AustralieFrV1, PascalFrancis, Corpus, bibRecord, 001587

Morphology of swift heavy ion tracks in metallic glasses

Identifieur interne : 001587 ( PascalFrancis/Corpus ); précédent : 001586; suivant : 001588

Morphology of swift heavy ion tracks in metallic glasses

Auteurs : M. D. Rodriguez ; B. Afra ; C. Trautmann ; M. Toulemonde ; T. Bierschenk ; J. Leslie ; R. Giulian ; N. Kirby ; P. Kluth

Source :

Journal of non-crystalline solids [ 0022-3093 ] ; 2012.

RBID : Pascal:12-0102085

Descripteurs français

Pascal (Inist)
- Microstructure, Ion lourd, Irradiation ion, Rayonnement synchrotron, Diffusion RX centrale, Effet rayonnement, Fluence, Densité électron, Diffusion inélastique, Interaction électron phonon, Verre métallique, Alliage base fer, Métal transition alliage.

English descriptors

KwdEn :
- Electron density, Electron-phonon interactions, Fluence, Heavy ions, Inelastic scattering, Ion irradiation, Iron base alloys, Metallic glasses, Microstructure, Radiation effects, Small angle X ray scattering, Synchrotron radiation, Transition element alloys.

Abstract

Swift heavy ion irradiated metallic glasses were studied using synchrotron based small angle X-ray scattering (SAXS). Ribbons of Fe₈₀B₂₀, Fe₈₅ B₁₅, Fe₈₁B_13.5Si_3.5C₂ and Fe₄₀Ni₄₀B₂₀ were irradiated with 11.1 MeV/nucleon (MeV/u) ¹³²Xe, ¹⁵²S_m, ¹⁹⁷Au and 8.2 MeV/u ²³⁸U ions to fluences between 1 ×10¹⁰ and 1 × 10¹² ions/cm². The SAXS measurements provide evidence for the formation of ion tracks and allow a quantitative analysis of the track ensemble in all studied materials. The ion tracks have been well described by cylinders with abrupt boundaries and an electronic density change of (0.03 ± 0.01)% between track and matrix material. An inelastic thermal spike model was fitted to the experimental track radii to determine the critical energy density required to create an ion track. Despite the similar energy loss and track cross-sections, 30% higher track creation threshold is apparent for the binary alloys.

Notice en format standard (ISO 2709)

Pour connaître la documentation sur le format Inist Standard.

