12.4.2010 application of multi-resolution method on flow measurement in cbm vojtech petracek gsi –...
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12.4.201012.4.2010
Application of multi-Application of multi-resolution method on flow resolution method on flow
measurement in CBMmeasurement in CBM
Vojtech PetracekVojtech Petracek
GSI – CBM weekGSI – CBM week
OutlineOutline
Motivation – event-by-event reaction plane & v2 Motivation – event-by-event reaction plane & v2 & fluct.& fluct.
Fluctuations in event shape – statistics, fireball Fluctuations in event shape – statistics, fireball instability and granularity, jets ...instability and granularity, jets ...
Event-by-event fluctuation in particle density in Event-by-event fluctuation in particle density in 1D and 2D1D and 2D
Multi-resolution analysis of particle density Multi-resolution analysis of particle density fluctuationsfluctuations
Strategy of domain analysisStrategy of domain analysis Reaction plane and v2 parametersReaction plane and v2 parameters Summary & outlookSummary & outlook
Elliptic flow measurement & Elliptic flow measurement & backgroundbackground
?
Elliptic flow reflects the original geometry of thecollision zone
We measure azimuthal anisotropy in Pt,y slice of the phase space
Background : stat. fluctuations, fireball granularity, jets
Apart of statistical fluctuationseven the background is an interesting signal
Can we detect the critical pointCan we detect the critical pointfrom fluctuations? from fluctuations?
• Onset of spinodal instability for larger Onset of spinodal instability for larger ? ?• Source structure in crossover region (bags) ?Source structure in crossover region (bags) ?
B. Tomasik
CBM
Fireball instabilityFireball instability
Fast cooling can bring Fast cooling can bring the system to the the system to the unstable configurationunstable configuration
Fireball decomposes Fireball decomposes as it reaches the as it reaches the spinodal pointspinodal point
Cooling must be fast Cooling must be fast bubble nucleation rate bubble nucleation rate < expansion rate< expansion rate
V
B. Tomasik
Granular fireballGranular fireball
Fireball can decompose to spherical dropletsFireball can decompose to spherical droplets Or to objects with more complicated shapes with Or to objects with more complicated shapes with
larger surface/volume ratiolarger surface/volume ratio Or nothing like that happensOr nothing like that happens Can we distinguish between these options -> MRACan we distinguish between these options -> MRA Can we eliminate jet background -> MRACan we eliminate jet background -> MRA BUT we need to work on different scales (resolutions) BUT we need to work on different scales (resolutions)
Multi-resolution analysis (MRA)Multi-resolution analysis (MRA)
• MRA method uses 2D Cauchy-Lorentz functionMRA method uses 2D Cauchy-Lorentz function• We can observe We can observe -- particleparticle densitydensity distribution with different resolutiondistribution with different resolution• We can characterize fluctuation between different resolutionsWe can characterize fluctuation between different resolutions
Example - MRA in 1D Example - MRA in 1D This method can isolate large scale structuresThis method can isolate large scale structures which would be otherwise hidden in noisewhich would be otherwise hidden in noiseJets, DCC, elliptic flow pattern, reaction plane..Jets, DCC, elliptic flow pattern, reaction plane..
If we define a set of resolutions, it is possibleIf we define a set of resolutions, it is possible to reconstruct from L and F functions to reconstruct from L and F functions recursively the original density distributionrecursively the original density distribution like in wavelet transformlike in wavelet transform
Compared to the discrete wavelet Compared to the discrete wavelet transformation method this approachtransformation method this approach doesn’t have problem with domain splittingdoesn’t have problem with domain splitting
Mother & Father functionsMother & Father functions
Mother functions L smooth the high freq. noiseMother functions L smooth the high freq. noise Father functions F determine the fluctuation between the two Father functions F determine the fluctuation between the two
resolution scalesresolution scales Original domain is optimally reproduced when its characteristic Original domain is optimally reproduced when its characteristic
scale coincide with resolutionscale coincide with resolution
L1L1
L2L2
F12F12
Event-by-event fluctuation Event-by-event fluctuation domain detectiondomain detection
Events with isotropic particle distribution are used for Events with isotropic particle distribution are used for the detection threshold calibrationthe detection threshold calibration
Threshold is set to 2Threshold is set to 2, so that ~5% of random signal , so that ~5% of random signal is above itis above it
Events containing non-statistical local fluctuations in Events containing non-statistical local fluctuations in particle density will have the fraction of signal above particle density will have the fraction of signal above the threshold significantly higher the threshold significantly higher
