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Rev. Sci. Instrum. 81, 043305 (2010); http://dx.doi.org/10.1063/1.3374123 (14 pages)

The DCU laser ion source

P. Yeates1, J. T. Costello1,2, and E. T. Kennedy1,2

1National Centre for Plasma Science and Technology (NCPST), Dublin, Ireland
2School of Physical Sciences, Dublin City University (DCU), Glasnevin, Ireland

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(Received 28 July 2009; accepted 8 March 2010; published online 27 April 2010)

Laser ion sources are used to generate and deliver highly charged ions of various masses and energies. We present details on the design and basic parameters of the DCU laser ion source (LIS). The theoretical aspects of a high voltage (HV) linear LIS are presented and the main issues surrounding laser-plasma formation, ion extraction and modeling of beam transport in relation to the operation of a LIS are detailed. A range of laser power densities (I ∼ 108–1011 W cm−2) and fluences (F = 0.1–3.9 kJ cm−2) from a Q-switched ruby laser (full-width half-maximum pulse duration ∼ 35 ns, λ = 694 nm) were used to generate a copper plasma. In “basic operating mode,” laser generated plasma ions are electrostatically accelerated using a dc HV bias (5–18 kV). A traditional einzel electrostatic lens system is utilized to transport and collimate the extracted ion beam for detection via a Faraday cup. Peak currents of up to I ∼ 600 μA for Cu+ to Cu3+ ions were recorded. The maximum collected charge reached 94 pC (Cu2+). Hydrodynamic simulations and ion probe diagnostics were used to study the plasma plume within the extraction gap. The system measured performance and electrodynamic simulations indicated that the use of a short field-free (L = 48 mm) region results in rapid expansion of the injected ion beam in the drift tube. This severely limits the efficiency of the electrostatic lens system and consequently the sources performance. Simulations of ion beam dynamics in a “continuous einzel array” were performed and experimentally verified to counter the strong space-charge force present in the ion beam which results from plasma extraction close to the target surface. Ion beam acceleration and injection thus occur at “high pressure.” In “enhanced operating mode,” peak currents of 3.26 mA (Cu2+) were recorded. The collected currents of more highly charged ions (Cu4+–Cu6+) increased considerably in this mode of operation.

© 2010 American Institute of Physics

Article Outline

  1. INTRODUCTION
  2. LASER ION SOURCES: GENERAL OVERVIEW
  3. LASER ION SOURCES: GENERAL PRINCIPLES
    1. Plasma generation and expansion
    2. Extraction dynamics
    3. Ion beam transport
  4. EXPERIMENTAL SETUP
  5. BASIC OPERATIONAL PERFORMANCE
  6. PLASMA SIMULATION AND BEAM TRANSPORT MODELING
    1. MEDUSA simulations
    2. Ion probe measurements
    3. SIMION simulations
  7. ENHANCED OPERATIONAL PERFORMANCE
  8. DISCUSSION
  9. CONCLUSION

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KEYWORDS and PACS

PACS

  • 52.50.Jm

    Plasma production and heating by laser beams (laser-foil, laser-cluster, etc.)

  • 52.50.Dg

    Plasma sources

  • 52.40.Mj

    Particle beam interactions in plasmas

  • 52.70.-m

    Plasma diagnostic techniques and instrumentation

ARTICLE DATA

PUBLICATION DATA

ISSN

0034-6748 (print)  
1089-7623 (online)

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