A01	`01`	`1`		`@0 0022-3093`
A02	`01`			`@0 JNCSBJ`
A03		`1`		`@0 J. non-cryst. solids`
A05				`@2 358`
A06				`@2 3`
A08	`01`	`1`	`ENG`	`@1 Morphology of swift heavy ion tracks in metallic glasses`
A11	`01`	`1`		`@1 RODRIGUEZ (M. D.)`
A11	`02`	`1`		`@1 AFRA (B.)`
A11	`03`	`1`		`@1 TRAUTMANN (C.)`
A11	`04`	`1`		`@1 TOULEMONDE (M.)`
A11	`05`	`1`		`@1 BIERSCHENK (T.)`
A11	`06`	`1`		`@1 LESLIE (J.)`
A11	`07`	`1`		`@1 GIULIAN (R.)`
A11	`08`	`1`		`@1 KIRBY (N.)`
A11	`09`	`1`		`@1 KLUTH (P.)`
A14	`01`			`@1 Research School of Physics and Engineering, The Australian National University @2 Canberra ACT 0200 @3 AUS @Z 1 aut. @Z 2 aut. @Z 5 aut. @Z 6 aut. @Z 7 aut. @Z 9 aut.`
A14	`02`			`@1 Gesellschaft für Schwerionenforschung (GSI) @2 64291 Darmstadt @3 DEU @Z 3 aut.`
A14	`03`			`@1 Centre interdisciplinaire de recherche sur les Ions, les Materiaux et la Photonique (CIMAP) @2 Caen @3 FRA @Z 4 aut.`
A14	`04`			`@1 Australian Synchrotron, Melbourne @2 VIC 3168 @3 AUS @Z 8 aut.`
A20				`@1 571-576`
A21				`@1 2012`
A23	`01`			`@0 ENG`
A43	`01`			`@1 INIST @2 14572 @5 354000508894280170`
A44				`@0 0000 @1 © 2012 INIST-CNRS. All rights reserved.`
A45				`@0 58 ref.`
A47	`01`	`1`		`@0 12-0102085`
A60				`@1 P`
A61				`@0 A`
A64	`01`	`1`		`@0 Journal of non-crystalline solids`
A66	`01`			`@0 GBR`
C01	`01`		`ENG`	@0 Swift heavy ion irradiated metallic glasses were studied using synchrotron based small angle X-ray scattering (SAXS). Ribbons of Fe₈₀B₂₀, Fe₈₅ B₁₅, Fe₈₁B_13.5Si_3.5C₂ and Fe₄₀Ni₄₀B₂₀ were irradiated with 11.1 MeV/nucleon (MeV/u) ¹³²Xe, ¹⁵²S_m, ¹⁹⁷Au and 8.2 MeV/u ²³⁸U ions to fluences between 1 ×10¹⁰ and 1 × 10¹² ions/cm². The SAXS measurements provide evidence for the formation of ion tracks and allow a quantitative analysis of the track ensemble in all studied materials. The ion tracks have been well described by cylinders with abrupt boundaries and an electronic density change of (0.03 ± 0.01)% between track and matrix material. An inelastic thermal spike model was fitted to the experimental track radii to determine the critical energy density required to create an ion track. Despite the similar energy loss and track cross-sections, 30% higher track creation threshold is apparent for the binary alloys.
C02	`01`	`3`		`@0 001B60A80J`
C03	`01`	`3`	`FRE`	`@0 Microstructure @5 02`
C03	`01`	`3`	`ENG`	`@0 Microstructure @5 02`
C03	`02`	`3`	`FRE`	`@0 Ion lourd @5 03`
C03	`02`	`3`	`ENG`	`@0 Heavy ions @5 03`
C03	`03`	`X`	`FRE`	`@0 Irradiation ion @5 04`
C03	`03`	`X`	`ENG`	`@0 Ion irradiation @5 04`
C03	`03`	`X`	`SPA`	`@0 Irradiación ión @5 04`
C03	`04`	`3`	`FRE`	`@0 Rayonnement synchrotron @5 05`
C03	`04`	`3`	`ENG`	`@0 Synchrotron radiation @5 05`
C03	`05`	`X`	`FRE`	`@0 Diffusion RX centrale @5 06`
C03	`05`	`X`	`ENG`	`@0 Small angle X ray scattering @5 06`
C03	`05`	`X`	`SPA`	`@0 Difusión rayo X central @5 06`
C03	`06`	`3`	`FRE`	`@0 Effet rayonnement @5 07`
C03	`06`	`3`	`ENG`	`@0 Radiation effects @5 07`
C03	`07`	`X`	`FRE`	`@0 Fluence @5 08`
C03	`07`	`X`	`ENG`	`@0 Fluence @5 08`
C03	`07`	`X`	`SPA`	`@0 Fluencia @5 08`
C03	`08`	`3`	`FRE`	`@0 Densité électron @5 09`
C03	`08`	`3`	`ENG`	`@0 Electron density @5 09`
C03	`09`	`3`	`FRE`	`@0 Diffusion inélastique @5 10`
C03	`09`	`3`	`ENG`	`@0 Inelastic scattering @5 10`
C03	`10`	`3`	`FRE`	`@0 Interaction électron phonon @5 11`
C03	`10`	`3`	`ENG`	`@0 Electron-phonon interactions @5 11`
C03	`11`	`3`	`FRE`	`@0 Verre métallique @5 15`
C03	`11`	`3`	`ENG`	`@0 Metallic glasses @5 15`
C03	`12`	`3`	`FRE`	`@0 Alliage base fer @2 NK @5 16`
C03	`12`	`3`	`ENG`	`@0 Iron base alloys @2 NK @5 16`
C03	`13`	`3`	`FRE`	`@0 Métal transition alliage @5 48`
C03	`13`	`3`	`ENG`	`@0 Transition element alloys @5 48`
N21				`@1 079`

