Back to Search Start Over

Electroexcitation of the Roper resonance for1.7<Q2<4.5GeV2ine→p→enπ+

Authors :
B. Zhao
F. W. Hersman
Marco Ripani
S. Dhamija
R. W. Gothe
K. Y. Kim
J. Kuhn
J. P. Santoro
E. De Sanctis
Latifa Elouadrhiri
B. M. Preedom
P. Eugenio
R. C. Minehart
Kei Moriya
D. I. Sober
M. Taiuti
G. Rosner
C. A. Meyer
M. Battaglieri
G. V. Fedotov
P. Collins
J. J. Melone
Lorenzo Zana
R. Bradford
K. Lukashin
J. Shaw
V. Batourine
D. P. Weygand
H. Hakobyan
Friedrich Klein
H. S. Jo
Michael Wood
K. Hafidi
Brian Raue
Gerald Feldman
Elton Smith
R. Fatemi
V. S. Serov
A. V. Vlassov
T. Lee
M. Anghinolfi
P. Coltharp
James Mueller
I. I. Strakovsky
N. A. Baltzell
R. De Vita
P. D. Rubin
A. Cazes
Maryam Moteabbed
C. Salgado
Bernhard Mecking
Y. G. Sharabian
A. Deur
K. A. Griffioen
K. S. Egiyan
K. V. Dharmawardane
Baile Zhang
Alexei V. Klimenko
S. Anefalos Pereira
Z. Krahn
W. K. Brooks
Shifeng Chen
J. D. Kellie
Y. Prok
N. Hassall
M. Bellis
J. Langheinrich
Barry Ritchie
N. Baillie
P. Mattione
M. S. Saini
L. C. Dennis
B. E. Bonner
S. S. Stepanyan
S. A. Philips
R. A. Miskimen
B. McKinnon
H. Avakian
J. T. Goetz
E. Polli
B. L. Berman
D. Sharov
M. Mirazita
D. Branford
K. Livingston
D. S. Dale
Ji Li
L. M. Qin
J. M. Laget
H. Denizli
N. Gevorgyan
C. Paterson
G. Gavalian
W. J. Briscoe
E. Pasyuk
S. Tkachenko
M. D. Mestayer
S. A. Dytman
J. Donnelly
G. Asryan
A. V. Skabelin
N. Benmouna
Gerard Gilfoyle
O. P. Dzyubak
R. A. Niyazov
E. L. Isupov
A. Fradi
D. Sokhan
M. Guillo
V. Crede
Michael L. Williams
W. Gohn
N. Markov
V. Sapunenko
Dinko Pocanic
J. R. Calarco
P. Corvisiero
E. Golovatch
S. Boiarinov
S. E. Kuhn
Charles Hyde
V. P. Kubarovsky
O. Pogorelko
C. Tur
M. J. Amaryan
M. MacCormick
I. Hleiqawi
R. Nasseripour
S. L. Careccia
S. McAleer
F. X. Girod
Laird Kramer
B. E. Stokes
G. S. Adams
J. P. Cummings
Cynthia Marie Hadjidakis
G. E. Dodge
H. Y. Lu
K. L. Giovanetti
L. Blaszczyk
P. V. Degtyarenko
M. Kossov
V. Gyurjyan
K. Joo
I. Popa
Sergey Kuleshov
M. Bektasoglu
Michael Dugger
D. Heddle
M. Nozar
P. Stoler
I. Niculescu
D. Lawrence
J. Zhang
R. De Masi
D. Schott
S. A. Morrow
C. Djalali
R. A. Schumacher
M. Guidal
Larry Weinstein
K. Hicks
M. Holtrop
L. Graham
H. Bagdasaryan
C. I O Gordon
P. Ambrozewicz
S. Bültmann
L. Morand
T. A. Forest
S. Stepanyan
J. Pierce
Avraham Klein
K. Mikhailov
L. Cheng
Nikolay Shvedunov
A. I. Ostrovidov
L. Casey
A. C S Lima
K. Park
N. Kalantarians
B. B. Niczyporuk
D. G. Ireland
Michael Vineyard
N. Pivnyuk
Giovanni Ricco
Atilla Gonenc
E. Wolin
Volker D. Burkert
A. S. Biselli
J. P. Ball
D. S. Carman
D. G. Crabb
J. Salamanca
J. W C McNabb
M. Yurov
J. W. Price
S. Mehrabyan
C. Bookwalter
G. Riccardi
H. Funsten
P. Nadel-Turonski
C. Butuceanu
Tsutomu Mibe
N. Dashyan
K. Hafnaoui
C. Hanretty
G. V. O'Rielly
J. R. Johnstone
Z. W. Zhao
D. Keller
Paolo Rossi
D. G. Jenkins
J. Lachniet
A. Tkabladze
S. Park
Sylvain Bouchigny
D. Rowntree
M. M. Ito
R. S. Hakobyan
L. El Fassi
M. Khandaker
H. G. Juengst
A.V. Stavinsky
D. J. Tedeschi
V. Mokeev
I. Bedlinskiy
L. C. Smith
E. Munevar
B. S. Ishkhanov
M. R. Niroula
V. Kuznetsov
S. Strauch
R. Suleiman
L. Guo
G. S. Mutchler
M. Ungaro
S. Niccolai
J. Hardie
D. Doughty
W. Kim
D. P. Watts
G. Niculescu
J. Yun
D. Cords
H. Egiyan
T. Takeuchi
A. Yegneswaran
M. Osipenko
F. Sabatié
Kalvir S. Dhuga
M. Y. Gabrielyan
R. Dickson
R. J. Feuerbach
N. Guler
Inna Aznauryan
P. L. Cole
S. Barrow
L. Todor
D. Protopopescu
S. Pozdniakov
M. Garçon
Y. Ilieva
B. Moreno
Source :
Physical Review C. 78
Publication Year :
2008
Publisher :
American Physical Society (APS), 2008.

