Lithium ion sources for the investigations of fast ion transport in magnetized plasmas
Download
1 / 30

a {x... - PowerPoint PPT Presentation


  • 371 Views
  • Updated On :

Lithium Ion Sources for the Investigations of Fast Ion Transport in Magnetized Plasmas. H. Boehmer, Y. Zhang, W. Heidbrink, R. McWilliams, Department of Physics and Astronomy, University of California, Irvine, California 92697 D. Leneman and S. Vincena,

loader
I am the owner, or an agent authorized to act on behalf of the owner, of the copyrighted work described.
capcha
Download Presentation

PowerPoint Slideshow about 'a {x...' - albert


An Image/Link below is provided (as is) to download presentation

Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author.While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server.


- - - - - - - - - - - - - - - - - - - - - - - - - - E N D - - - - - - - - - - - - - - - - - - - - - - - - - -
Presentation Transcript
Lithium ion sources for the investigations of fast ion transport in magnetized plasmas

Lithium Ion Sources for the Investigations of Fast Ion Transport in Magnetized Plasmas

H. Boehmer, Y. Zhang, W. Heidbrink, R. McWilliams, Department of Physics and Astronomy, University of California, Irvine, California 92697

D. Leneman and S. Vincena,

Department of Physics and Astronomy, University of California, Los Angeles, California 90095


Abstract
Abstract Transport in Magnetized Plasmas

In order to study the interaction of ions of intermediate energies

with plasma fluctuations, two plasma immersible Lithium ion

sources of different size, based on solid-state thermionic emitters

(Li-6 Aluminosilicate), were developed. Compared to discharge

based ion sources, they are compact, have zero gas load, small

energy dispersion, and can be operated at any angle with respect to

an ambient magnetic field of magnitude generally found in plasma

experiments. Beam energies range from 400 eV to 2.0 keV with typical

beam current densities in the 1 mA/cm2 range. Because of the low ion

mass of 6 amu, beam velocities of 100 – 300 km/s are in the range of

Alfvén speeds in Helium plasmas. Design considerations

and operation in a high vacuum test chamber as well as in the high density

magnetized plasma of the LArge Plasma Device (LAPD) at UCLA will

be detailed.

The work is supported by DOE.


Fast ions in magnetized plasmas
Fast Ions in Magnetized Plasmas Transport in Magnetized Plasmas

  • Definition: A plasma ion component whose energy is large compared to the thermal energy of plasma ions.

  • Generated by shocks and instabilities in space plasmas.

  • In fusion related plasmas they are formed by ionization of neutral beams, by ion cyclotron and lower hybrid heating and as byproducts of fusion reactions.

  • Anomalous transport frequently observed in toroidal plasmas.

  • Fast ion transport due to turbulence difficult to study in fusion devices: Lack of in situ diagnostics.

  • This program: Test particle transport in diagnostics accessible plasmas: High density, large volume LAPD plasma with small, internal ion sources.


Experimental configuration of fast ion transport experiments in lapd
Experimental Configuration of Fast Ion Transport Experiments in LAPD

Plasma parameters:

Diameter: 75 cm; Magnetic field 0.5 – 2 kG

Pulsed at 1 Hz, peak density 2.5x1012 cm-3, Te = 10 eV

Turbulence: Drift waves; Launched and unstable Alfvén Waves



Publications

Publications: in LAPD

H. Boehmer, et al., “Operation of a 0.2 – 1.1 keV ion source within a magnetized laboratory plasma”. Rev. Sci. Instr. 75, 1013 (2004)

L. Zhao, et al., “Measurement of classical transport of fast ions”. Physics of Plasmas, 12, 052108 (2005)

Y. Zhang, et al., “Lithium ion source for investigation of fast ion transport in magnetized plasmas”. Submitted to Rev. Sci. Instr.


Internal fast ion beam sources for lapd
Internal Fast Ion Beam Sources in LAPDFor LAPD

  • Required orbits:

  • Arbitrary pitch angle, helical orbits: Internal sources.

Desirable Properties:

  • Wide energy range, 400 eV to 2 keV to investigate the energy dependence of the interaction.

  • Low ion beam mass to match the phase velocity of Alfvén waves in helium plasmas.

