Swift heavy ion

Swift heavy ions are a special form of particle radiation for which electronic stopping dominates over nuclear stopping.[1] [2] They are accelerated in particle accelerators to very high energies, typically in the MeV or GeV range and have sufficient energy and mass to penetrate solids on a straight line. In many solids swift heavy ions release sufficient energy to induce permanently modified cylindrical zones, so-called ion tracks. If the irradiation is carried out in an initially crystalline material, ion tracks consist of an amorphous cylinder.[1] Ion tracks can be produced in many amorphizing materials, but not in pure metals, where the high electronic heat conductivity dissipates away the electronic heating before the ion track has time to form.

Mechanisms

Four atomic scale images of a SHI track in quartz at different times
Time evolution of a Molecular Dynamics simulation of a swift heavy ion track in crystalline quartz, producing a cylindrical amorphous track in the material. Image size 17 nm * 13 nm.

The mechanisms by which ion tracks are produced are subject to some debate. They can in some sense considered to produce thermal spikes [3][4] in the sense that they lead to strong lattice heating and a transient disordered atom zone. However, at least the initial stage of the damage might be better understood in terms of a Coulomb explosion mechanism .[5] Regardless of what the heating mechanism is, it is well established that swift heavy ions typically produce a long cylindrical track of damage in insulators ,[1][3] which has been shown to be underdense in the middle at least in SiO2 .[6]

Applications

Swift heavy ion tracks have several established and potential practical applications. Ion tracks in polymers can be etched to form a nanometer-thin channel through a polymer foil, so called track etch membranes. These are in industrial use.[7]

Irradiation of polyimide resists have potential to be used as templates for nanowire growth [8] Tracks can also be used to sputter materials [9] .[10] They can also be used to elongate nanocrystals embedded in materials [11] [12] .[13]

References

  1. 1 2 3 D. Kanjijal, Swift heavy ion-induced modification and track formation in materials, Current Science 80, 1560 (2001)
  2. ↑ M. Toulemonde, W. Assmann, C. Dufour, A. Meftah, F. Studer, and C. Trautmann, Experimental phenomena and thermal spike model description of ion tracks in amorphisable inorganic insulators, Mat. Fys. Medd. Kong. Dan. Vid. Selsk. 52, 263 (2006).
  3. 1 2 A. Meftah, F. Brisard, J. M. Costantini, E. Dooryhee, M. Hage-Ali, M. Hervieu, J. P. Stoquert, F. Studer, and M. Toulemonde, Track formation in SiO2 quartz and the thermal-spike mechanism, Phys. Rev. B 49, 12457 (1994)
  4. ↑ C. Trautmann, S. Klaumünzer, and H. Trinkaus, Effect of Stress on Track Formation in Amorphous Iron Boron Alloy: Ion tracks as Elastic Inclusion, Phys. Rev. Lett. 85, 3648 (2000)
  5. ↑ E. M. Bringa and R. E. Johnson, Coulomb Explosion and Thermal Spikes, Phys. Rev. Lett. 88, 165501 (2002)
  6. ↑ P. Kluth, C. S. Schnohr, O. H. Pakarinen, F. Djurabekova, D. J. Sprouster, R. Giulian, M. C. Ridgway, A. P. Byrne, C. Trautmann, D. J. Cookson, K. Nordlund, and M. Toulemonde, Fine structure in swift heavy ion tracks in amorphous SiO2, Phys. Rev. Lett. 101, 175503 (2008).
  7. ↑ P. Apel, Swift ion effects in polymers: industrial applications, Nucl. Instr. Meth. Phys. Res. B 208 (2003) 11
  8. ↑ M. Skupinski, M. Toulemonde, M. Lindeberg, and K. Hjort, Ion tracks developed in polyimide resist on Si wafers as templates for nanowires, Nucl. Instr. Meth. Phys. Res. B 240, 681 (2005).
  9. ↑ H. M. Urbassek, H. Kafemann, and R. E. Johnson, Atom ejection from a fast-ion track: A molecular-dynamics study, Phys. Rev. B 49, 786 (1994)
  10. ↑ M. Toulemonde, W. Assman, C. Trautmann, F. Gruner, H. D. Mieskes, H. Kucal, and Z. G. Wang, Electronic sputtering of metals and insulators by swift heavy ions, Nucl. Instr. Meth. Phys. Res. B 212, 346 (2003)
  11. ↑ C. D. Orléans, J. P. Stoquert, C. Estournès, J. J. Grob, D. Muller, J. L . Guille, M. Richard-Plouet, C. Cerruti, and F. Haas, Elongated Co nanoparticles induced by swift heavy ion irradiations, Nucl. Instr. Meth. Phys. Res. B 216, 372 (2004)
  12. ↑ M. C. Ridgway, P. Kluth, R. Giulian, D. J. Sprouster, L. L. Araujo, C. S. Schnohr, D. J. Llewellyn, A. P. Byrne, G. J. Foran, and D. J. Cookson, Changes in metal nanoparticle shape and size induced by swift heavy-ion irradiation, Nucl. Instr. Meth. Phys. Res. B 267, 931 (2009)
  13. ↑ K. Awazu, X. Wang, M. Fujimaki, J. Tominaga, H. Aiba, Y. Ohki, and T. Komatsubara, Elongation of gold nanoparticles in silica glass by irradiation with swift heavy ions, Phys. Rev. B 78, 054102 (2008).
This article is issued from Wikipedia - version of the 2/11/2013. The text is available under the Creative Commons Attribution/Share Alike but additional terms may apply for the media files.