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Journal of Radiation Research logoLink to Journal of Radiation Research
. 2022 Nov 14;64(1):195–201. doi: 10.1093/jrr/rrac071

Tolerance levels of mass density for adaptive helical tomotherapy using MVCT

Shogo Tsunemine 1,2, Shuichi Ozawa 3,4,5,, Minoru Nakao 6,7, Hideharu Miura 8,9, Akito Saito 10, Daisuke Kawahara 11, Yasuhiko Onishi 12, Takashi Onishi 13, Fumito Okawa 14, Atsushi Terai 15, Taiki Hashiguchi 16, Hidetoshi Yamasaki 17, Tsutomu Maruta 18, Yuji Murakami 19,20, Yasushi Nagata 21,22
PMCID: PMC9855312

Abstract

Daily dose distributions for adaptive radiotherapy (ART) using helical tomotherapy (HT) are calculated using megavoltage computed tomography (MVCT). Generally, the MVCT number is converted to mass density (MD) using an MD calibration table (MVCT-MD table). The aims of this study are to calculate the tolerance levels of the MD for ART and to evaluate the tolerance levels using clinical patient plans. These tolerance levels of MD were calculated based on the tissue maximum ratio (TMR) of 6MV flattening-filter-free (FFF) beam of HT and the effective tissue thickness data from an International Commission on Radiological Protection 110 phantom data for lung, adipose/muscle and cartilage/spongy-bone. These tolerance levels were determined by considering both the MD causing a dose error of 2% and the variation in MVCT numbers. Subsequently, the stability of the MD values was estimated with the standard deviations (SD) in the MVCT number over 6 months. The dose distribution for clinical patient plans was calculated using the MVCT-MD table with added tolerance levels. These tolerance levels were determined as MD differences causing a dose error of 2%, and were ± 0.049 g/cm3, ± 0.030 g/cm3 and ± 0.049 g/cm3 for lung, adipose/muscle and cartilage/spongy-bone, respectively. The calculated dose distribution errors using the MVCT-MD table added tolerance levels were within 2%. We proposed these tolerance levels in MD for the quality control of the MVCT-MD table.

Keywords: adaptive radiotherapy (ART), helical tomotherapy (HT), mass density (MD), megavoltage computed tomography (MVCT) number, tolerance levels

INTRODUCTION

Helical tomotherapy (HT) (Accuray Inc., Madison, WI, USA) megavoltage computed tomography (MVCT) images are used for image-guided radiotherapy to improve the precision and accuracy of treatment delivery [1, 2]. MVCT images are also used in adaptive radiotherapy (ART) to evaluate dose distributions and modify treatment plans according to body shape changes and tumor shrinkage during the treatment period [3]. The accuracy of this dose calculation for ART is important for calculating the accurate doses received by the tumor and normal tissues.

The MVCT numbers (Hounsfield unit [HU]) are converted to mass density (MD) [g/cm3] according to a MVCT number to MD calibration (MVCT-MD) table for dose calculation of ART. The accuracy of the MVCT-MD table is critical for dose calculation in inhomogeneous medium. A previous study reported that dose calculation accuracy using MVCT images with the TomoTherapy Hi-ART system (Accuray Inc., Madison, WI, USA) is similar to kilovoltage CT (kVCT) dose calculations [4]. However, several studies have been reported that changes in the MVCT-MD table due to variations in the MVCT number lead to uncertainties in the calculations [5, 6]. Therefore, a quality assurance (QA) method for the stability and reproducibility of the MVCT number has been developed to improve the accuracy of dose calculations for ART [5, 7]. HT guidelines recommend tolerances of ±30 HU, ± 50 HU and ± 50 HU from the baseline for water, lung and bone MVCT numbers, respectively, to achieve a dose calculation accuracy of 2% [7]. The another study calculated the tolerance levels for the CT number to relative electron density (CT-RED) of water, lung and bone, which has a 2% dose error in linear accelerators (4 MV, 6 MV, 6 MV flattening-filter-free [FFF], 10 MV, 10 MVFFF, 15 MV) and Co-60 from the tissue maximum ratio (TMR) data and effective depth [8, 9]. In these reports, 2–8 beam field 3-dimensional radiotherapy (3DCRT) with general-purpose linear accelerators were evaluated for multiple treatment plans [8, 9]. However, dose distributions for helical intensity-modulated radiation therapy (IMRT) using MVCT images for ART have not been researched. MVCT image-based ART, the standard tool for tomotherapy, is used in the chest and head and neck regions where weight loss and tumor shrinkage often occur [3, 10].

