Simulation of Silicon Irradiation with C60 Ions: Unveiling the Role of the Interaction Potential

Molecular dynamic simulation was used to study the processes of molecular 2 to 14 keV C60 ion impact on the (100) Si surface at 0 to 1000 K. Tersoff-ZBL and Airebo interaction potentials were used, and electronic energy loss were taken into account as quasifriction force for fast particles. It is sh...

Ausführliche Beschreibung

Gespeichert in:
Bibliographische Detailangaben
Veröffentlicht in:Surface investigation, x-ray, synchrotron and neutron techniques x-ray, synchrotron and neutron techniques, 2024-04, Vol.18 (2), p.433-438
Hauptverfasser: Karasev, K. P., Strizhkin, D. A., Titov, A. I., Karaseov, P. A.
Format: Artikel
Sprache:eng
Schlagworte:
Online-Zugang:Volltext
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
container_end_page 438
container_issue 2
container_start_page 433
container_title Surface investigation, x-ray, synchrotron and neutron techniques
container_volume 18
creator Karasev, K. P.
Strizhkin, D. A.
Titov, A. I.
Karaseov, P. A.
description Molecular dynamic simulation was used to study the processes of molecular 2 to 14 keV C60 ion impact on the (100) Si surface at 0 to 1000 K. Tersoff-ZBL and Airebo interaction potentials were used, and electronic energy loss were taken into account as quasifriction force for fast particles. It is shown that, when single impact events are simulated, the target temperature does not affect the development of the displacement cascade but affects its thermalization and the formation of the crater on the surface. As the energy increases, the carbon penetration depth, the size of the formed crater, and the size of the rim increase. The sputtering coefficient of silicon atoms in this case increases linearly with energy, while for carbon atoms it reaches a steady-state value at 10 keV. A higher number of atomized carbon atoms in single impact events is found using the Tersoff potential compared to the Airebo potential. In the event of cumulative events, the formation of an etch pit is observed at the initial stage followed by carbon film growth. In the case of cumulative ion accumulation, the use of the Airebo potential yields a higher sputtering coefficient than the use of the Tersoff potential. The formation of carbide bonds in the crystal and the increase in their concentration with ion fluence slightly reduce the number of sputtered particles. Therefore, for the correct comparison of simulation results with experiment it is not enough to use the results of single impact event analysis. It is necessary to perform cumulative fluence accumulation simulation.
doi_str_mv 10.1134/S1027451024020319
format Article
fullrecord <record><control><sourceid>proquest_cross</sourceid><recordid>TN_cdi_proquest_journals_3052080869</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>3052080869</sourcerecordid><originalsourceid>FETCH-LOGICAL-c268t-cc8bbdd8b8121f01318b21aab69a35fe90f30bf4dc45bd7530b02e821b0f6c1a3</originalsourceid><addsrcrecordid>eNp1kE1PwzAMhiMEEmPwA7hV4lxwkn6k3NDER6VJIMbOJUmTLVOXjKQD8e9JKRIHxMV-bb-PLRmhcwyXGNPsaoGBlFkeYwYEKK4O0AQzXKUlVNlh1HGcDvNjdBLCBiAvaV5M0OvCbPcd742zidPJwnRGRll7z1sztj9Mv05mBSS1s-E6Wdp3FV12lfRrlTy7Tg3goGvbK8_lN_TkemV7w7tTdKR5F9TZT56i5d3ty-whnT_e17ObeSpJwfpUSiZE2zLBMMEaMMVMEMy5KCpOc60q0BSEzlqZ5aIt81gAUYxgAbqQmNMpuhj37rx726vQNxu39zaebCjkBBiwooouPLqkdyF4pZudN1vuPxsMzfDI5s8jI0NGJkSvXSn_u_l_6AtuMHRu</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>3052080869</pqid></control><display><type>article</type><title>Simulation of Silicon Irradiation with C60 Ions: Unveiling the Role of the Interaction Potential</title><source>SpringerNature Journals</source><creator>Karasev, K. P. ; Strizhkin, D. A. ; Titov, A. I. ; Karaseov, P. A.</creator><creatorcontrib>Karasev, K. P. ; Strizhkin, D. A. ; Titov, A. I. ; Karaseov, P. A.