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The pp→pp 0 0 reaction and its limiting case, the fusion to quasibound , in search of ABC effect. T. Skorodko, University Tuebingen for CELSIUS-WASA. ► motivation and detector setup ► results and discussions ► summary and outlook. ABC effect. WASA-at-COSY. M=2360 MeV. - PowerPoint PPT Presentation
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The pp→pp00 reaction and its limiting case,
the fusion to quasibound ,
in search of ABC effect
T. Skorodko, University Tuebingen
for CELSIUS-WASA
► motivation and detector setup
► results and discussions
► summary and outlook
He2
ABC effect
M=2360 MeV
=90 MeV
(t-channel)
Roper
pre
limin
ary
WASA-at-COSY
“ABC” effect in ANKE data
pp→{pp}SX
selection:
Epp < 3 MeV,
cosθpp > 0.95
1.1 GeV
0.8 GeV
2 GeV
1.4 GeV
S.Dymov et al., PRL 102, 192301 (2009)
phase space
“ABC” effect in ANKE datapp→{pp}SX
selection: Epp < 3 MeV, cosθpp > 0.95
1100 MeV 1400 MeV
• final {pp} in
• asume S-wave in
initial protons in or
01S
01S
21D
only S-wave amplitude
only D-wave amplitude
S- and D-wave amplitudes
S.Dymov et al., PRL 102, 192301 (2009)
Mx [GeV/c2]
Oservation of an “ABC” effect in proton-proton collisions
pp→{pp}SX
S.Dymov et al., PRL 102, 192301 (2009)
“If ABC is not a resonance, it does not have to have a definite isospin …”
“… pp→{pp}SX kinematics are very similar to those of pn→d00 and
so a comparison with CELSIUS-WASA data is instructive”
“… we certainly have no evidence for an I=1 dibaryon …”
“… pp→{pp}SX kinematics are very similar to those of pn→d00 and
so a comparison with CELSIUS-WASA data is instructive”
pp→pp00 at 4 CELSIUS-WASA detector
Tp = 775, 895, 1000, 1100, 1200, 1300, 1360 MeV
p
pγ γ
γ
γ
production
CELSIUS-WASA
N* →N
N* →
L.Alvarez-Ruso et al., Nucl. Phys. A 633 (1998), 519L.Alvarez-Ruso et al., Nucl. Phys. A 633 (1998), 519
N* →N
N* →
00 production at Tp < 1 GeV
Valencia model A(tot) A(N*→N)+A(N*→)Tp=0.795 GeV COSY-TOF
1)(00*
0*
NN
NR
(PDG) 4)(00*
0*
NN
NR
At Roper mass M=1440 MeV
Tp=0.895 GeVAll theoretical curves are normalized in area to the data
00 production at Tp > 1 GeV
VC with readjusted N→ branch
Tp = 1 GeV Tp = 1.1 GeV Tp = 1.2 GeV Tp = 1.3 GeV
00 production at Tp > 1 GeV
VC with readjusted N*→ branch
VC with readjusted total N* strength (T. Skorodko et al., Phys.Lett. B 679 (2009) 30)
Tp = 1 GeV Tp = 1.1 GeV Tp = 1.2 GeV Tp = 1.3 GeV
00 production at Tp > 1 GeV
modification of the excitation
include relativistic corrections
reduce the contribution from ρ-exchange in excitation by an order of magnitude (Xu Cao et al., nucl-th:1004.0140, today plenary session)
00 production at Tp > 1 GeV
VC with readjusted N→ branch
VC with readjusted total N* strength
VC with readjusted total N* strength and with modified excitation
Tp = 1 GeV Tp = 1.1 GeV Tp = 1.2 GeV Tp = 1.3 GeV
Total pp→pp00 cross section
VC with readjusted total N* strength and with modified excitation
original VC
VC with readjusted
N→ branch
VC with readjusted
total N* strength
Comparison ANKE data with modified VC
VC with readjusted total N* strength and with modified excitation (ANKE cuts)
CELSIUS-WASA data with Mpp < 10 MeV cut
VC with readjusted total N* strength and with modified excitation (Mpp < 10 MeV cut)
Conclusions
pp00 production can be described by a conventional t-channel calculations with small contribution from ρ-exchange
no evidence is found for a significant ABC effect (no low mass enhancement in M)
since pp00 is isospin I=1 channel, it is not instructive to compare these data with isospin I=0 pn→d00 data
Outlook
pn→pn00
p+(nps) at Tp=1.0 GeV
p+(nps) at Tp=1.2 GeV
Tp Tp
ABC
WASA-at-COSY
Thank you