A hybrid techinique to evaluate the line spread function

Detalhes bibliográficos
Autor(a) principal: Almeida, Gevaldo Lisboa
Data de Publicação: 2002
Outros Autores: Souza, Maria Inês Silvani, Lopes, Ricardo Tadeu, Instituto de Engenharia Nuclear
Tipo de documento: Relatório
Idioma: eng
Título da fonte: Repositório Institucional do IEN
Texto Completo: http://carpedien.ien.gov.br:8080/handle/ien/2112
Resumo: A hybrid technique to evaluate the Line Spread (LSF) has been developed. It’s based on an experimental-theoretical approach aiming the reduction of the required experimental efforts to reach an acceptable level of accuracy on the width of the Gaussian representing the LSF. Using this technique, the several spectra required to fill up the space domain with an adequate density, usually done by shifting slightly the object with respect to the source-detector system after each spectrum is taken, are replaced by few spectra and a theoretical treatment involving numerical integration and non-linear fittings. In order to accomplish this task, a function is fitted to the experimental data, allowing the accurate determination of the center of the cylindrical object in the spectrum. Once this center is determined, it becomes possible to compare channel by channel the experimental counts with the expected theoretical ones. The first ones represent an integration of the transmitted neutron beam, as automatically performed by the detector, and hence, to achieve the aimed comparison, the theoretical counts should as well arise from a similar integration. Since the function expressing the transmitted beam intensity cannot be symbolically integrated, the task in done numerically over regular intervals corresponding to each given nominal collimator aperture. The sum of quadratic differences between the experimental and calculated counts reaches a minimum at an effective collimator aperture, which in somewhat different from the nominal aperture actually used in the experiments due to the unavoidable neutron scattering process and statistical fluctuations. This effective aperture is then used to get through integration the theoretical Edge Response Function (ERF) spectrum for any displacement step. Such a feature makes possible the simulation of high density spectra which are otherwise experimentally unfeasible due to the limited mechanical tolerances of the positioning devices. A derivation of the ERF yields the aimed LSF. Several comparisons and simulations have then be made by using a computer program written in Fortran, to evaluate the applicability and advantages of the developed technique.
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spelling Almeida, Gevaldo LisboaSouza, Maria Inês SilvaniLopes, Ricardo TadeuInstituto de Engenharia Nuclear2018-01-12T12:31:39Z2018-01-12T12:31:39Z2002-06http://carpedien.ien.gov.br:8080/handle/ien/2112Submitted by Marcele Costal de Castro (costalcastro@gmail.com) on 2018-01-12T12:31:39Z No. of bitstreams: 1 RT-IEN-12-2002.pdf: 903300 bytes, checksum: 7d4367f996bea83aa73b599c4033ae7c (MD5)Made available in DSpace on 2018-01-12T12:31:39Z (GMT). No. of bitstreams: 1 RT-IEN-12-2002.pdf: 903300 bytes, checksum: 7d4367f996bea83aa73b599c4033ae7c (MD5) Previous issue date: 2002-06A hybrid technique to evaluate the Line Spread (LSF) has been developed. It’s based on an experimental-theoretical approach aiming the reduction of the required experimental efforts to reach an acceptable level of accuracy on the width of the Gaussian representing the LSF. Using this technique, the several spectra required to fill up the space domain with an adequate density, usually done by shifting slightly the object with respect to the source-detector system after each spectrum is taken, are replaced by few spectra and a theoretical treatment involving numerical integration and non-linear fittings. In order to accomplish this task, a function is fitted to the experimental data, allowing the accurate determination of the center of the cylindrical object in the spectrum. Once this center is determined, it becomes possible to compare channel by channel the experimental counts with the expected theoretical ones. The first ones represent an integration of the transmitted neutron beam, as automatically performed by the detector, and hence, to achieve the aimed comparison, the theoretical counts should as well arise from a similar integration. Since the function expressing the transmitted beam intensity cannot be symbolically integrated, the task in done numerically over regular intervals corresponding to each given nominal collimator aperture. The sum of quadratic differences between the experimental and calculated counts reaches a minimum at an effective collimator aperture, which in somewhat different from the nominal aperture actually used in the experiments due to the unavoidable neutron scattering process and statistical