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DOI:10.2214/AJR.06.0556
AJR 2007; 188:W199-W201
© American Roentgen Ray Society


Technical Innovation

Isotropic 3D Fast Spin-Echo with Proton-Density-Like Contrast: A Comprehensive Approach to Musculoskeletal MRI

Lawrence Yao1, John T. Pitts2 and David Thomasson1

1 Diagnostic Radiology Department, Clinical Center, National Institutes of Health, 10 Center Dr., Rm. 1C360, Bethesda, MD 20892.
2 InVivo Corporation, Orlando, FL.

Received April 23, 2006; accepted after revision July 17, 2006.

 
Address correspondence to L. Yao.

J. T. Pitts is employed by InVivo Corporation, Orlando, FL.

WEB This is a Web exclusive article.


Abstract
Top
Abstract
Introduction
Materials and Methods
Discussion
References
 
OBJECTIVE. Scanning time considerations have restricted routine use of 3D Fourier transform (3DFT)-encoded MRI to gradient-recalled echo sequences. We sought to combine isotropic 3DFT acquisition with fast spin-echo at a practical scan duration. This strategy offers versatile image contrast for musculoskeletal evaluation and facilitates image reformation tailored to the depiction of small anatomic features.

CONCLUSION. Isotropic 3DFT fast spin-echo is feasible on current MRI scanners and has the potential to improve musculoskeletal evaluation.

Keywords: ankle • high resolution • MRI • MR technique


Introduction
Top
Abstract
Introduction
Materials and Methods
Discussion
References
 
Currently, the most versatile type of sequence for musculoskeletal MRI evaluation is arguably a fast spin-echo acquisition with proton density-weighting. Fast spin-echo sequences are preferred over conventional spin-echo sequences for reasons of efficiency. This type of sequence has favorable contrast characteristics for assessment of hyaline cartilage, ligaments, tendons, and fibrocartilage [1-3]. Proton density-weighting also confers favorable signal-to-noise ratio characteristics, which facilitates the high image resolution that is necessary for evaluation of small body parts.

The nature of small body parts evaluation poses special challenges for routine MRI scan plane selection and prescription. Depiction of important structures may require complex oblique scan planes. Variances in body part positioning may alter the relationships between structures of interest and anatomic landmarks. Optimal oblique or double oblique scan plane prescription therefore requires detailed knowledge of clinical anatomy.

For these reasons, 3D Fourier transform (3DFT) acquisition is conceptually attractive for small body parts MRI evaluation, both because of signal-to-noise ratio efficiency [3] and the facilitation of image reformation in complex, oblique planes after scan acquisition. Practical application of 3DFT imaging has been largely restricted to gradient-recalled echo (GRE) sequences, which can be implemented at high resolution in reasonable scanning times. Despite varied strategies for GRE scan acquisition, GRE sequences typically lack the tissue contrast necessary for broad musculoskeletal diagnosis [4]. These sequences are therefore more commonly adjunctive to spin-echo imaging or used for imaging after IV contrast administration.

In this article, we illustrate the emerging feasibility of 3DFT acquisition of turbo spin-echo (TSE) images for routine musculoskeletal evaluation. The efficiencies of parallel imaging have brought the scanning duration for this strategy into a clinically acceptable range. We illustrate how this sequence can be implemented with an efficient, relatively short repetition time and a driven equilibrium pulse [5] to create tissue contrast that is similar to the proton density-weighting preferred for many musculoskeletal applications.


Materials and Methods
Top
Abstract
Introduction
Materials and Methods
Discussion
References
 
An isotropic 3DFT TSE, proton density-weighted sequence was implemented for musculoskeletal evaluation on a commercial 3-T MRI system (Intera, Philips Medical Systems). Scanning parameters for 3DFT TSE were TR/TE effective, 720/40; echo-train length, 11; slice partitions, 142; imaging matrix, 256 x 256. The k-space sampling order was low to high (centric). A terminal -90° radiofrequency pulse was used for restoration of longitudinal magnetization (DRIVen Equilibrium pulse, [DRIVE]). Refocusing radiofrequency pulses were reduced in amplitude (140°) to reduce the specific absorption rate (SAR). These refocusing pulses were spatially broad to enable echo spacings of 7 milliseconds at a receiver bandwidth of ± 56.3 kHz.

