Presentation is loading. Please wait.

Presentation is loading. Please wait.

Charm production with neutrinos Physics motivation Results Outlook Giovanni De Lellis University of Naples (on behalf of the CHORUS Collaboration)

Similar presentations


Presentation on theme: "Charm production with neutrinos Physics motivation Results Outlook Giovanni De Lellis University of Naples (on behalf of the CHORUS Collaboration)"— Presentation transcript:

1 Charm production with neutrinos Physics motivation Results Outlook Giovanni De Lellis University of Naples (on behalf of the CHORUS Collaboration)

2 c |V cd | 2,|V cs | 2 d,s ----  Beam knowledge Quark density functions, strange sea (  ) ,h E had h Charm fragmentation f D0 ; f D+ ; f Ds ; f  c z = p D /p c, p T 2 DIS charm production Production from d(anti-d) quarks Cabibbo suppressed  large s contribution:  50% in and  90% in anti-

3 measure strange content of the nucleon Possible s/anti-s asymmetry  non-p QCD effects crucial role in relating F 2 structure function for charged- and neutral-lepton strange sea is important for “stop” searches at hadron colliders: largest background: g+s  W+c R.Demina et al., Phys. ReV. D 62 (2000) 035011 S.J.Brodsky and B.Ma, Phys. Lett. B 381 (1996) 317 constrain/study charm production models –in NLO pQCD is a challenging theoretical problem »2 scales,  QCD and charm mass (J.Conrad et al. Rev.Mod.Phys. 70 (1998) 1341-1392) measure charm mass and V cd Physics motivation

4 Experimental techniques –massive high density detectors (CDHS, CCFR, CHARMII, NuTeV, NOMAD, CHORUS Calo): Pro: large statistics Contra: background from p, K decays; not sensitive to low- neutrino energies (E n <15GeV); not possible to study separately the different charmed types; B  is needed –bubble chamber filled with heavy liquid (BEBC, Fermilab 15-ft) –nuclear emulsions (E531, CHORUS)

5 Emulsion experiments Look “directly” at the decay topology of the charmed hadron with sub-micron resolution Contra: the anti- statistics is still poor Pro: –low background; sensitivity to low E –  m c threshold effect –hadron species identification –reconstruction of charmed hadron kinematics –  fragmentation studies 100  m

6 Inclusive charm production cross-section induced by Inclusive charm-production cross-section measurement possible only with nuclear emulsions So far only E531: 122 events CHORUS is currently analysing about 1000 events Final statistics (~1year from now) about 3000-4000 events!

7  p/p = 0.035 p (GeV/c)  0.22   p/p = 10  15% (p < 70 GeV/c) -nuclear emulsion target (770kg) -scintillating fiber tracker CHORUS detector  E/E = 32 %/  E (hadrons) = 14 %/  E (electrons)  h = 60 mrad @ 10 GeV E ~ 27 GeV Air-core magnet Active target muon spectrometer Calorimeter Neutrino beam :: :   :  : e : e : : : 1.00 : 0.05 : 0.017 : 0.007

8 0  m -21  m -36  m -54  m MIP: 30  40 grains/100  m Resolution ~ 0.3  m Focal depth: 1 to 3  m S. Aoki et., Nucl. Instr. Meth. A 447 (2000) 361 CHORUS emulsion  350  m  90  m

9 8 plates 1.5 mm All tracks (θ<400mrad) in the scanning volume (1.5X1.5X6.3mm 3 ) are recorded at 11 min./event scanning speed CHORUS Phase II

10 All track segments (  < 0.4 rad)All track segments (  < 0.4 rad) Fiducial volume: 1.5 x 1.5 mm 2 x 8 platesFiducial volume: 1.5 x 1.5 mm 2 x 8 plates Offline analysis of emulsion dataOffline analysis of emulsion data Track segments from 8 plates overlapped At least 2-segment connected tracks Eliminate passing- through tracks Reconstruct full vertex topology Emulsion data acquisition

11 Selection criteria At least one among daughter particle and muon tracks formed by at least 2 segments and reconstructed by the fiber tracker systems Tracks with big impact parameter with respect to vertex point  visual inspection for decay confirmation impact parameter vs. vertex depth dz = vertex depth parameterize the angular error θ=0.4 rad θ=0. rad Selected events

12  N  D s *  - N’ D s +   +   +   Diffractive D s production Phys. Lett. B 435 (1998) 458, CHORUS Coll.

13 D 0 production rate D 0  V4 / D 0  V2 = 0.231  0.04 25,693  CC analyzed (~15% of the full statistics) 25,693  CC analyzed (~15% of the full statistics) 851 (3.3%) selected events for visual inspection851 (3.3%) selected events for visual inspection Confirmed D 0 sample: 226 V2, 57 V4Confirmed D 0 sample: 226 V2, 57 V4 σ(D0)/σ(CC) E (GeV) Phys. Lett. B 527 (2002) 173, CHORUS Coll. J.Phys.G28 (2002) 713 (all channels): all existing data are combined σ(D 0 )/σ(CC) = 2.58  0.26(stat.)  0.13(syst.) % E531 CHORUS σ (D 0 )/σ (CC)x Br(D 0  V2+V4 ) = 1.99  0.13 (stat.)  0.17 (syst.)%

