HRIBF NEWS |
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Edition 10, No. 2 | Spring Quarter 2002 | Price: FREE |
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Feature Articles Regular Articles
Editors: C. J. Gross, W. Nazarewicz, and C.-H. Yu
Feature contributors: D. Bardayan, J. R. Beene,
C. J. Gross, B. A. Tatum
Regular contributors: M. R. Lay, M. J. Meigs, P. E. Mueller,
D. W. Stracener, B. A. Tatum, P. Hausladen
Presently, we have a short tank opening to replace bearings and prepare for the neutron-rich RIB campaign originally planned for June-July. However, if we are confident that the KENIS failure mode has been corrected, we will continue the Fluorine RIB campaign and move the neutron-rich runs to July-August. There will be a break for the RIA Summer School when the students will be doing hands-on activities with stable tandem beams.
We have two new members on our PAC: Robert Janssens (Argonne National Laboratory) and Walter Loveland (Oregon State University). They replace Noemie Koller (Rutgers University) and Jim Kolata (Notre Dame University) whom we thank for their service to the facility and the RIB community.
J. Aysto | CERN & University of Jyvaskyla |
C. Baktash | Oak Ridge National Laboratory |
J. C. Hardy (chair) | Texas A&M University |
R. V. F. Janssens | Argonne National Laboratory |
W. Loveland | Oregon State University |
I. Y. Lee | Lawrence Berkeley National Laboratory |
M. Wiescher | Notre Dame University |
We are pleased to announce that the first annual RIA Summer School on Exotic Beam Physics will be held at Oak Ridge National Laboratory from August 12-17, 2002, at the Holifield Radioactive Ion Beam Facility (HRIBF) on the campus of Oak Ridge National Laboratory, Oak Ridge, Tennessee. The aim of the summer school is to nurture future RIA scientists so that the community will have sufficient manpower to effectively use RIA when it comes online. The RIA summer school is jointly organized by the 88-Inch Cyclotron, ATLAS, HRIBF, and NSCL, and will be an annual event, rotating among these laboratories. The summer school will be divided equally between lectures on RIA science in the mornings and "hands-on" experimental demonstrations in the afternoons. The topics of the lectures are given below.
ORIC attained a significant milestone on March 18, 2002, which marked the 40th anniversary of the first circulated beam. On March 17, 1962, the ORIC logbook indicated a cautious optimism that something important was about to happen: Good Operation. Looks very hopeful. Indeed, on March 18, 1962, the first ion beam was circulated in ORIC, approximately 3 years after groundbreaking for building 6000. Specifically the log records that a beam of 8-MeV protons, 65 uA reached extraction radius.
A celebration was held at ORNL to commemorate the occasion and nearly 100 current and former staff members attended. The celebration was dedicated to the memory of Dr. Robert S. (Bob) Livingston who, as Director of the ORNL Electronuclear Division, worked diligently to obtain funding and assure completion of ORIC. Dr. Livingston regrettably passed away just two weeks prior to the celebration. The program included remarks by former ORNL Director Dr. Alvin Weinberg, former Physics Division Director Dr. Jim Ball, and several of the literally hundreds of support personnel, crafts, operators, engineers, and physicists who made the day possible through 40 years of dedicated service to the physics community.
The manufacturer of our original UC targets is no longer able to make these for us, so we initiated a collaboration with a group from the Metals and Ceramics Division at ORNL to manufacture our UC targets in-house. The initial batch of these targets has recently been tested at the UNISOR facility. The finished UC/RVC disks have diameters of 1.5 cm and are 0.2 cm thick, which are the same dimensions as the initial RVC substrates, so no shrinkage occurred during the heating cycles. The density of the newly delivered samples (0.8g/cm3) was lower than that of the original samples (1.2 g/cm3), so the number of disks required to make a RIB production target will increase to 13 compared to the 9 presently used.
Off-line tests involved heating the targets up to 2000 C in a target holder that was coupled to an electron-beam-plasma (EBP) ion source. If the conversion of uranium oxide to uranium carbide is incomplete, oxygen and carbon monoxide will be present at levels that can adversely affect the efficiency of the ion source. Fortunately low levels of O and CO ions were observed and the targets were relatively free of any volatile contaminants.
The yields of several radioactive ions were measured using a low intensity proton beam from the tandem to irradiate the targets. The extracted radioactive ion beam intensities were comparable (+/- 15%) to those previously measured. There were no immediately obvious trends in the yield differences based on radioactive half-life or chemical species, but the analysis is continuing. Based on these results, work on the remainder of the targets has begun. We plan a series of tests varying the uranium content and the thickness of the UC layer to determine the optimum target configuration for various species.