Scanning acceleration was achieved by using sensitivity encoding (SENSE) in both the slice and in-plane phase-encoding dimensions, with an acceleration factor of two. Half-Fourier sampling was also used in the in-plane phase direction. The total scanning time was 7 minutes 20 seconds.


Figure 1
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Fig. 1A —Several anatomic structures in ankle and hindfoot of healthy 43-year-old male volunteer. Parameters for axial 2D turbo spin-echo (TSE) image, A, were TR/TE, 2,800/30 and echo-train length, 7. Parameters for various optimized, view planes reformatted from single 3D Fourier transform TSE acquisitions, B-F, were 720/40 and echo-train length, 11. Axial 2D TSE image shows calcaneofibular ligament (arrowhead) and portion of anterior talofibular ligament (arrow). Synovial fluid in anterolateral gutter is nearly isointense to cartilage and inconspicuous.

 


Figure 2
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Fig. 1B —Several anatomic structures in ankle and hindfoot of healthy 43-year-old male volunteer. Parameters for axial 2D turbo spin-echo (TSE) image, A, were TR/TE, 2,800/30 and echo-train length, 7. Parameters for various optimized, view planes reformatted from single 3D Fourier transform TSE acquisitions, B-F, were 720/40 and echo-train length, 11. Axial oblique 3D TSE image reformatted to show anterior talofibular ligament (arrow) to advantage. Joint fluid deep in relation to this ligament is relatively bright because of driven equilibrium technique, creating useful positive contrast relative to cartilage.

 


Figure 3
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Fig. 1C —Several anatomic structures in ankle and hindfoot of healthy 43-year-old male volunteer. Parameters for axial 2D turbo spin-echo (TSE) image, A, were TR/TE, 2,800/30 and echo-train length, 7. Parameters for various optimized, view planes reformatted from single 3D Fourier transform TSE acquisitions, B-F, were 720/40 and echo-train length, 11. Second axial oblique 3D TSE image is reformatted to show calcaneofibular ligament (arrow) to advantage. This ligament is typically not well seen on axial images oriented for best depiction of anterior talofibular ligament.

 


Figure 4
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Fig. 1D —Several anatomic structures in ankle and hindfoot of healthy 43-year-old male volunteer. Parameters for axial 2D turbo spin-echo (TSE) image, A, were TR/TE, 2,800/30 and echo-train length, 7. Parameters for various optimized, view planes reformatted from single 3D Fourier transform TSE acquisitions, B-F, were 720/40 and echo-train length, 11. Sagittal oblique 3D TSE image reformatted to course of flexor hallucis longus tendon (arrowheads) as it traverses tarsal tunnel.

 


Figure 5
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Fig. 1E —Several anatomic structures in ankle and hindfoot of healthy 43-year-old male volunteer. Parameters for axial 2D turbo spin-echo (TSE) image, A, were TR/TE, 2,800/30 and echo-train length, 7. Parameters for various optimized, view planes reformatted from single 3D Fourier transform TSE acquisitions, B-F, were 720/40 and echo-train length, 11. Axial oblique 3D TSE image reformatted to show both inferoplantar, longitudinal (arrowhead), and medioplantar oblique (arrow) portions of spring ligament. These structures are not consistently visualized on routine axial or sagittal 2D image acquisitions.

