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Experimental preview ofLHCb results
PatrickRobbe,LALOrsay,5February 2017,
FortheLHCb Collaboration
• LHCb joined the LHC Heavy Ion program in 2013: pPb (1.1 nb-1) + Pbp (0.5 nb-1) collisions at 5 TeV, and performed several measurements from thesedata:
• J/y [JHEP 02 (2014) 72], y(2S) [JHEP 03 (2016) 133] and Y(nS) [JHEP 07 (2014) 094]
• Z [JHEP 09 (2014) 030], D0 [LHCb-CONF-2016-003], particle correlations [PLB 762C (2016) 473]
• The program continued in the Run 2 of the LHC and new collision data recorded:
• PbPb in 2015, for the first time• pPb + Pbp in 2016, with 10 times more statistics
• In parallel, development of a fixed target program2
LHCb andHeavyIons
TheLHCb experiment
3
~20m
~12m
10-300mrad
10-250mrad
VertexDetectorreconstructverticesdecaytimeresolution:45fsIPresolution:20μm
RICHdetectorsK/π/pseparationε(K→K) ~ 95 %, mis-ID ε(π→K) ~ 5 %
DipoleMagnetbendingpower:4Tm
Trackingsystem:TTandOTmomentumresolutionΔp/p=0.5%–1.0%(5GeV/c– 100GeV/c)
Calorimeters(ECAL,HCAL)energymeasuremente/γ identificationΔE/E=1%⨁10%/√E(GeV)
Muon systemμ identificationε(μ→μ)~97%,mis-IDε(π→μ)~1-3%
b𝑏" acceptance
[IJMPA30(2015)1530022][JINST3(2008)S08005]
LHCb andHeavyIons• LHCb is specialised in heavy flavour precision
physics, beauty and charm:• Optimised for low pile-up collisions (ie low multiplicity):
• Precise reconstruction of production and decay vertices: time dependent CP violation
• Correlations between particles: flavour tagging
• Some characteristics of the experiment make itattractive for measurements in Heavy ion physicstoo:
• Instruments fully the forward region: 2<h<5• Precise vertexing: separation of prompt production
from B decay products• Precise tracking: reconstruction down to pT=0• Particle identification: reconstruction of hadronic
decays4
5
LHCb operates intwo modesUn
ique
to
LHCb
Uniq
ue e
nerg
ies
Collider mode:PbPb collisions(2015)• LHCb took part for the first time to a LHC PbPb run end of
2015, with emphasis on low multiplicity events.• Up to 54 colliding bunches, ie 10% of the luminosity provided
to the other LHC experiments, and a total of 3-5 µb-1 integratedluminosity recorded with the detector running in standard conditions (same as with proton-proton collisions)
• Centrality reach: up to 50%, where measurements of J/y, D0, Ks
0, L, … production can be done• No final measurement but latest news in presentation by
Michael Winn (7 February, session 4.3, 5:10 pm)
6
]2) [MeV/cπM(K1800 1850 1900 1950
2C
andi
date
s per
8.0
MeV
/c
100
200
300
400
500
600
70050%<Event Activity<70%LHCb preliminary
= 5 TeVNNs
D0➝ K- p+
]2) [MeV/cππM(460 480 500 520 540
2C
andi
date
s per
1.0
MeV
/c
50010001500200025003000350040004500 50%<Event Activity<70%LHCb preliminary
= 5 TeVNNs
K0S➝ p- p+
• pPb collisions at 5 TeV: « small » sample collected (~50% of the 2013 sample)
• pPb (~13nb-1) and Pbp (~17nb-1) collisions at 8.2 TeV: more than 10 times the 2013 statistics. Possibility to perform many new or improved measurements [LHCb-PUB-2016-011]
7
Collider mode:pPb collisions(2016)
D+➝ K- p+p+
• Due to geometry of detector: when reverting beams, two different coverages: large statistics accumulatedin both configurations in 2016
8
Collider mode:pPb collisions(2016)
pPb
Pbp
p
Pb
Pb
p
1.5<y*<4.5
-5.5<y*<-2.5 Measurement of Forward-Backward ratios in a commonrange (2<|y*|<4.5)y* = center of mass rapidity
9
Collider mode:pPb collisions(2016)
For the first time for heavy ion collisions, we usedthe trigger scheme introduced in Run 2 for ppcollisions.