</creatorcontrib><description>Molecular dynamic simulation was used to study the processes of molecular 2 to 14 keV C60 ion impact on the (100) Si surface at 0 to 1000 K. Tersoff-ZBL and Airebo interaction potentials were used, and electronic energy loss were taken into account as quasifriction force for fast particles. It is shown that, when single impact events are simulated, the target temperature does not affect the development of the displacement cascade but affects its thermalization and the formation of the crater on the surface. As the energy increases, the carbon penetration depth, the size of the formed crater, and the size of the rim increase. The sputtering coefficient of silicon atoms in this case increases linearly with energy, while for carbon atoms it reaches a steady-state value at 10 keV. A higher number of atomized carbon atoms in single impact events is found using the Tersoff potential compared to the Airebo potential. In the event of cumulative events, the formation of an etch pit is observed at the initial stage followed by carbon film growth. In the case of cumulative ion accumulation, the use of the Airebo potential yields a higher sputtering coefficient than the use of the Tersoff potential. The formation of carbide bonds in the crystal and the increase in their concentration with ion fluence slightly reduce the number of sputtered particles. Therefore, for the correct comparison of simulation results with experiment it is not enough to use the results of single impact event analysis. It is necessary to perform cumulative fluence accumulation simulation.</description><identifier>ISSN: 1027-4510</identifier><identifier>EISSN: 1819-7094</identifier><identifier>DOI: 10.1134/S1027451024020319</identifier><language>eng</language><publisher>Moscow: Pleiades Publishing</publisher><subject>Accumulation ; Atomic properties ; Atomizing ; Atoms &amp; subatomic particles ; Buckminsterfullerene ; Carbon ; Chemistry and Materials Science ; Etch pits ; Film growth ; Fluence ; Impact analysis ; Ion impact ; Materials Science ; Molecular dynamics ; Penetration depth ; Silicon ; Simulation ; Sputtering ; Surfaces and Interfaces ; Thermalization (energy absorption) ; Thin Films</subject><ispartof>Surface investigation, x-ray, synchrotron and neutron techniques, 2024-04, Vol.18 (2), p.433-438</ispartof><rights>Pleiades Publishing, Ltd. 2024. ISSN 1027-4510, Journal of Surface Investigation: X-ray, Synchrotron and Neutron Techniques, 2024, Vol. 18, No. 2, pp. 433–438. © Pleiades Publishing, Ltd., 2024.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c268t-cc8bbdd8b8121f01318b21aab69a35fe90f30bf4dc45bd7530b02e821b0f6c1a3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1134/S1027451024020319$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1134/S1027451024020319$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>314,780,784,27924,27925,41488,42557,51319</link.rule.ids></links><search><creatorcontrib>Karasev, K. P.</creatorcontrib><creatorcontrib>Strizhkin, D. A.</creatorcontrib><creatorcontrib>Titov, A. I.</creatorcontrib><creatorcontrib>Karaseov, P. A.</creatorcontrib><title>Simulation of Silicon Irradiation with C60 Ions: Unveiling the Role of the Interaction Potential</title><title>Surface investigation, x-ray, synchrotron and neutron techniques</title><addtitle>J. Surf. Investig</addtitle><description>Molecular dynamic simulation was used to study the processes of molecular 2 to 14 keV C60 ion impact on the (100) Si surface at 0 to 1000 K. Tersoff-ZBL and Airebo interaction potentials were used, and electronic energy loss were taken into account as quasifriction force for fast particles. It is shown that, when single impact events are simulated, the target temperature does not affect the development of the displacement cascade but affects its thermalization and the