 


Figure 6
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Fig. 1F —Several anatomic structures in ankle and hindfoot of healthy 43-year-old male volunteer. Parameters for axial 2D turbo spin-echo (TSE) image, A, were TR/TE, 2,800/30 and echo-train length, 7. Parameters for various optimized, view planes reformatted from single 3D Fourier transform TSE acquisitions, B-F, were 720/40 and echo-train length, 11. Coronal oblique 3D TSE image reformatted to show separate fascicles of anterior tibiofibular ligament (arrowhead). This structure, which is deranged in high ankle sprain, is challenging diagnosis on routine 2D imaging. Tibiospring fibers of deltoid ligament (arrow) and tibiotalar joint are also well shown in this viewing plane.

 
Conventional 2D TSE imaging with proton density-weighting was also performed in the axial plane with the following scan parameters: 2,800/30; echo-train length, 7; imaging matrix, 320 x 256; slice thickness, 3 mm; field of view, 14 cm; averages, 2. The total scanning time for the 2D acquisition was 3 minutes 25 seconds.

The utility of this scanning strategy was illustrated in the ankle and hindfoot. The ankles of healthy volunteers (four men; age range 25-57 years) were scanned in the prone position using a 6-channel, 8-element volume extremity receiver coil. Images were acquired in the oblique sagittal plane using a 14-cm field of view. The voxel dimensions were 0.5 x 0.55 x 0.55 mm. Frequency encoding was oriented along the craniocaudal axis. Images from the 3D acquisition were reformatted on a commercially available workstation (Advantage Windows, GE Healthcare). Multiplanar reformations were generated at a 1.6-mm slice thickness.

MR images of the ankle of a healthy volunteer are shown in Figure 1A, 1B, 1C, 1D, 1E, 1F. Figure 1A is a sample axial 2D TSE image with proton density-weighting. Figures 1B, 1C, 1D, 1E, 1F are illustrative reformations of a 3D TSE acquisition in compound oblique planes tailored to depict anatomic structures of routine interest. Image contrast in the 3D TSE images is similar to the 2D TSE images, although there is relatively lower signal in muscle and higher signal in synovial fluid. Whereas the axial 2D image has an apparent advantage in in-plane resolution, the reformations of the 3D acquisition show how anatomy can be retrospectively viewed in complex view-plane orientations without a discernible compromise in spatial resolution. In this way, a single 3DFT TSE scan facilitates a detailed assessment of various structures that would require a multiplicity of carefully prescribed compound oblique 2D TSE acquisitions.


Discussion
Top
Abstract
Introduction
Materials and Methods
Discussion
References
 
Long scan times have limited the clinical utility of 3D spin-echo imaging implementations [6, 7]. On current high-field scanning platforms that support multichannel coil technology, 3D TSE is now a viable alternative to traditional multiplanar 2D scanning protocols because of the acceleration of phase encoding afforded by parallel acquisition strategies such as simultaneous acquisition of spatial harmonics (SMASH) or SENSE. Although 3D TSE scanning times are longer than individual 2D TSE scanning times, the 3D technique may decrease overall scanning time by obviating multiple orthogonal 2D acquisitions that are routinely required for clinical evaluation. Three-dimensional TSE acquisition may improve evaluation of complex anatomy by facilitating multiplanar image reformation in arbitrary planes tailored to specific anatomic regions of interest. Isotropic or near isotropic 3D data sets offer potentially superior evaluation of small body parts, given that optimally oriented 2D scans cannot be acquired for all potential structures of interest in regions of complex anatomy.

Volumetric 3D TSE imaging may offer practical advantages as well. Two-dimensional multiplanar scanning prescription requires a thorough working knowledge of clinical anatomy. The optimal scanning plane may also be influenced by body part position, which is particularly variable for the extremities. Scanning prescription is therefore imperfect, subjective, and dependent on user experience. A 3D volumetric scanning prescription is inherently simpler and more robust.

Limitations to the 3D TSE approach are several. The technique is only feasible for anatomic parts in which a parallel imaging technique can be applied in two dimensions. Foldover artifact must be avoided in two orthogonal dimensions. SAR limitations pose challenges to implementation of this strategy, particularly at 3-T and higher magnetic field strengths. For these reasons, the full potential of this strategy may await the availability of send-receive, multichannel extremity, or smallvolume coils.

