Cargando…

A new phantom and empirical formula for apparent diffusion coefficient measurement by a 3 Tesla magnetic resonance imaging scanner

The aim of this study was to create a new phantom for a 3 Tesla (3T) magnetic resonance imaging (MRI) device for the calculation of the apparent diffusion coefficient (ADC) using diffusion-weighted imaging (DWI), and to mimic the ADC values of normal and tumor tissues at various temperatures, includ...

Descripción completa

Detalles Bibliográficos
Autores principales: HARA, MARINA, KURODA, MASAHIRO, OHMURA, YUICHI, MATSUZAKI, HIDENOBU, KOBAYASHI, TOMOKI, MURAKAMI, JUN, KATASHIMA, KAZUNORI, ASHIDA, MASAKAZU, OHNO, SEIICHIRO, ASAUMI, JUN-ICHI
Formato: Online Artículo Texto
Lenguaje:English
Publicado: D.A. Spandidos 2014
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4081373/
https://www.ncbi.nlm.nih.gov/pubmed/25013504
http://dx.doi.org/10.3892/ol.2014.2187
_version_ 1782324097617756160
author HARA, MARINA
KURODA, MASAHIRO
OHMURA, YUICHI
MATSUZAKI, HIDENOBU
KOBAYASHI, TOMOKI
MURAKAMI, JUN
KATASHIMA, KAZUNORI
ASHIDA, MASAKAZU
OHNO, SEIICHIRO
ASAUMI, JUN-ICHI
author_facet HARA, MARINA
KURODA, MASAHIRO
OHMURA, YUICHI
MATSUZAKI, HIDENOBU
KOBAYASHI, TOMOKI
MURAKAMI, JUN
KATASHIMA, KAZUNORI
ASHIDA, MASAKAZU
OHNO, SEIICHIRO
ASAUMI, JUN-ICHI
author_sort HARA, MARINA
collection PubMed
description The aim of this study was to create a new phantom for a 3 Tesla (3T) magnetic resonance imaging (MRI) device for the calculation of the apparent diffusion coefficient (ADC) using diffusion-weighted imaging (DWI), and to mimic the ADC values of normal and tumor tissues at various temperatures, including the physiological body temperature of 37°C. The phantom was produced using several concentrations of sucrose from 0 to 1.2 M, and the DWI was performed using various phantom temperatures. The accurate ADC values were calculated using the DWIs of the phantoms, and an empirical formula was developed to calculate the ADC values of the phantoms from an arbitrary sucrose concentration and arbitrary phantom temperature. The empirical formula was able to produce ADC values ranging between 0.33 and 3.02×10(−3) mm(2)/sec, which covered the range of ADC values of the human body that have been measured clinically by 3T MRI in previous studies. The phantom and empirical formula developed in this study may be available to mimic the ADC values of the clinical human lesion by 3T MRI.
format Online
Article
Text
id pubmed-4081373
institution National Center for Biotechnology Information
language English
publishDate 2014
publisher D.A. Spandidos
record_format MEDLINE/PubMed
spelling pubmed-40813732014-07-10 A new phantom and empirical formula for apparent diffusion coefficient measurement by a 3 Tesla magnetic resonance imaging scanner HARA, MARINA KURODA, MASAHIRO OHMURA, YUICHI MATSUZAKI, HIDENOBU KOBAYASHI, TOMOKI MURAKAMI, JUN KATASHIMA, KAZUNORI ASHIDA, MASAKAZU OHNO, SEIICHIRO ASAUMI, JUN-ICHI Oncol Lett Articles The aim of this study was to create a new phantom for a 3 Tesla (3T) magnetic resonance imaging (MRI) device for the calculation of the apparent diffusion coefficient (ADC) using diffusion-weighted imaging (DWI), and to mimic the ADC values of normal and tumor tissues at various temperatures, including the physiological body temperature of 37°C. The phantom was produced using several concentrations of sucrose from 0 to 1.2 M, and the DWI was performed using various phantom temperatures. The accurate ADC values were calculated using the DWIs of the phantoms, and an empirical formula was developed to calculate the ADC values of the phantoms from an arbitrary sucrose concentration and arbitrary phantom temperature. The empirical formula was able to produce ADC values ranging between 0.33 and 3.02×10(−3) mm(2)/sec, which covered the range of ADC values of the human body that have been measured clinically by 3T MRI in previous studies. The phantom and empirical formula developed in this study may be available to mimic the ADC values of the clinical human lesion by 3T MRI. D.A. Spandidos 2014-08 2014-05-28 /pmc/articles/PMC4081373/ /pubmed/25013504 http://dx.doi.org/10.3892/ol.2014.2187 Text en Copyright © 2014, Spandidos Publications http://creativecommons.org/licenses/by/3.0 This is an open-access article licensed under a Creative Commons Attribution-NonCommercial 3.0 Unported License. The article may be redistributed, reproduced, and reused for non-commercial purposes, provided the original source is properly cited.
