shape of hadrons athens 27.-29. april 2006 real photon experiments m. kotulla e2/m1 @ mami and legs...
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![Page 1: Shape of Hadrons Athens 27.-29. April 2006 Real Photon Experiments M. Kotulla E2/M1 @ MAMI and LEGS magnetic dipole moment of the](https://reader035.vdocuments.site/reader035/viewer/2022081520/5697bf861a28abf838c882fd/html5/thumbnails/1.jpg)
Shape of Hadrons Athens 27.-29. April 2006
Real Photon Experiments
M. Kotulla
E2/M1 @ MAMI and LEGSmagnetic dipole moment of the
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Nucleon Structure
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first excited State
1 2 3 2
E / M eV
9 3 8
´
pro to n
precise electro- and photoproduction data: magnetic dipole transition M1
electric quadrupole transition E2
Coulomb quadrupole transition C2
incoming photon: M1, E2, C2
outgoing pion: 2/31
2/31
2/31 CEM
N transition intrinsic
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methods:
isospin decomposition:
most sensitive:shape of angular distributionbeam asymmetry at 90° E1+ M1+
multipol analysis, dispersion relation
np pp 0
2/31
2/31
M
EREM
||
||
12A
CREM
REM Extraction
)(cos)cos()( 2
||/||/||/||/
CBAk
q
d
d
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DAPHNE @ MAMI
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TAPS @ MAMI
6 62, 1 138 detectors with individualveto detector, solid angle: ~0.40 4 sr
MAMI 1999-2000 100cm
beam
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LEGS setup
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Photon Asymmetry
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Differential Cross Sections
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Comparison LEGS - MAMI
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P33 Partial Waves (MAMI)
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MAMI Results:
DAPHNE measurement:C||/(12A||) dispersion relation analysismultiplol ana (S,P waves + Born)
LEGS Results:
multipol analysis (up to F waves + Born)
)%2.01.05.2( sysstatEMR 2)003.0085.0( fmQN
NN )03.046.3(
)%24.026.007.3( syssysstatEMR
2)034.0009.0108.0( fmQN
NN )085.0019.0642.3(
228.0 fmQd
R. Beck et al., PRC 61 031204 (2000) G. Blanpied et al., PRC 64 025203 (2001)
REM
for comparison:deuteron
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The Beamline
LH2CB (inside 2MWPCs, PID)TAPS beam
production runs 22.6.2004-4.4.2005
CB:672 NaI(Tl)
covers 20° - 160°
TAPS:510 BaF2
covers 1° - 20°
)GeV(E
%.E
E
%.)GeV(E
%.E
E
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Photon Asymmery
15% of total statistics
Photon Asymmetry :
@400MeV:
CBT =0.619 0.015
Leukel =0.592 0.036
pp
cosp)(dd
),(dd
@420MeV:
CBT =0.632 0.015
Leukel =0.591 0.033
E. Downie preliminary
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Magnetic Moment
p p
´
measurement: excitation of the + and
identification of the ´p state
reaction description necessary
1 2 3 2
E / M eV
9 3 8
´
pro to n
M1, (E2), M3 ´transition
p
p´
p p
´
basic principle
resonance: isolated excited state of the nucleon
lifetime ~ 20-23 s
Pn
p Q;2
3
pp '0
M.Kotulla et al., PRL 89, 272001 (2002)
PDG2004 = (2.7 2.2 3)N
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Reaction DescriptionPascalutsa, Vanderhaeghen PRL 94 102003 (2005)M. Kotulla et al., PRL 89, 272001 (2002)
''
1
dE
dER
Recent progress:
chiral effective field theory ansatzV. Pascalutsa, M. Vanderhaeghen PRL 94 102003 (2005)
systematic ansatz (NLO)error estimation
rescattering: MDM acquires real and imaginary part
pp '0
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(1232) MDM cross sections:
angular distribution of ´
comparison:pioneering experiment
(TAPS1999) = (2.7 2.2 3)
M.K. et al., PRL 89, 272001 (2002)
preliminary Crystal Ball / TAPS data
much higher precision
new Crystal Ball / TAPS Data
(1232) MDM experiment:
p ´p
exclusive measurement
kinematical overdetermination
identification checks
preliminary
B. Boillat
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new Crystal Ball / TAPS Data
checks:
photon beam asymmetry
p
meson
p
´
p
ppp
ppp 0
pp /0
E. Downie
=0.619 0.015
S. Schumann
preliminary
preliminary
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Summary
magnetic moment
pioneering experiment TAPS@MAMI1999 (proof of principle)
new (CB/TAPS) measurement is currently being analyzedmuch higher precision
reaction calculation (systematic ansatz):chiral effective field theory
Outlook: experiment feasible
S11+(1535): p ´p
S110(1535): n ´n(LD2 target)
Nsys )35.17.2( 0.13.1
N REM: precise data from MAMI and LEGS
very good agreement in photon asymmetryslight deviation in (differential) cross sections
)%2.01.05.2( sysstatEMR
)%24.026.007.3( syssysstatEMR