SAR considerations dictate the use of refocusing radiofrequency pulses of reduced amplitude, which may have unanticipated effects on tissue contrast [8]. These effects, and the use of fast recovery or tip-back radiofrequency pulses [5], may warrant a reformulation of the scanning parameters that define a 3D TSE sequence with the most broadly useful contrast characteristics for musculoskeletal evaluation. In the implementation we have presented, we sought to mimic the proton-density contrast that is popular in 2D TSE scans. The contrast in the 3D TSE sequence is not strictly a reflection of proton density weighting, however, but a complex function of T1, T2, and the ratio of T2 to T1. The utility of a DRIVE pulse to confer "arthrographic" contrast to T1-weighted 2D TSE imaging, creating a mixed-contrast sequence useful for musculoskeletal evaluation, has also been highlighted in another recent report [9].

A volumetric, isotropic 3D approach to routine musculoskeletal diagnosis presents new challenges for MR image review and interpretation. The strength of the approach is the facility to view the data in arbitrary and customized cross-sectional planes. To fully exploit the potential of 3D data sets, the interpretative process demands real-time interactive image reformation. Fortunately, many diagnostic workstation environments have already incorporated these important image navigation capabilities.


References
Top
Abstract
Introduction
Materials and Methods
Discussion
References
 

  1. Yoshioka H, Stevens K, Hargreaves BA, et al. Magnetic resonance imaging of articular cartilage of the knee: comparison between fat-suppressed three-dimensional SPGR imaging, fat-suppressed FSE imaging, and fat-suppressed three-dimensional DEFT imaging, and correlation with arthroscopy. J Magn Reson Imaging 2004; 20:857 -864[CrossRef][Medline]
  2. Potter HG, Linklater JM, Allen AA, Hannafin JA, Haas SB. Magnetic resonance imaging of articular cartilage in the knee: an evaluation with use of fast-spin-echo imaging. J Bone Joint Surg Am1998; 80:1276 -1284[Abstract/Free Full Text]
  3. Kowalchuk RM, Kneeland JB, Dalinka MK, Siegelman ES, Dockery WD. MRI of the knee: value of short echo time fast spin-echo using high performance gradients versus conventional spin-echo imaging for the detection of meniscal tears. Skeletal Radiol 2000;29 : 520-524[CrossRef][Medline]
  4. Carlson J, Crooks L, Ortendahl D, Kramer DM, Kaufman L. Signal-to-noise ratio and section thickness in two-dimensional versus three-dimensional Fourier transform MR imaging. Radiology 1988;166 (1 Pt 1):266 -270[Abstract/Free Full Text]
  5. Hargreaves BA, Gold GE, Lang PK, et al. MR imaging of articular cartilage using driven equilibrium. Magn Reson Med1999; 42:695 -703[CrossRef][Medline]
  6. Yuan C, Schmiedl UP, Weinberger E, Krueck WR, Rand SD. Three-dimensional fast spin-echo imaging: pulse sequence and in vivo image evaluation. J Magn Reson Imaging 1993;3 : 894-899[Medline]
  7. Zhou X, Cofer GP, Suddarth SA, Johnson GA. High-field MR microscopy using fast spin-echoes. Magn Reson Med1993; 30:60 -67[Medline]
  8. Hennig J, Weigel M, Scheffler K. Multiecho sequences with variable refocusing flip angles: optimization of signal behavior using smooth transitions between pseudo steady states (TRAPS). Magn Reson Med 2003; 49:527 -535[CrossRef][Medline]
  9. Woertler K, Rummeny EJ, Settles M. A fast highresolution multislice T1-weighted turbo spin-echo (TSE) sequence with a DRIVen equilibrium (DRIVE) pulse for native arthrographic contrast. AJR2005; 185:1468 -1470[Abstract/Free Full Text]

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