status & recent results from the alice collaboration · status & recent results from the...
TRANSCRIPT
Status & recent Results from the
ALICE Collaboration
David Evans
The University of Birmingham, UK
HEP-MAD 11
Madagascar August 2011
Outline of Talk
• Introduction
• The ALICE Experiment
• Status of Experiment
• Selection of results from ALICE– Particle spectra & ratios
– Flow
– Jet and high pT
suppression (RAA
)
– charm
• Future outlook
• Summary
Aims of ALICE
� Study strongly interacting matter at extreme energy
densities over large volumes and long time-scales (study of
QCD at its natural scale, ΛQCD ~ 200 MeV).
� Study the QCD phase transition from hadronic matter to a
deconfined state of quarks and gluons - The Quark-Gluon
Plasma.
�Study the physics of the Quark-Gluon Plasma (QCD under
extreme conditions).
4
Phases of Strongly Interacting Matter
Lattice QCD, µB = 0
Both statistical and lattice QCD predict that
hadronic matter will undergo a phase
transition, in to a deconfined state of
quarks and gluons – a quark-gluon plasma,
at a temperature of,
T ~ 170 MeV and energy density,
ε ~ 1 GeV/fm3.
ALICE will far exceed these
temperatures & densities at the
LHC.
5
Heavy Ion Collisions
pre-equilibration ⇒ QGP ⇒
hadronisation ⇒ freeze out
Colliders: AGS, SPS, RHIC, LHC
Create QGP by colliding ultra-relativistic heavy ions
√SNN (GeV) = 5.4 19 200 2360 (5200)
6
Observables
Jets
Open charm, beauty
7 7
Detector:
Size: 16 x 26 metres
Weight: 10,000 tons
Collaboration:
> 1000 Members
> 100 Institutes
> 30 countries
ALICE Detector
Technologies:18
Tracking: 7
PID: 6
Calo. : 5
Trigger, Nch
:11
ICPAQGP Goa 2010 J. Schukraft
8
Detector Status
PLC 20J. Schukraft8
Complete since 2008:
ITS, TPC, TOF, HMPID,
FMD, T0, V0, ZDC,
Muon arm, Acorde
PMD , DAQ
Partial installation (2010):
4/10 EMCAL* (approved 2009)
7/18 TRD* (approved 2002)
3/5 PHOS (funding)
~ 60% HLT (High Level Trigger)
2011
10/10 EMCAL
10/18 TRD
TRD to be completed end 2012
*upgrade to the original setup
ITS
TPC
TRD
TOF
EMCAL
PHOS
HMPID
L3 Magnet
Data Samples
Beam Energy # of Events
pp 900 GeV 300 k MB 2009, analysis finished
pp 900 GeV ~ 8 M MB 2010, partially analyzed
pp 2.36 TeV ~ 40 k MB 2009, only ITS, dNch/dη
pp 7 TeV ~ 800 M MB~ 120 M muons~ 20 M high Nch
2010
PbPb 2.76 TeV/N ~ 30 M MB 2010
pp 2.76 TeV ~ 70 M MB~ 20 nb-1 (rare triggers)
2011, analysis started
30 h only
Charged Particle Multiplicity
dNch
/dηηηη versus √√√√sdNch
/dηηηη (Pb-Pb) Theory
dNch
/dηηηη = 1584 ±±±± 4 (stat.) ±±±± 76 (syst.)
Larger than most model predictions
Rises with √s faster than pp
Fits power law: Pb-Pb ~ s0.15
Bjorken formula estimates energy density, εεεε > 15 GeV/fm3 (3 x RHIC)
11
Bose–Einstein correlations
(HBT)
• medium size: 2x larger than at RHIC– volume ~ 300 fm3
• medium life time: 40% longer than at RHIC– ττττ ~ 10-11 fm/c
ALICE, Phys. Lett. B 696 (2011) 328.
QM enhancement of identical Bosons at small
momentum difference
enhancement of e.g. like-sign pions at low
momentum difference qinv=|p1-p2|,
12
• dE/dx:
5% resolution
• Time-of flight,
resolution:
86 ps (Pb-Pb)
160 ps (p-p)
• TPC dE/dx: separate p from K up to 1.1 GeV
• Time of flight: separate K from πup to ~ 2.2 GeV
Particle ID
Identified Particle spectra
QM2011 J. Schukraft 13
Very significant changes in slope compared to RHIC
Most dramatically for protons
Very strong radial flow, ββββ ≈ 0.66even larger than predicted by most recent hydro
Blast Wave Fit
RHIC
Hydro Prediction
RHIC
RHIC
Pb-Pb: K/π
STAR (including feed down)
PHENIX, Brahms (feed down corrected)
p/π
Particle Ratios
14
- pp: Thermus thermal fit rather poor
(wasn't this better for pp at lower energies ??)
- K/ππππ grows slightly from pp value
- p/ππππ ≈ like pp
Pb: p/ππππ off by factor > 1.5
from predictions !but very compatible with RHIC !! ?
pp: 900 GeV & 7 TeV
Range of Thermal model prediction
Before we can conclude anything
we need more particle species..
'Baryon anomaly': ΛΛΛΛ/K0
15
Baryon/Meson ratio still strongly enhanced
x 3 compared to pp at 3 GeV
- Enhancement slightly larger than at RHIC 200 GeV
- Maximum shift very little in pT
compared to RHIC
despite large change in underlying spectra !
Ratio at Maximum
RHIC
Λ/K0
x 3
16
Does QGP Flow?
Ed 3Nd 3p
= 12π
d2NpTdpTdy
1+ 2vn cosn φ − Ψr( )[ ]n=1
∞∑
Angle of reaction planeFourier coefficient
φ
pT
Equal energy density contours
P
v2
v2 = cos2φ
V1 = directed flow. V2 = elliptic flow.