Therefore, this study aimed to propose the MD tolerance levels (TLMD) for ART. We calculated the TLMD that caused a 2% dose error for ART using MVCT images from HT, according to previous work [8, 9]. Furthermore, we confirmed the stability of the daily MVCT number and proposed tolerance levels for the lung, adipose/muscle and cartilage/spongy-bone in the MVCT-MD table. The proposed TLMD calculated for ART was validated by adding dose errors to the MVCT-MD table for these clinical patient plans.

METHODS AND MATERIALS

MD tolerance levels

Difference in MD levels that result in 2% dose error

The depth dose is expressed as a function of the effective depth and the TMR. The relative electron density (RED) error causing the dose error is defined by the following equation (1), corresponding to the equivalent thickness of water [8]:

graphic file with name DmEquation1.gif (1)

Here, i denotes the tissue index; Δρe.i, and ti denote the RED error and the tissue thickness of index i, respectively; ΔD/D denotes the relative dose error to the local dose; TMR denotes the tissue maximum ratio; deff denotes effective depth; (dTMR/d(deff))/TMR is the gradient of TMR relative to the local TMR.

The RED tolerance levels that cause 2% dose error (Inline graphicwere converted to MD tolerance levels Inline graphicusing the conversion coefficient, as seen in equation (2) [11]:

graphic file with name DmEquation2.gif (2)

Here, Inline graphic and Inline graphic denote the tolerance levels of MD and RED, respectively; C is the conversion factor between MD and RED for human tissues. Conversion factors were 1.009, 1.005 and 1.015 for the lung, adipose/muscle and cartilage/spongy-bone, respectively, based on a previous study [11].

The Inline graphicdepends on the energy of the treatment beam and is not influenced by CT scanner. The TMR used for (dTMR/d(deff)))/TMR was acquired using a TomoTherapy HD system (Accuray Inc., Sunnyvale, CA). This system was used to generate the photon beam (6 MV FFF) with an irradiation field of 10 cm × 5 cm. The TMR effective depth gradient at a depth of 10 cm was 3.2% cm−1. The TMR data was measured in a water-equivalent phantom (Kyoto Kagaku Co., Kyoto, Japan) from 0 to 25 cm with a source-to-axis distance (SAD) of 85 cm. The recommended accuracy of the calculated dose distribution was less than 2% in heterogeneous materials [12]. Therefore, we applied 2% of ΔD/D for relative dose error to the local dose. The effective tissue thicknesses of each tissue type were required to evaluate the dose error with RED in a previous study [8]. The effective tissue thicknesses of each tissue were estimated based on the maximum tissue thickness from an International Commission on Radiological Protection110 (ICRP-110) standard phantom for adults [13]. The effective tissue thicknesses for lung, adipose/muscle and cartilage/spongy-bone tissue were 10, 20 and 10 cm, respectively [9].

Variation of the MVCT number

To determine the TLMD, the stability of the MD values was estimated with standard deviations (SD) of MVCT number over six months in our institution. MVCT images of a cheese phantom (Accuray Inc. Madison, WI, USA) with eight tissue equivalent density plugs (Gammex, Sun Nuclear Corporation, USA) were acquired using a HD system. The tissue equivalent density plug used lung to bone with MD values of 0.29–1.822 g/cm3. These MVCT images were acquired in normal mode with a slice thickness of 2 mm. These MVCT numbers for air and the water-equivalent substance of cheese phantom were adjusted to −1000 and 25 HU once a week, respectively. The acquisition of the MVCT number for each tissue equivalent density plug (diameter = 20 mm) was measured using ImageJ software (v1.51) on the MVCT images. Data were collected over 6 months (n = 78). Figure 1 shows MVCT images of a cheese phantom with eight tissue equivalent density plugs. The root mean square (RMS) of the MVCT number for all tissue-equivalent density plugs was converted to the variation of MD, Inline graphic. Inline graphic is given by equation (3).

graphic file with name DmEquation3.gif (3)
Fig. 1.

Fig. 1

The names (A) and nominal MD values (g/cm3) (B) of the tissue equivalent density plugs inserted into the cheese phantom.

