HRIBF NEWS |
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Edition 7, No. 5 | Fall Quarter 1999 | Price: FREE |
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Feature ArticlesRegular Articles
- 1. Update of RIB Delivery Plans
- 2. Recent HRIBF Research - Breakup of Weakly Bound 17F at 10 MeV/A
- 3. Recent HRIBF Research - Shell Model Monte Carlo Calculations in Nuclear Structure and Astrophysics
- 4. SNEAP and Proton-emitting Nuclei Conferences Held in East Tennessee
- 5. Witek Nazarewicz Appointed HRIBF Deputy Director for Science
- 6. Three New PAC Members Appointed
- RA1 - RIB Development
- RA2 - Accelerator Systems Status
- RA3 - Experimental Equipment - CLARION
- RA4 - Users Group Election Results Presented at Annual Meeting
- RA5 - Experiments, Spokespersons, and Dates Run During the Past Quarter
Editor: Carl J. Gross
Feature contributors: J. C. Batchelder, J. R. Beene, F. E. Bertrand,
D. J. Dean, F. Liang, M. J. Meigs, W. Nazarewicz,
D. C. Radford.
Regular contributors: F. P. Ervin,
C. J. Gross, M. J. Meigs, W. Nazarewicz,
D. W. Stracener, B. A. Tatum, R. F. Welton
A detailed discussion of our near-term plans for RIB delivery at HRIBF was presented in the summer issue of the HRIBF Newsletter. The substance of those plans remains unchanged, but we have made some changes in the sequence. The next 17F run, which has been delayed somewhat by target and tandem problems, will continue through December. Before we proceed to an extended period of batch-mode beam operations, which include tests with 18F or 11C and a long run with 56Ni, we plan an approximately one-month-long run on neutron-rich beams produced with the HRIBF Uranium-Carbide Target System. The intention of this neutron-rich test run prior to the batch-mode experiments is to provide us with experience using the UC target with intense proton beams before we request proposals for neutron-rich experiments.
The proton separation energy of 17F is only 600 keV. It is speculated that the breakup of 17F would influence the fusion rates at energies near and below the Coulomb barrier for 17F induced reactions [1,2,3]. Fusion excitation functions for 17F + Pb were measured by Rehm et al. [4] where no fusion enhancement due to breakup was observed.
Measurements have been carried out to study the breakup mechanism of the weakly bound 17F. The experiment was performed using a 170 MeV 17F beam incident on a 2 mg/cm**2 Pb target. The 17F was stripped to charge state 9+ to assure purity. The beam intensity was 200,000 particles per second on target for a total of 5 days. A Si detector mounted at 10 degrees with respect to the beam axis was used to monitor the beam and for normalization. The Enge split-pole spectrograph was placed at 2 degrees on the other side of the beam axis to monitor the beam.
The breakup products, proton and 16O, were measured in coincidence by a double-sided strip detector (DSSD) located near the grazing angle and a Si surface barrier detector (SBD) mounted on the back of the DSSD. The thickness of the DSSD is 300 um which stops the heavy fragment, 16O, but allows the light fragment, one proton, to punch through and be detected by the SBD. The DSSD is 5x5 cm**2 with 16x16 strips and spans from 33 to 57 degrees. Protons are identified by a dE-E technique using the energy loss in the DSSD (dE) and the energy deposited in the SBD (E). The coincident 16O is sought in the events where a proton has been identified.
The data, as detected by the experimental setup, was simulated by Monte Carlo calculations. The energy distribution of the breakup protons was reproduced by the Monte Carlo simulation assuming a direct mechanism. In the simulation, the 17F was excited to energy between 0.6 and 1.3 MeV and disintegrated at the distance of closest approach. The excitation function of low-energy radiative capture of proton on 16O [5] was folded in the simulation to generate events. The angular correlation of the breakup fragments was also reproduced by the Monte Carlo simulation. The measured breakup cross section was found to be very small, although further measurements are underway to reduce the uncertainty. It is expected that at energies near the barrier the breakup cross section will be smaller than that measured in this work. This suggests that the influence of the breakup of 17F on near barrier fusion may be too small to be measurable.
References
[1] C. H. Dasso and A. Vitturi, Phys. Rev. C 50, R12 (1994).
[2] M. S. Hussein et al., Phys. Rev. C 46, 377 (1992).
[3] N. Takigawa et al., Phys. Rev. C. 47, R2470 (1993).
[4] K. E. Rehm et al., Phys. Rev. Lett. 81, 3341 (1998).
[5] R. Morlock et al., Phys. Rev. Lett. 79, 3837 (1997).
As facilities, including HRIBF, explore the structure of neutron-rich nuclei, a challenge remains to understand these systems from a shell model perspective. From the technical point of view, the shell-model space needed to treat the relevant degrees of freedom properly grows enormously as one adds neutrons. An equally difficult complication involves developing useful two-body shell-model interactions in regions of the periodic table where little is known experimentally.
