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MICROCOPY RESOLUTION TEST CHART
NATIONAL BUREAU OF STANDARDS -1963
.
ORNUD 1512
Conf. 650512-8
996191893
MASTERP
DCX-2 SCANNING ENERGY SPECTROMETER*
J. S. Culver
Oak Ridge National Laboratory
Oak Ridge, Tennessee
In the DCX-2 machine the injected 600 kev Ha* ion beam is introduced
9 in. off axis and at an angle of 7° from the vertical as shown in Fig. 1.
The resulting path of the molecular ions is helical as is the trapped pro-
ton plasma resulting from dissociation in the lithium arc. The path of the
particles reflected by the mirror field retains the original radius and
pitch angle, but the orbit has precessed by a few degrees. After passing
down the length oť the machine and back, the molecular beam is dumped on
the injection snout. Also, al? protons whose orbits extend beyond the inner
surface of the injection snout will be wiped off as indicated in Fig. 2.
Because of the helical path of the injected and trapped particles in the
machine it is desirable to be able to observe the angular distribution of
these particles and their radial position. To accomplish this, a scanning
version of an existing collimated energy spectrometer was constructed.
.
..
.
.
..
*
.
RELEASED FOR ANROURI BERT
IN HUCL.BAR SCIENCE ABSTRACTS
.:
::!
The essential parts of the spectrometer are shown schematically in Fig.
3. The collimating system currently being used consists of a 5 u slit and
a 20 w round aperture arranged to admit a fan-shaped beam of particles 0.1°
spola
wide and 60° high. In addition to providing good resolution of the angular
and radial distribution of particles in the machine, the collimator atten-
uates the neutral beam to a counting rate compatible with the speed of ::
available electronics.
"Research sponsored by the U. S. Atomic Energy Commission under contract
with the Union Carbide Corporation.
'
*