Study angular dependence of emitted particles
17
Elliptic Flow
� v2 shape is identical to
RHIC
� v 2 ~30% larger than
RHIC: larger <pT>
� π,K reproduced by
hydro calculation
� p ok for semi-
peripheral but is a
remaining challenge for
central collisions
ALICE, Phys. Rev. Lett. 105 (2010) 252302.
Hydro-calcs.: Shen, Heinz, Huovinen and Song, arXiv:1105.3226.
� Precision measurement of η/s:� current RHIC limit: η/S < (2-5) x 1/4π� η/S < 1/4π => conjectured AdS/CFT limit is wrong� η/S > 1/4π => measure σ� η/S ≈ 1/4π => quantum corrections
which are O(10-30%) in AdS/CFT!� 20% in v2 ~ 1/4π =>π =>π =>π => need few % precision
�Precision: How ? � fix initial conditions (geometrical shape is model dependent, eg Glauber, CGC)� quantify flow fluctuations σ (influence measured v2, depending on method)� measure non-flow correlations δδδδ (eg jets)� improve theory precision (3D hydro, 'hadronic afterburner', ...)� .........
18
Azimuthal Flow:
What next ?
ση mkT2=
22
22
}4{
}2{
nnn
nnn
vv
vv
σδσ
−≅
++≅
19
Higher Harmonics: v3,
v4, v5, ...
� fluctuations in the initial distribution
� non zero v3
� particle correlation is described by first five harmonics
Chiral Magnetic Effect
('strong parity violation')( )RPΨ−+ 2cos βα ϕϕ
B+-
Same charge correlations positiveOpposite charge correlations negativeRHIC ≈ LHCsomewhat unexpected
should decrease with Nchmay decrease with √s
RHIC : (++), (+-) different sign and magnitudeLHC: (++),(+-) same sign, similar magnitude?
( )βα ϕϕ −cos
+ -
B
?
RHIC
RHIC
Local Parity Violation in strong magnetic Field ?
21
Charged Jets in Pb-Pb
Large suppression of jets seen in central collisions
192 GeV168 GeV
10-20% peripheral
∆η∆η∆η∆η∆φ∆φ∆φ∆φ bin size: 0.1x0.147 GeV
102 GeV
0-10% central
∆η∆η∆η∆η∆φ∆φ∆φ∆φ
Back-to-back high-energy jets seen in peripheral collisions
Another way to study this effect is to look at high pTsuppression.
22
Nuclear Modification Factor
• particle interaction with
medium
• stronger suppression at LHC
• ~factor 7 at 7 GeV/c
TDppcoll
TDAA
TDAA dpdN
dpdpR
/
/)(
σσ
×><=
quark-gluon plasma
Divide pT
spectra in Pb-Pb by p-p
(with suitable normalisation factor)
RAA
vs centrality
• Suppression
increases with
centrality.
• Minimum remains
around 6-7 GeV
RAA
for different particles
Peripheral collisions
Central collisions
25
Charm Cross-Section in pp
26
RAA
Open Charm:
Nuclear Modification Factor
• mass ordering predicted: ∆E(π) > ∆E(D) > ∆E(B)
• charm RAA
is approaching πat p
T> 6 GeV/c
• Possible indication of smaller charm suppression at low p
T but overall
comparable with πs.
TDppcoll
TDAA
TDAA dpdN
dpdpR
/
/)(
σσ
×><=
27
RAA
Heavy Quarks to Leptons:
Nuclear Modification Factor
• semi-leptonic decays:
• b, c → e+X
• b, c → µ+X
• heavy quark suppressed
by factor ~ 3
• B feed-down
uncorrected
28
J/ψψψψ in Pb-Pb
•J/ψ→e+ e-
•J/ψ→µ+µ-
29
RAA
J/ψψψψ:
Nuclear Modification Factor
TDppcoll
TDAA
TDAA dpdN
dpdpR
/
/)(
σσ
×><=
• J/ψ suppressed by factor ~ 2
• inclusive J/ψ: ~10% B feed-down
• cold nuclear effect not
measured: need pPb collisions
• small centrality dependence
• a test of statistical hardonization
will need data in mid rapidity:
PbPb runs in this year
Inclusive J/ψψψψ RAA = 0.49 ±±±± 0.03 (stat.)
±±±± 0.08 (syst.)
Rather small suppression and less than at RHIC
30
LHC: Tentative Schedule
2010: long run with pp collisions at 7 TeV
08-Nov-2010: 1st Pb+Pb collisions at 2.76 TeV
2011: short run with pp at 2.76 TeV
long run with pp at 7 TeV
2nd Pb+Pb collisions at 2.76 TeV – 10x stats ?
2012: long run with pp at 7 TeV
2012/2013: Pb+Pb; or p+Pb control measurement
2013/14: Machine shutdown
2014 - : pp and Pb+Pb at full energy
Summary
� Charged particle multiplicity ~ factor 2 larger than RHIC
� energy density ~ 3 x RHIC
� 2 x volume, 40% longer lived than RHIC
� baryon anomaly still exists at LHC (similar to RHIC)
� stronger radial flow at LHC (β ~ 0.66)
� elliptic flow: v2
increases from RHIC to LHC
� same centrality and pT
dependence
� High PT
suppression (RAA): suppression stronger at LHC
� suppression decreases at pT
> 5-6 GeV
� no strong flavour dependence
� J/ψ has smaller suppression
�We are at the very beginning of a 10 year programme and have just
scratched the surface (with ~1% of required data).
� lots of work and exciting physics to look forward to.
� Thank you for listening