Laser-assisted atom probe tomography of c-plane and m-plane InGaN test structures
Laser-assisted atom probe tomography (APT) was used to measure the indium mole fraction x of c-plane, MOCVD-grown, GaN/In(x)Ga(1-x)N/GaN test structures and the results were compared with Rutherford backscattering analysis (RBS). Four sample types were examined with (RBS determined) x = 0.030, 0.034...
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creator | Sanford, N. A Blanchard, P. T Brubaker, M. D Rishinaramangalam, A. K Zhang, Q Roshko, A Feezell, D. F Klein, B. D. B Davydov, A. V |
description | Laser-assisted atom probe tomography (APT) was used to measure the indium
mole fraction x of c-plane, MOCVD-grown, GaN/In(x)Ga(1-x)N/GaN test structures
and the results were compared with Rutherford backscattering analysis (RBS).
Four sample types were examined with (RBS determined) x = 0.030, 0.034, 0.056,
and 0.112. The respective In(x)Ga(1-x)N layer thicknesses were 330 nm, 327 nm,
360 nm, and 55 nm. APT data were collected at (fixed) laser pulse energy (PE)
selected within the range of (2-1000) fJ. Sample temperatures were = 54 K. PE
within (2-50) fJ yielded x values that agreed with RBS (within uncertainty) and
were comparatively insensitive to region-of-interest (ROI) geometry and
orientation. By contrast, approximate stoichiometry was only found in the GaN
portions of the samples provided PE was within (5-20) fJ and the analyses were
confined to cylindrical ROIs (of diameters =20 nm) that were coaxial with the
specimen tips. m-plane oriented tips were derived from c-axis grown,
core-shell, GaN/In(x)Ga(1-x)N nanorod heterostructures. Compositional analysis
along [0 0 0 1] (transverse to the long axis of the tip), of these m-plane
samples revealed a spatial asymmetry in charge-state ratio (CSR) and a
corresponding asymmetry in the resultant tip shape along this direction; no
asymmetry in CSR or tip shape was observed for analysis along [-1 2-1 0].
Simulations revealed that the electric field strength at the tip apex was
dominated by the presence of a p-type inversion layer, which developed under
typical tip-electrode bias conditions for the n-type doping levels considered.
Finally, both c-plane and m-plane sample types showed depth-dependent
variations in absolute ion counts that depended upon ROI placement. |
doi_str_mv | 10.48550/arxiv.2102.06340 |
format | Article |
fullrecord | <record><control><sourceid>arxiv_GOX</sourceid><recordid>TN_cdi_arxiv_primary_2102_06340</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>2102_06340</sourcerecordid><originalsourceid>FETCH-LOGICAL-a670-52269a051fb5bf6a26735ecff0c42fa24a7ec2f4bef1b3ebc0db53104b092f223</originalsourceid><addsrcrecordid>eNotz8tOwzAQhWFvWKDCA7DCL5AwGV9Cl6iCtlJEhdR9NHbGEKm5yHYRfftC6er8qyN9QjxUUOpnY-CJ4k__XWIFWIJVGm7FR0OJY0Ep9SlzJylPg5zj5Fj-1vQZaf46ySlIX8wHGlnS2Mnh2ttxTe8yc8oy5Xj0-Rg53YmbQIfE99ddiP3b6361KZrdert6aQqyNRQG0S4JTBWcccES2loZ9iGA1xgINdXsMWjHoXKKnYfOGVWBdrDEgKgW4vH_9mJq59gPFE_tn6292NQZpY1KTw</addsrcrecordid><sourcetype>Open Access Repository</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Laser-assisted atom probe tomography of c-plane and m-plane InGaN test structures</title><source>arXiv.org</source><creator>Sanford, N. A ; Blanchard, P. T ; Brubaker, M. D ; Rishinaramangalam, A. K ; Zhang, Q ; Roshko, A ; Feezell, D. F ; Klein, B. D. B ; Davydov, A. V</creator><creatorcontrib>Sanford, N. A ; Blanchard, P. T ; Brubaker, M. D ; Rishinaramangalam, A. K ; Zhang, Q ; Roshko, A ; Feezell, D. F ; Klein, B. D. B ; Davydov, A. V</creatorcontrib><description>Laser-assisted atom probe tomography (APT) was used to measure the indium
mole fraction x of c-plane, MOCVD-grown, GaN/In(x)Ga(1-x)N/GaN test structures
and the results were compared with Rutherford backscattering analysis (RBS).
