Breast PET scanners
Three dedicated breast PET systems were evaluated in this study: opposed-type PEM, photomultiplier tube-based dbPET (dbPET1), and silicon photomultiplier-based dbPET (dbPET2) (Fig. 1).
PEM (PEMGRAPH, Mirai Imaging Inc., Japan)
The PEM system is composed of an opposed-type device equipped with two flat-panel detectors arranged in a face-to-face configuration, enabling high-resolution imaging of the soft-compressed breast (Fig. 1a). Previous studies have described its basic design and clinical performance, demonstrating its utility for detecting small BCs [7,8]. PEM has a larger defection of the lines of response (LOR) compared with dbPET scanners, in which cylindrical detector arrays are placed around the breast. Therefore, usually only one direction of maximum intensity projection (MIP) is adopted per acquisition (not tomographic images). In this study, the images were reconstructed using the 3D-Maximum Likelihood Expectation Maximization algorithm with eight iterations and an anti-aliasing filter with dead time, random and decay correction, and no attenuation correction. Based on a phantom scan with known 18F- fluorodeoxyglucose (FDG) radioactivity, the pixel values of clinical PEM images were converted into standardized uptake values (SUVs).
dbPET1 (Elmammo Avant Class™, Shimadzu Corporation, Japan) and dbPET2 (BresTome™, Shimadzu Corporation, Japan)
The dbPET system is equipped with a cylindrical detector module arrangement, enabling high-resolution imaging of the breast while it is hanging due to gravity [5,9]. Because dbPET scanners have fewer missing LORs than PEM scanners, both mediolateral and craniocaudal MIPs as well as cross-sectional images are usually used for diagnosis per acquisition. In dbPET, pixel values are converted to the SUV through attenuation correction using a µ-map, which is obtained by detecting the skin surface from the emission scan data and assuming the breast is a homogeneous absorber.
dbPET1 is an earlier-generation ring-type dbPET system that employs conventional photomultiplier tubes, and dbPET2 is a next-generation ring-type dbPET system incorporating digital silicon photomultipliers, offering better sensitivity and spatial resolution compared with dbPET1(Fig. 1B and C) [5,10].
The primary specifications of these three systems are summarized in Table 1. Further technical details can be found in previous studies [11].
Table 1
Main specifications of the three breast-specific PET systems evaluated in this study
|
System Type
|
PEM
|
dbPET1
|
dbPET2
|
|
Scanner Name
|
PEMGRAPH
|
Elmammo™
|
BresTome™
|
|
Vendor
|
Mirai Imaging Co., Ltd.
|
Shimadzu
|
Shimadzu
|
|
Detector shape
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Opposed plate-type
|
Ring- type
|
Ring- type
|
|
Detector aperture
|
100–250 mm* (gap, plate)
|
φ195 mm (circ.)
|
φ300 mm (circ.)
|
|
FOV (mm)
|
202.4×140.8 (rect.)×100–250 mm*
|
φ182 (circ.)×103
|
φ264 (circ.) ×162
|
|
Material of crystal
|
LuAG
|
LGSO
|
LGSO
|
|
Crystal size (mm3)
|
1.5×1.5×11
|
1.44×1.44×18
|
2.1×2.1×15
|
|
Photo device
|
PMT
|
PMT
|
SiPM
|
|
Number of DOI layers
|
1
|
4
|
1
|
|
TOF Technology
|
Not available
|
Not available
|
Available
|
|
Matrix size (mm)
|
254 (X)×176 (Y)
|
236 (X)×132(Y)×236 (Z)
|
240 (X)×148 (Y)×240 (Z)
|
|
Pixel size (mm2)
|
0.8
|
0.78
|
1.1
|
|
Spatial resolution at 5 mm offset from the center of the FOV (mm)⁑
|
up to 2.0
|
up to 1.5
|
from to 1.0 to 2.5
|
|
Sensitivity at 0cm in the center of the FOV (cps/kBq)⁑
|
0.005
|
from 0.05 to 0.09
|
from 0.06 to 0.11
|
| *Adjustable in 25 mm increments, ⁑NEMA NU 4-2008 22Na source |
Abbreviations: PET, positron emission tomography; PEM, positron emission mammography; dbPET, dedicated breast PET; FOV, field of view; rect., rectangular; circ., circular; LuAG, lutetium aluminum garnet; LGSO, lutetium gadolinium oxyorthosilicate; PMT, photomultiplier tube; SiPM, silicon photomultiplier; DOI, depth-of-interaction; TOF, time of flight; NEMA-NU, National Electrical Manufacturers Association – NU standard; cps/Bq, counts per second per becquerel
Phantom preparation
A cylindrical phantom containing four hot spheres was used for the comparison of the breast PET scanners. In order to detect BC lesions with a diameter of 5 mm, which corresponds to T1a in the Union for International Cancer Control (UICC) TNM classification, spheres of four different sizes (3, 5, 7.5, and 10 mm) were adopted. For PET image evaluation based on phantom studies, the sphere-to-background radioactivity concentration ratio (SBR) is commonly set at 8:1. However, most previous studies were designed for whole-body PET scanners, lacking verification of the suitability of this SBR for breast PET. Therefore, in this study, the SBR was determined by measuring the radioactivity counts of the breast lesion, background mammary glands, and subcutaneous fat on the clinical breast PET images of patients with BC or suspected BC.
