55 research outputs found
Energy Calibration of the JLab Bremsstrahlung Tagging System
In this report, we present the energy calibration of the Hall B
bremsstrahlung tagging system at the Thomas Jefferson National Accelerator
Facility. The calibration was performed using a magnetic pair spectrometer. The
tagged photon energy spectrum was measured in coincidence with pairs
as a function of the pair spectrometer magnetic field. Taking advantage of the
internal linearity of the pair spectrometer, the energy of the tagging system
was calibrated at the level of . The absolute energy scale
was determined using the rate measurements close to the end-point of
the photon spectrum. The energy variations across the full tagging range were
found to be MeV.Comment: 15 pages, 12 figure
A New Measurement of the Radiative Decay Width
High precision measurements of the differential cross sections for
photoproduction at forward angles for two nuclei, C and Pb, have
been performed for incident photon energies of 4.9 - 5.5 GeV to extract the
decay width. The experiment was done at Jefferson
Lab using the Hall B photon tagger and a high-resolution multichannel
calorimeter. The decay width was extracted by
fitting the measured cross sections using recently updated theoretical models
for the process. The resulting value for the decay width is . With the 2.8% total uncertainty, this result is a factor of 2.5 more
precise than the current PDG average of this fundamental quantity and it is
consistent with current theoretical predictions.Comment: 4 pages, 5 figure
Search for pentaquark in high statistics measurement of at CLAS
The exclusive reaction was studied in the
photon energy range between 1.6-3.8 GeV searching for evidence of the exotic
baryon . The decay to requires the assignment of
strangeness to any observed resonance. Data were collected with the CLAS
detector at the Thomas Jefferson National Accelerator Facility corresponding to
an integrated luminosity of 70 . No evidence for the
pentaquark was found. Upper limits were set on the production cross section as
function of center-of-mass angle and mass. The 95% CL upper limit on the
total cross section for a narrow resonance at 1540 MeV was found to be 0.8 nb.Comment: Submitted to Physical Review Letter
Search for the pentaquark in the reaction
A search for the \thp in the reaction was completed
using the CLAS detector at Jefferson Lab. A study of the same reaction,
published earlier, reported the observation of a narrow \thp resonance. The
present experiment, with more than 30 times the integrated luminosity of our
earlier measurement, does not show any evidence for a narrow pentaquark
resonance. The angle-integrated upper limit on \thp production in the mass
range of 1.52 to 1.56 GeV/c for the reaction is
0.3 nb (95% CL). This upper limit depends on assumptions made for the mass and
angular distribution of \thp production. Using \lamstar production as an
empirical measure of rescattering in the deuteron, the cross section upper
limit for the elementary reaction is estimated to be
a factor of 10 higher, {\it i.e.}, nb (95% CL).Comment: 5 figures, submitted to PRL, revised for referee comment
First measurement of direct photoproduction on the proton
We report on the results of the first measurement of exclusive
meson photoproduction on protons for GeV and GeV. Data were collected with the CLAS detector at the Thomas
Jefferson National Accelerator Facility. The resonance was detected via its
decay in the channel by performing a partial wave analysis of the
reaction . Clear evidence of the meson
was found in the interference between and waves at GeV. The -wave differential cross section integrated in the mass range of
the was found to be a factor of 50 smaller than the cross section
for the meson. This is the first time the meson has been
measured in a photoproduction experiment
Nuclear Targets for a Precision Measurement of the Neutral Pion Radiative Width
A technique is presented for precision measurements of the area densities,
density * T, of approximately 5% radiation length carbon and 208Pb targets used
in an experiment at Jefferson Laboratory to measure the neutral pion radiative
width. The precision obtained in the area density for the carbon target is +/-
0.050%, and that obtained for the lead target through an x-ray attenuation
technique is +/- 0.43%
Measurement of the J/ photoproduction cross section over the full near-threshold kinematic region
We report the total and differential cross sections for
photoproduction with the large acceptance GlueX spectrometer for photon beam
energies from the threshold at 8.2~GeV up to 11.44~GeV and over the full
kinematic range of momentum transfer squared, . Such coverage facilitates
the extrapolation of the differential cross sections to the forward ()
point beyond the physical region. The forward cross section is used by many
theoretical models and plays an important role in understanding
photoproduction and its relation to the proton interaction. These
measurements of photoproduction near threshold are also crucial inputs
to theoretical models that are used to study important aspects of the gluon
structure of the proton, such as the gluon Generalized Parton Distribution
(GPD) of the proton, the mass radius of the proton, and the trace anomaly
contribution to the proton mass. We observe possible structures in the total
cross section energy dependence and find evidence for contributions beyond
gluon exchange in the differential cross section close to threshold, both of
which are consistent with contributions from open-charm intermediate states.Comment: 15 pages 18 figure
Search for the pentaquark in the reactions and
The exclusive reactions and have been studied in the photon energy range 1.6--3.8 GeV, searching
for evidence of the exotic baryon in the decays and . Data were collected with the CLAS detector at
the Thomas Jefferson National Accelerator Facility. The integrated luminosity
was about 70 pb. The reactions have been isolated by detecting the
and proton directly, the neutral kaon via its decay to
and the neutron or neutral kaon via the missing mass technique. The mass and
width of known hyperons such as , and were
used as a check of the mass determination accuracy and experimental resolution.
Approximately 100,000 's and 150,000 's were observed in
the and final state respectively. No evidence
for the pentaquark was found in the or invariant mass
spectra. Upper limits were set on the production cross section of the reaction
as functions of center-of-mass angle,
and masses. Combining the results of the two reactions, the 95% C.L.
upper limit on the total cross section for a resonance peaked at 1540 MeV was
found to be 0.7 nb. Within most of the available theoretical models, this
corresponds to an upper limit on the width, ,
ranging between 0.01 and 7 MeV.Comment: 1 tex file (16 pages) + 23 figures (25 eps files
Beam asymmetry ÎŁ for the photoproduction of η and ηâČ mesons at EÎł = 8.8GeV
We report on the measurement of the beam asymmetry
ÎŁ
for the reactions
â
Îł
p
â
p
η
and
â
Îł
p
â
p
η
âČ
from the GlueX experiment using an 8.2â8.8-GeV linearly polarized tagged photon beam incident on a liquid hydrogen target in Hall D at Jefferson Laboratory. These measurements are made as a function of momentum transfer
â
t
with significantly higher statistical precision than our earlier
η
measurements and are the first measurements of
η
âČ
in this energy range. We compare the results to theoretical predictions based on
t
-channel quasiparticle exchange. We also compare the ratio of
ÎŁ
η
to
ÎŁ
η
âČ
to these models as this ratio is predicted to be sensitive to the amount of
s
ÂŻ
s
exchange in the production. We find that photoproduction of both
η
and
η
âČ
is dominated by natural parity exchange with little dependence on
â
t
- âŠ