Four sample types were examined with (RBS determined) x = 0.030, 0.034, 0.056,
and 0.112. The respective In(x)Ga(1-x)N layer thicknesses were 330 nm, 327 nm,
360 nm, and 55 nm. APT data were collected at (fixed) laser pulse energy (PE)
selected within the range of (2-1000) fJ. Sample temperatures were = 54 K. PE
within (2-50) fJ yielded x values that agreed with RBS (within uncertainty) and
were comparatively insensitive to region-of-interest (ROI) geometry and
orientation. By contrast, approximate stoichiometry was only found in the GaN
portions of the samples provided PE was within (5-20) fJ and the analyses were
confined to cylindrical ROIs (of diameters =20 nm) that were coaxial with the
specimen tips. m-plane oriented tips were derived from c-axis grown,
core-shell, GaN/In(x)Ga(1-x)N nanorod heterostructures. Compositional analysis
along [0 0 0 1] (transverse to the long axis of the tip), of these m-plane
samples revealed a spatial asymmetry in charge-state ratio (CSR) and a
corresponding asymmetry in the resultant tip shape along this direction; no
asymmetry in CSR or tip shape was observed for analysis along [-1 2-1 0].
Simulations revealed that the electric field strength at the tip apex was
dominated by the presence of a p-type inversion layer, which developed under
typical tip-electrode bias conditions for the n-type doping levels considered.
Finally, both c-plane and m-plane sample types showed depth-dependent
variations in absolute ion counts that depended upon ROI placement.</description><identifier>DOI: 10.48550/arxiv.2102.06340</identifier><language>eng</language><subject>Physics - Materials Science</subject><creationdate>2021-02</creationdate><rights>http://arxiv.org/licenses/nonexclusive-distrib/1.0</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>228,230,776,881</link.rule.ids><linktorsrc>$$Uhttps://arxiv.org/abs/2102.06340$$EView_record_in_Cornell_University$$FView_record_in_$$GCornell_University$$Hfree_for_read</linktorsrc><backlink>$$Uhttps://doi.org/10.48550/arXiv.2102.06340$$DView paper in arXiv$$Hfree_for_read</backlink></links><search><creatorcontrib>Sanford, N. A</creatorcontrib><creatorcontrib>Blanchard, P. T</creatorcontrib><creatorcontrib>Brubaker, M. D</creatorcontrib><creatorcontrib>Rishinaramangalam, A. K</creatorcontrib><creatorcontrib>Zhang, Q</creatorcontrib><creatorcontrib>Roshko, A</creatorcontrib><creatorcontrib>Feezell, D. F</creatorcontrib><creatorcontrib>Klein, B. D. B</creatorcontrib><creatorcontrib>Davydov, A. V</creatorcontrib><title>Laser-assisted atom probe tomography of c-plane and m-plane InGaN test structures</title><description>Laser-assisted atom probe tomography (APT) was used to measure the indium
mole fraction x of c-plane, MOCVD-grown, GaN/In(x)Ga(1-x)N/GaN test structures
and the results were compared with Rutherford backscattering analysis (RBS).
Four sample types were examined with (RBS determined) x = 0.030, 0.034, 0.056,
and 0.112. The respective In(x)Ga(1-x)N layer thicknesses were 330 nm, 327 nm,
360 nm, and 55 nm. APT data were collected at (fixed) laser pulse energy (PE)
selected within the range of (2-1000) fJ. Sample temperatures were = 54 K. PE
within (2-50) fJ yielded x values that agreed with RBS (within uncertainty) and
were comparatively insensitive to region-of-interest (ROI) geometry and
orientation. By contrast, approximate stoichiometry was only found in the GaN
portions of the samples provided PE was within (5-20) fJ and the analyses were
confined to cylindrical ROIs (of diameters =20 nm) that were coaxial with the
specimen tips. m-plane oriented tips were derived from c-axis grown,
core-shell, GaN/In(x)Ga(1-x)N nanorod heterostructures. Compositional analysis
along [0 0 0 1] (transverse to the long axis of the tip), of these m-plane
samples revealed a spatial asymmetry in charge-state ratio (CSR) and a
corresponding asymmetry in the resultant tip shape along this direction; no
asymmetry in CSR or tip shape was observed for analysis along [-1 2-1 0].
Simulations revealed that the electric field strength at the tip apex was
dominated by the presence of a p-type inversion layer, which developed under
typical tip-electrode bias conditions for the n-type doping levels considered.
