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NON-EQUILIBRIUM HEAVY GASES PLASMA MHD-STABILIZATION IN AXISYMMETRIC MIRROR MAGNETIC TRAP. A.V. Sidorov 2 , P.A. Bagryansky 1 , A.D. Beklemishev 1 , I.V. Izotov 2 , V.V.Prikhodko 1 , S.V.Razin 2 , V.A. Skalyga 2 and V.G. Zorin 2. - PowerPoint PPT Presentation
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NON-EQUILIBRIUM HEAVY GASES PLASMA MHD-STABILIZATION IN
AXISYMMETRIC MIRROR MAGNETIC TRAP
A.V. Sidorov2, P.A. Bagryansky1, A.D. Beklemishev1, I.V. Izotov2, V.V.Prikhodko1, S.V.Razin2, V.A. Skalyga2 and V.G. Zorin2
1Budker Institute of Nuclear Physics, 630090, Novosibirsk, Russia2Institute of Applied Physics, 603950, Nizhny Novgorod, Russia
Applications
Accelerator injectorsTechnologies
Hadron therapy
Beta beamproject
Heavy Ion Fusion
High density energyphysics
Surface processing
Ion implantation(SOI-technologies etc)
ECR Multicharged Ion Sources
Principles of Gas-dynamic ECR Ion Source Operation
Gyrotron radiation 100 kW @ 37.5 GHz
ECR dischargeECR discharge beam
PullerFC
L~35 cm
Magnetic trap, 2 T, R=5
Lp~30 cm
U~30 kV Plasma electrode
(PE)
Np~Ncutoff~1013cm-3
Te~70eV
τc=1/νei << τg=Leff/Vs
High e-i collision frequency
Loss cone is filled
EDF is isotropic Gas-dynamic regime of confinementGas-dynamic regime of confinement
Plasma lifetime = τg
λii<<L
SMIS 37
Solenoid Coils
Sextupole
e- heatingµ wave
gas
ions
Minimum-B field Confinement in ECR Ion Source
Ø 1 mm
Ion beam
Magnetic coils
MW
MHD stabilization: Cusp-type magnetic configuration
sg 10810n
N: <Z>=2Ag: <Z>=3.5
Losses trough the axial slit is too high!
GDT experiment parameters (D - beams, Н – plasma)
Center magnetic field: 2.83 kG D-injection power: 3.5 MW Trapped power: 2 MW
Plasma density: 1.531013 cm-3
Electron temperature: 140 eV Hot ions density: 41013 cm-3
Injection
Plasma source InjectionLimiter (+150 V)
Plasmareceivers
+150 V
Vortex confinement: potential profile control
VV
VV
cm
V
Potential profile
β ~ 0.6!!
E. I. SOLDATKINA, P. A. BAGRYANSKY and A. L. SOLOMAKHIN. Plasma Physics Reports, 34, 259 (2008).
Finite larmor radius (FLR) effect
21,
L
a
- ion gyroradius, L – trap length, a – plasma radius.
At m=1 mode dominates in spatial spectrum
of the flute instability
21,
L
a
Ion beam emittance ~ , so in ECR ion sources ion temperatureis low, 1÷10 eV and FLR effects are negligible.
iT
GDT
SMIS 37
Vortex confinement: theory
Calculated energy life-time changing in
SMIS 37 setup for helium plasma. Times
normalized on the time of external layers
turning according to internal layers. Initial
unperturbed state of the plasma cord
(time=0) was chosen axisymmetric with the
symmetry center equal to the magnetic
system center. τE=50 correspond to the gas
dynamic confinement time.
In case of the absence of the shear flow
τE=5.
Calculation results (A. D. Beklemishev)
A.D.Beklemishev, Shear Flow Effects in Open Traps, Theory of Fusion Plasmas, AIP Conference Proceedings 1069 (2008) pp.3-14.
Discharge vacuum chamber
Isolators
Limiter
Magnetic field coils
Expanding chamber
Zonds
Edge magnetic force line
MW100 kW@ 37.5 GHz
Scheme of the experiments
0 20 40 60 80 1000.0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1.0
1.1
1.2
Q (
a.u
.)
U, limiter (V)
Total charge registered by zonds #1-3, Helium
Magnetic field at the plug: 1.7 T
1 2 3
zonds #1-3
Total charge registered by zonds #1-3, Nitrogen
Magnetic field at the plug: 1.7 T
0 20 40 60 80 100 1200.0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1.0
Q (
a.u
.)
U, limiter (V)
Critical value of the U limiterin both cases is about of70 V what is close to electrontemperature and it is in goodagreement with calculations
Mode structure: calculations and experimentPlasma potential and electron temperature distribution in the plasma cord section.Potential is normalized on the electron temperature; 1 – corresponds to limiter radius projection in central plane of the trap.
Calculations show that azimuthal modes m=1, m=2 and m=3 have to dominate in the spatial spectrum under conditions of “vortex” confinement.
Experiments show that azimuthal modes m=1 and m=2 dominate in the spatial spectrum under conditions of “vortex” confinement what is in good agreement with calculations.
“Decay” experiment: microwave pulse-length 400μs
Ion saturation current on the center zond (#1)
Limiter voltage Ulim=150 V Limiter voltage Ulim=0 V
13700 13800 13900 14000 14100
0.0
0.5
1.0
1.5
2.0
2.5
(s
Cu
rre
nt
(a.u
.)
Time (s)
13700 13800 13900 14000 14100-0.2
0.0
0.2
0.4
0.6
0.8
1.0
1.2
1.4
1.6
(s
Cu
rren
t (a
.u.)
Time (s)
End of the microwave pulse
Future plans
In future it is planned to improve electrode-limiter for the opportunity to control the potential profile and to extract the ions from the plasma at the same time. In this case it will be possible to research multicharged ion creation in theplasma of ECR ion source under conditions of “vortex” confinement regime realization.
The experiments demonstrated good agreement with calculation: mode structure,critical value of the limiter potential for “vortex” confinement regime realization
Thank you for your attention!