formation of the crater on the surface. As the energy increases, the carbon penetration depth, the size of the formed crater, and the size of the rim increase. The sputtering coefficient of silicon atoms in this case increases linearly with energy, while for carbon atoms it reaches a steady-state value at 10 keV. A higher number of atomized carbon atoms in single impact events is found using the Tersoff potential compared to the Airebo potential. In the event of cumulative events, the formation of an etch pit is observed at the initial stage followed by carbon film growth. In the case of cumulative ion accumulation, the use of the Airebo potential yields a higher sputtering coefficient than the use of the Tersoff potential. The formation of carbide bonds in the crystal and the increase in their concentration with ion fluence slightly reduce the number of sputtered particles. Therefore, for the correct comparison of simulation results with experiment it is not enough to use the results of single impact event analysis. It is necessary to perform cumulative fluence accumulation simulation.</description><subject>Accumulation</subject><subject>Atomic properties</subject><subject>Atomizing</subject><subject>Atoms &amp; subatomic particles</subject><subject>Buckminsterfullerene</subject><subject>Carbon</subject><subject>Chemistry and Materials Science</subject><subject>Etch pits</subject><subject>Film growth</subject><subject>Fluence</subject><subject>Impact analysis</subject><subject>Ion impact</subject><subject>Materials Science</subject><subject>Molecular dynamics</subject><subject>Penetration depth</subject><subject>Silicon</subject><subject>Simulation</subject><subject>Sputtering</subject><subject>Surfaces and Interfaces</subject><subject>Thermalization (energy absorption)</subject><subject>Thin Films</subject><issn>1027-4510</issn><issn>1819-7094</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><recordid>eNp1kE1PwzAMhiMEEmPwA7hV4lxwkn6k3NDER6VJIMbOJUmTLVOXjKQD8e9JKRIHxMV-bb-PLRmhcwyXGNPsaoGBlFkeYwYEKK4O0AQzXKUlVNlh1HGcDvNjdBLCBiAvaV5M0OvCbPcd742zidPJwnRGRll7z1sztj9Mv05mBSS1s-E6Wdp3FV12lfRrlTy7Tg3goGvbK8_lN_TkemV7w7tTdKR5F9TZT56i5d3ty-whnT_e17ObeSpJwfpUSiZE2zLBMMEaMMVMEMy5KCpOc60q0BSEzlqZ5aIt81gAUYxgAbqQmNMpuhj37rx726vQNxu39zaebCjkBBiwooouPLqkdyF4pZudN1vuPxsMzfDI5s8jI0NGJkSvXSn_u_l_6AtuMHRu</recordid><startdate>20240401</startdate><enddate>20240401</enddate><creator>Karasev, K. P.</creator><creator>Strizhkin, D. A.</creator><creator>Titov, A. I.</creator><creator>Karaseov, P. A.</creator><general>Pleiades Publishing</general><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>20240401</creationdate><title>Simulation of Silicon Irradiation with C60 Ions: Unveiling the Role of the Interaction Potential</title><author>Karasev, K. P. ; Strizhkin, D. A. ; Titov, A. I. ; Karaseov, P. A.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c268t-cc8bbdd8b8121f01318b21aab69a35fe90f30bf4dc45bd7530b02e821b0f6c1a3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2024</creationdate><topic>Accumulation</topic><topic>Atomic properties</topic><topic>Atomizing</topic><topic>Atoms &amp; subatomic particles</topic><topic>Buckminsterfullerene</topic><topic>Carbon</topic><topic>Chemistry and Materials Science</topic><topic>Etch pits</topic><topic>Film growth</topic><topic>Fluence</topic><topic>Impact analysis</topic><topic>Ion impact</topic><topic>Materials Science</topic><topic>Molecular dynamics</topic><topic>Penetration depth</topic><topic>Silicon</topic><topic>Simulation</topic><topic>Sputtering</topic><topic>Surfaces and Interfaces</topic><topic>Thermalization (energy absorption)</topic><topic>Thin Films</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Karasev, K. P.</creatorcontrib><creatorcontrib>Strizhkin, D. A.</creatorcontrib><creatorcontrib>Titov, A. I.</creatorcontrib><creatorcontrib>Karaseov, P. A.