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Study of charm hadroproduction Tau neutrino production at CERN SPS

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1 Study of charm hadroproduction Tau neutrino production at CERN SPS
BEACH2018 The XIII International Conference on Beauty, Charm and Hyperon Hadrons Peniche, Portugal Study of charm hadroproduction & Tau neutrino production at CERN SPS A.Murat GÜLER METU Ankara On behalf of the DsTau Collaboration 4/7/2019 A. Murat

2 Physics Motivations Tau neutrinos are the least known particle in the Standard Model. Testing the lepton universality in ντ CC cross section ντ cross section was measured with a large uncertainty Important for future neutrino experiments, SHiP, DUNE, Hyper-K.. 4/7/2019 A. Murat

3 Concept of ντ Detection
Proton beam τ ντ X ντ production ντ detection: Statistical uncertainty 33% in DONUT. D+ Ds τ ντ X X' Primary proton Main ντ source: Ds →  decays produced in proton interactions  No experimental data on differential cross section of Ds  Large systematic uncertainty (~50%) in the ντ flux prediction 4/7/2019 A. Murat

4 DONuT Experiment 9 ντ CC events observed ντ CC cross section
where n is the parameter controlling the longitudinal part of the Ds differential cross section “Final tau-neutrino results from the DONuT experiment”, Physical Review D 78, 5 (2008) longitudinal dependence transverse dependence 4/7/2019 A. Murat

5 DsTau Experiment Emulsion based experiment @ CERN SPS
Precise mesurement of ντ CC cross section Aiming to detect 103 Dsτ Systematic uncertainties DONuT DsTau Ds differential cross section (xF dependence) ~0.5 0.1 Charm production cross section 0.17 Decay branching ratio 0.23 Target atomic mass effects (A dependence) 0.14 0.05 4/7/2019 A. Murat

6 Emulsion detectors Highest position resolution AgBr crystal
1014 crystals in a film Highest position resolution Emulsion film Cross-sectional view Emulsion layer (44 m) Plastic base (200 m) Emulsion layer (44 m) 200 nm 20 m 10GeV/c  beam Sensitivity 36 grains/100 m 3D tracking device 4/7/2019 A. Murat

7 High precision measurement
Intrinsic resolution of each grain = 50 nm Two grains on top and bottom of 200 mm base  0.35 mrad Discrimination of 2 mrad at 4σ level A new system with piezo-based Z axis under development Angular measurement reproducibility of 0.15 mrad was achieved Piezo objective scanner Position reproducibility ~ 8 nm Angular reproducibility ~ 0.15 mrad θ σx = 50nm 200 μm base Beam angle 4/7/2019 A. Murat

8 A pion Interaction in Emulsion
3D Vector information, position and slope . Tracking by 35 nm position resolution. m.i.p and nuclear fragment is easily distinguished

9 Detector Structure 400 ECCs will be exposed to accumulate 2.3x108 interactions 10 units (total 100 emulsion films) ECC for momentum measurement (26 emulsion films interleaved with 1 mm thick lead plates) Proton Ds τ X D+ X’ Tungsten / molybdenum 4/7/2019 A. Murat

10 Detection of Ds → τ → X event
Kink angle of Ds The analysis chain: 1) Tag X decay (mean ~100 mrad) 2) Perform high precision measurement to detect Ds decay <θ> 7 mrad Need high precision measurement! Flight length of Ds <FL> = 3.3 mm Flight length of τ <FL>=2.0 mm 4/7/2019 A. Murat

11 Ds momentum reconstruction
Difficult to measure Ds momentum directly due to short lifetime Artificial Neural Network (ANN) using 4 variables Ds τ Primary proton FLDs FL τ Δθ Ds → τ FL: flight length Δθ: kink angle Δθ τ →X Measure xFdistribution Δp/p= 18% Fit to (1-|xF|)n n = 5.8 4/7/2019 A. Murat

12 Expected Performace Relative systematic uncertainty for cross section measurement: ~30% with 2018 run  Re-evaluation of the DONUT result ~10% with run  Input for future measurement 2018 run 2021 run Uncertainties Aiming at 10% precision to look for new physics effects in ντ -nucleon CC interactions 4/7/2019 A. Murat

