DWI has shown promise for detecting and characterizing breast cancers but is limited by the low spatial resolution of standard spin-echo EPI techniques. Several strategies have been proposed to generate high resolution DWI, including reduced field-of view, steady-state imaging, readout-segmented EPI, and simultaneous multi-slice imaging (SMS). In this work we adopt the Crété-Roffet blur metric to objectively compare resolution of three DWI strategies, including standard SE-EPI, and RO-segmented EPI and SMS-EPI high resolution approaches. In this comparison, both high-resolution DWI methods showed an improvement in in-plane resolution over the standard technique. The Crété-Roffet blur metric appears to be a robust and objective means of comparing effective resolution.
While diffusion weighted imaging (DWI) has shown promise for breast cancer treatment[1] the low spatial resolution of the standard technique (spin-echo (SE)-EPI) limits lesion detection and biases apparent diffusion coefficients (ADCs) due to partial volume effects. Several strategies have been proposed to generate high resolution DWI, including reduced field-of-view[2], steady-state imaging[3], readout-segmented EPI[4], and simultaneous multi-slice imaging (SMS)[5,6]. It is important to objectively compare techniques throughout development to guide protocol optimization. However, comparing resolution can be difficult for several reasons: nominal resolution does not reliably reflect the true image resolution due to blurring effects from off-resonance and T2*-decay, especially in EPI; subjective assessment is laborious and prone to bias[7]; and phantom assessments cannot fully replicate all in vivo sources of blurring. This work adapts an objective measurement from the computer vision field, the Crété-Roffet metric[8], to assess the resolution of several DWI strategies. The Crété-Roffet metric quantitatively measures blurring from 0 (sharp) to 1 (blurry) and has previously been validated against subjective blur assessment.
Purpose: To compare the resolution of three different breast DWI protocols using the Crété-Roffet method.
Fifteen breast cancer patients were scanned under an IRB-approved protocol on a Siemens 3T PrismaFit using a 16-channel Sentinelle breast coil. DWI was acquired with 3 protocols, each constrained to a 5-minute acquisition: standard single-shot SE-EPI (Std) following the ACRIN 6698 protocol[9], readout-segmented EPI (RS-EPI) with 5 segments based on Wisner et al.’s protocol[2], and a simultaneous multi-slice (SMS) acquisition acquired sagittally and reformatted axially[6]. A standard anatomical T2-weighted image (T2w) was included for comparison. All protocols were repeated on a quantitative breast phantom[10] that includes a resolution grid and tissue mimics. Table 1 provides sequence details.
Image processing was performed in Matlab using DICOM (magnitude) images. Because each protocol was acquired with different nominal resolutions, all images were resampled onto a common 0.5 mm isotropic grid (smaller than any nominal resolution). The blur metric was calculated independently for each Cartesian direction.
Figure 1 shows axial b=0 s/mm2 DWI and T2w images of the breast phantom resolution grids. The 2 mm feature (red) is barely detectible in the Std approach and readily visible with RS-EPI. While SMS-DWI can detect the smallest 1 mm feature (blue) and 1.25 mm grid (yellow), they are sharpest in the anatomical T2w image.
Figure 2 shows the three DWI methods and the T2w anatomical image from an example in vivo case after resampling to a 0.5 mm common grid. The increase in effective resolution from (a) to (d) can be readily observed. Figure 2 shows the blur metric measured in the axial plane (average of right-left and anterior-posterior) for the three DWI methods at both b=0 and 800 s/mm2, and also for the T2w image. Consistent with Figures 1 and 2, T2w shows the least blurring, followed by SMS-EPI, RS-EPI, and finally the standard SE-EPI technique. Note that the b=800 image is more blurry than b=0 for all DWI methods due to increased relative fat signal, eddy currents, and averaging over respiratory cycles.
In Figure 3 the standard method shows more in-plane blurring than the readout-segmented method even though its nominal pixel size is smaller. Figure 4 explores this further by plotting the blur metric as a function of nominal pixel size in all 3 directions. There is a general trend for greater sharpness with smaller pixel sizes (green line), but this does not hold for PE in single-shot EPI.
NIH P41 EB015894
NIH R21 CA201834
NIH 1S10 OD017974-01
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