Here, j denotes tissue equivalent density plug index; Inline graphic denotes the variation of MD converted from the SD of MVCT number using MVCT-MD table for each tissue-equivalent density plug; n denotes the number of tissue equivalent density plug.

Overall tolerance levels of MD

The variation of MVCT number is larger than that of kVCT number [9]. The tolerance levels should include the variation of MVCT number. Therefore, we considered as the variation of the MVCT number using equation (3) and added it to the tolerance levels. Finally, the overall TLMD were calculated using the following equation (4):

graphic file with name DmEquation4.gif (4)

Verification of MD tolerance levels using clinical patient treatment plans

Multiple helical IMRT treatment plans based on kVCT images were created using the TomoTherapyHDA™ planning station v5.1.1 (Accuray Inc., Sunnyvale, CA). Table 1 showed the parameters of the treatment plans. The dose distributions were compared with and without the addition of TLMD to MVCT-MD table. Dose distributions of treatment planning for brain, head and neck, chest and prostate are shown in Fig. 2. Daily MVCT images acquired with the HD system were used to calculate the ART treatments. This study was approved by the Institutional Review Board (IRB). Dose calculations for the ART treatments and rigid image registration between the kVCT and MVCT images were performed using planned adaptive software (Accuray Inc., Sunnyvale, CA). The dose calculations were performed using convolution/superposition algorithms. A modified MVCT-MD table was created by adding the TLMD to the original table in the radiation therapy planning system (RTPS). TLMD is calculated for the effective maximum tissue thicknesses of lung, adipose/muscle and cartilage/spongy-bone from the RED tolerance levels for tissue thickness with a relative dose error of 2% from equation (1) converted to MD from equation (2), and added MVCT number variation equation (4). In previous study, the MD ranges were determined as 0.2 to 0.8 g/cm3, 0.9 to 1.07 g/cm3 and greater than 1.07 g cm3 for lung, adipose/muscle and cartilage/spongy, respectively [13, 14] The dose calculation including the addition of tolerance levels was performed by adding TLMD to MVCT-MD table for each tissue equivalent density plug. Hence the MDs from 0.1 to 0.9 g/cm3, 1.0 g/cm3 and 1.1 to 1.9 g/cm3 were added to the TLMD for the lung, adipose/muscle and cartilage/spongy-bone regions, respectively. The dose distribution was calculated using the MVCT-MD table with and without the addition of the calculated TLMD. The MVCT-MD table added the TLMD, and the calculated plan were defined as ‘modified plans’. Dose-volume histograms were compared between the original and modified plans. The planning target volume (PTV) dosimetric parameters were computed to evaluate the dose assessment metrics D98%, D2%, homogeneity index (HI) and conformity index (CI) which are recommended in the ICRU report 83 [15]. Dmax, Dmean, D10% of the organs at risk (OARs) and V20Gy of lung were calculated to evaluate the difference between original and modified plans.

Table 1.

Treatment planning characteristics: case, prescription, fractions, treatment parameters

Case Prescription Fractions FW (cm) Pitch Initial MF Final MF
Brain 50 Gy to D90% of PTV 20 2.5 0.215 2.000 1.791
Head and neck 70 Gy to D95% of PTV 35 2.5 0.430 2.500 1.941
Chest 70 Gy to D95% of PTV 35 2.5 0.430 2.000 1.891
Prostate 78 Gy to D95% of PTV 39 2.5 0.430 2.000 1.539

PTV, planning target volume; Dx%, dose received by ≥ x% of volume; FW, field width; MF, modulation factor.

Fig. 2.

Fig. 2

Treatment planning images of (A) the brain, (B) the head and neck, (C) the chest, (D) the Prostate cases. PTV, planning target volume.

RESULTS

Difference in the MD levels that result in 2% dose error

Figure 3 displays the relationship between the RED tolerance levels and tissue thickness (cm) corresponding to a dose error of 2% using equation (1). The effective tissue thicknesses of lung, adipose/muscle and cartilage/spongy-bone tissue groups were 10, 20 and 10 cm, respectively [9]. Thus, these tolerance levels of RED corresponding to a dose error of 2% were ± 0.045, ± 0.022 and ± 0.045 for the lung, adipose/muscle and cartilage/spongy-bone, respectively. Additionally, these tolerance levels of RED were converted into Inline graphic using equation (2). The Inline graphic were ± 0.045 g/cm3, ± 0.022 g/cm3 and ± 0.045 g/cm3 for the lung, adipose/muscle and cartilage/spongy-bone regions, respectively.