  • Low beam divergence to make the beam observable at large distances.

  • Sufficient current to facilitate diagnostics but small enough to prevent collective wave excitation (test particle investigation).

  • Small size and floating capability to minimize perturbation of background plasma.

  • Low gas load.

  • Operation at any pitch angle and at high magnetic fields.

  • No magnetic materials.


Rf ion source for fast ion experiments at lapd ref h boehmer et al rev sci instr 75 1013 2004
RF Ion Source for Fast Ion Experiments at LAPD in LAPDRef.: H. Boehmer, et.al., Rev. Sci. Instr., 75, 1013 (2004)

  • Commercial source (IONTECH).

  • Operating frequency: 18 MHz.

  • Ion beam energy: 50 eV to 1200 eV.

  • Typical beam current density (Argon): 0.4 mA/cm2


Difficulty of operating the rf gun in a magnetic field
Difficulty of Operating the RF Gun in a Magnetic Field in LAPD

  • For ωce >> ωRF the gun plasma electrons are not sufficiently energized for gas ionization.

  • Operated at an angle with respect to an external magnetic field, only a fraction of the plasma is in contact with the extraction grids.

  • Beam energy: 600 eV.


Argon ion beam profiles measured in the afterglow of the lapd plasma 32 cm from ion source
Argon Ion Beam Profiles in LAPDMeasured in the Afterglow of the LAPD Plasma 32 cm from Ion Source


Disadvantages of rf source
Disadvantages of in LAPDRF Source

  • Large gas load.

  • Operation at small magnetic fields and small pitch angles, only.

  • Large physical size.

  • Operation with Argon, only (large ion mass). Not adaptable to investigations for Alfvén wave interactions.


Surface ionization sources
Surface Ionization Sources in LAPD

Ion species: Li, K, Cs, Ba.

  • Aluminosilicate source (Li)


  • Solid ceramic material loaded with the element to be emitted in LAPD

  • Ion species:

    • Alkaline metals: Cs,K, Li6, Li7, Na.

    • Alkaline earth: Ba (“experimental”, LIF diagnostics).

  • Operation like electron guns with dispenser cathodes.

  • Typical beam densities: 1 mA/cm2 at 11500 C.

  • Inert at room temperature to atmospheric constituents.

  • Poisoned at operating temperature by O2, Vac. Oil, etc.

  • Lifetime depends on emission current.

  • Pulsed or DC operation.


Cross section of a generic lithium ion source for lapd at ucla
Cross Section of a Generic Lithium Ion in LAPDSource for LAPD at UCLA

  • Two emitter sizes: 0.6 and 0.25”

  • Immersion in plasma and magnetic field: Pierce configuration not possible.

  • Gridded source.

  • Short emitter – grid distance: Orbit modifications by vxB and ExB forces small.

  • Development and tests at UCI.

  • For sufficient beam current at low beam energies (< 500 eV): acceleration-deceleration sections.

  • At high plasma densities (1012 cm-3): emitter current loaded by e-, geometric cut-off of plasma.


Lithium ion guns
Lithium Ion Guns in LAPD

0.60” dia.Emitter

Size: 3.0” dia., 4.78” long

0.25” dia. Emitter

Size: 1.285x1.260x1.630”

Fits through 50mm port


Lithium ion gun with 0 6 emitter emission current vs temperature extraction voltage 2 kv
Lithium ion gun with 0.6” Emitter in LAPDEmission Current vs. TemperatureExtraction Voltage: 2 kV

  • Maximum achieved emitter current: 5.8 mA.

  • Typical current density: 1 mA/cm2 (at 2 mA)


Lithium ion beam emission and grid transmission for 0 6 diameter emitter
Lithium Ion Beam Emission and Grid Transmission in LAPDfor 0.6” Diameter Emitter

  • Low emission current to prevent beam blow-up due to space

  • charge.

  • Space charge limited flow at low voltages.

  • Field enhanced emission at high voltages.

  • Grid transmission: 80%.


Equipotential Pattern in the Lithium – Ion Sources in LAPD

Improvement of Performance

Dashed box: Space charge due to

1 mA/cm2, 600 eV beam included.

  • 0.6” Emitter: Fringing field errors

    and errors around grid wires are small

    at the useful center section.

