Title: Charm production measurement
1Charm production measurementStatus of PPR 6.5
- Andrea Dainese
- University of Padova
2Outline
- Exclusive D0 reconstruction
- ALICE sensitivity for charm
production at the LHC - physics motivation for charm at LHC
- reminder of results of detection study
- estimate of statistical errors
- estimate of (main) systematic errors
- errors combined and sensitivity to
- a nice surprise from the D0
- Status of PPR 6.5
3Charm present experimental picture
4Charm what do we expect at LHC ?
- Thermal charm production
- maximum predicted T 800-1000 MeV not much lower
than charm mass - some models predict additional production
comparable to initial hard yield
precise measure of cross sections in pp, (pA), AA - Energy loss
- fast partons loose energy (mainly) by gluon
radiation - study energy loss of charm quarks
(RAA AA/pp(pA) vs pt) - dead cone effect suppresses energy loss in
heavy quarks w.r.t. light quarks
study D/p vs pt in AA (pA) and in pp
5Charm D0? Kp strategy
- Weak decay with mean proper length ct 124 mm
- Impact Parameter (distance of closest approach
- of a track to the primary vertex)
- of the decay products
- d0 100 mm
- STRATEGY invariant mass analysis of
fully-reconstructed topologies originating from
(displaced) secondary vertices - Measurement of Impact Parameters
- Measurement of Momenta
- Particle identification to tag the two decay
products
6Charm Results
S/B initial (M?3s) S/evt final (M?1s) S/B final (M?1s) Significance S/?SB (M?1s)
Pb-Pb 5 ? 10-6 1.3 ? 10-3 11 37 (for 107 evts)
pp 2 ? 10-3 1.9 ? 10-5 11 44 (for 109 evts)
Note in pp, large uncertainty on primary vertex
position beams de-focused to reduce luminosity
to 1030 cm-2s-1
7Binning Smoothing in dN/dpT pp
- Optimize binning in the range 0-14 GeV/c bin
size increasing with pT - good precision on measurement of pT slope
- small statistical error up to high pT
- Fit pT distributions to remove fluctuations due
to reduced statistics of simulation at high pT
(especially for Bkg) - Use fitted function to obtain smooth dN/dpT for
S and B
8Binning Smoothing in dN/dpT Pb-Pb
9Statistical Error
- Rel. Statisitical error on S expected to be
1/Significance - S (SB)observed Bestimated
- error on (SB)observed sqrt(SB)
- error on Bestimated negligible (uses info
from wide range mass distr.) - error on S error on (SB)observed
sqrt(SB) - relative error on S sqrt(SB)/S
1/Significance - This has been checked by generating and fitting a
large number of invariant mass distributions,
using as input parameters the results of the
simulation, namely - statistics for S and B VS pT
- width of D mass distribution VS pT
- slope of exponential bkg VS pT
10Statistical Error - pp
- Fit with expo gaus
- with 4 free parameters
- expo slope
- gaus integral (S)
- gaus mean
- gaus sigma
- (total integral fixed)
- Many (10,000) iterations
- study resolution on S
- (statistical error)
- study robustness of fit
11Statistical Error Pb-Pb
12Systematic Errors
- Main systematic errors considered
- correction for feed-down from beauty (B.R. B ? D0
is 65!) - error of 8 assuming present uncertainty
(80) on _at_ LHC - Monte Carlo corrections 10
- B.R. D0? Kp 2.4
- extrapolation from N(D0)/event to ds(D0)/dy
- pp error on (5, will be measured by
TOTEM) - Pb-Pb error on centrality selection (8)
error on TAB (10)
13Charm d2s(D0)/dptdy and ds(D0)/dy
14Charm B? D a la CDF
- Impact parameter of D0 can be used to separate
primary and secondary D0 - Background shape from
- side-bands in inv. mass
- Background subtracted
15Conclusions
- Pb-Pb and pp sensitivity studies being finalized
- Statistical errors on pt distribution estimated
- Main systematic errors considered
- Physics performance on charm X-section
measurement - Dominant systematic errors MC corrections and
- cross section normalization
Statistical Systematic
Pb-Pb 7 19
pp 3 14
16Outlook (1)
- Study sensitivity to comparison with NLO pQCD
- Run MNR program with different choices of
parameters (c-mass, PDF, shadowing) for pp and
Pb-Pb - check dependence of total cross section on
parameters - check dependence of pt shape on parameters
- study sensitivity of our errors bars to pQCD
input and to shadowing (low-pt region) - Study extrapolation to pt 0 in Pb-Pb
(uncertainty on total X-section) - Define strategy for comparison of different
energies by means of pQCD
17Outlook (2)
- Observables to study shadowing, energy loss,
thermal production - total X-section and pt slope
- shadowing expected to suppress low pt
- energy loss expected not to change total
X-section but increase pt slope how much?
