Title: HIGHLIGHTS FROM THE COMPASS EXPERIMENT @ CERN
1HIGHLIGHTS FROM THE COMPASSEXPERIMENT _at_ CERN
- F. Bradamante
- University of Trieste and INFN Trieste
- on behalf of the
Collaboration - Sixth International Conference on Perspectives in
Hadronic Physics - Trieste, May 16, 2008
2COmmon Muon and Proton
Apparatus for
Structure and
Spectroscopy NA58
- Czech Republic, Finland, France, Germany, India,
Israel, Italy, Japan, Poland, Portugal, Russia - Bielefeld, Bochum, Bonn, Burdwan, Calcutta, CERN,
- Dubna, Erlangen, Freiburg, Heidelberg, Helsinki,
Lisbon, - Mainz, Miyazaky, Moscow, Munich, Nagoya, Prague,
Protvino, - Saclay, Tel Aviv, Torino, Trieste, Warsaw
- 28 Institutes, 230 physicists
3COMPASS
experiment thought of in April 94 Nov. 94 Trento workshop Trieste workshop _at_ICTP
LoI encouraged March 95 June 95 SPSLC in Cogne
Proposal recommended approved by RB March 96 Sept. 96 Feb. 97 as NA58
Technical run 2000 2000
Commissioning 2001 2001
- since 2002 taking data with
- a new spectrometer with outstanding performances
- merging of two programmes
HMC (muon beam) CHEOPS (hadron beam)
4Physics program of COMPASS
- Experiments with hadron beams
- Pion and Kaon polarizabilities
- Diffractive production of exotic states
- Search for glueballs
- Light meson spectroscopy
- Production of double charmed baryons
- Experiments with muon beam
- ?G/G
- g1
- Transverse spin effects
- Flavor decomposition of spin distribution
functions - Vector meson production
- Spin transfer in ?-hyperon production
5luminosity 5 . 1032 cm-2 s-1 beam
intensity 2.108 m/spill (4.8s/16.2s) beam
momentum 160 GeV/c
longitudinally polarised muon beam longitudinally
or transversely polarised target calorimetry
particle identification
LHC
SPS
N
6The Spectrometer for the Muon Programme
Trigger-hodoscopes
µ Filter
ECal HCal
50 m
RICH
MWPC
Straws
TWO STAGE SPECTROMETER
Gems
Drift chambers
Polarized beam and target
Micromegas
SAT,
LAT,
PID
Silicon
SciFi
0.003 lt x lt 0.5 10-3 lt Q2 lt 10 GeV2
7WHERE ARE WE ?
- in 2002, 2003, 2004, 2006 and 2007 COMPASS has
taken data in the muon program configuration
160 GeV, polarized m beam2002-2006 6LiD
polarized target (polarized deuterons)
2007 NH3 polarized target (polarized
protons)
2000 TB 51010 events
- pilot run in 2004 for hadron program
- 2008 hadron beam at 190 GeV for diffractive and
central production
- physics results
- DG/G 1.
