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Physical Program for VEPP2000 e e Collider

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Antiprotons annihilate in. material before drift chamber. Photon-2003. VEPP-2000 Physical Program ... antineutron detector antineutron annihilates in NaI(Tl) ... – PowerPoint PPT presentation

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Title: Physical Program for VEPP2000 e e Collider


1
Physical Program for VEPP-2000 ee- Collider
Sergey Serednyakov
Budker Institute of Nuclear Physics, Novosibirsk
April 11, 2003
  • OUTLINE
  • VEPP-2000 Collider
  • SND and CMD-3 Detectors
  • Physical Program
  • Conclusions

2
VEPP-2000
  • Start of VEPP-2000 project 2000
  • Energy range 2E0.4-2.0 GeV
  • Two collider detectors
  • SND and CMD-3
  • VEPP-2000 parameters
  • perimeter 24.4 m
  • collision time 82 nsec
  • beam current 0.2 A
  • bunch length 3.3 cm
  • energy spread 0.7 MeV
  • ?x? ?z 6.3 cm
  • L ? 1.1032 at 2E2.0 GeV

3
VEPP-2000 View
CMD-3
SND
Refs for VEPP-2000 1. In Proc.Frascati
Phys.Series,v XVI, p.393,Nov.16-19,1999 2. In
Proc. 7-th Europ.Part.Accel.Conf., EPAC 2000,
p.439, Vienna,2000
CMD-3
SND
4
SND Detector
Ref. NIM A449 (2000) 125-139
1 beam pipe, 2 tracking system, 3 aerogel
cherenkov counter, 4 NaI(Tl) counters, 5
vacuum phototriodes, 6 absorber, 7-9 muon
system, 10 s.c focusing solenoids.
5
SND Detector
  • Calorimeter
  • 1680 crystals
  • VPT readout
  • 3 spherical layers
  • 3.5 tons
  • 13.5 X0
  • 90 4?
  • ?? x ??90 x 90

View of DC prototype
NaI Calorimeter
Energy resolution Angular resolution
6
CMD-3
1 beam pipe, 2 drift chamber, 3 BGO, 4
Z chamber, 5 s.c. solenoid, 6 LXe, 7
CSI, 8 yoke , 9 VEPP s.c. solenoid
7
CMD-3
Barrel EMC 5Xo Cs(Tl) 8Xo LXE ?E/E3-5
(0.1-0.9 GeV) ??? 0.2o
DC
?x2.3mm
LXe
? DC ?Z 2mm, charge div. ?r 0.14mm, ???
0.4o, ??? 0.2o
DC
Endcap EMC 13.4Xo BGO ?E/E4-8 (0.1-0.7
GeV) ???,? 1.4o
SC 1.5 Tesla 0.13Xo
8
CMD-3
Refs. for CMD-3 1.V.M.Aulchenko et al, Preprint
BINP 2001-45, Novosibirsk 2. D.Grigoriev in
Proc. Intern. Workshop on ee- Physics at
Intermediate Energy, SLAC, Stanford, 30 Apr.-2
May 2001, p.116-121
BGO
LXe
9
Physical program
1. Precise measurement of the quantity
R?(ee-- gt hadrons)/ ?(ee--gt??--) 2. Study of
hadronic channels ee-- gt 2h, 3h, 4h , h
?,K,?, 3. Study of excited vector mesons ?,
?, ?, ?,.. 4. CVC tests comparison of ee--
gt hadr. (T1) cross section with ?-decay
spectra 5.Study of nucleon-antinucleon
production nucleon electromagnetic
formfactors, search for NNbar resonances,
.. 6. Hadron production in radiative return
(ISR) processes 7. Two photon physics 8. Test of
the QED high order processes 2-gt4,5
10
Contribution of R into muon anomaly
Muon anomaly (g-2)/2? ,(AMM) a?(E821)1.1659203(8
) .10-9 0.7ppm (2002)
a?(hadr)58.8-0.6ppm, (from S.Eidelman)
a?exp-- a?ee- 2.9-0.9 ppm a?exp-- a?? 0.8
-0.9 ppm
Conclusions for VEPP-2000 --
experimental and theoretical accuracy of AMM
reached lt1 ppm accuracy -- VEPP-2000 energy
range lt2.0 GeV gives ?90 of contribution
into a?(hadr) -- new mesaurements with 1-2
accuracy at 2Egt1 GeV and 0.5 at ?(770) are
awaited from CMD-3 and SND at VEPP-2000
Experimental data (from hep-ph/0208177)
11
Contribution of R into fine structure constant at
sM2Z
?em(s0) ? 1/137, Shift ?(sM2Z)/?(0)1-
??(s)exp ? 0.062, ??(s)theor ??lept(s)
??hadr(s) ??top(s),
??hadr(s M2Z) ? 0.0279?0.0004,
?em(sM2Z) ? 1/129
E-W relation
?G F/ G F ?10 -5, ?MZ / MZ ? 2 .10 -5, ???? 4.10
4.
VEPP-2000 region 2E0.4 1.4 GeV --
contribution at MZ ?20. -- uncertainty at MZ
?40.
12
Exclusive channels of ee- annihilation into
hadrons
? ?- ? ?-
? ?-
??0
? ?- ?0
?? ?-
? ?- ?0 ?0
13
ee- annihilation with kaon production
ee- gt K K--
ee- gt KS K ?--
ee- gt KS KL
Total integrated luminosity in the range
2E1.4-2.0 GeV is ?5 /pb.
14
Light vector meson table
Nearly all excitations are within VEPP-2000 range
Table of masses, widths
?(1450) M1465 ?25 ?310? 60, ?(1700) M1700
?20 ?240? 60, ?(2150) M2149 ?17 ?363?
50, ?(1420) M1419 ?31 ?174? 60, ?(1650)
M1649 ?24 ?220? 35, ?(1680) M1680 ?20
?150? 50,
Main decay channels
?(1450) -gt 4? , ??, ???, .. ?(1700) -gt 2?, 4? ,
??, .. ?(1420)-gt 3?, .. ?(1700)-gt ???, .. ?(1680)
-gt KK, KK, ..
Summary for VEPP-2000 with 1 fb-1 the knowledge
of vector excitations can be improved to the
level of knowledge of ?(770), ?(782), ?(1020)
15
CVC tests comparison of ?decay spectra with
ee- cross section
The accuracy of CVC tests for ? -branching
ratios (? -data/ee- data) (S.Eidelman,2002)
Standard model test
??
  • ?? 2.2 ? 1.2
  • ?? ?? 8.4 ? 6.9
  • ?? 3.6 ? 3.6
  • ---
  • total 2.7 ? 1.5
  • IPG 1-- ,
  • -gt2??, 4??, ???,
  • ????

