Measurement of the G double-polarisation observable in positive pion photoproduction
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Abstract
Establishing the resonance spectrum of the nucleon with accuracy would
provide important new information about the dynamics and degrees of freedom
of its constituents. The spectrum and properties of nucleon resonances are a
fundamental test of the emerging predictions from Lattice QCD calculations
and will guide re finements to QCD-based phenomenological models. Pion
photoproduction is an excellent tool to study the nucleon resonance spectrum,
as this channel is expected to couple strongly to most resonances. The new
generation of measurements for this reaction, of which the measurement presented
in this thesis forms a crucial part, will provide a great improvement in the quality
of available experimental data. For the photoproduction process in particular, the
use of photon beams and targets with high degrees of polarisation, coupled with
large acceptance particle detectors is essential for disentangling the spectrum of
excited states.
There are many nucleon resonances predicted by recent Lattice QCD calculations
and by phenomenological nucleon models which are only observed
inconsistently by different analyses of the same experimental data or which
are not observed at all. It is of upmost importance to establish if this means
that the resonances do not exist in nature, reflecting inappropriate degrees of
freedom in the theoretical description of the nucleon or if the current experimental
measurements have not been sensitive enough. As such, there is a current
world effort at modern tagged photon facilities to measure the \complete set" of
photoproduction observables necessary to fully constrain the partial wave analyses
used to extract the experimental excitation spectrum from the data.
This thesis will present the first detailed measurement to date of positive pion
photoproduction in the 730-2300 MeV photon energy (1400-2280 MeV centre-of-mass
energy) region with a linearly polarised photon beam and a longitudinally polarised proton target with a close-to-complete angular coverage in detection
of the reaction products. This unique set up allows for the extraction of
the double-polarisation observable, G. The data were taken as part of the g9
experiment at the Thomas Jefferson National Accelerator Facility in Virginia,
using a tagged, polarised photon beam and the Frozen Proton Spin Target,
FROST, in conjunction with the CEBAF Large Acceptance Spectrometer, CLAS.
The results of the study presented here are compared to the sparse existing
data set for the G double-polarisation observable along with the current solutions
of the the three main partial wave analyses: MAID, SAID and Bonn-Gatchina.
Some agreement is obtained with the expectations of these PWA at lower energies,
while disagreement at higher energies is clearly evident. This is the energy region
where many of the missing resonances are expected to lie. Once incorporated
into the MAID, SAID and Bonn-Gatchina models, these new data will provide
an important contribution to constraining the amplitudes and therefore the
resonance spectrum and properties of the nucleon. The new data will form a
central part of the world effort to accurately establish the nucleon excitation
spectrum for the first time by achieving the first complete measurement of
experimental observables in meson photoproduction.
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