Format Inist (serveur)

NO :	PASCAL 12-0102085 INIST
ET :	Morphology of swift heavy ion tracks in metallic glasses
AU :	RODRIGUEZ (M. D.); AFRA (B.); TRAUTMANN (C.); TOULEMONDE (M.); BIERSCHENK (T.); LESLIE (J.); GIULIAN (R.); KIRBY (N.); KLUTH (P.)
AF :	Research School of Physics and Engineering, The Australian National University/Canberra ACT 0200/Australie (1 aut., 2 aut., 5 aut., 6 aut., 7 aut., 9 aut.); Gesellschaft für Schwerionenforschung (GSI)/64291 Darmstadt/Allemagne (3 aut.); Centre interdisciplinaire de recherche sur les Ions, les Materiaux et la Photonique (CIMAP)/Caen/France (4 aut.); Australian Synchrotron, Melbourne/VIC 3168/Australie (8 aut.)
DT :	Publication en série; Niveau analytique
SO :	Journal of non-crystalline solids; ISSN 0022-3093; Coden JNCSBJ; Royaume-Uni; Da. 2012; Vol. 358; No. 3; Pp. 571-576; Bibl. 58 ref.
LA :	Anglais
EA :	Swift heavy ion irradiated metallic glasses were studied using synchrotron based small angle X-ray scattering (SAXS). Ribbons of Fe₈₀B₂₀, Fe₈₅ B₁₅, Fe₈₁B_13.5Si_3.5C₂ and Fe₄₀Ni₄₀B₂₀ were irradiated with 11.1 MeV/nucleon (MeV/u) ¹³²Xe, ¹⁵²S_m, ¹⁹⁷Au and 8.2 MeV/u ²³⁸U ions to fluences between 1 ×10¹⁰ and 1 × 10¹² ions/cm². The SAXS measurements provide evidence for the formation of ion tracks and allow a quantitative analysis of the track ensemble in all studied materials. The ion tracks have been well described by cylinders with abrupt boundaries and an electronic density change of (0.03 ± 0.01)% between track and matrix material. An inelastic thermal spike model was fitted to the experimental track radii to determine the critical energy density required to create an ion track. Despite the similar energy loss and track cross-sections, 30% higher track creation threshold is apparent for the binary alloys.
CC :	001B60A80J
FD :	Microstructure; Ion lourd; Irradiation ion; Rayonnement synchrotron; Diffusion RX centrale; Effet rayonnement; Fluence; Densité électron; Diffusion inélastique; Interaction électron phonon; Verre métallique; Alliage base fer; Métal transition alliage
ED :	Microstructure; Heavy ions; Ion irradiation; Synchrotron radiation; Small angle X ray scattering; Radiation effects; Fluence; Electron density; Inelastic scattering; Electron-phonon interactions; Metallic glasses; Iron base alloys; Transition element alloys
SD :	Irradiación ión; Difusión rayo X central; Fluencia
LO :	INIST-14572.354000508894280170
ID :	12-0102085

