In general, many radioactive nuclei of interest to the research programs
at the HRIBF have short lifetimes, are only produced in small quantities
and undergo substantial losses during release, transport and ionization
in the target/ ion source. Production of usable intensities of RIBs, therefore,
is usually preceded by the development of a target/ ion source technique
which optimizes release of the radioactive species from the target material,
transport to ionization region and efficient ionization of the specific
chemical species. This page presents a few highlights of some new target
techniques which have been or shortly will be employed on the RIB injector.
New Oxide Target Materials and Techniques
Early investigations into 17 F production through the
16
O(d,n)17F
reaction were conducted with fibrous targets of Al2O3
and the maximum
17
F - yield measured leaving the
RIB platform was 5x104 ions/s, an insufficient intensity for
RIB experiments. To solve this problem we have designed several new target
systems which are based on a technique of forcing a reactive, electropositive
transport vapor through a fibrous metal oxide network which is considerably
more refractory than Al2O3. The table below shows
several oxides which are commercially available in fiber form (4-6 um dia.)
and packed to densities of 3-10% of the pure material generally in the
form of a weave or felt. See for example, Zircar
Products Inc.
Material
|
Temperature at which the
vapor pressure reaches 10-4 Torr
|
|
HfO2
|
2500 C
|
|
ZrO2
|
2200 C
|
|
Y2O3
|
2000 C
|
|
CeO2
|
2310 C
|
|
ZrO2/Y2O3
|
1900 C
|
|
Al2O3
|
1550 C
|
The maximum operating temperature of the target material is set by the
characteristic vapor pressure curve for that material since the closely
coupled ion source cannot tolerate a vapor loads greater than 10-4
Torr.
Since, the major RIB loss processes; diffusion, desorption and effusion
generally depend exponentially on temperature, we expected the gains made
by increased operating temperature and increased production (more production
beam on target) to far out weight the effect of shorter production ranges
due to increased stopping power of the higher Z, more refractory materials:
Hf, Zr, Y, Ce versus Al. HfO2 is the most refractory
of these materials and the microstructure of HfO2
target is shown here. The following target system designs are based
on this material and have been used or are being developed for use at the
HRIBF.
-
This figure shows the initial configuration of the HfO2
target system which was tested on the RIB injector. The target system
features a high temperature BN transport vapor oven which was used with
Al vapor and a W-Re target material reservoir heater capable of sustained
operation at 2300 C. Initial tests of this system have yielded 17F-
beams of 2x107 ions/s measured leaving the RIB platform, a significant
improvement over the best yield of 5x104 ions/s from Al2O3.
This system was employed in the first HRIBF astrophysical
investigation of 17F.
-
This figure shows a sketch of a high power HfO2
target and associated elongated heater which has been designed
and is presently being constructed. This design increases the effective
radiating surface area of the target by a factor of ~20 over the present
design (shown above). This is accomplished by accepting a wider beam and
inclining the target material 85 degrees with respect to the beam axis.
Widening the beam will be accomplished either by rastering, diffusing or
defocusing the present ORIC beam.
-
A second design under development increases still further the effective
radiating surface of the target by longitudinally spacing the HfO2
disks thereby allowing direct radiative heat transfer from the interior
of the target material to the relatively cool enclosure walls. By
uniformly spacing the HfO2 disks this effective area can
be increased by a factor of ~50 over the present design. This figure
shows the concept of a longitudinally distributed
target system which employs the same elongated target heater shown
above. Here, the disks are supported with a thin W rod which intercepts
only a few percent of the beam while drawing several hundred watts of beam
heat directly from the hottest portion of the target to an external sink.
New Liquid Target Techniques
A simple non re-circulating liquid Ge target system was employed for 69
As
and 67Ga produced through the
70Ge(p,2n)69As
and
70Ge(p,a)67Ga reactions. Approximately
1x106 ions/s of 69As and 1x105 ion/s of
67Ga
ions/s were delivered to an experimental target. In the near future, several
experiments are planned which require roughly an order of magnitude more
intensity. To achieve these goals several new liquid target systems have
been designed and are currently being tested:
-
A liquid target system has been developed which utilizes a highly pervious,
low density structure to support the liquid material by virtue of the cohesive
force. Metallic or carbide materials are used to suspend um coatings of
the liquid onto a fiber or foam structure thereby dramatically decreasing
the effective diffusion length from mm to um for a given target thickness.
This format also has the effect of increasing the surface area of the target
by a factor of 102-103 over traditional liquid targets.
Specifically, liquid Ge has been shown to readily wick in a uniform fashion
onto fibers of Mo or SiC when contained by a graphite reservoir. This highly
pervious liquid target system target system is shown here along with
a cooled re-circulating vapor trap and a secondary target material reservoir.
The vapor trap has been added to the system to suppress unwanted target
material vapors which should be more prevelent in this design compared
with the traditional dense liquid targets for a given operating temperature.
The secondary reservoir can be heated through the same temperature range
as the primary target reservoir and serves to extend the operational lifetime
of the system by replenishing lost target material. In general terms this
target system maybe operated with other liquid and non liquid target materials
allowing in situ vapor deposition of variable thickness (um) coatings on
small scale structures such as graphite fibers. At present, this system
is being tested at our on-line test facility.
-
A re-circulating, high power liquid target system
has also been developed which inclines a thin layer of liquid target material
at an 85 degree incidence angle with respect to the production beam. This
has the effect of increasing the total beam current tolerated by the target
since the actual effective radiating area is increased by a factor of ~5
due to the incline. This system has been designed and built and awaits
testing. Both liquid target systems employ the cooled re-circulating baffle
which allows the target material to operate at temperatures hotter than
would be allowed by the material's vapor pressure without the baffle.
Actinide Target Materials
-
A UC2 target has been developed at the HRIBF which is based
on chemically vapor depositing thin um coatings of UC2 on RVC
fiber matrixes. The target material is able to withstand high temperatures
(2000 C) while maintaining highly pervious structure without sintering.
The microstructure of the UC2 target material is
shown in this figure. The results of RIB yield experiments with this material
are shown on the yields page.
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