13 DsTau Collaboration Status of the project Japan: Nagoya Kyusyu Aichi
Romania: Bucharest Russia: Dubna Turkey: Ankara Switzerland: Bern Japan: Nagoya Kyusyu Aichi Kobe Letter of Intent Submitted to the CERN-SPSC in Feb. 2016 Test Beam Studies in November and May 2017 Physics runs : 2018, 4/7/2019 A. Murat

14 Beam Exposure schedule
Run Beam time Emulsion surface Goal 2016 test beam (10 modules) Test of the setup Proof of principle 2017 test beam (~2 modules) Improvement of exposure scheme pilot run (approved) 1 week 48 m2 (30 modules) Test of large data taking and analysis BG estimation with data Physics results (~80 Ds →  detected) 2021 physics run (recommended) 2 weeks 545 m2 (338 modules) Physics results (~1000 Ds →  detected) 2022 physics run 4/7/2019 A. Murat

15 Test Beam @ CERN H4 beam line
Target mover ECC Stage controled By each spill Proton Silicon detector 4/7/2019 A. Murat

16 Automatic Scanning Microscope
A fast scanning in Nagoya Univ. Scanning speed of 22 m2/day Precision measurement in Bern Resolution ~0.3 mrad Hyper Track Selector (HTS) System 2. Precision measurement to detect Ds  τ decay (a few mrad) High speed scanning of full area to select τ  X + partner-charm decays (Δθ ~100 mrad) 4/7/2019 A. Murat

17 Automatic Scanning Microscope
~4000 tracks in 2 x 2 mm2, 15 films 1000 μm 4/7/2019 A. Murat

18 Efficiency of Ds detection
X qX FLDs FLt qt Proton MC with 400 GeV beam Selection Total efficiency (%) (1) Flight length of Ds ≥ 2 emulsion layers 77 (2) Flight length of  ≥ 2 layers & Δθ(Ds) ≥ 2 mrad 43 (3) Flight length of Ds < 5 mm & flight length of  < 5 mm 31 (4) Δθ() ≥ 15mrad 28 (5) Pair charm: 0.1 mm < flight length < 5 mm (charged decays with Δθ > 15 mrad or neutral decays) 20 4/7/2019 A. Murat

19 Z distribution of observed vertices Interactions in a tungsten plate
Event reconstruction Measured proton beam density in the analyzed region: 4.36x105 beam tracks/3.61 cm2 Z distribution of observed vertices Interactions in a tungsten plate 200 μm # of vertices Expected 1860 Observed With parent 1832 Without parent 130 Tungsten target 4/7/2019 A. Murat

20 Reconstructed Double vertex
Kink IP of daughter μm FL μm kink angle 118 mrad Vee IP of daughters 20.9, μm FL μm opening angle 242 mrad 1000 μm 200 μm 4/7/2019 A. Murat

21 Double-decay topology event (open charm)
(Video in ppt) Kink IP of daughter μm FL μm kink angle 118 mrad Vee IP of daughters 20.9, μm FL μm opening angle 242 mrad N1ry 40本以上 100 μm

22 Summary The DsTau project is proposed to measure ντ production (Ds differential production cross section) reduce systematic uncertainty in the cross section measurement to 10% Emulsion detectors with nano-precision readout About 1,000 Ds →  decays in 2.3×108 proton interactions will be detected. By-product: study charm physics (~105 charm production) Test experiments conducted in Pilot run in 2018 and physics run from 2021 4/7/2019 A. Murat

23 Physics Motivations Charmed hadron interaction cross section measurement D+ X To be sure requesting daughter as electron D- X’ D+ 4/7/2019 A. Murat

24 Physics Motivations Precise mesurement of in ντ CC cross section
reduce uncertainity to 10% ντ : only the DONuT experiment Measured as a function of a parameter n describing dσ(Ds)/dxF ~(1-|xF|)n No experimental data giving n for Ds 4/7/2019 A. Murat


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