Links to Exploration step

Pascal:12-0102085

Le document en format XML

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<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Electron density</term>
<term>Electron-phonon interactions</term>
<term>Fluence</term>
<term>Heavy ions</term>
<term>Inelastic scattering</term>
<term>Ion irradiation</term>
<term>Iron base alloys</term>
<term>Metallic glasses</term>
<term>Microstructure</term>
<term>Radiation effects</term>
<term>Small angle X ray scattering</term>
<term>Synchrotron radiation</term>
<term>Transition element alloys</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Microstructure</term>
<term>Ion lourd</term>
<term>Irradiation ion</term>
<term>Rayonnement synchrotron</term>
<term>Diffusion RX centrale</term>
<term>Effet rayonnement</term>
<term>Fluence</term>
<term>Densité électron</term>
<term>Diffusion inélastique</term>
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<front><div type="abstract" xml:lang="en">Swift heavy ion irradiated metallic glasses were studied using synchrotron based small angle X-ray scattering (SAXS). Ribbons of Fe<sub>80</sub>
B<sub>20</sub>
, Fe<sub>85</sub>
 B<sub>15</sub>
, Fe<sub>81</sub>
B<sub>13.5</sub>
Si<sub>3.5</sub>
C<sub>2</sub>
 and Fe<sub>40</sub>
Ni<sub>40</sub>
B<sub>20</sub>
 were irradiated with 11.1 MeV/nucleon (MeV/u) <sup>132</sup>
Xe, <sup>152</sup>
S<sub>m</sub>
, <sup>197</sup>
Au and 8.2 MeV/u <sup>238</sup>
U ions to fluences between 1 ×10<sup>10</sup>
 and 1 × 10<sup> 12</sup>
 ions/cm<sup>2</sup>
. The SAXS measurements provide evidence for the formation of ion tracks and allow a quantitative analysis of the track ensemble in all studied materials. The ion tracks have been well described by cylinders with abrupt boundaries and an electronic density change of (0.03 ± 0.01)% between track and matrix material. An inelastic thermal spike model was fitted to the experimental track radii to determine the critical energy density required to create an ion track. Despite the similar energy loss and track cross-sections, 30% higher track creation threshold is apparent for the binary alloys.</div>
</front>
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<fA11 i1="04" i2="1"><s1>TOULEMONDE (M.)</s1>
</fA11>
<fA11 i1="05" i2="1"><s1>BIERSCHENK (T.)</s1>
</fA11>
<fA11 i1="06" i2="1"><s1>LESLIE (J.)</s1>
</fA11>
<fA11 i1="07" i2="1"><s1>GIULIAN (R.)</s1>
</fA11>
<fA11 i1="08" i2="1"><s1>KIRBY (N.)</s1>
</fA11>
<fA11 i1="09" i2="1"><s1>KLUTH (P.)</s1>
</fA11>
<fA14 i1="01"><s1>Research School of Physics and Engineering, The Australian National University</s1>
<s2>Canberra ACT 0200</s2>
<s3>AUS</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>5 aut.</sZ>
<sZ>6 aut.</sZ>
<sZ>7 aut.</sZ>
<sZ>9 aut.</sZ>
</fA14>
<fA14 i1="02"><s1>Gesellschaft für Schwerionenforschung (GSI)</s1>
<s2>64291 Darmstadt</s2>
<s3>DEU</s3>
<sZ>3 aut.</sZ>
</fA14>
<fA14 i1="03"><s1>Centre interdisciplinaire de recherche sur les Ions, les Materiaux et la Photonique (CIMAP)</s1>
<s2>Caen</s2>
<s3>FRA</s3>
<sZ>4 aut.</sZ>
</fA14>
<fA14 i1="04"><s1>Australian Synchrotron, Melbourne</s1>
<s2>VIC 3168</s2>
<s3>AUS</s3>
<sZ>8 aut.</sZ>
</fA14>
<fA20><s1>571-576</s1>
</fA20>
<fA21><s1>2012</s1>
</fA21>
<fA23 i1="01"><s0>ENG</s0>
</fA23>
<fA43 i1="01"><s1>INIST</s1>
<s2>14572</s2>
<s5>354000508894280170</s5>
</fA43>
<fA44><s0>0000</s0>
<s1>© 2012 INIST-CNRS. All rights reserved.</s1>
</fA44>
<fA45><s0>58 ref.</s0>
</fA45>
