TY - JOUR
T1 - Validation of the tail replacement method in MTF calculations using the homogeneous and non-homogeneous edges of a phantom
AU - Anam, C.
AU - Budi, W. S.
AU - Fujibuchi, T.
AU - Haryanto, F.
AU - Dougherty, G.
N1 - Funding Information:
This work was funded by the Penelitian Dasar Unggulan Perguruan Tinggi (PDUPT), Ministry of Research Technology and Higher Education of the Republic of Indonesia, contract number: 532z/I1.C01/PL/2018.
Publisher Copyright:
© Published under licence by IOP Publishing Ltd.
PY - 2019/6/6
Y1 - 2019/6/6
N2 - We validated the tail replacement technique in the modulation transfer function (MTF) calculation of CT images using edges of homogeneous and non-homogeneous phantom using an automated method. The algorithm for the automated MTF calculation consists of several steps. The upper edge of the phantom was detected from its axial image and pixel values was taken to create an edge spread function (ESF). The left tail of the ESF was flipped horizontally to replace the right tail. Differentiating the ESF produced a line spread function (LSF) which was Fourier transformed to produce the MTF. To validate the result for the non-homogeneous phantom was compared with that for a homogeneous phantom. Results showed that in the homogeneous module, the MTF curve generated without tail replacement corresponded to its shape in use. However for the non-homogeneous module, the MTF obtained without tail replacement differed considerably from its shape in use. The 50% value of MTF (MTF-50) without tail replacement was 0.44 cycles/mm compared to 0.33 cycles/mm in use. Using the tail replacement, the MTFs in the homogeneous and non-homogeneous modules were comparable, with MTF-50 values of 0.33 cycles/mm for both. In summary, the MTF cannot be conventionally measured from the edge of the non-homogeneous module, but it can be resolved using the tail replacement technique on the ESF curve.
AB - We validated the tail replacement technique in the modulation transfer function (MTF) calculation of CT images using edges of homogeneous and non-homogeneous phantom using an automated method. The algorithm for the automated MTF calculation consists of several steps. The upper edge of the phantom was detected from its axial image and pixel values was taken to create an edge spread function (ESF). The left tail of the ESF was flipped horizontally to replace the right tail. Differentiating the ESF produced a line spread function (LSF) which was Fourier transformed to produce the MTF. To validate the result for the non-homogeneous phantom was compared with that for a homogeneous phantom. Results showed that in the homogeneous module, the MTF curve generated without tail replacement corresponded to its shape in use. However for the non-homogeneous module, the MTF obtained without tail replacement differed considerably from its shape in use. The 50% value of MTF (MTF-50) without tail replacement was 0.44 cycles/mm compared to 0.33 cycles/mm in use. Using the tail replacement, the MTFs in the homogeneous and non-homogeneous modules were comparable, with MTF-50 values of 0.33 cycles/mm for both. In summary, the MTF cannot be conventionally measured from the edge of the non-homogeneous module, but it can be resolved using the tail replacement technique on the ESF curve.
UR - http://www.scopus.com/inward/record.url?scp=85067640944&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=85067640944&partnerID=8YFLogxK
U2 - 10.1088/1742-6596/1248/1/012001
DO - 10.1088/1742-6596/1248/1/012001
M3 - Conference article
AN - SCOPUS:85067640944
SN - 1742-6588
VL - 1248
JO - Journal of Physics: Conference Series
JF - Journal of Physics: Conference Series
IS - 1
M1 - 012001
T2 - 18th Asia-Oceania Congress of Medical Physics, AOCMP 2018 and 16th South-East Asia Congress of Medical Physics, SEACOMP 2018
Y2 - 11 November 2018 through 14 November 2018
ER -