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Reconstruction of short-lived resonances in pp collisions

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Presentation on theme: "Reconstruction of short-lived resonances in pp collisions"— Presentation transcript:

1 Reconstruction of short-lived resonances in pp collisions
F.Blanco – INFN e Università di Catania - Italy Content Identification strategy Code development Results on resonances (K*(892),(1520),(1020),..) from simulated p-p 900 GeV TeV Summary and Outlook Convegno Nazionale Fisica di Alice, Frascati, Novembre 2007

2 Signal extraction Inside same event, correlations between
K+ and π- candidates K- and π+ candidates Evaluate invariant mass spectrum Example: K*(892)  Kπ (~100%) Mixed-event technique Combinatorial background: Like-sign technique

3 Only events with Δm<5 and Δzv < 3 cm mixed
Study of the combinatorial background by the mixed-event technique Studied dependence on event selection criteria ●Charged multiplicity ●z-vertex location Only events with Δm<5 and Δzv < 3 cm mixed Multiplicity Comparison of the event mixing background to the “true” combinatorial backgroung ‘True’ background = (Signal) – (True pairs) z-vertex

4 (Mixed events background)
Effect of event selection on mixing procedure (True Background) (Mixed events background) Only events with Δm<5 and Δzv < 3 cm mixed No event selection

5 Like-sign technique also explored
Unlike-sign Like-sign Comparison of the like-sign background to the “true” combinatorial background

6 PID influence on K*(892) reconstruction
Perfect PID Realistic PID True PID influence on K*(892) reconstruction Found No thresh on maxprob Maxprob > 0.7 (K) Maxprob > 0.7 (π) Maxprob > 0.7 (K) No PID (π) Perfect PID Realistic PID True K* = 7599 Found K* = 7488 S/B = 0.138 S/√B = 30.68 True K* = 4306 Found K* = 4139 S/B = 0.11 S/√B = 20.28

7 How the code works From generation and reconstruction …
Selection of primary and identified tracks: AliRsnReaderRL From generation and reconstruction AOD: Analysis Object Data: AliRsnEvent, contains arrays of AliRsnDaughter objects ESD: Event Summary Data Kinematics Analysis, Cuts,histograms,… AliRsnAnalysis

8 Results from p-p events @ 900 GeV and 14 TeV 2 Data Sets
Events of PYTHIA were generated and fully reconstructed using Realistic simulation of the detector response for the whole ALICE assembly Realistic clusters and tracks reconstruction 2 Data Sets 2 x 105 minimum bias p-p PHYTIA 900 GeV. Running scenario at LHC startup 1.5 x 106 minimum bias p-p PHYTIA 14 TeV (about 0.2% 1-year data taking) PDC06 data, distributed GRID analysis

9 900 GeV

10 K*(892) results with realistic PID
True K* (within 2σ) = 4728 Found K* (within 2σ) = 4274 S/B = 0.105 S/√B = 20.12

11 (1020) and (1520) with realistic PID
True  (± 2σ) = 186 Found  (±2σ) = 168 S/B = 2.87 S/√B = 13.86 * True Λ (±2σ) = 146 Found Λ (±2σ) = 128 S/B = 1.23 S/√B = 19.5

12 Yields and particle ratios uncertainties
Resonance Discrepancy w.r.t. true pairs K* % Φ % Λ* % Particle ratios Statistical K*/K % Λ*/Λ % Φ/K* % Φ/Λ* % K*/Λ* %

13 K*(892)± analysis Total B.R. ~ 23 % π+ + π- B.R. ~ 69%
K*(892)± KS0 + π± B.R. ~ 33% Total B.R. ~ 23 % π+ + π B.R. ~ 69% Need to identify the associated V0 They are reconstructed by association of two opposite charge tracks, and then applying some topological cuts

14 3042 KS0 reconstructed (2978 true)
Results on charged K*(892) PPR cuts cosθp > 0.994 dca < 3.46 cm r > 0.34 cm b+/- > cm Efficiency = 52.0 % Purity = 97.9 % 0.48 < m < 0.51 GeV 3042 KS0 reconstructed (2978 true)

15 Results on charged K*(892)

16 Neural network approach to V0 finding
Aim: ● Improve V0 selection (efficiency & purity) by ANN ● Combine V0 with pion tracks bj = tanh (∑ wij ai – Θj) output = ∑ wk bk w’s = synaptic weights Θ = neuron thresholds ai = input bi = hidden layer Various possibilities for the training algorithm exploited, BFGS chosen 7 inputs, 1 hidden layer

17 Results on charged K*(892) using ANN approach
True and found K*(892)± V0 selection strategy True K* Found K* Notes PPR cuts Overestimated yield/width ANN Reason. agreement, best present condition Yield improvement by 15-20% with respect to PPR Reasonable agreement between true and found K*

18 14 TeV

19 (1020) and *(1520) with realistic PID
(1520) True =4893 Found =4967 True *=3879 Found *=3649

20 Mass resolution ~ 3MeV/c2
K*(892) with realistic PID Found K*(±2)=89182 True K*(±2)=85360 Mass resolution ~ 3MeV/c2

21 K*(892)0 pT-analysis with realistic PID

22 Correction matrix

23 (1020): signal vs. event mixing background

24 Λ(1520): comparison between signal and event mixing

25 Looking for f0(980) 100k pp TeV

26 Summary Short-lived resonances in pp LHC energies could be studied in ALICE from the very beginning With a small sample of events 900 GeV and realistic PID: ● Extraction of yields at least for K*(892), Φ(1020), Λ*(1520) ● Rough pT - distribution for K*(892) up to 1.5 GeV/c ● Particle ratios Φ/K*, Λ*/K*, Φ/Λ* measurable Analysis of O(106) pp events at 14 TeV fully reconstructed on the GRID ● Resonance yields with large statistics ● pT-analysis of K*(892)0 ● Correction matrix (y,pT) Extension to other resonances (Σ(1385), Δ, f0(980)) is in progress.

27 Backup

28 Neural network approach to charged K*(892) reconstruction
Huge background


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