pion polarizability - DS
2. PWA in diffractive - Transversity
scattering - Cahn asymmetry
- Pentaquark
- Exclusive ?0
- ? physics
8THE COMPASS MUON PROGRAM
- TWO CLASSES OF PHENOMENA
- LONGITUDINAL SPIN CASE
- TRANSVERSE SPIN CASE
9LONGITUDINAL SPIN CASE the beginning
EMC 1988
G1p 0.123 ? 0.013 ? 0.019 DS 0.12 ? 0.17
? SPIN CRISIS
10LONGITUDINAL SPIN CASE
- from polarised lepton polarised nucleon DIS
with
and
first moments
from measurement of EMC in 1988 and using
complementary information from neutron and
hyperon ßdecay one obtained
at variance with naïve expectation
since
necessity for measuring
SMC, SLAC, HERMES
and in SIDIS
SMC, HERMES, COMPASS
in SIDIS
HERMES, COMPASS
11LONGITUDINAL SPIN CASE
12MEASUREMENTS OF THEGLUON POLARIZATION
- FOUR LINES OF ATTACK
- Double spin asymmetry of the OPEN CHARM
cross-section in high energy µD scattering - Double spin asymmetry of the HIGH-pt HADRON PAIRS
in high energy µD DIS (Q2 gt 1 GeV2) - Double spin asymmetry of the high-pt hadron pairs
in high energy µD scattering (Q2 lt 1 GeV2) - Measurement of g1 of the deuteron and QCD fit of
all the world data
13DG/G at COMPASS
Photon Gluon Fusion
- q c cross section differencein charmed
meson production - ? theory well understood
- ? experiment challenging
- q u,d,s cross section difference in 21 jet
productionin COMPASS events with 2 hadrons
with high-pt - ? experiment easy
- ? theory more difficult
14 15D mass spectra
APS, 13 April 2008
G.K. Mallot
15
16DG/G from open charm
-
- 2002 2006 data D0 D
-
- ?G/G -0.49 0.27 (stat) 0.11 (syst)
-
- _at_ ltxggt 0.11, ltm2gt 13 (GeV/c)2
preliminary
16
17- ?G/G
- from High-pt hadron pairs
18?G/G from High-pt hadrons, Q2 gt 1 (GeV/c)2
19?G/G from High-pt hadrons, Q2 gt 1 (GeV/c)2
- 2002 2004 data High pT, Q2 gt 1 GeV/c2
-
- ?G/G 0.08 0.10 (stat) 0.05(syst)
-
- _at_ ltxggt 0.082 (range 0.055 0.123), m2
3 (GeV/c)2
preliminary
20?G/G from High-pt hadrons
all Q2
low Q2
resolved photon
21?G/G from High-pt hadrons, Q2 lt 1 (GeV/c)2
- 2002 2004 data High pT, Q2 lt 1 GeV/c2
-
- ?G/G 0.016 0.058 (stat) 0.055 (syst)
- _at_ ltxggt 0.085, m2 3 GeV2
preliminary
22Gluon Polarization
COMPASS preliminary results
high-pT pairs, Q2gt1GeV2
20022004
- ?G/G 0.08 0.10 (stat) 0.05(syst)
- _at_ ltxggt 0.082 (range 0.055 0.123), m2
3 (GeV/c)2
high-pt pairs, Q2lt 1GeV2
20022004
- ?G/G 0.016 0.058 (stat) 0.055 (syst)
- _at_ ltxggt 0.085, m2 3 GeV2
open charm
20022006
- ?G/G -0.49 0.27 (stat) 0.11 (syst)
- _at_ ltxggt 0.11, ltm2gt 13 (GeV/c)2
23Summary of results
new high-pT point
new charm point
G.K. Mallot
24 25g1 of the deuteron (2002-2003)
Phys Lett B 612 (2005) 154
- most precise measurement for 0.004 lt x lt 0.03
- new NLO QCD fit, precision of a0 improves factor
2 (Q2 4 GeV2)
26CONCLUSION from ?G MEASUREMENTS
?G SMALL
more precise measurements will come soon
COMPASS 2006 RHIC RUN6 .
interest in orbital angular momentum GPDs
Jis SUM RULE
27more on LONGITUDINAL SPIN CASE
MEASUREMENT OF VALENCE QUARK POLARISATION
28valence quark polarisation
29valence quark polarisation
- comparison with other experiments
30 31Transverse Spin case
- Large effects observed in hadronic interactions
32Transverse Spin case
- Large effects observed in hadronic interactions
at leading order a third PDF is necessary for a
complete description of the structure of the
nucleon
Theoretical developments
- DTq(x) being chiral-odd, it can be measured
only in conjunction - with another chiral-odd partner
Collins function
SIDIS
DY
measurable in ee-? hadrons
- relevance of transverse momentum dependent
(TMD) PDF and FF
Sivers function
Many Workshops in recent years on Transverse
Momentum, spin, and position distributions of
partons in hadrons
33Collins and Sivers angles
Transversity single hadron - 1
- ?C ?h - ?S
-
- ? S ?h - ?S
- ?S azimuthal angle of spin vector of
fragmenting quark (?S p - ?S) - ?h azimuthal angle of hadron momentum
34Transversity single hadron - 2
- first measurements of transverse spin asymmetries
in DIS of high energy - muons on a transversely polarized deuteron target
- published single hadron asymmetries from
2002-2004 runs - Collins related to transverse quark
distributions - Sivers related to intrinsic kT
Phys Rev Lett 94 (2005) 202002 Nucl Phys B765
(2007) 31
35Collins asymmetry for pions and kaons
preliminary 2002-2004 data proton (virtual photon
asymm)
(lepton beam 2002-05 ? DIS07)
final CERN-PH-EP/2008-002hep-ex/0802.2160
(PRL) 2003-2004 data deuteron (virtual photon
asymm)
COMPASS sign convention
36Independent Measurement of the Collins FF
- measurable in ee annihilation
- first attempts to measured it from the
correlation between the azimuthal angles of ps
from ee annihilation using LEP data
last years great news from BELLE
the Collins FF is being measured in ee
annihilation, and it is different from zero!