Fig. 3.

Fig. 3

Relationship between the relative RED tolerance for tomotherapy (6 MV FFF) and the tissue thickness corresponding to a dose error of 2%.

Stability of the MVCT number

Table 2 shows the variation in MVCT number over six months (n = 78) for each material and the converted MD from MVCT number with MVCT-MD table. The Inline graphicwas calculated by equation (3). The RMS of MVCT number for all plugs was 9.2 (HU), which corresponds to the Inline graphicof 0.010 g/cm3. The Inline graphic was converted MVCT number to MD in the MVCT-MD table.

Table 2.

The MDs, the measured MVCT numbers, and the converted MD from MVCT numbers with MVCT-MD table for tissue equivalent plugs inserted into the cheese phantom

Tissue equivalent density plugs MD (g/cm3) MVCT number [HU] Converted MD [g/cm3]
Mean SD Mean SD
Air 0.001 −936.8 4.3 0.023 0.005
LN-300lung 0.29 −677.0 7.6 0.295 0.008
LN-450lung 0.47 −508.7 9.6 0.480 0.011
True water 1 16.2 8.7 1.057 0.010
Inner bone 1.139 103.7 10.3 1.154 0.011
CB2 30% 1.333 284.3 10.2 1.352 0.011
CB2 50% 1.599 459.5 9.1 1.545 0.010
Cortical bone 1.822 677.4 12.1 1.785 0.013
All plugs RMS 9.2 0.010

MVCT, megavoltage computed tomography; HU, Hounsfield unit; MD, mass density; SD, standard deviation; RMS, root mean square.

Overall tolerance levels of the MD

Table 3 shows the TLMD for each MD and tissue group. The TLMD were calculated by including the variation of the MVCT number and estimated to cause 2% relative dose error to local dose error at tissue group. The TLMD of the MD were ± 0.049 g/cm3, ± 0.030 g/cm3 and ± 0.049 g/cm3 for the lung, adipose/muscle and cartilage/spongy-bone regions, respectively. Figure 4 shows the MVCT -MD table added overall tolerance levels of the MD.

Table 3.

MD tolerance levels for each tissue group

Tissue group MD (g/cm3) Inline graphic Inline graphic TL MD
Lung 0.1–0.9 ±0.045 ±0.020 ±0.049
Adipose/muscle 1.0 ±0.022 ±0.020 ±0.030
Cartilage/spongy bone 1.1–1.9 ±0.045 ±0.020 ±0.049

MD, mass density; Inline graphic, The MD tolerance levels that cause 2% dose error; Inline graphic, The variation of MD converted from the SD of MVCT number using MVCT-MD table for each tissue-equivalent density plug; TLMD, overall tolerance levels of MD.

Fig. 4.

Fig. 4

Relationship between MVCT number and MD for the cheese phantom. The black line is from the MVCT-MD table, and the red dashed lines represent the MVCT-MD table data ± the proposed MD tolerance levels.

Validation of MD tolerance using clinical patient treatment plans

Table 4 summarizes the dose assessment metric differences of the brain, head and neck, chest and prostate cases. The dose metric difference between the original and modified plans for the brain and head and neck cases were within −1.7% and −1.6%, respectively. The maximum dose metric difference in the D2% of PTV and Dmean of lung of the chest were −1.1% and −1.3%, respectively. The maximum dose metric difference in the D98% of PTV and Dmax of rectum for the prostate were −2% and −1.9%, respectively, which were equal to or just below the proposed TLMD of 2%. The HI result for the brain was 0.01, and CI result for the prostate was 0.02. The HI and CI results did not exhibit any differences.

Table 4.