<fA47 i1="01" i2="1"><s0>12-0102085</s0>
</fA47>
<fA60><s1>P</s1>
</fA60>
<fA61><s0>A</s0>
</fA61>
<fA64 i1="01" i2="1"><s0>Journal of non-crystalline solids</s0>
</fA64>
<fA66 i1="01"><s0>GBR</s0>
</fA66>
<fC01 i1="01" l="ENG"><s0>Swift heavy ion irradiated metallic glasses were studied using synchrotron based small angle X-ray scattering (SAXS). Ribbons of Fe<sub>80</sub>
B<sub>20</sub>
, Fe<sub>85</sub>
 B<sub>15</sub>
, Fe<sub>81</sub>
B<sub>13.5</sub>
Si<sub>3.5</sub>
C<sub>2</sub>
 and Fe<sub>40</sub>
Ni<sub>40</sub>
B<sub>20</sub>
 were irradiated with 11.1 MeV/nucleon (MeV/u) <sup>132</sup>
Xe, <sup>152</sup>
S<sub>m</sub>
, <sup>197</sup>
Au and 8.2 MeV/u <sup>238</sup>
U ions to fluences between 1 ×10<sup>10</sup>
 and 1 × 10<sup> 12</sup>
 ions/cm<sup>2</sup>
. The SAXS measurements provide evidence for the formation of ion tracks and allow a quantitative analysis of the track ensemble in all studied materials. The ion tracks have been well described by cylinders with abrupt boundaries and an electronic density change of (0.03 ± 0.01)% between track and matrix material. An inelastic thermal spike model was fitted to the experimental track radii to determine the critical energy density required to create an ion track. Despite the similar energy loss and track cross-sections, 30% higher track creation threshold is apparent for the binary alloys.</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001B60A80J</s0>
</fC02>
<fC03 i1="01" i2="3" l="FRE"><s0>Microstructure</s0>
<s5>02</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG"><s0>Microstructure</s0>
<s5>02</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE"><s0>Ion lourd</s0>
<s5>03</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG"><s0>Heavy ions</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="X" l="FRE"><s0>Irradiation ion</s0>
<s5>04</s5>
</fC03>
<fC03 i1="03" i2="X" l="ENG"><s0>Ion irradiation</s0>
<s5>04</s5>
</fC03>
<fC03 i1="03" i2="X" l="SPA"><s0>Irradiación ión</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="3" l="FRE"><s0>Rayonnement synchrotron</s0>
<s5>05</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG"><s0>Synchrotron radiation</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="X" l="FRE"><s0>Diffusion RX centrale</s0>
<s5>06</s5>
</fC03>
<fC03 i1="05" i2="X" l="ENG"><s0>Small angle X ray scattering</s0>
<s5>06</s5>
</fC03>
<fC03 i1="05" i2="X" l="SPA"><s0>Difusión rayo X central</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Effet rayonnement</s0>
<s5>07</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Radiation effects</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="X" l="FRE"><s0>Fluence</s0>
<s5>08</s5>
</fC03>
<fC03 i1="07" i2="X" l="ENG"><s0>Fluence</s0>
<s5>08</s5>
</fC03>
<fC03 i1="07" i2="X" l="SPA"><s0>Fluencia</s0>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Densité électron</s0>
<s5>09</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Electron density</s0>
<s5>09</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Diffusion inélastique</s0>
<s5>10</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>Inelastic scattering</s0>
<s5>10</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE"><s0>Interaction électron phonon</s0>
<s5>11</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG"><s0>Electron-phonon interactions</s0>
<s5>11</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>Verre métallique</s0>