measurement of the correlation between the
azimuthal angles of ps in the near jet and in
the far jet from ee annihilation
- 547 fb-1 charm corrected data sample,
- UL and UC double ratios
37Collins asymmetries SUMMARY
- The facts
- HERMES has measured on a proton targetnon-zero
Collins asymmetries for p and p- - COMPASS has measured on a deuteron targetCollins
asymmetries compatible with zero - BELLE has produced the first results on Collins
FF - Conclusion
- Collins mechanism is a real phenomenon
- universality of Collins FF
- transversity can be measured in SIDIS
- Present picture
- Collins DTu - DTd DT0D(fav.) -
DT0D(unfav) - To extract TMD DF and FF GLOBAL ANALISYS are
necessary
38HERMES, COMPASS, BELLE
39Sivers asymmetry for pions and kaons
preliminary 2002-2005 data proton
(DIS07)
CERN-PH-EP/2008-002hep-ex/0802.2160
(PRL) 2003-2004 data deuteron
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41Sivers asymmetry
the measured asymmetry on deuteron compatible
with zero has been interpreted as Evidence for
the Absence of Gluon Orbital Angular Momentum in
the Nucleon S.J. Brodsky and S. Gardner, PLB643
(2006) 22
42SUMMARY AND OUTLOOK
- a technically challenging new experiment is IN
OPERATION SINCE 2002
LHC technologies detectors read-out data handling
- a privileged situation at CERN
- MANY PHYSICS RESULTS have been produced
MANY MORE IN THE PIPE-LINE
- COMPASS is foreseen to run up to the end of the
present mid-term plan of CERN (2010)
BIG DISCOVERY POTENTIAL
- with some upgrade COMPASS might be an interesting
option even in the second decade of this century
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44 45 Transversity two hadrons - 1
46Transversity two hadrons - 2
all /- combinations
- precise measurement of few
- systematics seems well under control
- also compatible with zero
- interesting to see proton in 2006
47 48Exclusive ?0 production (2002 data) - 1
49Exclusive ?0 production - 2
ANGULAR DISTRIBUTIONS
preliminary, statistical errors only, limited by
MC
corrected for acceptance, smearing and efficiency
(MCDIPSI gen) background not subtracted
50measurement of r
Exclusive ?0 production - 3
04 00
distribution
Spin density matrix element
T?? ?? are helicity amplitudes
meson photon
51measurement of rand Im r
Exclusive ?0 production - 4
0 4 1-1
3 1-1
distribution
beam polarisation
Spin density matrix element
if SCHC holds
weak violation
52 53F(1860) Pentaquark search - 1
- motivated by NA49 report of pentaquark candidate
- COMPASS has large sample of the double-strange ?
baryon (18000 ?, 11000 ?) from 2002-2003 data - search for ? p resonance
- F(1860) ? ? p ? ?p p ? p ppp
54F(1860) Pentaquark search - 2
Eur Phys J C41 (2005) 469
- compare to yields
- opposite-sign pairs ?(1530)0 ? ? p , 1700
and 920 evts - like-sign pairs evts lt79 and lt89 at 99 CL
- (expected 400)
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58Transversity ? polarization
2002-2003 data
59- Longitudinal polarization
- of ? and anti? in DIS
60Event selection
? POLARIZATION (2002 data) - 1
N(?) N(??)
E665 750 650
NOMAD 8087 649
HERMES1996-2000 10568 1687
COMPASS2002 7919 5062
COMPASS2003 34789 20651
61? POLARIZATION
2002 data
62? POLARIZATION
2002 data