Secondary ion mass spectrometry depth profiling of ultrashallow phosphorous in silicon
High-precision quantitative secondary ion mass spectrometry (SIMS) trace analyses of ultrashallow 31 P distributions in Si (i.e., junction depths of 50 nm or less) require the ability to eliminate the 30 Si 1 H mass interference while simultaneously minimizing primary ion impact energy and maximizin...
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Veröffentlicht in: | Journal of Vacuum Science & Technology B: Microelectronics and Nanometer Structures 2000-01, Vol.18 (1), p.509-513 |
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container_title | Journal of Vacuum Science & Technology B: Microelectronics and Nanometer Structures |
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creator | Loesing, R. Guryanov, G. M. Hunter, J. L. Griffis, D. P. |
description | High-precision quantitative secondary ion mass spectrometry (SIMS) trace analyses of ultrashallow
31
P
distributions in Si (i.e., junction depths of 50 nm or less) require the ability to eliminate the
30
Si
1
H
mass interference while simultaneously minimizing primary ion impact energy and maximizing sensitivity. Elimination of
30
Si
1
H
requires a relatively high mass resolution SIMS instrument such as the Cameca IMS-6f used in this work. A range of
Cs
+
primary ion energies ranging from 9.5 to 1.6 keV was investigated to determine which provided the best depth resolution as measured by decay length for ultrashallow depth profiles of 2 keV P in Si. Improvements (or lack thereof) in decay length as the primary ion impact energy was reduced were correlated with crater bottom roughness measurements. Changes in the ion yields of P and Si resulting from both the appreciable fraction of the analyzed depth made up of the surface native oxide and also from the depth required for the primary ion yield enhancing
Cs
+
to reach a constant level were also investigated utilizing bulk-doped P in Si. The resulting ion yield transients obtained were then used to generate an empirical correction function with the aim of improving the quantitative accuracy of the ultrashallow depth profile selected as having the minimum decay length obtained in this work. Finally, improvements in the P detection limit provided by optimization of the secondary ion postacceleration system are discussed. |
doi_str_mv | 10.1116/1.591222 |
format | Article |
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31
P
distributions in Si (i.e., junction depths of 50 nm or less) require the ability to eliminate the
30
Si
1
H
mass interference while simultaneously minimizing primary ion impact energy and maximizing sensitivity. Elimination of
30
Si
1
H
requires a relatively high mass resolution SIMS instrument such as the Cameca IMS-6f used in this work. A range of
Cs
+
primary ion energies ranging from 9.5 to 1.6 keV was investigated to determine which provided the best depth resolution as measured by decay length for ultrashallow depth profiles of 2 keV P in Si. Improvements (or lack thereof) in decay length as the primary ion impact energy was reduced were correlated with crater bottom roughness measurements. Changes in the ion yields of P and Si resulting from both the appreciable fraction of the analyzed depth made up of the surface native oxide and also from the depth required for the primary ion yield enhancing
Cs
+
to reach a constant level were also investigated utilizing bulk-doped P in Si. The resulting ion yield transients obtained were then used to generate an empirical correction function with the aim of improving the quantitative accuracy of the ultrashallow depth profile selected as having the minimum decay length obtained in this work. Finally, improvements in the P detection limit provided by optimization of the secondary ion postacceleration system are discussed.</description><identifier>ISSN: 0734-211X</identifier><identifier>ISSN: 1071-1023</identifier><identifier>EISSN: 1520-8567</identifier><identifier>DOI: 10.1116/1.591222</identifier><identifier>CODEN: JVTBD9</identifier><language>eng</language><subject>Ion implantation ; Phosphorus ; Silicon ; Surface roughness</subject><ispartof>Journal of Vacuum Science & Technology B: Microelectronics and Nanometer Structures, 2000-01, Vol.18 (1), p.509-513</ispartof><rights>American Vacuum Society</rights><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c325t-f36d13a3618b23bc45a1e5c72233bedd952ba083639c266e695701121bc38293</citedby><cites>FETCH-LOGICAL-c325t-f36d13a3618b23bc45a1e5c72233bedd952ba083639c266e695701121bc38293</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>309,310,314,780,784,789,790,794,4512,23930,23931,25140,27924,27925</link.rule.ids></links><search><creatorcontrib>Loesing, R.</creatorcontrib><creatorcontrib>Guryanov, G. M.</creatorcontrib><creatorcontrib>Hunter, J. L.</creatorcontrib><creatorcontrib>Griffis, D. P.</creatorcontrib><title>Secondary ion mass spectrometry depth profiling of ultrashallow phosphorous in silicon</title><title>Journal of Vacuum Science & Technology B: Microelectronics and Nanometer Structures</title><description>High-precision quantitative secondary ion mass spectrometry (SIMS) trace analyses of ultrashallow
31
P
distributions in Si (i.e., junction depths of 50 nm or less) require the ability to eliminate the
30
Si
1
H
mass interference while simultaneously minimizing primary ion impact energy and maximizing sensitivity. Elimination of
30
Si
1
H
requires a relatively high mass resolution SIMS instrument such as the Cameca IMS-6f used in this work. A range of
Cs
+
