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1 Е. Кокоулина, А. Кутов Е. Кокоулина, А. Кутов *) *) , , В. Никитин и Ю. Петухов В. Никитин и Ю. Петухов СВД -2 Коллаборация: СВД -2 Коллаборация: JINR, IHEP and SINP MSU JINR, IHEP and SINP MSU *) ОМ УрО РАН, Сыктывкар *) ОМ УрО РАН, Сыктывкар Gold Sands Gold Sands , , Belarus, Belarus, September , September , 4-9, 4-9, 200 200 9 9 Поиск коллективных явлений в адронных взаимодействиях
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Е. Кокоулина, А. Кутов *) , В. Никитин и Ю. Петухов

Jan 15, 2016

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Поиск коллективных явлений в адронных взаимодействиях. Е. Кокоулина, А. Кутов *) , В. Никитин и Ю. Петухов СВД -2 Коллаборация: JINR, IHEP and SINP MSU *) ОМ УрО РАН, Сыктывкар. Gold Sands , Belarus, September , 4-9, 200 9. Outline. - PowerPoint PPT Presentation
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Page 1: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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Е. Кокоулина, А. КутовЕ. Кокоулина, А. Кутов*)*),, В. Никитин и Ю. Петухов В. Никитин и Ю. Петухов

СВД -2 Коллаборация: СВД -2 Коллаборация: JINR, IHEP and SINP MSUJINR, IHEP and SINP MSU*) ОМ УрО РАН, Сыктывкар*) ОМ УрО РАН, Сыктывкар

Gold SandsGold Sands, , Belarus, Belarus, September ,September , 4-9, 4-9, 20020099

Поиск коллективных явлений в адронных

взаимодействиях

Page 2: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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Outline

The extreme multiplicity puzzles

SVD-2 setup and data processing

Search of the collective phenomena

Gluon Dominance Model

Outlook

Page 3: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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The extreme multiplicity puzzles

Page 4: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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chn

mb

nch )(

The extreme multiplicity puzzlesThe extreme multiplicity puzzles1)1) MC PHYTHIA code has MC PHYTHIA code has

shown that standard shown that standard generator predicts a value generator predicts a value of the cross section which of the cross section which is in reasonably good is in reasonably good agreement with data at agreement with data at small multiplicity nsmall multiplicity nchch < 10, < 10, but it underestimates the but it underestimates the value value σσ(n(nchch) by two orders ) by two orders of the magnitude at nof the magnitude at nchch > > 18. 18.

2)2) The existing models are The existing models are very much sensitive in the very much sensitive in the region of the extreme, region of the extreme, more significantly than more significantly than mean multiplicity (ExMu).mean multiplicity (ExMu).

3)3) The various manifestation The various manifestation of the collective of the collective phenomena is caused by phenomena is caused by the dense system the dense system formation at the ExMu formation at the ExMu region.region.

chnNApp 2)(

Page 5: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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SVD-2 setup and data processing

Page 6: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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10 10

mm

MMSS

MSMSVDVD

EMEMCC

Č

DT

ScH

SVD-2 setupSVD-2 setupU-70 U-70 acceleration at acceleration at IHEP (Protvino), IHEP (Protvino), 50-70 GeV. The 50-70 GeV. The trigger systemtrigger system selects the rare selects the rare events with the events with the charged charged multiplicity more multiplicity more than 20 - 30. than 20 - 30. The The suppression suppression factorfactor of events of events with lower with lower multiplicity multiplicity amounts about amounts about 101044. The . The TargetTarget itself is a 7-cm itself is a 7-cm thick, 25mm-thick, 25mm-diameter vessel diameter vessel for liquid for liquid hydrogen. hydrogen.

MicroStrip Vertex Detector MicroStrip Vertex Detector Scintillator HodoscopeScintillator Hodoscope Drift Drift Tube TrackerTube Tracker Magnetic Spectrometer Cherenkov counter Magnetic Spectrometer Cherenkov counter ElectroMagnetic Calorimeter ElectroMagnetic Calorimeter

Page 7: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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MC event generator is designed for the setup element simulation;

Data processing software for ExMu;

Alignment;

GEANT-3 program reconstruction analysis.

Software Software developmentdevelopment

Page 8: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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Multiplicity Distributions (MD) in pp interactions at different trigger levels: 8, 10, 12.run 2008,PVD.

Software Software developmentdevelopment

Page 9: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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Kalman Filter as Track Fitter for SVD

1. Drift tubes calibration - from raw TDC time to drift distance.

2. Recognize track candidates – find track-like groups of hits: pattern recognition.

3. Taking into account REALITY: alignment.4. From track candidates to real track

parameters: track fitting.5. From tracks to vertexes: vertex fitting

Software Software developmentdevelopment

Page 10: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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Track fitting

It is necessary to take into account:

- non-uniform magnetic field (from table);- multiple scattering;- energy losses.

Software Software developmentdevelopment

Page 11: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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1. VD + MS reconstruction: track parameter determination; use MS data for momentum estimation.