??
Perspectives for VEPP-2000 -- EVEPP gtM ? very
important, -- VEPP-2000 has higher than VEPP-2M
luminosity by 30 times,
16
Hadron producion via radiative return (ISR)
?(783)gt ?0?
ee-gt??-gt?0??, SND, VEPP-2M
?(770)-gt ??-
(??0.067 at ?(4S) )
(??0.088 at ?(4S) )
Estimation for VEPP-2000 ?L?1 fb-1, N? ?107, N?
?106,
ee-gt??-gt ??-?, KLOE, DAFNE
17
N Nbar production cross section
For ee?p pbar
C1 at Tkin. ? 1 MeV
At the threshold we have s4MN2 and GEGM,
if GE GM0.3, then
At s0 GEp(0)1, GEn(0)0, GMp(0)2.79,
GMn(0)-1.79
Radiative correction
For T1Mev e-n0.62 For T50 Mev e-n0.82
18
Experimental data on ppbar and nnbar cross
sections
  • Estimates of statistics at threshold
  • Instant luminosity - 0.1/(nb.sec)
  • Time 107 sec
  • Integrated luminosity - 1/fb
  • Detection efficiency 0.1
  • Number of events 104
  • No radiative corrections applied
  • VEPP-2000 range is shown by green line
  • Curves correspond to GE0.3 and GM0.3
  • Data are mainly from DM2, FENICE
  • There is no data below 10 MeV (kin.en.)
  • The cross section in the maximum is 1 nb
  • The cross section at the threshold is 0.1 nb
  • if GEGM0.3

19
Experimental data on proton and neutron timelike
e.m. formfactor
The goals at VEPP-2000 -- separate measurement
of GM and GE -- check the rise of FF to
threshold -- check the relation GMGE at
threshold
Value
From exp. data r ?1

Models PQCD r0.25 (not supported)
EVDM r1-100 Skyrme r ?1 Accurate
measurement of r is challenge for VEPP-2000
20
Indications on possible resonance structure near
NNbar threshold
?Be-gt6?Be
Diffr.photoproduction, E687, BNl, 2001?
Antineutron-proton cross section
  • Fitting of 6?
  • mass spectrum
  • M 1911 - 4 MeV,
  • 29 - 11 MeV,
  • 62 - 12 deg.
  • Ares/Anres0.31-0.07
  • ?2/ND 1.1
  • ------------------
  • JPCIG 1- - 1

Models 1.vector hybrid ?1.9 GeV, 2.vector
glueballs ?? 2 GeV, 3.NNbar resonance
  • Fitting results
  • M ? 1881 (- 1MeV)
  • ? 4 (- 2MeV)
  • Above threshold !!
  • Isovector (nbar p) !
  • If L0 (S-wave)
  • S(spin)0,1
  • JPC 0- or 1- -
  • If 1- - -gt VEPP-2000

? 3?!
  • Conclusions for VEPP-2000
  • if Nnbar state is above threshold, it could be
  • seen in ee-gtNnbar and in ee-gthadrons cross
    section
  • if below only in ee-gthadron cross section.