The dose assessment metric differences between the original and modified plans for PTV and OAR

Case Structure name Metric Difference Case Structure name Metric Difference
Brain PTV D98% −1.2% Chest PTV D98% −0.9%
D2% −1.7% D2% −1.1%
HI 0.01 HI 0.00
CI 0.00 CI 0.00
Eyeball R Dmax −1.4% Lung Dmean −1.3%
Eyeball L Dmax −0.7% D10% −0.4%
Brain Dmax −1.4% V20 Gy −0.7%
Dmean −1.1% Spinal cord Dmax −1.0%
Head and neck PTV D98% −1.0% Prostate PTV D98% −2.0%
D2% −0.9% D2% −1.9%
HI 0.00 HI 0.00
CI 0.00 CI 0.02
CTV node D10% −1.0% Rectum Dmax −1.9%
Brainstem Dmax −1.6% Dmean −1.2%
Spinal cord Dmax −0.9% D10% −1.8%

CTV, clinical target volume; PTV, planning target volume; HI, homogeneity index; CI, conformity index; Dx%, dose received by ≥ x% of volume; Vx Gy, percentage of volume receiving x Gy of the prescribed dose.

DISCUSSION

The aim of this study was to propose TLMD in ART and evaluate the proposed tolerance levels. The variation in the SD of the MVCT number over six months was 2–8 times larger than that of the kVCT number from a previous study (Table 2) [9]. MVCT images are created with higher energy than kVCT images, which implies that noise increases due to the dominance of Compton interactions. The variation in MVCT numbers should be included in the tolerance levels. The HT guideline recommends that MVCT number tolerances of ±30 HU, ± 50 HU and ± 50 HU be used for water, lung and bone, respectively [7]. When these values were converted to MD using the MVCT-MD table registered in RTPS, they were ± 0.033 g/cm3 ± 0.055 g/cm3 and ± 0.055 g/cm3, respectively [7]. These values are almost consistent with the proposed TLMD. These factors that determine TLMD are Inline graphicand Inline graphic (equation (4)). Inline graphicdepends only on the energy of the treatment beam. We determined this first term by measuring the TMR for the HD system. We did not measure the TMR in the latest model of TomoTherapy (Radixact) and the previous model of TomoTherapy (HI-ART), we expect that it will be close to the Inline graphicfor HD system determined in this study. Therefore, the first term (Inline graphic) can be used to other facilities, but the second term (δMD) is the variation in MVCT number, which differs significantly among HI-ART, HD system and Radixact and must be evaluated in each model. The SD of MVCT number for HI-ART is 13.0 HU at 9 months [4]. The SD of MVCT number for the HD system was 9.2 HU at 6 months (Table 2). There are no results of stability for Radixact, but reports indicate that the noise is one-third of that of the HD system, so it is expected to be less variable [16]. The difference in SD of MVCT number between HI-ART and HD system is 3.8 HU. This effect increases the TLMD of the lung from 0.049 g/cm3 to 0.053 g/cm3 in HI-ART. This study is the result of a single HD system. To use TLMD at other facilities, you need to estimate the MD of the MVCT for each facility.

In the brain, head and neck, chest and prostate clinical treatments performed using HT, the MD values calculated in this study can be used as the proposed TLMD for patients. A previous study showed that those generated using the TMR method are dependent on the tissue thickness [8]. In this study, the dose errors in the brain and chest were approximately 1%, while those in the head and neck and prostate cases, were approximately 2%, which is equal to the proposed TLMD of 2% (Table 3). For the prostate, as the tissue is thicker than the brain, head and neck and the center of the body, the MD difference added to the MVCT-MD table accumulated along the treatment beam resulted in a dose error close to 2%. The prostate may exhibit a dose difference of more than 2% owing to variations in body thickness. A previous study reported that emphysema decreases lung density to 0.11 g/cm3, wherein the normal lung density is approximately 0.25 to 0.37 g/cm3 [17]. Assuming the same lung thickness of 20 cm and a density of 0.27 g/cm3 and 0.37 g/cm3, this lung MD difference would result in a dose error of 0.2%. If we assume a standard human lung from ICRP 110 [13], the dose error may increase.

A previous study reported that tissue equivalent density plugs inserted into the phantom at the CT-RED table differed the physical densities of human tissues, and some tissue equivalents exceeded the density tolerance for a dose error of 2% [17]. The results of this study may differ owing to the difference in the nominal density and actual human tissue of physical density.

CONCLUSION

In this study, we proposed for TLMD the MVCT-MD table for ART dose calculations. The QA of the MVCT-MD table using HT for ART recommends these tolerance values of the MD to be ±0.049 g/cm3, ± 0.030 g/cm3 and ± 0.049 g/cm3 for the lung, adipose/muscle and cartilage/spongy-bone, respectively, indicating a dose error within 2%.

