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Mendoza, C., S. Peuget, T. Charpentier, M. Moskura, R. Caraballo, O. Bouty, A. H. Mir, I. Monnet, C. Grygiel, and C. Jegou. "Oxide glass structure evolution under swift heavy ion irradiation." Nuclear
Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Kluth, P.; Schnohr, C. S.; Pakarinen, O. H.; Djurabekova, F.; Sprouster, D. J.; Giulian, R.; Ridgway, M. C.; Byrne, A. P.; Trautmann, C.; Cookson, D. J.; Nordlund, K.; Toulemonde, M. (24 October 2008). "Fine
Structure in Swift Heavy Ion Tracks in AmorphousSiO2".
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mechanism. Regardless of what the heating mechanism is, it is well established that swift heavy ions typically produce a long nearly cylindrical track of damage in insulators, which has been shown to be underdense in the middle, at least in
753:
D’Orléans, C.; Stoquert, J.P.; Estournès, C.; Grob, J.J.; Muller, D.; Guille, J.L.; Richard-Plouet, M.; Cerruti, C.; Haas, F. (2004). "Elongated Co nanoparticles induced by swift heavy ion irradiations".
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growth. Tracks can also be used to sputter materials. They can also be used to elongate nanocrystals embedded in materials. SHI irradiation can also be used for structural modification of nanomaterials.
46:
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
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Kaniukov, E Yu; Ustarroz, J; Yakimchuk, D V; Petrova, M; Terryn, H; Sivakov, V; Petrov, A V (15 February 2016). "Tunable nanoporous silicon oxide templates by swift heavy ion tracks technology".
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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
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Lang, Maik; Djurabekova, Flyura; Medvedev, Nikita; Toulemonde, Marcel; Trautmann, Christina (2020). "Fundamental
Phenomena and Applications of Swift Heavy Ion Irradiations".
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Structural, functional and magnetic ordering modifications in graphene oxide and graphite by 100 MeV gold ion irradiation, Vacuum, Volume 182, December 2020, 109700, DOI:
710:
Toulemonde, M.; Assmann, W.; Trautmann, C.; Grüner, F.; Mieskes, H.D.; Kucal, H.; Wang, Z.G. (2003). "Electronic sputtering of metals and insulators by swift heavy ions".
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Meftah, A.; Brisard, F.; Costantini, J. M.; Dooryhee, E.; Hage-Ali, M.; Hervieu, M.; Stoquert, J. P.; Studer, F.; Toulemonde, M. (1 April 1994). "Track formation in SiO
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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
624:
Skupinski, Marek; Toulemonde, Marcel; Lindeberg, Mikael; Hjort, Klas (2005). "Ion tracks developed in polyimide resist on Si wafers as template for nanowires".
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Ridgway, M.C.; Kluth, P.; Giulian, R.; Sprouster, D.J.; Araujo, L.L.; Schnohr, C.S.; Llewellyn, D.J.; Byrne, A.P.; Foran, G.J.; Cookson, D.J. (2009).
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divided by the mass of the atomic nucleus, written "MeV/u". In order for an ion beam to be considered "swift", the constituent ions should be
202:
M. Toulemonde, W. Assmann, C. Dufour, A. Meftah, F. Studer, and C. Trautmann, Experimental phenomena and thermal spike model description of
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Awazu, Koichi; Wang, Xiaomin; Fujimaki, Makoto; Tominaga, Junji; Aiba, Hirohiko; Ohki, Yoshimichi; Komatsubara, Tetsuro (6 August 2008).
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27:
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Urbassek, H. M.; Kafemann, H.; Johnson, R. E. (1 December 1993). "Atom ejection from a fast-ion track: A molecular-dynamics study".
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in crystalline quartz, producing a cylindrical amorphous track in the material. Image size 17 nm × 13 nm.
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Nuclear
Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Nuclear
Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Nuclear
Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Nuclear
Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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335:"Effect of Stress on Track Formation in Amorphous Iron Boron Alloy: Ion Tracks as Elastic Inclusions"
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in amorphisable inorganic insulators, Mat. Fys. Medd. Kong. Dan. Vid. Selsk. 52, 263 (2006).
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or heavier, and the energy such that the beam particles have a velocity comparable to the
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846:"Elongation of gold nanoparticles in silica glass by irradiation with swift heavy ions"
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Bringa, E. M.; Johnson, R. E. (4 April 2002). "Coulomb
Explosion and Thermal Spikes".
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799:"Changes in metal nanoparticle shape and size induced by swift heavy-ion irradiation"
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Apel, P. (2003). "Swift ion effects in polymers: industrial applications".
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are produced are subject to some debate. They can be considered to produce
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179:"Swift heavy ion-induced modification and track formation in materials"
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Heavy ion beams are generally described in terms of their energy in
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Trautmann, C.; Klaumünzer, S.; Trinkaus, H. (23 October 2000).
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have several established and potential practical applications.
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290:(18). American Physical Society (APS): 12457–12463.
150:resists have potential to be used as templates for
348:(17). American Physical Society (APS): 3648–3651.
675:(2). American Physical Society (APS): 786–795.
469:(17). American Physical Society (APS): 175503.
399:(16). American Physical Society (APS): 165501.
856:(5). American Physical Society (APS): 054102.
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902:https://doi.org/10.1016/j.vacuum.2020.109700
915:https://doi.org/10.1016/j.nimb.2014.02.002
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22:are the components of a type of
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143:. These are in industrial use.
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530:(11). IOP Publishing: 115305.
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732:10.1016/s0168-583x(03)01721-x
603:10.1016/s0168-583x(03)00634-7
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26:with high enough energy that
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809:(6). Elsevier BV: 931–935.
632:(3). Elsevier BV: 681–689.
362:10.1103/physrevlett.85.3648
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823:10.1016/j.nimb.2009.02.025
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34:. They are accelerated in
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72:Mega electron volts (MeV)
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220:: 485–516.
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927:Categories
227:2001.03711
204:ion tracks
159:References
137:Ion tracks
133:ion tracks
108:ion tracks
66:Definition
56:Ion tracks
52:ion tracks
48:ion tracks
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312:0163-1829
262:210165042
148:polyimide
100:ion track
60:ion track
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152:nanowire
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