We have also made further tests of the technique for selecting specific beams by adding sulfur vapor to the system (via H2S gas through a variable-rate leak valve) and extracting the desired nucleus as a sulfide molecular ion. This technique has been previously reported for Sn beams. We now have shown that it also works for Ge beams. The yield of the radioactive GeS beam is about 1.8 times higher than the yield of the atomic Ge beam, while the SnS beam intensity is about equal to the Sn beam intensity. In both cases, the neighboring elements are suppressed by at least a factor of 1000 and, in most cases, the extracted beam intensity of these 'contaminant' beams is well below our detection threshold.
ORIC was then utilized to deliver 2-3 uA of 40-MeV deuterons to the KENIS on the RIB injector platform for the production of 17F during the latter portion of February and early March. In mid-March, the ORIC coaxial magnetic extraction channel developed an internal water leak on the insert, and the operation cycle was interrupted for several weeks for diagnosis and repair of the highly activated channel. Following the repairs, ORIC operation resumed with the delivery of 44-MeV deuterons to the RIB injector for 17F production.
Fig. RA2-1 - A drawing to scale of the KENIS showing the positions of the grid and cone which had shorted.
We will perform autopsies on these ion sources to determine the causes of the failures. In addition, the KENIS from last fall will also be examined; it had a very successful run of several hundred hours and successfully completed its expected campaign. We will also reexamine our procedures for ion source assembly.
A new diagnostic station has been commissioned at the zero degree viewport of the RMS first dipole. This viewport directly views the CLARION target position, and in the present implementation, the diagnostic station is equipped with an axial ion chamber, or Bragg-Curve Spectrometer for the purpose of characterizing the isobaric content of RIBs. A photo of the station with the Bragg-Curve Spectrometer installed can be seen in fig. RA3-1.
Fig. RA3-1 - Photograph of the Bragg-Curve Spectrometer as installed behind D1 of the RMS.
Initial testing of the detector was performed with 3-MeV/A 124Sn and 124Te beams. Transmission to the detector and isobaric resolution were characterized in the absence and presence of a 1 mg/cm2 C target at the CLARION target position. Transmission to the detector with the present 1-inch diameter window was 100% without the target and 30% with the target. Isobaric resolution at 3 MeV/A was determined to be roughly one FWHM per Z at Z=50, and the performance with the target present was consistent with the energy loss of the beam in the target. A plot of E vs. dE for a mixed beam of 124Sn and 124Te with the target present can be seen in fig. RA3-2.
Fig. RA3-2 - A spectrum of the energy loss versus total energy of a beam "cocktail" comprised of Sn and Te isotopes with A=124.
The portion of the diagnostic station where the Bragg-Curve spectrometer is mounted can be easily removed to accommodate other detectors as dictated by experimental needs. A scale drawing of the station with the Bragg-Curve Spectrometer removed can be viewed in fig. RA3-3.
Fig. RA3-3 - Scale drawing of station.
The HRIBF Users group is sponsoring a workshop on transfer experiments with RIBs at the HRIBF. The goal of the workshop is to bring together users who are interested in utilizing transfer reactions with RIBs in inverse kinematics with the equipment at the HRIBF. The HRIBF is well equipped to address low-energy transfer reaction studies with three magnetic and/or electrostatic separators, a large collection of silicon strip detectors, as well as other charged particle and heavy ion detectors.
The workshop is chaired by Jolie Cizewski (Rutgers University, cizewski@physics.rutgers.edu) and Ray Kozub (Tennessee Technological University, rkozub@tntech.edu) and locally organized by Jeff Blackmon blackmon@mail.phy.ornl.gov and Felix Liang liang@mail.phy.ornl.gov.
More information, including the tentative program and registration form, may be found at http://www.phy.ornl.gov/workshops/transfer/.
HRIBF welcomes suggestions for future radioactive beam development. Such suggestions may take the form of a Letter of Intent or an e-mail to the Liaison Officer at liaison@mail.phy.ornl.gov. In any case, a brief description of the physics to be addressed with the proposed beam should be included. Of course, any ideas on specific target material, production rates, and/or the chemistry involved are also welcome but not necessary. In many cases, we should have some idea of the scope of the problems involved.
Beam suggestions should be within the relevant facility parameters/capabilities listed below.
Schedules may be found by choosing this link.
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Witek Nazarewicz | Carl J. Gross | Chang-Hong Yu |
Deputy Director for Science | Scientific Liaison | Newsletter Editor |
Mail Stop 6368 | Mail Stop 6371 | Mail Stop 6371 |
witek@mail.phy.ornl.gov | cgross@mail.phy.ornl.gov | chy@mail.phy.ornl.gov |
+1-865-574-4580 | +1-865-576-7698 | +1-865-574-4493 |
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Holifield Radioactive Ion Beam Facility | ||
Oak Ridge National Laboratory | ||
Oak Ridge, Tennessee 37831 USA | ||
Telephone: +1-865-574-4113 | ||
Facsimile: +1-865-574-1268 |