity
for particles from resonance decays & a small source size LL’96
e.g. noticeable strong FSI effect even
on CF of identical charged pions:
CFFSI ~ 2f0/lr* 2ln|B| f0/lr
*
For example, if res = -meson:
00 +-
CFFSI (k=0) -0.10 0.25 0.30
50
Even stronger effect of KK-bar FSI on KsKs correlations in pp-collisions at LHC
ALICE: PLB 717 (2012) 151
e.g. for kt < 0.85 GeV/c, Nch=1-11 the neglect of FSI increases by ~100% and Rinv by ~40%
= 0.64 0.07 1.36 0.15 > 1 !
Rinv= 0.96 0.04 1.35 0.07 fm
Resonance FSI contributions to π+- K+K- CF’s • Complete, inner and outer
contributions of p-wave resonance (*) FSI to π+- CF for two cut parameters 0.4 and 0.8 fm and Gaussian radius of 5 fm FSI contribution overestimates measured * by a factor 4 (3) for r0 = 5 (5.5) fm factor 3 (2) if accounting for out
-6 fm • The same for p-wave resonance
() FSI contributions to K+K-
CF FSI contribution overestimates measured by 20% for r0 = 4.5 fm
• Little or no room for direct production when neglecting r-k correlation!
Rpeak(NA49)
» 0.10 0.14after purity correction
Rpeak(STAR)
0.025 ----------- -----
----------- -----
---------------------
r0 = 5 fm no r-k correlation
References related to resonance formation in final state:
R. Lednicky, V.L. Lyuboshitz, SJNP 35 (1982) 770
R. Lednicky, V.L. Lyuboshitz, V.V. Lyuboshitz, Phys.At.Nucl. 61 (1998) 2050
S. Pratt, S. Petriconi, PRC 68 (2003) 054901
S. Petriconi, PhD Thesis, MSU, 2003
S. Bekele, R. Lednicky, Braz.J.Phys. 37 (2007) 994
B. Kerbikov, R. Lednicky, L.V. Malinina, P. Chaloupka, M. Sumbera, arXiv:0907.061v2 B. Kerbikov, L.V. Malinina, PRC 81 (2010) 034901
R. Lednicky, Phys. Part. Nucl. Lett. 8 (2011) 965
R. Lednicky, P. Chaloupka, M. Sumbera, in preparation
53
Discrete spectrum: A2
n0(r*) = cn0(0) [1- r*/|a|+f(0)/r* + O(f(0)/a) + O(r*2/a2)]
n0(r*) exp(-r*/|na|) 0 at r* >> |na|
-k*(r*) Ac [1 - r*(1+cos*)/|a| + f(0)/r* + O(f(0)/a) + O(r*2/a2)] p-wave
|-k*(r*)| 1 at r* >> |a|
k* 0
Continuum: +-
Universal dependence of the WF on r* and scattering amplitude f RL’04
in continuum (at k* 0) and discrete spectrum at a given orbital angular
momentum and r*<< -1
=(2b)1/2 = virtual momentum (k*=i), b(r*) exp(-r*) at r* > -1
Particularly, for +- atom with the main q.n. n: n=|na|-1, |a|=387 fm
FSI effect on CF of neutral kaons
STAR data on CF(KsKs)
Goal: no Coulomb. But R may go up by ~1 fm if neglected FSI in
l = 1.09 0.22r0 = 4.66 0.46 fm 5.86 0.67 fm
KK (~50% KsKs) f0(980) & a0(980)RL-Lyuboshitz’82 couplings from Martin
or Achasov
t
Achasov’01,03Martin’77
no FSI
Lyuboshitz-Podgoretsky’79: KsKs from KK also showBE enhancement
r0 ↓ Mt Universal expansion !
55
NA49 central Pb+Pb 158 AGeV vs RQMD: FSI theory OKLong tails in RQMD: r* = 21 fm for r* < 50 fm
29 fm for r* < 500 fm
Fit CF=Norm [Purity RQMD(r* Scaler*)+1-Purity]
Scale=0.76 Scale=0.92 Scale=0.83
RQMD overestimates r* by 10-20% at SPS cf ~ OK at AGS worse at RHIC
p
56
Correlation study of particle interaction
-
+ scattering length f0 from NA49 CF
Fit CF(+) by RQMD with SI scale: f0 sisca f0
input f0
input = 0.232 fm
sisca = 0.60.1 Compare with ~0.8 from SPT
& BNL E765 K e
+
CF=Norm [Purity RQMD(r* Scaler*)+1-Purity]
57
Simplified idea of CF asymmetry(valid for Coulomb FSI)
x
x
v
v
v1
v2
v1
v2
k*/= v1-v2
p
p
k*x > 0v > vp
k*x < 0v < vp
Assume emitted later than p or closer to the center
p
p
Longer tint
Stronger CF
Shorter tint Weaker CF
CF
CF
58
ad hoc time shift t = –10 fm/c
CF+/CF
Sensitivity test for ALICEa, fm
84
226
249CF+/CF 1+2 x* /a
k* 0
Here x*= - vt
CF-asymmetry scales as - t/a
Erazmus et al.’95
Delays of several fm/ccan be easily detected
59
Large lifetimes evaporation or phase transitionx || v |x| |t| CF-asymmetry yields time delay
Ghisalberti’95 GANILPb+Nb p+d+X
CF+(pd)
CF(pd)
CF+/CF< 1
Deuterons earlier than protonsin agreement with coalescencee-tp/ e-tn/ e-td/(/2) since tp tn td
Two-phase thermodynamic
model
CF+/CF< 11 2 3
1
2
3
Strangeness distillation: K earlier than K in baryon rich QGP
Ardouin et al.’99
60
Decreasing R(pt): x-p correlation
• usually attributed to collective flow• taken for granted• femtoscopy the only way to confirm
x-p correlations
x2-p correlation: yesx-p correlation: yes
Non-flow possibility• hot core surrounded by cool shell• important ingredient of Buda-Lund
hydro pictureCsörgő & Lörstad’96
x2-p correlation: yesx-p correlation: no
x = RG bx 0 /[02+T/mt+T/Tr]
radial gradient of T
Þ decreasing asymmetry ~1 ? problem