Upload
others
View
0
Download
0
Embed Size (px)
Citation preview
Modeling of an Extraction Lens System
Thesis Defense Bachelor of Applied Science
Karine Le Du Engineering Physics
School of Engineering Science, SFU
March 2003 Thesis Defence
Overview
Dehnel Consulting Ltd.
Use of Commercial Cyclotrons
Cyclotron Components Extraction Lens System
Scope of the Study Computer Simulation Model
Results
Acknowledgements
Karine Le Du
March 2003 Thesis Defence Karine Le Du
Current Expertise: Complete Beamline Design
Injection System Design
Beamline Simulator Software
My Project…
Extraction Lens System Design
Future Endeavors
Ion Implantation
March 2003 Thesis Defence
Use of Commercial Cyclotrons
Photo Courtesy of Ebco Technologies Inc.
Radioisotopes for medical use
Detection of soft tissue damage
On-site at hospitals
Short half-lives of radioisotopes
Bombard target with protons
Necessitates beam of H¯
(hydride ions)
Karine Le Du
March 2003 Thesis Defence
Cyclotron Components
Karine Le Du
Ion Source
Extraction Lenses
Injection Line
Inflector Cyclotron
Extraction Probe
Beamline
March 2003 Thesis Defence
Cyclotron Components
Karine Le Du
Ion Source
Extraction Lenses
Injection Line
Inflector Cyclotron
Extraction Probe
Beamline
March 2003 Thesis Defence
Extraction Lens Assembly
Karine Le Du
Assembly drawing courtesy of TRIUMF
vacuum
chamber
beamstop ion
source
z ~ 405mm
Plasma lens
Extraction lens
Shoulder lens
March 2003 Thesis Defence
Scope of the Study
Purpose
Identify how changes to system parameters (dimensions and voltage potentials) affect H¯ beam characteristics
Provide data to aid an engineer in optimizing the design of an extraction lens system with regards to beam characteristics
Karine Le Du
March 2003 Thesis Defence
Beam Characteristics
Normalized Beam Emittance, εN
Describes size of beam in phase space
Energy normalized
Beam Current, I Percent of beam transmitted
Low and high beam current applications
Beam Brightness, b
Karine Le Du
2N
Ib
March 2003 Thesis Defence
Phase Space
Four important coordinates that completely describe an ion’s trajectory are (x, x’, y, y’)
(x, y): transverse
position
(x’, y’): divergence
from longitudinal axis
z: longitudinal
position
Karine Le Du
March 2003 Thesis Defence
Beam Size
Beam Size: Area enclosed in beam ellipse
Beam Emittance: Proportional to beam size
Karine Le Du
x
x’ Beam ellipse
March 2003 Thesis Defence
Optimal Beam Characteristics
Normalized Beam Emittance, εN
minimize
Small emittance is more efficient
Beam Current, I
Depends on application
Beam Brightness, b
maximize
Achieved by maximizing beam current or minimizing normalized beam emittance
Karine Le Du
March 2003 Thesis Defence
Computer Simulation Model
SIMION 3D, Version 7.0, INEEL*
Model consists of 3 electrostatic lenses
*Idaho National Engineering and Environmental Laboratory
Karine Le Du
March 2003 Thesis Defence
Assumptions Made
ASSUMPTIONS
No plasma meniscus
JUSTIFICATIONS
Beyond the scope of this study
Karine Le Du
No filter magnet
Ignored space charge repulsion and image forces
e¯ stripped out early
Beyond the scope of this study
March 2003 Thesis Defence
System Parameters E1: Plasma Electrode
E2: Extraction Electrode
E3: Shoulder Electrode
V1: Voltage Potential of E1
V2: “ “ of E2
V3: “ “ of E3
A1: Aperture of E1
A2: “ “ E2
A3: “ “ E3
D12: Spacing between E1/E2
D23: “ “ E2/E3
Karine Le Du
March 2003 Thesis Defence
Table of Parameter Values List of design parameters by name
ID tags & nominal values
Variable parameter test values
Plasma Electrode E1
Voltage potential V1 = -25 kV
Aperture diameter A1 = 13 mm
Extraction Electrode E2
Voltage potential V2 = -22 kV -23 kV -22.5 kV -21.5 kV
Aperture diameter A2 = 9.5 mm 10.5mm 11.5mm 12.5mm
Shoulder Electrode E3
Voltage potential V3 = 0 V