When we Pt weight the MF, this way the jet area can When we Pt weight the MF, this way the jet area can bebe
detected as area of higher than average Pt detected as area of higher than average Pt
Example of droplet Example of droplet reconstruction in MF 2D reconstruction in MF 2D
analysisanalysisCharacteristic droplet Characteristic droplet dimensionsdimensions~ 0.5y x Pi/4~ 0.5y x Pi/4
For small number of For small number of droplets (<20) is possible droplets (<20) is possible direct droplet countingdirect droplet counting
For larger numbers For larger numbers droplets merge droplets merge
Individual droplet FF 2D Individual droplet FF 2D analysisanalysis
When the direct dropletWhen the direct droplet counting is possible, thecounting is possible, the best estimate is the #best estimate is the # of maxima in FF overof maxima in FF over certain thresholdcertain threshold
Droplets & the event Droplets & the event fluctuationfluctuation
Distribution of fraction Distribution of fraction of the area covered by of the area covered by detected domaindetected domain
Red : 100% particles Red : 100% particles from dropletsfrom droplets
Green : 0% particles Green : 0% particles from dropletsfrom droplets
Scale 2Scale 2
Jet reconstructionJet reconstruction
Example of jet reconstruction using the described MRA methodExample of jet reconstruction using the described MRA method
Pt weighting – necessary !! Pt*N ~ Et-JetPt weighting – necessary !! Pt*N ~ Et-JetMean Pt map Mean Pt map <Pt>(eta,phi)=<Pt*N>(eta,phi)/<N>(eta,phi)<Pt>(eta,phi)=<Pt*N>(eta,phi)/<N>(eta,phi)
Strategy of event analysisStrategy of event analysis
Compare Compare P in domains P in domains to surrounding => to surrounding => identify jetidentify jet
Check the charge Check the charge symmetry. Asymmetry symmetry. Asymmetry => DCC=> DCC
Density fluctuation due Density fluctuation due to the dropletto the droplet
Eliminate jet – replace Eliminate jet – replace by surrounding by surrounding backgroundbackground
Analyze event shape Analyze event shape for reaction plane & v2for reaction plane & v2
What v2 we want to measureWhat v2 we want to measure
Expected elliptic flow Expected elliptic flow in CBMin CBM
NA49 – PRC 68, 034903 (2003)
A. Wetzlar 2005
Below 10% for high Pt particlesComplicated event-by-eventbut when reaction plane is determinedevents can be combined
CBM
Examples of reaction plane Examples of reaction plane and v2 reconstruction event-and v2 reconstruction event-
by-eventby-event
Reaction plan
300 tracks, v2 =0.1
Reconstruction of reaction plane angle easy and stable at all scales
precission of RP estimatefrom spread between fits at different scales
v2 can be reconstructed
Examples of reaction plane Examples of reaction plane and v2 reconstruction event-and v2 reconstruction event-
by-eventby-event
Reaction plan
500 tracks v2 = 0.05
with 500 tracks is statistical fluctuation still weaker then signal
RP reconstruction stable
v2 can be reconstructed
Examples of reaction plane Examples of reaction plane and v2 reconstruction event-and v2 reconstruction event-
by-eventby-event
Reaction plan
500 tracks v2=0.02
In this case is the statisticalfluctuation comparable to the signal
RP estimate less precisebut still stable
v2 ?
RP reconstruction is stable-> events can be combined for v2 measurement
Examples of reaction plane Examples of reaction plane and v2 reconstruction event-and v2 reconstruction event-
by-eventby-event
Reaction plan
1000 tracks v2=0.02
RP reconstruction stable on most scales
v2 in single event not reliable
-> combine eventswhen RP is reconstructedconsistently on all scales
Summary & outlookSummary & outlook
Area of the Area of the ,, plane covered by domains with non-statistically plane covered by domains with non-statistically high particle density fluctuation is a robust measure which can be high particle density fluctuation is a robust measure which can be used for detection of events with granular source responsible at used for detection of events with granular source responsible at least for 20% of particle production (for 100 fmleast for 20% of particle production (for 100 fm3 3 droplets)droplets)
For small number of droplets the direct droplet counting is possibleFor small number of droplets the direct droplet counting is possible
Dijet reconstruction using the Pt weight works reliably in HI Dijet reconstruction using the Pt weight works reliably in HI environment for jets with Et>~30 GeVenvironment for jets with Et>~30 GeV
Reconstruction of jet parameters (Pt symmetry in Phi, y.....)Reconstruction of jet parameters (Pt symmetry in Phi, y.....) event-by-eventevent-by-event Deflection of fragmentation products by the radial and Deflection of fragmentation products by the radial and
longitudinal flow and resulting medium response need more study longitudinal flow and resulting medium response need more study => Mach cone ! => Mach cone !
Jet can be decoupled from underlying flow patternJet can be decoupled from underlying flow pattern
Reaction plane and v2 can be estimated for v2>=0.02 and Reaction plane and v2 can be estimated for v2>=0.02 and multiplicities >500multiplicities >500