spellingShingle Articles
HARA, MARINA
KURODA, MASAHIRO
OHMURA, YUICHI
MATSUZAKI, HIDENOBU
KOBAYASHI, TOMOKI
MURAKAMI, JUN
KATASHIMA, KAZUNORI
ASHIDA, MASAKAZU
OHNO, SEIICHIRO
ASAUMI, JUN-ICHI
A new phantom and empirical formula for apparent diffusion coefficient measurement by a 3 Tesla magnetic resonance imaging scanner
title A new phantom and empirical formula for apparent diffusion coefficient measurement by a 3 Tesla magnetic resonance imaging scanner
title_full A new phantom and empirical formula for apparent diffusion coefficient measurement by a 3 Tesla magnetic resonance imaging scanner
title_fullStr A new phantom and empirical formula for apparent diffusion coefficient measurement by a 3 Tesla magnetic resonance imaging scanner
title_full_unstemmed A new phantom and empirical formula for apparent diffusion coefficient measurement by a 3 Tesla magnetic resonance imaging scanner
title_short A new phantom and empirical formula for apparent diffusion coefficient measurement by a 3 Tesla magnetic resonance imaging scanner
title_sort new phantom and empirical formula for apparent diffusion coefficient measurement by a 3 tesla magnetic resonance imaging scanner
topic Articles
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4081373/
https://www.ncbi.nlm.nih.gov/pubmed/25013504
http://dx.doi.org/10.3892/ol.2014.2187
work_keys_str_mv AT haramarina anewphantomandempiricalformulaforapparentdiffusioncoefficientmeasurementbya3teslamagneticresonanceimagingscanner
AT kurodamasahiro anewphantomandempiricalformulaforapparentdiffusioncoefficientmeasurementbya3teslamagneticresonanceimagingscanner
AT ohmurayuichi anewphantomandempiricalformulaforapparentdiffusioncoefficientmeasurementbya3teslamagneticresonanceimagingscanner
AT matsuzakihidenobu anewphantomandempiricalformulaforapparentdiffusioncoefficientmeasurementbya3teslamagneticresonanceimagingscanner
AT kobayashitomoki anewphantomandempiricalformulaforapparentdiffusioncoefficientmeasurementbya3teslamagneticresonanceimagingscanner
AT murakamijun anewphantomandempiricalformulaforapparentdiffusioncoefficientmeasurementbya3teslamagneticresonanceimagingscanner
AT katashimakazunori anewphantomandempiricalformulaforapparentdiffusioncoefficientmeasurementbya3teslamagneticresonanceimagingscanner
AT ashidamasakazu anewphantomandempiricalformulaforapparentdiffusioncoefficientmeasurementbya3teslamagneticresonanceimagingscanner
AT ohnoseiichiro anewphantomandempiricalformulaforapparentdiffusioncoefficientmeasurementbya3teslamagneticresonanceimagingscanner
AT asaumijunichi anewphantomandempiricalformulaforapparentdiffusioncoefficientmeasurementbya3teslamagneticresonanceimagingscanner
AT haramarina newphantomandempiricalformulaforapparentdiffusioncoefficientmeasurementbya3teslamagneticresonanceimagingscanner
AT kurodamasahiro newphantomandempiricalformulaforapparentdiffusioncoefficientmeasurementbya3teslamagneticresonanceimagingscanner
AT ohmurayuichi newphantomandempiricalformulaforapparentdiffusioncoefficientmeasurementbya3teslamagneticresonanceimagingscanner
AT matsuzakihidenobu newphantomandempiricalformulaforapparentdiffusioncoefficientmeasurementbya3teslamagneticresonanceimagingscanner
AT kobayashitomoki newphantomandempiricalformulaforapparentdiffusioncoefficientmeasurementbya3teslamagneticresonanceimagingscanner
AT murakamijun newphantomandempiricalformulaforapparentdiffusioncoefficientmeasurementbya3teslamagneticresonanceimagingscanner
AT katashimakazunori newphantomandempiricalformulaforapparentdiffusioncoefficientmeasurementbya3teslamagneticresonanceimagingscanner
AT ashidamasakazu newphantomandempiricalformulaforapparentdiffusioncoefficientmeasurementbya3teslamagneticresonanceimagingscanner
AT ohnoseiichiro newphantomandempiricalformulaforapparentdiffusioncoefficientmeasurementbya3teslamagneticresonanceimagingscanner
AT asaumijunichi newphantomandempiricalformulaforapparentdiffusioncoefficientmeasurementbya3teslamagneticresonanceimagingscanner