fluctuations. This effective aperture is then used to get through integration the theoretical Edge Response Function (ERF) spectrum for any displacement step. Such a feature makes possible the simulation of high density spectra which are otherwise experimentally unfeasible due to the limited mechanical tolerances of the positioning devices. A derivation of the ERF yields the aimed LSF. Several comparisons and simulations have then be made by using a computer program written in Fortran, to evaluate the applicability and advantages of the developed technique.engInstituto de Engenharia NuclearIENBrasilLine spread functionEdge response functionTomographyImage qualityA hybrid techinique to evaluate the line spread functioninfo:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/reportinfo:eu-repo/semantics/openAccessreponame:Repositório Institucional do IENinstname:Instituto de Engenharia Nuclearinstacron:IENLICENSElicense.txtlicense.txttext/plain; charset=utf-81748http://carpedien.ien.gov.br:8080/xmlui/bitstream/ien/2112/2/license.txt8a4605be74aa9ea9d79846c1fba20a33MD52ORIGINALRT-IEN-12-2002.pdfRT-IEN-12-2002.pdfapplication/pdf903300http://carpedien.ien.gov.br:8080/xmlui/bitstream/ien/2112/1/RT-IEN-12-2002.pdf7d4367f996bea83aa73b599c4033ae7cMD51ien/2112oai:carpedien.ien.gov.br:ien/21122018-01-12 10:31:39.392Dspace IENlsales@ien.gov.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
dc.title.pt_BR.fl_str_mv A hybrid techinique to evaluate the line spread function
title A hybrid techinique to evaluate the line spread function
spellingShingle A hybrid techinique to evaluate the line spread function
Almeida, Gevaldo Lisboa
Line spread function
Edge response function
Tomography
Image quality
title_short A hybrid techinique to evaluate the line spread function
title_full A hybrid techinique to evaluate the line spread function
title_fullStr A hybrid techinique to evaluate the line spread function
title_full_unstemmed A hybrid techinique to evaluate the line spread function
title_sort A hybrid techinique to evaluate the line spread function
author Almeida, Gevaldo Lisboa
author_facet Almeida, Gevaldo Lisboa
Souza, Maria Inês Silvani
Lopes, Ricardo Tadeu
Instituto de Engenharia Nuclear
author_role author
author2 Souza, Maria Inês Silvani
Lopes, Ricardo Tadeu
Instituto de Engenharia Nuclear
author2_role author
author
author
dc.contributor.author.fl_str_mv Almeida, Gevaldo Lisboa
Souza, Maria Inês Silvani
Lopes, Ricardo Tadeu
Instituto de Engenharia Nuclear
dc.subject.por.fl_str_mv Line spread function
Edge response function
Tomography
Image quality
topic Line spread function
Edge response function
Tomography
Image quality
dc.description.abstract.por.fl_txt_mv A hybrid technique to evaluate the Line Spread (LSF) has been developed. It’s based on an experimental-theoretical approach aiming the reduction of the required experimental efforts to reach an acceptable level of accuracy on the width of the Gaussian representing the LSF. Using this technique, the several spectra required to fill up the space domain with an adequate density, usually done by shifting slightly the object with respect to the source-detector system after each spectrum is taken, are replaced by few spectra and a theoretical treatment involving numerical integration and non-linear fittings. In order to accomplish this task, a function is fitted to the experimental data, allowing the accurate determination of the center of the cylindrical object in the spectrum. Once this center is determined, it becomes possible to compare channel by channel the experimental counts with the expected theoretical ones. The first ones represent an integration of the transmitted neutron beam, as automatically performed by the detector, and hence, to achieve the aimed comparison, the theoretical counts should as well arise from a similar integration. Since the function expressing the transmitted beam intensity cannot be symbolically integrated, the task in done numerically over regular intervals corresponding to each given nominal collimator aperture. The sum of quadratic differences between the experimental and calculated counts reaches a minimum at an effective collimator aperture, which in somewhat different from the nominal aperture actually used in the experiments due to the unavoidable neutron scattering process and statistical fluctuations. This effective aperture is then used to get through integration the theoretical Edge Response Function (ERF) spectrum for any displacement step. Such a feature makes possible the simulation of high density spectra which are otherwise experimentally unfeasible due to the limited mechanical tolerances of the positioning devices. A derivation of the ERF yields the aimed LSF. Several comparisons and simulations have then be made by using a computer program written in Fortran, to evaluate the applicability and advantages of the developed technique.
