Swift heavy ion-beam induced amorphization and recrystallization of yttrium iron garnet

被引:26
作者
Costantini, Jean-Marc [1 ]
Miro, Sandrine [2 ]
Beuneu, Francois [3 ]
Toulemonde, Marcel [4 ]
机构
[1] CEA, DEN, SRMA, F-91191 Gif Sur Yvette, France
[2] CEA, DEN, Serv Rech Met Phys, Lab JANNUS, F-91191 Gif Sur Yvette, France
[3] CEA CNRS Ecole Polytech, LSI, F-91128 Palaiseau, France
[4] CEA CNRS ENSICAEN, CIMAP GANIL, F-14070 Caen, France
关键词
iron garnets; swift heavy ion irradiations; Raman spectroscopy; electrical conductivity; THERMAL SPIKE MODEL; QUANTUM-MECHANICAL SIMULATION; EARTH ALUMINUM GARNETS; RAMAN-SPECTROSCOPY; NUCLEAR TRACKS; MAGNETIC INSULATORS; OPTICAL PHONONS; VIBRATIONAL SPECTROSCOPY; PYROPE GARNET; CROSS-SECTION;
D O I
10.1088/0953-8984/27/49/496001
中图分类号
O469 [凝聚态物理学];
学科分类号
070205 ;
摘要
Pure and (Ca and Si)-substituted yttrium iron garnet (Y3Fe5O12 or YIG) epitaxial layers and amorphous films on gadolinium gallium garnet (Gd3Ga5O12, or GGG) single crystal substrates were irradiated by 50 MeV Si-32 and 50 MeV (or 60 MeV) Cu-63 ions for electronic stopping powers larger than the threshold value (similar to 4 MeV mu m(-1)) for amorphous track formation in YIG crystals. Conductivity data of crystalline samples in a broad ion fluence range (10(11)-10(16) cm(-2)) are modeled with a set of rate equations corresponding to the amorphization and recrystallization induced in ion tracks by electronic excitations. The data for amorphous layers confirm that a recrystallization process takes place above similar to 10(14) cm(-2). Cross sections for both processes deduced from this analysis are discussed in comparison to previous determinations with reference to the inelastic thermal-spike model of track formation. Micro-Raman spectroscopy was also used to follow the related structural modifications. Raman spectra show the progressive vanishing and randomization of crystal phonon modes in relation to the ion-induced damage. For crystalline samples irradiated at high fluences (>= 10(14) cm(-2)), only two prominent broad bands remain like for amorphous films, thereby reflecting the phonon density of states of the disordered solid, regardless of samples and irradiation conditions. The main band peaked at similar to 660 cm(-1) is assigned to vibration modes of randomized bonds in tetrahedral (FeO4) units.
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页数:13
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