Phantom setup
For the PEM system, a cylindrical phantom was positioned between the two flat-panel detectors, and a custom-made acrylate–styrene acrylonitrile stand was used to prevent rolling (Fig. 2). For dbPET1 and dbPET2, the phantom was placed directly within the ring-shaped detector bore. When the position of the hot spheres needed to be changed, the phantom was elevated with spacers to adjust the vertical alignment.
Data acquisition
Based on previous studies [1,5], the phantom was placed with four hot spheres arranged in the center of the field of view (FOV) (center) and 2 cm inside the edge of the FOV (periphery) of each scanner. A custom-made acrylate–styrene–acrylonitrile stand was prepared to hold the cylindrical phantom on the PEM detector. The phantom prepared in each SBR was imaged for 10 min in list-mode at two positions (center and periphery) [12,13].
Image reconstruction
All the breast PET images were reconstructed using the clinical conditions for each scanner, which were determined based on the results of previous studies and clinical experience [7,10,11]. However, the acquisition time can vary in routine clinical practice depending on the patient’s condition. To determine the minimum acquisition time required for diagnosis, the phantom images were reconstructed using full data (10 min) and short-time acquisitions (1, 3, 5, and 7 min) by dividing the list-mode data. The reconstruction conditions specific to each scanner are summarized in Table 2.
Table 2
Main reconstruction parameters of the three breast-specific PET systems evaluated in this study
|
System Type
|
PEM
|
dbPET1
|
dbPET2
|
|
Iterative reconstruction
|
3D-MLEM
|
3D-DRAMA
|
3D-DRAMA
|
|
Scatter correction
|
Not available
|
Convolution Subtraction
|
True estimate subtraction
|
|
Attenuation correction
|
Not available
|
Uniform attenuation map with object boundaries obtained from emission data
|
Uniform attenuation map with object boundaries obtained from emission data
|
|
Iterations / Subsets
|
8/1
|
1/128
|
1/100
|
|
Post filter
|
MRP
|
Median, Gaussian
|
Median, Gaussian, NLM
|
|
SUV conversion
|
Available
|
Available
|
Available
|
Abbreviations: PET, positron emission tomography; 3D, three-dimensional; ML-EM, maximum likelihood-expectation maximization; DRAMA, dynamic row-action maximum likelihood algorithm; MRP, Modified Ramp; NLM, non local means
Analysis of phantom image quality
All transverse phantom images that lined the largest cross-section of the hot spheres were displayed in inverse grayscale, with SUVs ranging from 0 to 4. In dbPET, all four hot spheres were displayed as a single transverse image, whereas in PEM, two spheres were displayed per image, resulting in two images covering all four spheres. First, two experienced nuclear medicine physicians and PET technologists each, who were blinded to the SBR settings, visually evaluated the visibility of the hot spheres in the reconstructed breast PET images using 10 min of acquisition data. Thereafter, the full-length and short-time acquired images were compared visually and quantitatively.
For quantitative evaluation, circular regions of interest (ROIs) with the same diameter as the sphere were placed on the spheres in the phantom images. Additionally, eight ROIs with a diameter of 10 mm were placed in the background, and the coefficient of variation of the background (CVBG), detection index (DI), and contrast recovery coefficient (CRC) were calculated using the following formulae:
CVBG = \(\:\frac{{SD}_{BG,10mm}}{{C}_{BG,10mm}}\),
where SDBG,10mm is the standard deviation of the background ROI for a 10-mm diameter circle, and CBG,10mm is the average of the background ROI values for a 10-mm diameter circle
DI = \(\:\frac{{C}_{H,5mm;max}-{C}_{BG,10mm;mean}}{{SD}_{BG}}\),
where CH,5mm;max is the maximum SUV (SUVmax) of the ROI for a 5-mm diameter sphere and CBG,10mm;mean is the average of the background ROIs for a 10-mm diameter circle
CRC = \(\:\frac{\left({C}_{H;max}/{C}_{BG:mean}\right)-1}{\left({a}_{H}/{a}_{BG}\right)-1}\),
where aH and aBG represent the activity concentrations in the hot sphere and background, respectively.
Human imaging
This study was approved by the Medical Research Ethics Review Committee of the Fujita Health University (HM25-186). All procedures were performed in accordance with the ethical standards outlined in the 1964 Declaration of Helsinki and its subsequent revisions. Based on the retrospective observational study design, informed consent was waived for all patients.
Patients fasted for at least 6 h before the 18F-FDG (3.7 MBq/kg) injection. Following a whole-body PET/CT scan, the breasts were scanned separately on each side, with breast PET commencing approximately 90 min after the administration of 18F-FDG. Breast PET images were also reconstructed using clinical conditions. Full and short-acquisition-time clinical PET images of representative cases scanned using each scanner were reviewed and discussed, along with the results of the phantom studies.
Representative BC images were presented using three breast PET scans and other modalities to compare the characteristics of the three breast PET systems. These cases were selected to demonstrate the typical imaging features of three different types of lesions based on previous studies[14,15]: i) mass-like uptake near the nipple, ii) mass-like uptake slightly near the chest wall, and iii) non-mass uptake (NMU).
In accordance with the phantom study, short-time acquisition images were reconstructed from the list-mode data of the clinical NMU lesions. For quantitative evaluation, SUVmax and tumor-to-background ratio (TBR) were calculated using the following equations:
TBR = \(\:\frac{{SUV}_{\:T,max}}{{SUV}_{BG,\:mean}}\),
where SUVT,max is the SUVmax of the tumor (BC lesion) and SUVBG,mean is the mean value of the largest circular ROI placed on the background to avoid breast tumors, skin, and noise at the edge of the FOV, respectively.