This scheme gives at the output of the trigger, fullyreconstructed and selected signal candidates (J/y, y(2S), D0, ….) using full detector information (PID, …) and with optimal alignment and calibration: no further reconstruction required.
This allows fast processing of the data: more details and previews of the LHCb pPb 2016 data for quarkonium, open charm and even open beauty in the presentation by Michael Winn(7 February, session 4.3, 5:10 pm))2) (MeV/c-µ+µMass(
3000 3050 3100 3150 3200
2Ev
ents
/ 2
MeV
/c
0
5000
10000
15000
20000
25000
30000
35000 LHCb preliminary = 8 TeVNNsp-Pb,
-1~13 nbJ/y➝µ+µ-
Fixed TargetPhysics With LHCb
• Gas can be injected inside the LHC vacuum, in the VELO detector.
• Used to determine the luminosity but since 2015 is used to also collect physics data. [JINST 7 (2012) P01010]
• Originally use Neon gas
• Other non-getterable noble gases can be used: in 2015 and 2016, we used also Ar and He
• The gas spreads in the beam pipe around LHCb: collision vertices over a range of ~1m (usable range)
• Physics events are collected by the LHCb detector, operated in standard configuration
10
• The pressure in the LHC when the gas is injected is ~2x10-7 mbar (insteadof 10-9 mbar with no injection), between 1 day to 2 weeks.
• The pressure is so low that it does not interfere with the running of the LHC.
• Data samples collected during special runs in 2015 and 2016:• p (6.5 TeV) Ne during van der Meer scan [2015, 20h]• p (6.5 TeV) He during large b* run [2015, 8h] and van der Meer scan [2016, 16h]• p (6.5 TeV) Ar during large b* run [2015, 18h]• p (2.5 TeV) Ar during van der Meer scan of reference 5 TeV pp run [2015, 11h]
• Data were also collected in parallel to LHCb taking data in collision mode (during the Heavy Ion runs), injecting the gas continuously:
• Pb (6.37 Z TeV) Ar during the PbPb run (2 weeks) [2015, 50h]
• p (4 TeV) He during the pPb 5 TeV run (several days) [2016, 80h]11
Fixed TargetPhysics With LHCb
Fixed TargetPhysics With LHCb
12
)2 K invariant mass (MeV/cπ1750 1800 1850 1900 1950 2000
2en
tries
/ 8
MeV
/c
0
10
20
30
40
50
60LHCb preliminary
2015 pNe data
)2 invariant mass (MeV/c-µ +µ2900 3000 3100 3200 3300 3400 3500
2en
tries
/ 16
MeV
/c
0
20
40
60
80
100LHCb preliminary
2015 pNe data
J/y➝ µ+ µ-
inpNe
D0➝ K- p+inpNe
[https://twiki.cern.ch/twiki/bin/view/LHCb/LHCbPlots2015#SMOG_plots_pNe_collisions_approv]
Physics program is for the moment:• Measurement of p production
cross-section in pHe collisions (useful for understanding of cosmological p production)
• Measurement of heavy flavourproduction: first measurement of J/y to D0 production ratio in the pAr sample will be shown by Emilie Maurice (session 4.4, Feb 7 at 5:50 pm)
Conclusions
• Main news for the LHCb heavy ion program:• Large sample of pPb and Pbp collisions at 8 TeV collected in optimal
conditions: this will provide new precise results in the very near future• First result on heavy flavour from the fixed target program
• LHCb talks in parallel sessions:• Emilie Maurice, session 4.4 (Open Heavy Flavours), Tuesday 7 Feb, 5:50 pm
New high resolution measurements of open and hidden charm production in proton-nucleus collisions at sqrt(s) = 110 GeV with the LHCb detector
• Michael Winn, session 4.3 (Quarkonia), Tuesday 7 Feb, 5:10 pm Heavy flavour production in proton-lead and lead-lead collisions with LHCb
13