</creatorcontrib><collection>CrossRef</collection><jtitle>Surface investigation, x-ray, synchrotron and neutron techniques</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Karasev, K. P.</au><au>Strizhkin, D. A.</au><au>Titov, A. I.</au><au>Karaseov, P. A.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Simulation of Silicon Irradiation with C60 Ions: Unveiling the Role of the Interaction Potential</atitle><jtitle>Surface investigation, x-ray, synchrotron and neutron techniques</jtitle><stitle>J. Surf. Investig</stitle><date>2024-04-01</date><risdate>2024</risdate><volume>18</volume><issue>2</issue><spage>433</spage><epage>438</epage><pages>433-438</pages><issn>1027-4510</issn><eissn>1819-7094</eissn><abstract>Molecular dynamic simulation was used to study the processes of molecular 2 to 14 keV C60 ion impact on the (100) Si surface at 0 to 1000 K. Tersoff-ZBL and Airebo interaction potentials were used, and electronic energy loss were taken into account as quasifriction force for fast particles. It is shown that, when single impact events are simulated, the target temperature does not affect the development of the displacement cascade but affects its thermalization and the formation of the crater on the surface. As the energy increases, the carbon penetration depth, the size of the formed crater, and the size of the rim increase. The sputtering coefficient of silicon atoms in this case increases linearly with energy, while for carbon atoms it reaches a steady-state value at 10 keV. A higher number of atomized carbon atoms in single impact events is found using the Tersoff potential compared to the Airebo potential. In the event of cumulative events, the formation of an etch pit is observed at the initial stage followed by carbon film growth. In the case of cumulative ion accumulation, the use of the Airebo potential yields a higher sputtering coefficient than the use of the Tersoff potential. The formation of carbide bonds in the crystal and the increase in their concentration with ion fluence slightly reduce the number of sputtered particles. Therefore, for the correct comparison of simulation results with experiment it is not enough to use the results of single impact event analysis. It is necessary to perform cumulative fluence accumulation simulation.</abstract><cop>Moscow</cop><pub>Pleiades Publishing</pub><doi>10.1134/S1027451024020319</doi><tpages>6</tpages></addata></record>
fulltext fulltext
identifier ISSN: 1027-4510
ispartof Surface investigation, x-ray, synchrotron and neutron techniques, 2024-04, Vol.18 (2), p.433-438
issn 1027-4510
1819-7094
language eng
recordid cdi_proquest_journals_3052080869
source SpringerNature Journals
subjects Accumulation
Atomic properties
Atomizing
Atoms & subatomic particles
Buckminsterfullerene
Carbon
Chemistry and Materials Science
Etch pits
Film growth
Fluence
Impact analysis
Ion impact
Materials Science
Molecular dynamics
Penetration depth
Silicon
Simulation
Sputtering
Surfaces and Interfaces
Thermalization (energy absorption)
Thin Films
title Simulation of Silicon Irradiation with C60 Ions: Unveiling the Role of the Interaction Potential
url https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-02T22%3A57%3A36IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Simulation%20of%20Silicon%20Irradiation%20with%20C60%20Ions:%20Unveiling%20the%20Role%20of%20the%20Interaction%20Potential&rft.jtitle=Surface%20investigation,%20x-ray,%20synchrotron%20and%20neutron%20techniques&rft.au=Karasev,%20K.%20P.&rft.date=2024-04-01&rft.volume=18&rft.issue=2&rft.spage=433&rft.epage=438&rft.pages=433-438&rft.issn=1027-4510&rft.eissn=1819-7094&rft_id=info:doi/10.1134/S1027451024020319&rft_dat=%3Cproquest_cross%3E3052080869%3C/proquest_cross%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_pqid=3052080869&rft_id=info:pmid/&rfr_iscdi=true