Effects of the positions of scintillation detectors with fast scintillators and photomultiplier tubes on TOF–PET performance
Abstract The objective of this study is to improve the time resolution value of a coincidence spectrometer used in a time-of-flight–positron emission tomography (TOF–PET) system. This spectrometer is used in medical imaging systems. The coincidence spectrometer is manufactured by using a BC420-type...
Ausführliche Beschreibung
Autor*in: |
Ermis, Elif Ebru [verfasserIn] |
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Format: |
Artikel |
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Sprache: |
Englisch |
Erschienen: |
2020 |
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Schlagwörter: |
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Anmerkung: |
© Indian Academy of Sciences 2020 |
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Übergeordnetes Werk: |
Enthalten in: Pramāna - Springer India, 1973, 94(2020), 1 vom: 10. Jan. |
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Übergeordnetes Werk: |
volume:94 ; year:2020 ; number:1 ; day:10 ; month:01 |
Links: |
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DOI / URN: |
10.1007/s12043-019-1895-z |
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Katalog-ID: |
OLC212309840X |
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10.1007/s12043-019-1895-z doi (DE-627)OLC212309840X (DE-He213)s12043-019-1895-z-p DE-627 ger DE-627 rakwb eng 530 VZ Ermis, Elif Ebru verfasserin aut Effects of the positions of scintillation detectors with fast scintillators and photomultiplier tubes on TOF–PET performance 2020 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 2020 Abstract The objective of this study is to improve the time resolution value of a coincidence spectrometer used in a time-of-flight–positron emission tomography (TOF–PET) system. This spectrometer is used in medical imaging systems. The coincidence spectrometer is manufactured by using a BC420-type plastic scintillator and R1828-01-type photomultiplier tube, and the time resolution value of the manufactured spectrometer is determined. The accuracy of the experimental results is determined using the FLUKA Monte Carlo simulation program. Detectors are first manufactured in this program. Experimental and simulation results are compared and are found to be in good agreement. Optimal positions of the detectors are investigated to improve the coincidence time resolution of the spectrometer. Time resolution improvement of the optimal detector positions enables higher time-of-flight (TOF) gain and spatial resolution, leading to better image quality, reduction in patient doses and detection of small lesions. Coincidence spectrometer time resolution time-of-flight gain FLUKA Monte Carlo simulation program Celiktas, Cuneyt aut Enthalten in Pramāna Springer India, 1973 94(2020), 1 vom: 10. Jan. (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:94 year:2020 number:1 day:10 month:01 https://doi.org/10.1007/s12043-019-1895-z lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 AR 94 2020 1 10 01 |
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10.1007/s12043-019-1895-z doi (DE-627)OLC212309840X (DE-He213)s12043-019-1895-z-p DE-627 ger DE-627 rakwb eng 530 VZ Ermis, Elif Ebru verfasserin aut Effects of the positions of scintillation detectors with fast scintillators and photomultiplier tubes on TOF–PET performance 2020 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 2020 Abstract The objective of this study is to improve the time resolution value of a coincidence spectrometer used in a time-of-flight–positron emission tomography (TOF–PET) system. This spectrometer is used in medical imaging systems. The coincidence spectrometer is manufactured by using a BC420-type plastic scintillator and R1828-01-type photomultiplier tube, and the time resolution value of the manufactured spectrometer is determined. The accuracy of the experimental results is determined using the FLUKA Monte Carlo simulation program. Detectors are first manufactured in this program. Experimental and simulation results are compared and are found to be in good agreement. Optimal positions of the detectors are investigated to improve the coincidence time resolution of the spectrometer. Time resolution improvement of the optimal detector positions enables higher time-of-flight (TOF) gain and spatial resolution, leading to better image quality, reduction in patient doses and detection of small lesions. Coincidence spectrometer time resolution time-of-flight gain FLUKA Monte Carlo simulation program Celiktas, Cuneyt aut Enthalten in Pramāna Springer India, 1973 94(2020), 1 vom: 10. Jan. (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:94 year:2020 number:1 day:10 month:01 https://doi.org/10.1007/s12043-019-1895-z lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 AR 94 2020 1 10 01 |