.
L
.
P
The neutral particles resulting from dissociation or charge exchange
impinge on a silicon barrier detector which produces pulses proportional
to the energy of the incident particle, providing both an energy spectrum
and a count rate.
To observe radial distribution, the slit is positioned parallel to the
axis of the machine and the scanning mechanism then rotates in a vertical
plane. If it is desired to observe angular distribution, the entire probe
is rotated in its seal until the slit is perpendicular to the machine axis. :)
By means of the motor drive and readout helipot geared to the scanning head,
it is possible to read angular position to about 0.1º.
Figure 4 shows a front view of the probe with the slit and axis of
rutation horizontal. The cylindrical member houses both the collimating
system and detector, providing an isolation seal between high and low :
vacuum systems as well. Figure 5 shows the rack and pinion drive mechanism
and the coaxial signal lead which is insulated from ground by the ceramic
bushing. ' In Fig. 6 one can see the drive mechanism and readout helipot.
.
:.
:..
The horizontal bar clamped to the probe shaft is set perpendicular to the
slit allowing it to be positioned in the machine by means of a level.
...
....
In addition to the mechanical flexibility built into the probe, the
output signal can be treated in several ways to expand the data obtained.
The block diagram in Fig. 7 shows the instrumentation presently in use.
The usual scan involves one sweep of about two minutes duration across
the region of interest, recording count rate vs angular position on the X-Y
recorder and simultaneous storage of the energy spectrum in the multichannel
analyzer. By adjusting the single channel analyzer ahead of the X-Y recorder,
.
.
.
2
, it is possible to look at a limited energy range and plot out angular dis-
tribution or radial position for that energy range. Since it is possible
to stop the scanner at any position, an energy spectrum is frequently taken
at some point of special interest such as the injected beam only, or trapped
plasma with no axial velocity, etc.
Figures 8, 9, and 10 are typical traces obtained on the X-Y recorder
with the spectrometer. Figure 8 was obtained with the slit perpendicular
to the machine axis and represents the count rate vs pitch angle of ejected
charge-exchange "neutrals of all energies. The side lobes are from those
trapped particles which have the characteristic pitch angle of the injected
beam. An energy spectrum shows these to be principally 300 kev protons as
might be expected. The high central peak is of particular interest because
. it contains high-energy neutrals with little or no axial velocity. The
:: mechanism which produces these particles is not well understood; however,
the particles are almost always present and have energies as high as 2 Mev.
To further explore this phenomenon, a series of scans were run at several
energies with a limited energy range. The results shown in Fig. 9 show an
interesting family of curves which indicates that the high energy particles
are indeed in the central peak.
..
.
.
.........
·
* Figure 10 is a typical scan obtained with the slit parallel to the
machine axis, giving the radial distribution of orbiting particles in the
plasma volume. This particular scan was obtaines using only a limited
energy range at about 200 kev which produced the accentuated 1st peaks.
The double peaks for 12 and 13* are the result of the precession of the
reflected molecular con beams. The large peak near the center of the ma-
chine represents dissociation neutrals from the lithium arc.
T
:
.
.
*
2.
he
.
.
.
1
.
Since the high central peak in Fig. 8 18 of particular interest, an
..
..
.....
accessory has been added to the probe as shown in Fig. 11. A plate has
been added containing a 6° bar and a 6° slit, either of which can be posi-
tioned in the exact center of the probe. With this device one can make a
scan similar to Fig. 10 looking only at the central peak (ilit in position)
. or, with the bar centered, the central peak 1e blocked out and the resulting
trace represents all other neutrals.
Although the scanning spectrometer described in this paper is specifi-
cally designed for machines having the unique properties of DCX-2 or OGRA,
It is hoped that it might suggest some possibilities for plasma diagnostics
in other CTR installations.
,;
;
-----
..
.!
.
. .
.
11
.
:
-
*
1.
IC
:-,
.
.
FIGURE CAPTIONS
Fig. No.
Title
Identilication
ORNL-Dwg-48280
ORNL-Dwg-64-257
ORNL-Dwg-65-4577
ORNL-Photo-72048
.-
.
-
-
The DCX-2 Machine (Schematic)
Section thru DCX-2 Showing Ion Orbits
DCX-2 Scanning Energy Spectrometer (Schematic)
Spectrometer Scanning Head (Front View)
Spectrometer Scanning Head (Side View)
Spectrometer Assembly
Energy Spectrometer Instrumentation
Typical Vertical suit Scan of Count Rate
V8 Angle
ORNL-Photo-72046
5 boran
ORNL-Photo-72047
ORNL-Dog-65-4576
ORNL-Dwg-64-11751
ORNL-Dwg-64-6665
Angular Distribution of Neutrals Seen From
Midplane of DCX-2 at Different Energies
Typical Horizontal Slit Scan of Count Rate
Vs Angle
ORNL-Dwg-64-11748
.
:
Spectrometer Head with Attachment for Studying
High-Energy Particles with Small Axial Velocity :
ORNL-Photo-72045
in
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LEGEND :
JAAAAAA
O ION SOURCE
ACCELERATOR TUBE
☺ MAGNETIC LENS
· MOLECULAR ION BEAM
TRAPPED PLASMA
O MAGNETICALLY SHIELDED INJECTOR
MAGNETIC FIELD COILS
O VACUUM ARC
O VACUUM PUMPS
reure lloguer
OCX-2
-
The DEX-2 Machine (Schematic)
Fig. 1

-
-
--
. moramo
ORNL-DWG 64-257
-36-in.-ID LINER

* INJECTOR
| "SNOUT"
600-kev Hot ION
ORBIT, 10-in. diam
4 in.
-POSITION
OF ARC
LIMIT OF PROTON
ORBITS TANGENT
TO INJECTOR
(11-in. diam)
-5/8-in. x 10-4 SLIT
0.003-in. HOLE
SILICON BARRIER
- DETECTOR
Fig. 2
Section thru DCX-2 Showing Ion Orbits
'
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ANGULAR POSITION
.READOUT HELIPOT –
3/8-16 SCREW
COAX SIGNAL LEAD-
20 U ROUND APERTURE
CVARIABLE SPEED
REVERSIBLE DRIVE
MOTOR
-SILICON BARRIER
DETECTOR
.
2
DCX-2 SCANNING ENERGY SPECTROMETER
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