<s5>15</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG"><s0>Metallic glasses</s0>
<s5>15</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>Alliage base fer</s0>
<s2>NK</s2>
<s5>16</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG"><s0>Iron base alloys</s0>
<s2>NK</s2>
<s5>16</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE"><s0>Métal transition alliage</s0>
<s5>48</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG"><s0>Transition element alloys</s0>
<s5>48</s5>
</fC03>
<fN21><s1>079</s1>
</fN21>
</pA>
</standard>
<server><NO>PASCAL 12-0102085 INIST</NO>
<ET>Morphology of swift heavy ion tracks in metallic glasses</ET>
<AU>RODRIGUEZ (M. D.); AFRA (B.); TRAUTMANN (C.); TOULEMONDE (M.); BIERSCHENK (T.); LESLIE (J.); GIULIAN (R.); KIRBY (N.); KLUTH (P.)</AU>
<AF>Research School of Physics and Engineering, The Australian National University/Canberra ACT 0200/Australie (1 aut., 2 aut., 5 aut., 6 aut., 7 aut., 9 aut.); Gesellschaft für Schwerionenforschung (GSI)/64291 Darmstadt/Allemagne (3 aut.); Centre interdisciplinaire de recherche sur les Ions, les Materiaux et la Photonique (CIMAP)/Caen/France (4 aut.); Australian Synchrotron, Melbourne/VIC 3168/Australie (8 aut.)</AF>
<DT>Publication en série; Niveau analytique</DT>
<SO>Journal of non-crystalline solids; ISSN 0022-3093; Coden JNCSBJ; Royaume-Uni; Da. 2012; Vol. 358; No. 3; Pp. 571-576; Bibl. 58 ref.</SO>
<LA>Anglais</LA>
<EA>Swift heavy ion irradiated metallic glasses were studied using synchrotron based small angle X-ray scattering (SAXS). Ribbons of Fe<sub>80</sub>
B<sub>20</sub>
, Fe<sub>85</sub>
 B<sub>15</sub>
, Fe<sub>81</sub>
B<sub>13.5</sub>
Si<sub>3.5</sub>
C<sub>2</sub>
 and Fe<sub>40</sub>
Ni<sub>40</sub>
B<sub>20</sub>
 were irradiated with 11.1 MeV/nucleon (MeV/u) <sup>132</sup>
Xe, <sup>152</sup>
S<sub>m</sub>
, <sup>197</sup>
Au and 8.2 MeV/u <sup>238</sup>
U ions to fluences between 1 ×10<sup>10</sup>
 and 1 × 10<sup> 12</sup>
 ions/cm<sup>2</sup>
. The SAXS measurements provide evidence for the formation of ion tracks and allow a quantitative analysis of the track ensemble in all studied materials. The ion tracks have been well described by cylinders with abrupt boundaries and an electronic density change of (0.03 ± 0.01)% between track and matrix material. An inelastic thermal spike model was fitted to the experimental track radii to determine the critical energy density required to create an ion track. Despite the similar energy loss and track cross-sections, 30% higher track creation threshold is apparent for the binary alloys.</EA>
<CC>001B60A80J</CC>
<FD>Microstructure; Ion lourd; Irradiation ion; Rayonnement synchrotron; Diffusion RX centrale; Effet rayonnement; Fluence; Densité électron; Diffusion inélastique; Interaction électron phonon; Verre métallique; Alliage base fer; Métal transition alliage</FD>
<ED>Microstructure; Heavy ions; Ion irradiation; Synchrotron radiation; Small angle X ray scattering; Radiation effects; Fluence; Electron density; Inelastic scattering; Electron-phonon interactions; Metallic glasses; Iron base alloys; Transition element alloys</ED>
<SD>Irradiación ión; Difusión rayo X central; Fluencia</SD>
<LO>INIST-14572.354000508894280170</LO>
<ID>12-0102085</ID>
</server>
</inist>
</record>

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Morphology of swift heavy ion tracks in metallic glasses

Morphology of swift heavy ion tracks in metallic glasses

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