Aperture diameter A3 = 10 mm 9 mm 11 mm
Separation between electrodes
E1 & E2 D12 = 4 mm 7 mm 10 mm
E2 & E3 D23 = 12 mm 8 mm 16 mm
Karine Le Du
List of design parameters by name
ID tags & nominal values
Variable parameter test values
Plasma Electrode E1
Voltage potential V1 = -25 kV
Aperture diameter A1 = 13 mm
Extraction Electrode E2
Voltage potential V2 = -22 kV -23 kV -22.5 kV -21.5 kV
Aperture diameter A2 = 9.5 mm 10.5mm 11.5mm 12.5mm
Shoulder Electrode E3
Voltage potential V3 = 0 V
Aperture diameter A3 = 10 mm 9 mm 11 mm
Separation between electrodes
E1 & E2 D12 = 4 mm 7 mm 10 mm
E2 & E3 D23 = 12 mm 8 mm 16 mm
List of design parameters by name
ID tags & nominal values
Variable parameter test values
Plasma Electrode E1
Voltage potential V1 = -25 kV
Aperture diameter A1 = 13 mm
Extraction Electrode E2
Voltage potential V2 = -22 kV -23 kV -22.5 kV -21.5 kV
Aperture diameter A2 = 9.5 mm 10.5mm 11.5mm 12.5mm
Shoulder Electrode E3
Voltage potential V3 = 0 V
Aperture diameter A3 = 10 mm 9 mm 11 mm
Separation between electrodes
E1 & E2 D12 = 4 mm 7 mm 10 mm
E2 & E3 D23 = 12 mm 8 mm 16 mm
List of design parameters by name
ID tags & nominal values
Variable parameter test values
Plasma Electrode E1
Voltage potential V1 = -25 kV
Aperture diameter A1 = 13 mm
Extraction Electrode E2
Voltage potential V2 = -22 kV -23 kV -22.5 kV -21.5 kV
Aperture diameter A2 = 9.5 mm 10.5mm 11.5mm 12.5mm
Shoulder Electrode E3
Voltage potential V3 = 0 V
Aperture diameter A3 = 10 mm 9 mm 11 mm
Separation between electrodes
E1 & E2 D12 = 4 mm 7 mm 10 mm
E2 & E3 D23 = 12 mm 8 mm 16 mm
March 2003 Thesis Defence
General Trends
0
0.5
1
1.5
2
2.5
0.5 0.75 1 1.25 1.5 1.75 2
normalized beam emittance (mm.mrad)
be
am
bri
gh
tne
ss
(m
m.m
rad
)-2
D12 = 4 mm
D12 = 7 mm
D12 = 10 mm
less than 39.9% trans.
40% to 49.9% trans.
50% to 59.9% trans.
60% to 69.9% trans.
70% to 79.9% trans.
80% to 89.9% trans.
90% to 99.9% trans.
100% transmission
V2 = -23 kV
V2 = -22.5 kV
V2 = -22 kV
V2 = -21.5 kV
Karine Le Du
March 2003 Thesis Defence
General Trends
Karine Le Du
1
1.25
1.5
1.75
2
2.25
2.5
0.5 0.55 0.6 0.65 0.7 0.75 0.8 0.85 0.9
normalized beam emittance (mm.mrad)
beam
bri
gh
tness (
mm
.mra
d)-2
D12 = 10mm 50% to 59.98% trans. 60% to 69.98% trans. 70% to 79.98% trans.
80% to 89.98% trans. 90% to 99.98% trans. 100% transmission V2 = -23 kV
V2 = -22.5 kV V2 = -22 kV V2 = -21.5 kV
March 2003 Thesis Defence
Ion Trajectories
Karine Le Du
Nominal Configuration, b = 0.341, N =1.136, I = 44%
Highest Beam Brightness, b = 2.351, N =0.508, I = 60.7%
Lowest Beam Brightness, b = 0.127, N =1.916, I = 46.6%
100% Beam Transmission, b = 1.731, N =0.76, I = 100%
b in [(mm·mrad)-2]
N in [mm·mrad]
March 2003 Thesis Defence
Limitations/Future Work
Test results limited to ranges of parameter values tested
Test wider ranges of values
Beam loss occurred at downstream aperture of E2
Downstream aperture had fixed size
May be cause of apparent ineffectiveness in changing A2 and A3 parameter values?
Implement space charge repulsion
Vary plasma meniscus curvature
Implement magnetic filter
Karine Le Du
March 2003 Thesis Defence
Acknowledgements
Dr. Morgan Dehnel Excellent mentoring and guidance
Dr. John F. Cochran and
Mr. Steve Whitmore Invaluable feedback
My family Support and encouragement
The Caskey Family, and friends Support and encouragement
Karine Le Du
March 2003 Thesis Defence
Crude Beam Current Adjustment
Parameter Suggested value
D12 10 mm
D23 16 mm
A2 9.5 mm (same)
A3 10 mm (same)
V2 Vary to achieve desired beam current make more positive for higher beam current
Karine Le Du
March 2003 Thesis Defence
Beam Optics
Karine Le Du
z
x
X’
X’
March 2003 Thesis Defence
Beam Size
Beam Emittance:
Ellipse Area:
Karine Le Du
nterceptiaximumm xx '
A
N
Normalized Emittance: