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Impacts of different b and TE values on quality of 3T diffusion-weighted imaging of the liver using a high gradient magnetic field: feasibility of ultrahigh b value of 3000
Keita Fukushima1, Katsuhiro Sano2, Haruhiko Machida3, Toshiya Kariyasu3, Isao Miyazaki1, Tatsuya Yoshioka1, Sanae Takahashi1, Saori Yuda1, Yuta Shimizu1, Takayuki Yonaha1, Akihito Nakanishi1, Hiroshi Kusahara4, Youhei Matsuoka4, Miho Kitamura4, Takao Yamamoto4, and Kenichi Yokoyama3

1Kyorin University Hospital, Tokyo, Japan, 2Diagnostic Imaging, Saitama medical University International medical Center, Saitama, Japan, 3Kyorin University School of Medicine, Tokyo, Japan, 4CANON MEDICAL SYSTEMS CORPORATION, Otawara, Japan

Synopsis

Diffusion-weighted imaging (DWI) with an ultrahigh b value is expected to improve assessment of tumor cellularity and fluid viscosity in the liver but can decrease signal-to-noise ratio (SNR) of the hepatic parenchyma. A state-of-the-art 3T MR scanner with the maximal gradient magnetic field of 100 mT/m can achieve sufficient SNR on liver DWI even at ultrahigh b value of 3000 with use of short TE. The present study using our original phantom and healthy volunteers shows that use of shorter TE significantly increased the SNR with preserved ADC value on DWI even at ultrahigh b value of 3000.

Introduction

Diffusion-weighted imaging (DWI) with a high b value of around 1000 sec/mm2 is commonly acquired to assess tumor cellularity and fluid viscosity in 3T MR examinations of the liver. Use of a higher b value is expected to improve this assessment but can degrade the image quality and interpretability with decreased signal-to-noise ratio (SNR) of the hepatic parenchyma. Recently, a state-of-the-art 3T MR scanner (Vantage Galan 3T/ZGO; Canon, Tochigi, Japan) with the maximal gradient magnetic field of 100 mT/m has been clinically introduced. This high gradient magnetic field allows the selection of an ultrahigh b value (e.g., b = 3000) without the need to increase echo time (TE) on liver DWI with preserving the SNR. The purpose of the present study was to assess impacts of different b and TE values on quality of liver DWI and to prove feasibility of the ultrahigh-b-value DWI using this MR scanner.

Methods

We originally generated a phantom consisting of seven tubes of 3-cm diameter containing gelatin/distilled water with various weight percentages (0, 10, 20, 30, 40, 45, and 50%), one at the center and six symmetrically placed around it, in a polyethylene container of 20-cm diameter filled with superabsorbent polymer (Figure 1). With this MR scanner, we scanned this phantom with various T2 (31.5-868.6 msec) and apparent diffusion coefficient (ADC) values (0.45-2.01 x 10-3 mm2/sec) using body (Atlas SPEEDER body) and spine coils (Atlas SPEEDER spine) and acquired DWI using a spin-echo echo planner imaging sequence with the following scan parameters: repetition time (TR), 7000 msec; flip angle, 90/180 degrees; field of view, 33 x 36 cm; matrix size, 160 x 160; b value, 1000 and 3000 sec/mm2; TE, 44 (b = 1000), 53 (b = 3000), and 70 msec (b = 1000 and 3000). We placed regions of interest (ROIs) in the cross-section image of each tube phantom and background to measure the SNR and ADC values. We also scanned 10 volunteers (5 men and 5 woman; age, 69.1±19.0 years) and 11 patients who had hepatic masses (5 men and 6 women; age, 72.8±9.7 years) including hepatocellular carcinoma in one patient; metastatic tumor, one; focal nodular hyperplasia, one; hemangioma, two; complicated cyst, one; and simple cyst, five. We placed four ROIs in the both hepatic lobes in each volunteer and one ROI in a hepatic mass in each patient. We calculated SNR and ADC values at different b and TE values. We used paired t test to compare the SNR and ADC values of the hepatic parenchyma and masses between different TE values (TE 70 vs. TE 44 or 53) at the same b value.

Results

In the phantom study (Figure 1), the SNR at TE 44 was higher than that at TE 70 at b value of 1000. The SNR at TE 53 was higher than that at TE 70 at b value of 3000. The ADC was comparable between different TE values at the both b values. The mean SNR of the hepatic parenchyma in volunteers was significantly higher at TE 44 (94.7±15.8) than at TE 70 (35.9±7.1) at b value of 1000; and at TE 53 (18.9±4.4) than at TE 70 (12.4±3.2) at b value of 3000 (p < 0.05 for both) (Figure 2). The mean ADC was comparable between different TE values (p > 0.05 for both) (Figure 3). The mean SNR of the hepatic masses was also significantly higher at TE 44 (122.1±61.7) than at TE 70 (86.5±52.0) at b value of 1000; and at TE 53 (25.7±17.4) than at TE 70 (19.4±11.8) at b value of 3000 (p < 0.05 for both) (Figure 2). The mean ADC was comparable between different TE values (p > 0.05 for both) (Figure 3).

Discussion

Use of short TE values offers higher SNR on DWI than at TE 70, commonly used for liver DWI, without affecting ADC values; actually, can reveal the hepatic parenchyma even at ultrahigh b value of 3000 (Figure 4) and more accurately differentiate malignant (e.g., metastatic tumor) from benign hepatic masses (e.g., hemangioma) at the b value (Figure 5).

Conclusion

Use of short TE values can achieve sufficient SNR on liver DWI even at ultrahigh b value of 3000 with this MR scanner.

Acknowledgements

No acknowledgement found.

References

No reference found.

Figures

Fig. 1 A photograph (a) and an ADC map of our original phantom (b) consisting of seven tubes containing gelatin/distilled water with various weight percentages, one at the center and six symmetrically placed around it, in a polyethylene container filled with superabsorbent polymer. Bar graphs representing SNR (c) and ADC values (d) at different TE values obtained from our phantom experiment at ultrahigh b value of 3000. The SNR is higher at TE 53 than at TE 70 and ADC is comparable between the both TE values at all the percentages of gelatin/distilled water.

Fig. 2 Bar graphs representing SNR value at different TE values of the hepatic parenchyma (a, b) obtained from our healthy volunteers at b values of 1000 (a) and 3000 (b) and that of hepatic masses (c, d) from our patients at b values of 1000 (c) and 3000 (d). The SNR is significantly higher at TE 44 (a, c) or TE 53 (b, d) than at TE 70 (p < 0.05), as represented by asterisks.

Fig. 3 Bar graphs representing ADC value at different TE values of the hepatic parenchyma (a, b) obtained from our healthy volunteers at b values of 1000 (a) and 3000 (b) and that of hepatic masses (c, d) from our patients at b values of 1000 (c) and 3000 (d). The ADC is comparable between TE 44 (a, c) or TE 53 (b, d) and TE 70 (p > 0.05).

Fig. 4 Liver DWI at b 3000 in a healthy volunteer at TE 70 (a) and 53 (b) acquired with the following scan parameters: TR, 7000 msec; flip angle, 90/180 degrees; field of view, 33 x 36 cm; matrix size, 160 x 160. The hepatic parenchyma is sufficiently visualized with higher SNR (26.1 [TE 53] vs. 15.9 [TE 70]) at TE 53 (b) even at ultrahigh b value of 3000 compared with TE 70 (a).

Fig. 5 Contrast-enhanced dynamic T1WI during the arterial phase (a, f) and DWI at b 1000 at TE 70 (b, g) and 44 (c, h) and at b 3000 at TE 70 (d, i) and 53 (e, j) in a patient with a hepatic hemangioma (a-e) and another patient with a hepatic metastatic tumor (f-j). Both the hepatic masses similarly show ring enhancement on the T1WI (a, f). Whereas the metastatic tumor (f-j) similarly shows high signal, the hemangioma shows lower signal on DWI at b 3000 (d, e) than at b 1000 (b, c).

Proc. Intl. Soc. Mag. Reson. Med. 27 (2019)
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