dependence on parton dE/dx - thermal charm expected to increase total
production and determine 2-component pt
distribution (?) - RAA RCP (central/peripheral)
- estimate errors on RAA from errors in Pb-Pb and
in pp extrapolation of pp to 5.5 TeV using pQCD - estimate errors on RCP
- study separately effect on RAA and RCP of
shadowing, energy loss, thermal charm - D/p ratio central/peripheral
- expected to increase with pt due to dead cone
effect
18PPR chapter 6.5
19Contents of chapter 6.5
December 02
- 6.5.1 Charm and beauty production at LHC
- 6.5.2 Charm detection in hadronic channels
- 6.5.3 Charm and beauty detection in the
semileptonic - channels
- 6.5.4 Charm and beauty detection via e-m
coincidences - 6.5.5 Charm and beauty in pp collisions
Total 25 pages
20Contents of chapter 6.5
June 03 on the web
- 6.5.1 Physics motivations
- 6.5.2 Present experimental measurements of open
- charm production in heavy ion
collisions - 6.5.3 Charm and beauty production at LHC
- 6.5.4 Exclusive charm reconstruction in hadronic
- decay channels
- 6.5.5 Beauty detection in the semi-electronic
decay - channel
- 6.5.6 Charm and beauty detection in the
semi-muonic - decay channel
- 6.5.7 Charm and beauty via e-m coincidences
Total 43 pages
216.5.3 Production at LHC
- Total cross sections in nucleon-nucleon
collisions - Extrapol. to Pb-Pb collisions
- Extrapol. to min. bias p-Pb _at_ 8.8 TeV (only for
MRST PDF) - Spectral shapes and tuning of event generators
- the comparison with NLO pQCD is shown for PYTHIA
and for Pb-Pb collisions _at_ 5.5 TeV - now also shown for pp collisions _at_ 14 TeV
- a small paragraph on HERWIG was included for
completeness - for p-Pb tuning of PYTHIA taken from R. Vogt and
comparison not shown - Hadronization and decays
- yields for hadrons in Pb-Pb, in pp and in p-Pb
- comparison for pT and y of quark and meson
parametrized pT shape of D and B mesons, but only
for Pb-Pb _at_ 5.5 TeV
226.5.4 Hadronic channels
- D0 ? Kp analysis in Pb-Pb ?
- done for B 0.4 T and dNch/dy 6000 ?
- extrapolations to lower multiplicity (3000) ?
- extrapolations to other values of magnetic field
should be included ? - In pp
- analysis final but text still missing
- New nice results on B ? D0
- In p-Pb (Raffaele Grosso)
- strategy defined and tools ready
- results during summer
- Physics Performance
- Other channels D ? D0p (P. Hristov summer
student), -
236.5.5 Semi-electronic B
- Detailed simulation of B ? e X done in Padova
- Pb-Pb 6000 B 0.4 Tesla
- Internal Note almost ready
- PPR text ready
246.5.6 D and B with muons
- Study in progress by Rachid Guernane (same inputs
as for other studies being used) - For the moment only strategy in the PPR
- Philippe Crochet will work on the simulation
starting from summer - Hopefully results by autumn
6.5.7 D and B via e-m coincidences
25Summary
- Text in good shape
- introduction motivations, present data
- production / cross sections
- hadronic D0 in Pb-Pb
- semi-electronic B in Pb-Pb
- Work done, text missing
- hadronic D0 in pp (Andrea)
- Work in progress
- hadronic D0 in p-Pb (Raffaele)
- charm cross section from D0 more physics
comparison with NLO pQCD and/or PYTHIA,
comparison of pp, pA, AA (Andrea) - D and B with muons (Rachid)
- e-m coincidences (Philippe)
chapter very healthy and growing !