14 Statistical approach using flight length distribution Λ c DsDs D+D+ Flight length in μm Λ c production rate  (A) Short flight decay: selection A (40 mm < FL <400 mm): Λ c enriched sample 128 candidates out of 50,414 CC Long flight decay: selection B (400 mm < FL < 2400 mm): D +, D s dominated sample 210 candidates out of 56,761 CC  (B)(B) parent particle track

15 Evidence for  c production: 3-prong decays (background free) MC: D and Ds Data Background check: Pt distribution for 1-prong decays b.g. excess Data Monte Carlo Data

16  c production rate Combining short (A) and long (B: only 3-prong) decay searches and correcting for efficiencies and background: 3 equations and 3 unknowns D+Ds = 1118  116(stat)D+Ds = 1118  116(stat)  c = 861  198 (stat.)  98 (syst.) +140 (QE)  c = 861  198 (stat.)  98 (syst.) +140 (QE) Br(  c  3prong) = 24  7 (stat.)  4 (syst.)%Br(  c  3prong) = 24  7 (stat.)  4 (syst.)% Phys. Lett. B 555 (2003) 156 σ(D+Ds)/σ (CC) = 2.00  0.21(stat)% by product σ (  c) / σ (CC)= 1.54  0.35(stat)  0.18 (syst)% -54

17 a)  n   -  c + b)  n   -  c + (  c *+ ) c)  p   -  c ++ (  c *++ ) Quasi-elastic charm production QE charm production has a peculiar topology “pure”  c sample with a small (<10%) contamination i.e. normalization error  absolute BR determination P. Migliozzi et al. Phys. Lett. B 462 (1999) 217-224 Many candidates have been found in CHORUS and the cross-section measurement is in progress

18 Associated charm production D+D+X c c W c c D+D+X Z CC Gluon BremsstrahlungZ-Gluon Fusion NC

19 Associated charm production in CC In the past this search was based on the observation of tri-muon events  - (  +  - ) and same-sign di-muons: Large background from  and K decays Observed rate 60 times larger than expected from theoretical calculations! (K.Hagiwara Nucl.Phys.B 173 (1980) 487) Currently a search is in progress in CHORUS 1 event observed and confirmed by kinematical analysis (Phys. Lett B 539 (2002) 188, CHORUS coll.) (Phys. Lett B 539 (2002) 188, CHORUS coll.) A new analysis with a larger statistics is in progress. The discrepancy between data and theoretical predictions will be clarified soon.

20 3029 21 1010  m 6735  m transverse plane -- D0D0 kink parent N s = 2 N h = 6  kink = 420 mrad D 0 f.l. = 340  m f.l. = 1010  m 22 = 310 mrad f.l. = 7560  m 2ry vertex p  MeV/c dE/dx proton P = 0.78 GeV/c P > 330 MeV/c +180 - 110 1st vertex Phys. Lett B 539 (2002) 188, CHORUS Coll. First observation in CC Phys. Lett B 539 (2002) 188, CHORUS Coll. B.G. = 0.04±0.01

21 Associated charm production in NC Neutral-current interactions (g-brem. + Z-g fusion) –In the past only one event observed in the E531 emulsion Production rate 1.3 +3.1 -1.1 x10 -3 normalised to CC –Indirect search performed by NuTeV A.Alton et al., Phys. Rev. D64 (2001) 539 Production rate (2.6  1.6)x10 -3 normalised to CC at 154 GeV m c =(1.40 +0.83 -0.36  0.26) GeV, in agreement with other measurements –Currently a search for this process is in progress in CHORUS Several candidates have been found and the cross-section measurement will be finalised by the end of this year.

22 1ry@pl23 Ns=1, Nh=3 V2(1) @pl 23  =96.3 mrad fl= 62.8  m V2(2) @pl 22 fl= 976.6  m  =203.4 mrad TT #6 TT #3 TT #8 TT #5 pl23 pl22 Event 81332312 V2&V2 in 0mu V2&V2 in 0mu

23 120µm 210µm PLATE 18 PLATE 17 140µm TT Event 77393952 Ns = 6 Nh = 1 (gray) 4Vee @ pl 17 FL = 884 µm C3 @ pl 17 FL = 426 µm

24 200K events in CHORUS for Charm analysis From a sub-sample of data CHORUS has measured: –Diffractive D s * production (Phys. Lett. B 435 (1998) 458) –σ (D 0 )/σ(CC) (Phys. Lett B 527 (2002) 173) –CC associated charm production (Phys.Lett. B 539 (2002) 188) –B   (Phys. Lett B 548 (2002) 48): first direct measurement –σ(  c )/σ(CC) (Phys.Lett.B 555 (2003)156) Conclusions and Outlooks Analyses in progress: –Associated charm production in CC and NC –D* production –D 0 decay  all neutrals –Charm topological branching ratio –Anti-neutrino charm production –QE  c production


Download ppt "Charm production with neutrinos Physics motivation Results Outlook Giovanni De Lellis University of Naples (on behalf of the CHORUS Collaboration)"

Similar presentations


Ads by Google