Finally, both c-plane and m-plane sample types showed depth-dependent
variations in absolute ion counts that depended upon ROI placement.</description><subject>Physics - Materials Science</subject><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><sourceid>GOX</sourceid><recordid>eNotz8tOwzAQhWFvWKDCA7DCL5AwGV9Cl6iCtlJEhdR9NHbGEKm5yHYRfftC6er8qyN9QjxUUOpnY-CJ4k__XWIFWIJVGm7FR0OJY0Ep9SlzJylPg5zj5Fj-1vQZaf46ySlIX8wHGlnS2Mnh2ttxTe8yc8oy5Xj0-Rg53YmbQIfE99ddiP3b6361KZrdert6aQqyNRQG0S4JTBWcccES2loZ9iGA1xgINdXsMWjHoXKKnYfOGVWBdrDEgKgW4vH_9mJq59gPFE_tn6292NQZpY1KTw</recordid><startdate>20210211</startdate><enddate>20210211</enddate><creator>Sanford, N. A</creator><creator>Blanchard, P. T</creator><creator>Brubaker, M. D</creator><creator>Rishinaramangalam, A. K</creator><creator>Zhang, Q</creator><creator>Roshko, A</creator><creator>Feezell, D. F</creator><creator>Klein, B. D. B</creator><creator>Davydov, A. V</creator><scope>GOX</scope></search><sort><creationdate>20210211</creationdate><title>Laser-assisted atom probe tomography of c-plane and m-plane InGaN test structures</title><author>Sanford, N. A ; Blanchard, P. T ; Brubaker, M. D ; Rishinaramangalam, A. K ; Zhang, Q ; Roshko, A ; Feezell, D. F ; Klein, B. D. B ; Davydov, A. V</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a670-52269a051fb5bf6a26735ecff0c42fa24a7ec2f4bef1b3ebc0db53104b092f223</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2021</creationdate><topic>Physics - Materials Science</topic><toplevel>online_resources</toplevel><creatorcontrib>Sanford, N. A</creatorcontrib><creatorcontrib>Blanchard, P. T</creatorcontrib><creatorcontrib>Brubaker, M. D</creatorcontrib><creatorcontrib>Rishinaramangalam, A. K</creatorcontrib><creatorcontrib>Zhang, Q</creatorcontrib><creatorcontrib>Roshko, A</creatorcontrib><creatorcontrib>Feezell, D. F</creatorcontrib><creatorcontrib>Klein, B. D. B</creatorcontrib><creatorcontrib>Davydov, A. V</creatorcontrib><collection>arXiv.org</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Sanford, N. A</au><au>Blanchard, P. T</au><au>Brubaker, M. D</au><au>Rishinaramangalam, A. K</au><au>Zhang, Q</au><au>Roshko, A</au><au>Feezell, D. F</au><au>Klein, B. D. B</au><au>Davydov, A. V</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Laser-assisted atom probe tomography of c-plane and m-plane InGaN test structures</atitle><date>2021-02-11</date><risdate>2021</risdate><abstract>Laser-assisted atom probe tomography (APT) was used to measure the indium
mole fraction x of c-plane, MOCVD-grown, GaN/In(x)Ga(1-x)N/GaN test structures
and the results were compared with Rutherford backscattering analysis (RBS).
Four sample types were examined with (RBS determined) x = 0.030, 0.034, 0.056,
and 0.112. The respective In(x)Ga(1-x)N layer thicknesses were 330 nm, 327 nm,
360 nm, and 55 nm. APT data were collected at (fixed) laser pulse energy (PE)
selected within the range of (2-1000) fJ. Sample temperatures were = 54 K. PE
within (2-50) fJ yielded x values that agreed with RBS (within uncertainty) and
were comparatively insensitive to region-of-interest (ROI) geometry and
orientation. By contrast, approximate stoichiometry was only found in the GaN
portions of the samples provided PE was within (5-20) fJ and the analyses were
confined to cylindrical ROIs (of diameters =20 nm) that were coaxial with the
specimen tips. m-plane oriented tips were derived from c-axis grown,
core-shell, GaN/In(x)Ga(1-x)N nanorod heterostructures. Compositional analysis
along [0 0 0 1] (transverse to the long axis of the tip), of these m-plane
samples revealed a spatial asymmetry in charge-state ratio (CSR) and a
corresponding asymmetry in the resultant tip shape along this direction; no
asymmetry in CSR or tip shape was observed for analysis along [-1 2-1 0].
Simulations revealed that the electric field strength at the tip apex was
dominated by the presence of a p-type inversion layer, which developed under
typical tip-electrode bias conditions for the n-type doping levels considered.
Finally, both c-plane and m-plane sample types showed depth-dependent
variations in absolute ion counts that depended upon ROI placement.</abstract><doi>10.48550/arxiv.2102.06340</doi><oa>free_for_read</oa></addata></record> |
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title | Laser-assisted atom probe tomography of c-plane and m-plane InGaN test structures |
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