primary ion energies ranging from 9.5 to 1.6 keV was investigated to determine which provided the best depth resolution as measured by decay length for ultrashallow depth profiles of 2 keV P in Si. Improvements (or lack thereof) in decay length as the primary ion impact energy was reduced were correlated with crater bottom roughness measurements. Changes in the ion yields of P and Si resulting from both the appreciable fraction of the analyzed depth made up of the surface native oxide and also from the depth required for the primary ion yield enhancing
Cs
+
to reach a constant level were also investigated utilizing bulk-doped P in Si. The resulting ion yield transients obtained were then used to generate an empirical correction function with the aim of improving the quantitative accuracy of the ultrashallow depth profile selected as having the minimum decay length obtained in this work. Finally, improvements in the P detection limit provided by optimization of the secondary ion postacceleration system are discussed.</description><subject>Ion implantation</subject><subject>Phosphorus</subject><subject>Silicon</subject><subject>Surface roughness</subject><issn>0734-211X</issn><issn>1071-1023</issn><issn>1520-8567</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2000</creationdate><recordtype>article</recordtype><recordid>eNp90E1LxDAQBuAgCq6r4E_ITT1UM0mTtkdZ_IIFDy7iLaRp6la6Tc1kFf-9kcpeBA9hIDy8zLyEnAK7BAB1BZeyAs75HpmB5CwrpSr2yYwVIs84wMshOUJ8Y4wpKcSMPD8564fGhC_a-YFuDCLF0dkY_MbF9Nu4Ma7pGHzb9d3wSn1Lt30MBtem7_0nHdce0wt-i7QbKCaVAo_JQWt6dCe_c05WtzerxX22fLx7WFwvMyu4jFkrVAPCCAVlzUVtc2nASVtwLkTtmqaSvDasFEpUlivlVCULBsChtqLklZiTsyk27fe-dRj1pkPr-t4MLi2ki1yqvJBMJXk-SRs8YnCtHkO3SWdrYPqnOA16Ki7Ri4mi7aKJqZad_fBh5_TYtP_ZP7nfCdp8Sw</recordid><startdate>200001</startdate><enddate>200001</enddate><creator>Loesing, R.</creator><creator>Guryanov, G. M.</creator><creator>Hunter, J. L.</creator><creator>Griffis, D. P.</creator><scope>AAYXX</scope><scope>CITATION</scope><scope>7TC</scope></search><sort><creationdate>200001</creationdate><title>Secondary ion mass spectrometry depth profiling of ultrashallow phosphorous in silicon</title><author>Loesing, R. ; Guryanov, G. M. ; Hunter, J. L. ; Griffis, D. P.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c325t-f36d13a3618b23bc45a1e5c72233bedd952ba083639c266e695701121bc38293</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2000</creationdate><topic>Ion implantation</topic><topic>Phosphorus</topic><topic>Silicon</topic><topic>Surface roughness</topic><toplevel>online_resources</toplevel><creatorcontrib>Loesing, R.</creatorcontrib><creatorcontrib>Guryanov, G. M.</creatorcontrib><creatorcontrib>Hunter, J. L.</creatorcontrib><creatorcontrib>Griffis, D. P.</creatorcontrib><collection>CrossRef</collection><collection>Mechanical Engineering Abstracts</collection><jtitle>Journal of Vacuum Science & Technology B: Microelectronics and Nanometer Structures</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Loesing, R.</au><au>Guryanov, G. M.</au><au>Hunter, J. L.</au><au>Griffis, D. P.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Secondary ion mass spectrometry depth profiling of ultrashallow phosphorous in silicon</atitle><jtitle>Journal of Vacuum Science & Technology B: Microelectronics and Nanometer Structures</jtitle><date>2000-01</date><risdate>2000</risdate><volume>18</volume><issue>1</issue><spage>509</spage><epage>513</epage><pages>509-513</pages><issn>0734-211X</issn><issn>1071-1023</issn><eissn>1520-8567</eissn><coden>JVTBD9</coden><abstract>High-precision quantitative secondary ion mass spectrometry (SIMS) trace analyses of ultrashallow
31
P
distributions in Si (i.e., junction depths of 50 nm or less) require the ability to eliminate the
30
Si
1
H
mass interference while simultaneously minimizing primary ion impact energy and maximizing sensitivity. Elimination of
30
Si
1
H
requires a relatively high mass resolution SIMS instrument such as the Cameca IMS-6f used in this work. A range of
Cs
+
primary ion energies ranging from 9.5 to 1.6 keV was investigated to determine which provided the best depth resolution as measured by decay length for ultrashallow depth profiles of 2 keV P in Si. Improvements (or lack thereof) in decay length as the primary ion impact energy was reduced were correlated with crater bottom roughness measurements. Changes in the ion yields of P and Si resulting from both the appreciable fraction of the analyzed depth made up of the surface native oxide and also from the depth required for the primary ion yield enhancing
Cs
+
to reach a constant level were also investigated utilizing bulk-doped P in Si. The resulting ion yield transients obtained were then used to generate an empirical correction function with the aim of improving the quantitative accuracy of the ultrashallow depth profile selected as having the minimum decay length obtained in this work. Finally, improvements in the P detection limit provided by optimization of the secondary ion postacceleration system are discussed.</abstract><doi>10.1116/1.591222</doi><tpages>5</tpages></addata></record> |
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ispartof | Journal of Vacuum Science & Technology B: Microelectronics and Nanometer Structures, 2000-01, Vol.18 (1), p.509-513 |
issn | 0734-211X 1071-1023 1520-8567 |
language | eng |
recordid | cdi_crossref_primary_10_1116_1_591222 |
source | AIP Journals Complete |
subjects | Ion implantation Phosphorus Silicon Surface roughness |
title | Secondary ion mass spectrometry depth profiling of ultrashallow phosphorous in silicon |
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