2. DT track finding separately in Y,U,V planes, then build 3D tracks.

3. DT + MS track fitting: track parameters from 1 or 2 as initial values and Kalman Filtering procedure.

4. Taking into account non-uniform magnetic field,

multiple scattering, energy losses.5. Re-fit vertexes, if it is necessary.6. Kinematical fit (we can use the Vt++ library)

Analysis sequence

Software Software developmentdevelopment

Page 12: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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Software Software developmentdevelopment

Page 13: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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Software Software developmentdevelopment

Page 14: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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Search of the collective phenomena

Page 15: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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1. Bose-Einstein Condensation (BEC);2. Ring Events (Cherenkov gluon

emission);3. Gluon Dominance Model (GDM);4. Excess of soft photon (SP) yield;5. Clusterization;6. Turbulence Phenomena …

Search of the collective Search of the collective phenomenaphenomena

Page 16: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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M. Gorenstein and V. Begun had predicted an abrupt and anomalous increase of the scaled variance ω of

neutral- and charged- pion-number fluctuations in the vicinity of the BEC line [Phys.Lett.B651:114 (2007)].

Bose-Einstein Condensation

Search of the collective Search of the collective phenomenaphenomena

Page 17: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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Ring Events in pp (n_ch >8), run 2008

Search of the collective Search of the collective phenomenaphenomena

Red Red - 7- 7thth order order PolynomialPolynomial

nch 9nch < 9

Page 18: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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Monte-Carlo (nch 9)

Search of the collective Search of the collective phenomenaphenomena

Page 19: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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Ring Events ,/,/1cos EpnC

n - the index of the refraction,

θC = 0.065 0.005, n = 1.0023 ± 0.0003

Our experiment:

Theory:

n (p) = 1+Δn (p) = 1+3mpr2 σ(p) h ρ(p) / 8πppr,

h – the number of scatters, ρ = Re F/ Im F, Δn (p) = 3 mp

3 Re F / 2p 2 = 0.0005 * Re F, at Re F =4.6 GeV (.92 fm)

Search of the collective Search of the collective phenomenaphenomena

Page 20: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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Gluon Dominance Model

Page 21: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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hadronsgqqqZee ?),()( 0

First stage (cascade): a) gluon fission; b) quark bremsstrahlung; c) quark pair creation; NBD.

A.Giovannini. NP, B161 (1979).

Second stage (hadronization): BD

Convolution of two stages.

.)1(1PN

p

hpH

p zN

nQ

.!

)1)...(1(pk

p

p

m

p

pppm km

k

km

m

m

mkkkP

Gluon Dominance Model

Page 22: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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GDM parameters: mean multiplicity of hadrons from 1 gluon while its passing through of hadronization stage remains constant ~1 (14 -189, GeV). Fragmentation mechanism of hadronization: 1 parton to 1 hadron.

qq

1Meson

Baryon

B.Muller [nucl-th/0404015]

Gluon Dominance Model

Page 23: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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Gluon Dominance Model

GDM had shown: quarks of initial protons are staying in leading particles (from 70 to 800 GeV/c). Multiparticle production is realized by gluons. We name them active ones.

Two schemes: with/without gluon branch. ConvolutionConvolution gluon gluon (Poisson/Farry) (Poisson/Farry) && hadron (PBD) hadron (PBD) MDs.MDs. pp–pp–

interactionsinteractions

Page 24: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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recombination mechanism of hadronization

qq

qqq1

Meson

Baryon

B.Muller [nucl-th/0404015]

in pp–in pp–interactionsinteractions

Gluon Dominance Model

Page 25: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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In GDM for pp at 70 GeV the maximal possible number of new formed charged, neutral & total hadrons is limited and is equal to 26, 16 and 42 particles, accordingly.

Preliminary experimental data corroborate these predictions. From PVD data (which has constricted acceptance) we see events with maximal multiplicity 24 charged particles only.

Gluon Dominance Model

Page 26: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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01.0,/1.0 xcGeVpt

At HE σ(SP) are 5-8 times more in the comparison with the QED predictions. Assumption:

QG system or excited new formed hadrons set in almost equilibrium state during a short period (we use the black body emission spectrum): 1.0)(,40,4 nTnmbmb inin

Estimations of SP emission region: 4-6 fm.

Soft Photons (SP)Soft Photons (SP)

Gluon Dominance Model

Page 27: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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GDM and experimental MD’s Mirabel: Mirabel: ■■ - 50 - 50 GeV GeV - 70 - 70 GeV GeV

SVD: SVD: - 50 GeV - 50 GeV

- GDM- GDM

preliminarypreliminary

Run 2008, Run 2008, 50 GeV 50 GeV pp interactionspp interactions

88thth level HM level HM triggertrigger

Page 28: Е. Кокоулина, А. Кутов *) ,                                       В. Никитин и Ю. Петухов

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Outlook

Software check-out for track Software check-out for track reconstruction in DT and MS with reconstruction in DT and MS with tracks reconstructed in PVD. tracks reconstructed in PVD.

The continuation of the searching of The continuation of the searching of the collective phenomena in pp (pA) the collective phenomena in pp (pA) interactions at the extreme interactions at the extreme multiplicity: the Bose-Einstein multiplicity: the Bose-Einstein condensation, ring events (dense condensation, ring events (dense groups in angle distributions), groups in angle distributions), clusterization, turbulence phenomena. clusterization, turbulence phenomena.

Soft photon studiesSoft photon studies