    (b) 0.25” Emitter with single accelerator

    Grid: Fringing fields extend to center of

    the beam. Field errors around the 40 lpi

    1st grid.

    (c) 0.25” Emitter with 90 lpi 1st grid.

    Addition of a second accelerator grid

    with 40 lpi.


Radial beam profiles in uci test chamber
Radial Beam Profiles in UCI Test Chamber in LAPD

Note: The beam current is

intentionally kept low to avoid

space charge blow-up of beam.

  • 0.6” Emitter w/o mask, 2.0 keV beam.

    Good beam profile with near

    parallel equipotential lines.

    (b) 0.25” Emitter.

    Blue: Single accelerator grid.

    Red: Double accelerator grid.

    Improvement of performance.


Beam temperature is larger than the 1100 o c emitter temperature 0 25 emitter source uci chamber
Beam Temperature is larger than the 1100 in LAPDo C Emitter Temperature0.25” Emitter Source, UCI Chamber

400 eV, ΔE = 3.7 eV

600 eV, ΔE = 12.3 eV

800 eV, ΔE = 15.0 eV

ΔE/E = 2.0 % = const

Note: The low energy tail of the distribution is probably due to a field error around the grid wires, an effect that becomes more severe with increasing beam voltage.


Ion beam detector and analyzer for operation in lapd
Ion Beam Detector and Analyzer for Operation in in LAPDLAPD

  • Collector biased positive to reflect plasma ions.

  • Intermediate grid(s) biased negative to suppress plasma electrons. Caution: The Debye length is small compared to the grid holes during the active discharge: Double grids.

  • For sufficiently large pitch angles plasma components are shielded out geometrically.


Ion gun waveforms and analyzer signal in lapd 1 during active discharge 2 during afterglow
Ion Gun Waveforms and Analyzer Signal in LAPD in LAPD(1) During active discharge (2) During afterglow

Interferometer

signal

Beam extraction

voltage

Emitter current

Analyzer Signal


Lithium Ion Beam Profiles in LAPD

In LAPD

0.6” Emitter with 0.5 cm mask.

(a) Profile 5 cm from gun.

(b) and (c) Profiles at 32 cm

from gun after one cyclotron

orbit; Pitch angle = 280: Profiles

appear elliptical.

(b) At low plasma density in the

afterglow.

(c) At high density (> 1012 cm-3).

The beam is attenuated and the

centroid is shifted due to energy

loss and/or plasma potential

change: change in cyclotron

radius.


Transverse Li-Ion Beam Profile in LAPD in LAPDof 0.6” emitter with 0.5 cm aperture at 32 cm after 1 cyclotron period, pitch angle 28o


Emitter lifetimes shorter than anticipated
Emitter Lifetimes Shorter than Anticipated in LAPD

  • Manufacturer quoted for typical emission current:

    200 hrs.

  • Observed during operation in LAPD:

    20 hrs.

  • Mechanism for decreased lifetime needs to be investigated.

  • Potential mechanism: Electron bombardment.

    (Private communication, E. Wolfrum, Max-Planck-Institut für Plasma Physik, Garching)_


Fast Ion Beam Interaction with Alfv in LAPDén Waves in LAPD

  • Waves launched with current loops or disk antennas.

  • Wave field detected with 3 dim. dB/dt loops.

    Option I:

  • Single disk launches Alfvén cone.

  • Li ion beam with proper pitch angle transmitted through cone.

    Option II:

  • “Picture frame” antenna launches center wave.

  • Zero pitch angle beam transmitted on axis.


Saw antennae configuration and field pattern
SAW in LAPDAntennaeConfiguration and Field Pattern

Fig. 2. Picture frame antenna (provided by T. Carter’s group)

Fig. 1. 0.5 cm disk antenna (W Gekelman, S Vincena and D Leneman, Plasma Phys. Control. Fusion 39 (1997) A101–A112.)


Conclusion and further work
Conclusion in LAPDand Further Work

  • Two operational Lithium-6 ion sources with 0.6” and 0.25” diameter emitters developed.

  • First experiments performed at LAPD with quiescent and turbulent plasmas.

  • Further evaluation of emitter lifetime needed.

  • Development of in-house recoating of emitter material.


ad