Contributor Information

Shogo Tsunemine, Program of Medicine Doctoral Course, Graduate School of Biomedical and Health Sciences, Hiroshima University, 1-2-3, Kasumi, Minamiku, Hiroshima, 734-8553  Japan; Department of Radiology, National Hospital Organization Himeji Medical Center, 68, Hommachi, Himeji, Hyogo, 670-8520, Japan.

Shuichi Ozawa, Department of Radiology, National Hospital Organization Himeji Medical Center, 68, Hommachi, Himeji, Hyogo, 670-8520, Japan; Hiroshima High-Precision Radiotherapy Cancer Center, Hiroshima, 3-2-2, Futabanosato, Higashiku, Hiroshima, 732-0057, Japan; Department of Radiation Oncology, Graduate School of Biomedical and Health Sciences, Hiroshima University, 1-2-3, Kasumi, Minamiku, Hiroshima, 734-8553  Japan.

Minoru Nakao, Hiroshima High-Precision Radiotherapy Cancer Center, Hiroshima, 3-2-2, Futabanosato, Higashiku, Hiroshima, 732-0057, Japan; Department of Radiation Oncology, Graduate School of Biomedical and Health Sciences, Hiroshima University, 1-2-3, Kasumi, Minamiku, Hiroshima, 734-8553  Japan.

Hideharu Miura, Hiroshima High-Precision Radiotherapy Cancer Center, Hiroshima, 3-2-2, Futabanosato, Higashiku, Hiroshima, 732-0057, Japan; Department of Radiation Oncology, Graduate School of Biomedical and Health Sciences, Hiroshima University, 1-2-3, Kasumi, Minamiku, Hiroshima, 734-8553  Japan.

Akito Saito, Department of Radiation Oncology, Graduate School of Biomedical and Health Sciences, Hiroshima University, 1-2-3, Kasumi, Minamiku, Hiroshima, 734-8553  Japan.

Daisuke Kawahara, Department of Radiation Oncology, Graduate School of Biomedical and Health Sciences, Hiroshima University, 1-2-3, Kasumi, Minamiku, Hiroshima, 734-8553  Japan.

Yasuhiko Onishi, Department of Radiology, National Hospital Organization Himeji Medical Center, 68, Hommachi, Himeji, Hyogo, 670-8520, Japan.

Takashi Onishi, Department of Radiology, National Hospital Organization Himeji Medical Center, 68, Hommachi, Himeji, Hyogo, 670-8520, Japan.

Fumito Okawa, Department of Radiology, National Hospital Organization Himeji Medical Center, 68, Hommachi, Himeji, Hyogo, 670-8520, Japan.

Atsushi Terai, Department of Radiology, National Hospital Organization Himeji Medical Center, 68, Hommachi, Himeji, Hyogo, 670-8520, Japan.

Taiki Hashiguchi, Department of Radiology, National Hospital Organization Himeji Medical Center, 68, Hommachi, Himeji, Hyogo, 670-8520, Japan.

Hidetoshi Yamasaki, Department of Radiology, National Hospital Organization Himeji Medical Center, 68, Hommachi, Himeji, Hyogo, 670-8520, Japan.

Tsutomu Maruta, Department of Therapeutic Radiology, National Hospital Organization Himeji Medical Center, 68, Hommachi, Himeji, Hyogo, 670-8520, Japan.

Yuji Murakami, Hiroshima High-Precision Radiotherapy Cancer Center, Hiroshima, 3-2-2, Futabanosato, Higashiku, Hiroshima, 732-0057, Japan; Department of Radiation Oncology, Graduate School of Biomedical and Health Sciences, Hiroshima University, 1-2-3, Kasumi, Minamiku, Hiroshima, 734-8553  Japan.

Yasushi Nagata, Hiroshima High-Precision Radiotherapy Cancer Center, Hiroshima, 3-2-2, Futabanosato, Higashiku, Hiroshima, 732-0057, Japan; Department of Radiation Oncology, Graduate School of Biomedical and Health Sciences, Hiroshima University, 1-2-3, Kasumi, Minamiku, Hiroshima, 734-8553  Japan.

CONFLICT OF INTEREST

The authors declare that they have no conflict of interest to disclose.

FUNDING

This work was supported by AMED under Grant Number 2031526, JSPS KAKENHI Grant Number 19 K12865 and 19 K17269.

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