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10.1007/s12043-019-1895-z doi (DE-627)OLC212309840X (DE-He213)s12043-019-1895-z-p DE-627 ger DE-627 rakwb eng 530 VZ Ermis, Elif Ebru verfasserin aut Effects of the positions of scintillation detectors with fast scintillators and photomultiplier tubes on TOF–PET performance 2020 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 2020 Abstract The objective of this study is to improve the time resolution value of a coincidence spectrometer used in a time-of-flight–positron emission tomography (TOF–PET) system. This spectrometer is used in medical imaging systems. The coincidence spectrometer is manufactured by using a BC420-type plastic scintillator and R1828-01-type photomultiplier tube, and the time resolution value of the manufactured spectrometer is determined. The accuracy of the experimental results is determined using the FLUKA Monte Carlo simulation program. Detectors are first manufactured in this program. Experimental and simulation results are compared and are found to be in good agreement. Optimal positions of the detectors are investigated to improve the coincidence time resolution of the spectrometer. Time resolution improvement of the optimal detector positions enables higher time-of-flight (TOF) gain and spatial resolution, leading to better image quality, reduction in patient doses and detection of small lesions. Coincidence spectrometer time resolution time-of-flight gain FLUKA Monte Carlo simulation program Celiktas, Cuneyt aut Enthalten in Pramāna Springer India, 1973 94(2020), 1 vom: 10. Jan. (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:94 year:2020 number:1 day:10 month:01 https://doi.org/10.1007/s12043-019-1895-z lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 AR 94 2020 1 10 01 |
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10.1007/s12043-019-1895-z doi (DE-627)OLC212309840X (DE-He213)s12043-019-1895-z-p DE-627 ger DE-627 rakwb eng 530 VZ Ermis, Elif Ebru verfasserin aut Effects of the positions of scintillation detectors with fast scintillators and photomultiplier tubes on TOF–PET performance 2020 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 2020 Abstract The objective of this study is to improve the time resolution value of a coincidence spectrometer used in a time-of-flight–positron emission tomography (TOF–PET) system. This spectrometer is used in medical imaging systems. The coincidence spectrometer is manufactured by using a BC420-type plastic scintillator and R1828-01-type photomultiplier tube, and the time resolution value of the manufactured spectrometer is determined. The accuracy of the experimental results is determined using the FLUKA Monte Carlo simulation program. Detectors are first manufactured in this program. Experimental and simulation results are compared and are found to be in good agreement. Optimal positions of the detectors are investigated to improve the coincidence time resolution of the spectrometer. Time resolution improvement of the optimal detector positions enables higher time-of-flight (TOF) gain and spatial resolution, leading to better image quality, reduction in patient doses and detection of small lesions. Coincidence spectrometer time resolution time-of-flight gain FLUKA Monte Carlo simulation program Celiktas, Cuneyt aut Enthalten in Pramāna Springer India, 1973 94(2020), 1 vom: 10. Jan. (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:94 year:2020 number:1 day:10 month:01 https://doi.org/10.1007/s12043-019-1895-z lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 AR 94 2020 1 10 01 |
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10.1007/s12043-019-1895-z doi (DE-627)OLC212309840X (DE-He213)s12043-019-1895-z-p DE-627 ger DE-627 rakwb eng 530 VZ Ermis, Elif Ebru verfasserin aut Effects of the positions of scintillation detectors with fast scintillators and photomultiplier tubes on TOF–PET performance 2020 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 2020 Abstract The objective of this study is to improve the time resolution value of a coincidence spectrometer used in a time-of-flight–positron emission tomography (TOF–PET) system. This spectrometer is used in medical imaging systems. The coincidence spectrometer is manufactured by using a BC420-type plastic scintillator and R1828-01-type photomultiplier tube, and the time resolution value of the manufactured spectrometer is determined. The accuracy of the experimental results is determined using the FLUKA Monte Carlo simulation program. Detectors are first manufactured in this program. Experimental and simulation results are compared and are found to be in good agreement. Optimal positions of the detectors are investigated to improve the coincidence time resolution of the spectrometer. Time resolution improvement of the optimal detector positions enables higher time-of-flight (TOF) gain and spatial resolution, leading to better image quality, reduction in patient doses and detection of small lesions. Coincidence spectrometer time resolution time-of-flight gain FLUKA Monte Carlo simulation program Celiktas, Cuneyt aut Enthalten in Pramāna Springer India, 1973 94(2020), 1 vom: 10. Jan. (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:94 year:2020 number:1 day:10 month:01 https://doi.org/10.1007/s12043-019-1895-z lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 AR 94 2020 1 10 01 |