description A hybrid technique to evaluate the Line Spread (LSF) has been developed. It’s based on an experimental-theoretical approach aiming the reduction of the required experimental efforts to reach an acceptable level of accuracy on the width of the Gaussian representing the LSF. Using this technique, the several spectra required to fill up the space domain with an adequate density, usually done by shifting slightly the object with respect to the source-detector system after each spectrum is taken, are replaced by few spectra and a theoretical treatment involving numerical integration and non-linear fittings. In order to accomplish this task, a function is fitted to the experimental data, allowing the accurate determination of the center of the cylindrical object in the spectrum. Once this center is determined, it becomes possible to compare channel by channel the experimental counts with the expected theoretical ones. The first ones represent an integration of the transmitted neutron beam, as automatically performed by the detector, and hence, to achieve the aimed comparison, the theoretical counts should as well arise from a similar integration. Since the function expressing the transmitted beam intensity cannot be symbolically integrated, the task in done numerically over regular intervals corresponding to each given nominal collimator aperture. The sum of quadratic differences between the experimental and calculated counts reaches a minimum at an effective collimator aperture, which in somewhat different from the nominal aperture actually used in the experiments due to the unavoidable neutron scattering process and statistical fluctuations. This effective aperture is then used to get through integration the theoretical Edge Response Function (ERF) spectrum for any displacement step. Such a feature makes possible the simulation of high density spectra which are otherwise experimentally unfeasible due to the limited mechanical tolerances of the positioning devices. A derivation of the ERF yields the aimed LSF. Several comparisons and simulations have then be made by using a computer program written in Fortran, to evaluate the applicability and advantages of the developed technique.
publishDate 2002
dc.date.issued.fl_str_mv 2002-06
dc.date.accessioned.fl_str_mv 2018-01-12T12:31:39Z
dc.date.available.fl_str_mv 2018-01-12T12:31:39Z
dc.type.status.fl_str_mv info:eu-repo/semantics/publishedVersion
dc.type.driver.fl_str_mv info:eu-repo/semantics/report
status_str publishedVersion
format report
dc.identifier.uri.fl_str_mv http://carpedien.ien.gov.br:8080/handle/ien/2112
url http://carpedien.ien.gov.br:8080/handle/ien/2112
dc.language.iso.fl_str_mv eng
language eng
dc.rights.driver.fl_str_mv info:eu-repo/semantics/openAccess
eu_rights_str_mv openAccess
dc.publisher.none.fl_str_mv Instituto de Engenharia Nuclear
dc.publisher.initials.fl_str_mv IEN
dc.publisher.country.fl_str_mv Brasil
publisher.none.fl_str_mv Instituto de Engenharia Nuclear
dc.source.none.fl_str_mv reponame:Repositório Institucional do IEN
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reponame_str Repositório Institucional do IEN
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instname_str Instituto de Engenharia Nuclear
instacron_str IEN
institution IEN
bitstream.url.fl_str_mv http://carpedien.ien.gov.br:8080/xmlui/bitstream/ien/2112/2/license.txt
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