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Poster Sessions<br />

3081. Imaging Near Metals with Phase Cycled SSFP<br />

Michael Nicholas Hoff 1 , Jordin D. Green 2 , Qing-San Xiang 1,3<br />

1 Department of Physics & Astronomy, University of British Columbia, Vancouver, British Columbia, Canada; 2 Siemens Healthcare,<br />

Calgary, Alberta, Canada; 3 Department of Radiology, University of British Columbia, Vancouver, British Columbia, Canada<br />

A fast bSSFP technique is devised for removing imaging artifacts near metals. 3D phase cycled TrueFISP provides comprehensive artifact reduction using<br />

powerful gradients, two dimensions of phase encoding, short TR, and thorough refocusing of magnetization. Problematic banding artifacts are eliminated<br />

using a technique which formulates expressions for each voxel’s modulated magnetization, and then analytically solves the system with a simple Cross-<br />

Solution (XS) to obtain the demodulated magnetization. Application to a phantom consisting of a hip prosthesis within a Lego structure confirms that 3D<br />

imaging with XS-SSFP is simple, efficient, and robust in artifact reduction.<br />

3082. B 1 Effects When Imaging Near Metal Implants at 3T<br />

Kevin M. Koch 1 , Kevin F. King 1 , Graeme C. McKinnon 1<br />

1 Applied Science Laboratory, GE Healthcare, Waukesha, WI, United States<br />

Recently developed techniques have enabled low susceptibility-artifact imaging near metal implants using conventional spin-echo acquisition strategies.<br />

Previous demonstrations of these techniques have been presented at 1.5T. While the susceptibility artifact mitigation of these techniques remains sufficient<br />

at 3T, here we address the effects of reduced B 1 wavelength applied at 3T. These effects introduce increased B 1 artifacts near metal implants, particularly<br />

those with long axes oriented collinear with B 0 . Finite element simulations and phantom images are presented to demonstrate and discuss these effects.<br />

3083. Adaptive Slice Encoding for Metal Artifact Correction<br />

Brian A. Hargreaves 1 , Garry E. Gold 1 , John M. Pauly 2 , Kim Butts Pauly 1<br />

1 Radiology, Stanford University, Stanford, CA, United States; 2 Electrical Engineering, Stanford University, Stanford, CA, United<br />

States<br />

Slice encoding for metal artifact correction (SEMAC) excites 2D slices, then uses a 3D encoding to resolve the distortion of slices due to large metalinduced<br />

susceptibility shifts. The addition of a simple, fast spectral prescan easily estimates the extent of this distortion, allowing the slab width and<br />

encoded field-of-view to be adapted to the subject. This, allows the total number of excited slices to be greatly reduced without diminishing final image<br />

quality, thus offering a substantial reduction in SEMAC scan time.<br />

3084. Fat-Suppressed and Distortion-Corrected MRI Near Metallic Implants<br />

Brian A. Hargreaves 1 , Wenmiao Lu 2 , Kim Butts Pauly 1 , John M. Pauly 3 , Garry E. Gold 1<br />

1 Radiology, Stanford University, Stanford, CA, United States; 2 Electrical & Electronic Engineering, Nanyang Tech University,<br />

Singapore, Singapore; 3 Electrical Engineering, Stanford University, Stanford, CA, United States<br />

Fluid-sensitive volumetric imaging of patients with metallic implants is potentially an important diagnostic tool to assess for infection, implant loosening, or<br />

other complications. Recent MR techniques use spin echoes combined with additional encoding to substantially reduce distortion and signal loss artifacts.<br />

Here we demonstrate the use of these sequences with short TI inversion recovery (STIR) to provide reliable fat suppression near metallic implants, which is<br />

particularly important in assessment of many disorders.<br />

3085. Spiral Chemical Shift Imaging in the Presence of Metal Artifacts<br />

Atsushi M. Takahashi 1<br />

1 Applied Science Laboratory, GE Healthcare, Menlo Park, CA, United States<br />

MRI in the presense of metal in the body is complicated by B0 field perturbations and by the shortening of the T2* relaxation times. With a multiinterleave,<br />

short readout, spiral k-space trajectory, chemical shift imaging method, we can image in the presence of metal. Here we describe a method which<br />

can be used in-vitro to visualize the field maps surrounding metal implants.<br />

3086. Evaluation of MR Image Artifacts of Stent Implants at 3 Tesla Using a Phantom Filled with Mineral<br />

Oil Compared to CuSO4<br />

A Koenig 1,2 , Frank Reintke 2 , Gerrit Schönwald, 2,3 , Gregor Schaefers 2<br />

1 University of applied Science Gelsenkirchen, Gelsenkirchen, NRW, Germany; 2 MR Safety Testing Laboratory, MR:comp GmbH,<br />

Gelsenkirchen, Germany; 3 University Witten/Herdecke<br />

The ASTM-Standard F2119-07 is used to evaluate artifacts of implants. According to the test method a phantom with CuSO4 is used. By replacing the<br />

solution by mineral oil it is desired to avoid standing waves in images. We tested both fluids in two sequences (SE/GRE) with 2 test devices, a Nitinol stent<br />

and an acryl reference tube. We compared a visual, a statistically and a manual analysis. We noticed non-significant results with one exception. Under<br />

certain conditions the standard CuSO4 can be exchanged with mineral oil allowing better and precise artifact analysis at higher field strengths ¡Ý 3 T.<br />

3087. Comparison of Fat Suppression Methods for Functional and Diffusion Studies Using SE EPI at 7T<br />

Dimo Ivanov 1 , Markus Streicher 1 , Andreas Schäfer 1 , Robert Turner 1<br />

1 Department of Neurophysics, Max Planck Institute for Human Cognitive and Brain Sciences, Leipzig, Germany<br />

The increased SNR of ultra-high-field MR scanners allows high resolution functional and diffusion studies to be performed. Because chemical-shift artifact<br />

suppression is essential for SE EPI images, we evaluated the performance of different fat suppression techniques. Conventional methods using additional<br />

radiofrequency (RF) and gradient pulses provide suboptimal results owing to increased B0 and B1 inhomogeneity at higher fields. They also increase RF<br />

power deposition. A recently developed method using different slice-select gradient strengths during the excitation and refocussing pulses was demonstrated<br />

to be most robust, and delivered best chemical shift selection.

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