Title: HIGHLIGHTS%20FROM%20THE%20COMPASS%20EXPERIMENT%20@%20CERN
1HIGHLIGHTS FROM THE COMPASSEXPERIMENT _at_ CERN
- F. Bradamante
- University of Trieste and INFN Trieste
- on behalf of the
Collaboration - WE Heraeus Seminar on Polarized Antiprotons
- Bad Honneff, June 23-25, 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
7the target system
solid state target operated in frozen spin mode
2002-2004 6LiD (polarised deuteron)
dilution factor f 0.38 polarization PT
50 two 60 cm long cells with opposite
polarisation (systematics)
- 2006
- PTM replaced with the large acceptance COMPASS
magnet (180 mrad) - 2 target cells ? 3 target cells
2007 NH3 (polarised protons) dilution factor
f 0.14 polarization PT 90
during data taking with transverse
polarisation, polarisation reversal in the cells
after 4-5 days
8WHERE 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
9THE COMPASS MUON PROGRAM
- TWO CLASSES OF PHENOMENA
- LONGITUDINAL SPIN CASE
- TRANSVERSE SPIN CASE
10LONGITUDINAL SPIN CASE the beginning
EMC 1988
G1p 0.123 ? 0.013 ? 0.019 DS 0.12 ? 0.17
? SPIN CRISIS
11LONGITUDINAL 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
12A1d from COMPASS
- Inclusive DIS asymmetry Q2gt1 (GeV/c)2
PLB 647(2007)8
- good agreement with previous experiments
- significantly improved statistics at low x !
13COMPASS QCD fit
using these results plus the same
asymmetries on p and n from the other
experiments
14LONGITUDINAL SPIN CASE
- direct measurement of
- ?G/G
- main objective of the
- longitudinal run
15MEASUREMENTS 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
16DG/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
17 18D mass spectra
APS, 13 April 2008
G.K. Mallot
18
19DG/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
19
20- ?G/G
- from High-pt hadron pairs
21?G/G from High-pt hadrons, Q2 gt 1 (GeV/c)2
22?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
23?G/G from High-pt hadrons
all Q2
low Q2
resolved photon
24?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
25Gluon 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
26Summary of results
new high-pT point
new charm point
G.K. Mallot
27CONCLUSION from ?G MEASUREMENTS
?G SMALL
more precise measurements will come soon
COMPASS 2006 RHIC RUN6 .
interest in orbital angular momentum GPDs
Jis SUM RULE
28 29Transverse Spin case
- Large effects observed in hadronic interactions
30Transverse 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
31Collins 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
32Transversity 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
33Collins 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
34Independent 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
35Collins 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
36HERMES, COMPASS, BELLE
37Sivers asymmetry for pions and kaons
preliminary 2002-2005 data proton
(DIS07)
CERN-PH-EP/2008-002hep-ex/0802.2160
(PRL) 2003-2004 data deuteron
38(No Transcript)
39conclusions from COMPASS deuteron data
- the unpolarised azimuthal asymmetries are
different from zero and different for positive
and negative hadrons
- all the transverse spin asymmetries have been
measured to be compatible with zero
HERMES, COMPASS, BELLE data consistent
picture first fits, extractions of the new
DFs, and predictions for other experiments
- still, a lot of expectation for the higher energy
COMPASS proton data
402007 Transverse data statistics
- 2007 run May to November equally
shared between transverse and longitudinal - Transverse polarization
- data taking
Period Weeks Target Polarization
1 25 / 26 - - / -
2 27 / 28 - - / -
3 30 / 31 - / - -
4 39 / 40 - / - -
5 41 / 42a - - / -
6 42b / 43 - / - -
Period Weeks Target Polarization
1 25 / 26 - - / -
2 27 / 28 - - / -
3 30 / 31 - / - -
4 39 / 40 - / - -
5 41 / 42a - - / -
6 42b / 43 - / - -
Data used for these results
- several stability tests have been performed
- detectors and triggers performances
- event reconstruction
- K0 reconstruction
- distributions of kinematical variables
- ( zvtx, Em, fm, xBj Q2,y, W, Ehad, fhadLab ,
qhadLab , fhadGNS , qhadGNS , pt)
20 of the total collected data has been used
for this analysis
41Collins asymmetry proton data
integrated over x and z
statistical errors only systematic errors 0.3
sstat
at small x, the asymmetries are compatible with
zero in the valence region the asymmetries are
different from zero, of opposite sign for
positive and negative hadrons, and have the
same strength and sign as HERMES
42Collins asymmetry proton data
comparison with M. Anselmino et al. predictions
43Sivers asymmetry proton data
integrated over x and z
statistical errors only systematic errors 0.5
sstat
the measured symmetries are small, compatible
with zero
44Sivers asymmetry proton data
comparison with the most recent predictions from
M. Anselmino et al.
arXiv0805.2677
45Results Sivers asymmetry
comparison with predictions from
S.Arnold, A.V.Efremov, K.Goeke, M.Schlegel and
P.Schweitzer, arXiv0805.2137
46conclusions
- COMPASS preliminary results on
- unpolarised hadron asymmetries on deuteron for
positive and negative hadrons - Collins and Sivers asymmetries on protons
- Collins asymmetry different from zero the
effect is there at COMPASS energies - Sivers asymmetry smaller, compatible with zero
to be understood
near future analysis of the whole 2007 proton
data sample
longer term transverse spin physics is one of
the items being spelled out for the future
COMPASS program the study of transverse spin
effects needs further precise measurements and
the COMPASS facility is the only place where
SIDIS can be measured at high energy