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Effects of the positions of scintillation detectors with fast scintillators and photomultiplier tubes on TOF–PET performance |
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Abstract The objective of this study is to improve the time resolution value of a coincidence spectrometer used in a time-of-flight–positron emission tomography (TOF–PET) system. This spectrometer is used in medical imaging systems. The coincidence spectrometer is manufactured by using a BC420-type plastic scintillator and R1828-01-type photomultiplier tube, and the time resolution value of the manufactured spectrometer is determined. The accuracy of the experimental results is determined using the FLUKA Monte Carlo simulation program. Detectors are first manufactured in this program. Experimental and simulation results are compared and are found to be in good agreement. Optimal positions of the detectors are investigated to improve the coincidence time resolution of the spectrometer. Time resolution improvement of the optimal detector positions enables higher time-of-flight (TOF) gain and spatial resolution, leading to better image quality, reduction in patient doses and detection of small lesions. © Indian Academy of Sciences 2020 |
abstractGer |
Abstract The objective of this study is to improve the time resolution value of a coincidence spectrometer used in a time-of-flight–positron emission tomography (TOF–PET) system. This spectrometer is used in medical imaging systems. The coincidence spectrometer is manufactured by using a BC420-type plastic scintillator and R1828-01-type photomultiplier tube, and the time resolution value of the manufactured spectrometer is determined. The accuracy of the experimental results is determined using the FLUKA Monte Carlo simulation program. Detectors are first manufactured in this program. Experimental and simulation results are compared and are found to be in good agreement. Optimal positions of the detectors are investigated to improve the coincidence time resolution of the spectrometer. Time resolution improvement of the optimal detector positions enables higher time-of-flight (TOF) gain and spatial resolution, leading to better image quality, reduction in patient doses and detection of small lesions. © Indian Academy of Sciences 2020 |
abstract_unstemmed |
Abstract The objective of this study is to improve the time resolution value of a coincidence spectrometer used in a time-of-flight–positron emission tomography (TOF–PET) system. This spectrometer is used in medical imaging systems. The coincidence spectrometer is manufactured by using a BC420-type plastic scintillator and R1828-01-type photomultiplier tube, and the time resolution value of the manufactured spectrometer is determined. The accuracy of the experimental results is determined using the FLUKA Monte Carlo simulation program. Detectors are first manufactured in this program. Experimental and simulation results are compared and are found to be in good agreement. Optimal positions of the detectors are investigated to improve the coincidence time resolution of the spectrometer. Time resolution improvement of the optimal detector positions enables higher time-of-flight (TOF) gain and spatial resolution, leading to better image quality, reduction in patient doses and detection of small lesions. © Indian Academy of Sciences 2020 |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000naa a22002652 4500</leader><controlfield tag="001">OLC212309840X</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230505071328.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">230505s2020 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s12043-019-1895-z</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC212309840X</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)s12043-019-1895-z-p</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">530</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Ermis, Elif Ebru</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Effects of the positions of scintillation detectors with fast scintillators and photomultiplier tubes on TOF–PET performance</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2020</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Indian Academy of Sciences 2020</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract The objective of this study is to improve the time resolution value of a coincidence spectrometer used in a time-of-flight–positron emission tomography (TOF–PET) system. This spectrometer is used in medical imaging systems. The coincidence spectrometer is manufactured by using a BC420-type plastic scintillator and R1828-01-type photomultiplier tube, and the time resolution value of the manufactured spectrometer is determined. The accuracy of the experimental results is determined using the FLUKA Monte Carlo simulation program. Detectors are first manufactured in this program. Experimental and simulation results are compared and are found to be in good agreement. Optimal positions of the detectors are investigated to improve the coincidence time resolution of the spectrometer. 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