21
Typical signature of ppbar and nnbar events in SND
Antineutrons give stars inside calorimeter
Antiprotons annihilate in material before
drift chamber
22
3 options of antineutron detector (based on SND)
1 - SND (as it is) as antineutron detector
antineutron annihilates in NaI(Tl) calorimeter,
which works as antineutron absorber. The
annihilation products are detected in all SND
elements
2 - modified SND (SnD) (n means
antineutron) - first and second NaI layers are
replaced by plastic scintillator with PMT
readout. Annihilation time can be measured,
which allows to suppress background
3 - completely new anti- neutron detector (AnD)
a la FENICE or with KLOE-type calorimeter or
something else. This option is beyond the scope
of the talk.
23
ee-gtp pbar process
Formation of ppbar Coulomb state (antiprotonium)
Collider energy calibration with ee-gtpbar
process at threshold
The ppbar cross section view at the threshold
Typical signature of Ppbar event
E ?2/412.5 KeV, R2/ Mp? 0.6 10 -11cm gtgt 10-13
cm, ??ee ??? Mp?5/63.3 meV, ??t ? 4?ee
, ?03??2 BeeBf 10-27cm2, ?vis ?0 ?t/ ?E, ?E ?
0.5 MeV, ?vis ? 30 pb for E Mp ,
Conclusions for VEPP-2000 The cross section
at the threshold is 50 pb with radiative
correction If L0.1/(nb s), t105sec (1 day),
?0.3, then we have NL t ? 150 events/day ?10
accuracy, Estimated calibration accuracy is ?
10-4
For comparison ?(ee-gt?? ) ? 25 nb, Then S/N ?
7.5 pb/25 nb ?1/3000 !
Conclusions antiprotonium doesnt give visible
contribution in ee- cross section
24
Two photon physics at 2Elt2.0 GeV
ee- gt ?'(958)ee-, ? ? 10-34 cm2 ee- gt
a0(980)ee-, f0(980)ee-, ? ? 10-35 cm2
ee- gt f2 -gt ?0?0 -gt 4?, ee- gt a2-gt ??0 -gt 4?,
? ? 10-36 cm2
ee- gt ?0?0 ee-, ? ? 10-35 cm2?
Main goals for VEPP-2000 -- ? 2? widths of
scalars a0(980), f0(980) ? 0.3KeV seems too
low, -- ? ?-gt ?0?0 at 2E?0.5 GeV
25
High order QED tests (2-gt4,5)
  • only electrons and/or photons in final state
  • large angles ??gt1/? between initial and/or final
    particles

ee-gtee-??
ee-gt?????
ee-gtee-ee-
For processes 2-gt4 ? ? 10-34 - 10-35 cm2 , N ?
104 ev.
The goals -- test of high order QED, physical
background e.g. ??0 -gt5?
26
Schedule
VEPP-2000 -- beam -- 2004
-- luminosity -- 2005
-- running -- 2005--2010
SND -- upgrade -- 2004
-- running --
2005--2010 -- physical results --
2006 -2012
CMD-3 -- end of construction -- 2005
-- running --
2005--2010 -- physical results
-- 2006 -2012
27
Conclusions
1. VEPP-2000 ee- collider with 2E0.4 -- 2.0
Gev energy range and maximum luminosity
Lmax1032 cm-2s-1 is under construction in
Novosibirsk
2. Two collider detectors CMD-3 and SND are being
upgraded for experiments at VEPP-2000 with
integrated luminosity of ?L ? 3 fb 1 in
2005-2010.
3. The measurements of the quantity R?(ee-- gt
hadrons)/ ?(ee--gt??--) with ultimate
precision is one of the main goals of experiments
at VEPP-2000
4. The precision measurements of exclusive
channels of ee-- gt hadrons process for
check such known models as VDM, CVC, QCD, is
important task of physical program.
5. Measurements of ee- -gtn nbar and ee- -gtp
pbar cross sections give unique possibility
to obtain nucleon timelike formfactors at
threshold
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