One such area is in the sd-pf shell, in which 16O is taken as a core. For neutron-rich nuclei in this region, neutrons typically occupy the upper part of the sd-shell and lower part of the pf-shell, while protons occupy mainly the sd-shell; however, the proton-neutron interaction across the shells plays an important role in determining the structure of these nuclei, and cannot be ignored. Thus, calculations that include both major-oscillator shells become necessary. Provided that a shell-model interaction and a technical method for computing observables exist, one can study interesting effects in the sd-pf shell model region. For example, studies of shell closures at the N=20,28 neutron magic numbers may be carried out.
While obtaining an effective two-body interaction for a given shell model space has a long history, seldom has the many-body perturbation theory been applied to large, multi-major oscillator shells. Work in this direction yielded an effective interaction that may be applied across the sd-pf shells [1]. Using Shell Model Monte Carlo (SMMC) technology that was specifically enhanced for cross-shell calculations (including center of mass removal), several interesting features of nuclei near the N=20 region were investigated. One conclusion, consistent with other work, was that nuclei such as 32Mg tend to have two particles in the pf-shell (specifically in the f7/2 orbital). A further feature of these shell-model interactions in neutron-rich systems is that they exhibit weak J=0 total pairing strengths across the N=20 shell gap [2].
SMMC has also recently been applied to the interesting astrophysical problem of characterizing the Type-Ia explosion mechanism [3]. The Chandrasekhar mass model for Type Ia Supernovae (SNe Ia) has received increasing support from recent comparisons of observations with light curve predictions and modeling of synthetic spectra. It explains SN Ia events via thermonuclear explosions of accreting white dwarfs in binary stellar systems, being caused by central carbon ignition when the white dwarf approaches the Chandrasekhar mass. As the electron gas in white dwarfs is degenerate, characterized by high Fermi energies for the high density regions in the center, electron capture on intermediate mass and Fe-group nuclei plays an important role in explosive burning. Electron capture affects the central electron fraction, which determines the composition of the ejecta from such explosions. Up to the present, astrophysical tabulations based on shell-model matrix elements were only available for light nuclei in the sd-shell. Recently, new SMMC and large-scale shell-model diagonalization calculations have also been performed for pf-shell nuclei. These led, in general, to a reduction of electron capture rates in comparison with previous, more phenomenological, approaches. Making use of these new shell-model-based rates, the first results were presented for the composition of Fe-group nuclei produced in the central regions of SNe Ia and possible changes in the constraints on model parameters like ignition densities and burning front speeds.
References
[1] D. J. Dean et al., Phys. Rev. C 59, 2474 (1999).
[2] P.-G. Reinhard et al., Phys. Rev. C 60, 014316 (1999).
[3] F. Brachwitz et al., submitted to ApJ (1999).
Effective October 1, 1999, Witek Nazarewicz assumed the position of HRIBF Deputy Director for Science. His responsibilities include operation of the HRIBF Program Advisory Committee, interaction with the Users Executive Committee, advising the facility on priorities for beam and equipment development, and presenting the HRIBF scientific program to the outside community. Witek will continue in his position as Professor of Physics at The University of Tennessee and will carry out his HRIBF responsibilities as a part-time ORNL Adjunct Staff Member. Carl Gross will continue as HRIBF Scientific Liaison, and Franda Ervin will continue to be responsible for the operation of the User Office.
Three new additions to the HRIBF Program Advisory Committee have been made. J. Aysto, C. Baktash, and M. Wiescher have replaced S. M. Austin, W. Gelletly, W. Nazarewicz, and P. D. Parker. We wish to thank the previous members for their service. The present PAC membership includes:
Since we have seen a thirty-fold increase in F- yields when aluminum oxide was added to the target, we decided to see if the same was true for Br- ions. When we added Al2O3 fibers to the UC target, we found that the yield doubled but it was still about 80 times less than the yield of Br+ ions from the EBP positive ion source. For Sn- ions there was no measurable change in the yield.
The control system was changed from VISTA to EPICS during this maintenance period. The EPICS system shows signs of much greater stability than VISTA software with no more crashes in the middle of the night. Work remains to convert all of the utility programs that had been developed for VISTA and to add logging and other functionality which was removed from VISTA software to reduce crash frequency. The next task will be to convert accelerator beam lines.
In late August and early September, the batch mode source was mounted on the RIB injector, and stable beams of C-, Si- and Ni- were extracted from targets made of these materials. Measured intensities were lower than expected for each of these beams suggesting target misalignment. Further examination of the sputter patterns on the targets confirmed this misalignment. Compound backlash associated with numerous drive couplings resulted in an unacceptable variation in the position of the target wheel. As a result, the target wheel positioning system has been completely redesigned. The drive motor is now close-coupled to the target wheel through a single worm coupling and the target position is also read back directly through a potentiometer. The position of the target can now be set to a 0.005" tolerance (~1% target diameter). This system has been constructed and awaits testing.