Abstract

The helicity amplitudes of the electroexcitation of the Roper resonance are extracted for $1.7l{Q}^{2}l4.5\phantom{\rule{0.3em}{0ex}}{\mathrm{GeV}}^{2}$ from recent high precision JLab-CLAS cross section and longitudinally polarized beam asymmetry data for ${\ensuremath{\pi}}^{+}$ electroproduction on protons at $W=1.15\ensuremath{-}1.69$ GeV. The analysis is made using two approaches, dispersion relations and a unitary isobar model, which give consistent ${Q}^{2}$ behavior of the helicity amplitudes for the ${\ensuremath{\gamma}}^{*}p\ensuremath{\rightarrow}$N(1440)P${}_{11}$ transition. It is found that the transverse helicity amplitude ${A}_{1/2}$, which is large and negative at ${Q}^{2}=0$, becomes large and positive at ${Q}^{2}\ensuremath{\simeq}2\phantom{\rule{0.3em}{0ex}}{\mathrm{GeV}}^{2}$, and then drops slowly with ${Q}^{2}$. The longitudinal helicity amplitude ${S}_{1/2}$, which was previously found from CLAS $\stackrel{\ensuremath{\rightarrow}}{e}p\ensuremath{\rightarrow}\mathit{ep}{\ensuremath{\pi}}^{0},\mathit{en}{\ensuremath{\pi}}^{+}$ data to be large and positive at ${Q}^{2}=0.4,0.65\phantom{\rule{0.3em}{0ex}}{\mathrm{GeV}}^{2}$, drops with ${Q}^{2}$. Available model predictions for ${\ensuremath{\gamma}}^{*}p\ensuremath{\rightarrow}$N(1440)P${}_{11}$ allow us to conclude that these results provide strong evidence in favor of N(1440)P${}_{11}$ as a first radial excitation of the $3q$ ground state. The results of the present paper also confirm the conclusion of our previous analysis for ${Q}^{2}l1$ GeV${}^{2}$ that the presentation of N(1440)P${}_{11}$ as a q$^{3}\mathrm{G}$ hybrid state is ruled out.

Details

ISSN :
1089490X and 05562813
Volume :
78
Database :
OpenAIRE
Journal :
Physical Review C
Accession number :
edsair.doi...........e3f4727514f20fb31b5753961e00a552