In late September, an elongated 5.5" HfO2 target was installed on the RIB injector. This target configuration allowed more efficient radiative cooling than earlier designs by incorporating spaces between disks of target material for heat to radiate through. The target diameter was also increased to accept a wobbling beam. We hoped this configuration would increase the target's ability to withstand higher ORIC beam intensities and thereby improve 17F yield. In early November, after ORIC became available, beam was put on target. With 5 uA of 2H beam on target, the 17F yield increased with target heater temperature to values of 6x10**5 particles/s (factor of 20 less than nominal yields with previous target configuration). Upon inspection, several observations were made which help to explain the lower yield 17F ions:
In collaboration with the Metals and Ceramics Division at ORNL, a stand-alone target material characterization apparatus has been constructed and tested. The instrument employs a small residual gas analyzer to measure the time profile of permeation of chemical species through a membrane constructed from candidate target material. This system has been tested with oxygen diffusing through yttria stabilized zirconia. Measured diffusion coefficients for this system show good agreement with literature values. We intend to use this apparatus in initial feasibility studies of the development of new beams and to gain insight into on-line experiments where the measured yields represent a convolution of diffusion, desorption, effusion and ionization. This matrix also allows the direct investigation and development of new ISOL techniques for mass transfer such as electrochemical transport.
The CLARION clover Ge detector array at the HRIBF will be completed within the next month or two, with the delivery of the last BGO Compton suppressor. The array comprises eleven segmented Clover Germanium detectors, each with a large BGO Compton Suppressor. They are positioned at the target chamber of the HRIBF Recoil Mass Spectrometer, mostly at backward angles. The target-to-detector distance is adjustable between 20.0 and 23.5 cm.
New dedicated electronics (CAMAC, FERA-readout) has been fully tested and debugged. These electronics are similar in many respects to the GAMMASPHERE electronics, but are housed in quadruple-wide CAMAC modules, with ECLine (FERA-type) readout. The modules require a first-level trigger within 1 microsecond of the event and a second-level trigger within 5 microseconds, thus allowing a trigger on delayed coincidences with recoils at the RMS focal plane. Total shaping, conversion, and readout times are typically 20-25 microseconds from the start of the event. Digitized outputs are:
The performance of the array at a target-detector distance of 21.8 cm and at 1.33 MeV is tabulated below. Pictures of the array being mounted in the support structure can be found at http://www.phy.ornl.gov/hribf/research/gallery
Individual relative photopeak efficiency | 154% (with add-back) at 1.33 MeV |
Measured Total Absolute Photopeak Efficiency | 2.25% at 1.33 MeV |
Measured Peak-to-Total Ratio | 0.57 at 1.33 MeV |
The annual HRIBF Users Meeting was held at the DNP Meeting in Asilomar, California on October 21. Approximately 70 people attended the hour-long meeting which featured reports by Fred Bertrand, Carl Gross, Alfredo Galindo-Uribarri, and Brad Sherrill. Topics covered included:
The Users Executive Committee election was won by K. Rykaczewski (ORNL) and L. L. Riedinger (Tennessee). They will join I. Y. Lee (LBNL), B. M. Sherrill (Michigan State), W. B. Walters (Maryland), and M. Wiescher (Notre Dame) in January of 2000. I. Y. Lee will be chairperson next year. We wish to thank N. Benczer-Koller (Rutgers) and M. S. Smith (ORNL) for their past three years of service to the Users Group. As always, the committee members are there to represent the interests of the users. You are encouraged to contact any member to express any concerns, suggestions, or opinions you wish to express and have brought up for discussion.
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RIB-050 - Selective Study of Excited States of N=Z Nucleus 66As Using Decay Tagging Technique |
Grzywacz/University of Tennessee |
8/2-5/99 |
RIB-000 - Commissioning of the RMS |
Gross/ORISE |
8/6/99 |
RIB-040 - Beam Diagnostics Development |
Shapira/ORNL |
8/9/99 |
RIB-037 - Tandem Development |
Meigs/ORNL |
8/10/99 |
RIB-014 - Target-Ion-Source Development - Arsenic and Fluorine |
Stracener/ORNL |
8/12/99 |
Scheduled Maintenance |
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8/16-9/17/99 |
Unscheduled Maintenance |
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9/20-10/15/99 |
For this quarter's schedule go to http://www.phy.ornl.gov/hribf/users/10-12-1999.html.
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Witek Nazarewicz | Carl J. Gross |
Deputy Director for Science | Scientific Liaison |
Mail Stop 6368 | Mail Stop 6371 |
witek@mail.phy.ornl.gov | cgross@mail.phy.ornl.gov |
+1-865-574-4580 | +1-865-576-7698 |
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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 |