Calculation of radiofrequency electromagnetic fields and their effects in MRI of human subjects
暂无分享,去创建一个
[1] Alexis Amadon,et al. Local SAR reduction in parallel excitation based on channel‐dependent Tikhonov parameters , 2010, Journal of magnetic resonance imaging : JMRI.
[2] James C. Lin,et al. ACOUSTIC PRESSURE WAVES INDUCED IN HUMAN HEADS BY RF PULSES FROM HIGH-FIELD MRI SCANNERS , 2010, Health physics.
[3] C. Collins,et al. MRI and localized proton spectroscopy in human leg muscle at 7 tesla using longitudinal traveling waves , 2010, Magnetic resonance in medicine.
[4] Niels Kuster,et al. The Virtual Family—development of surface-based anatomical models of two adults and two children for dosimetric simulations , 2010, Physics in medicine and biology.
[5] Thomas Neuberger,et al. Experimental and numerical assessment of MRI‐induced temperature change and SAR distributions in phantoms and in vivo , 2010, Magnetic resonance in medicine.
[6] Bu S. Park,et al. Faraday shields within a solenoidal coil to reduce sample heating: numerical comparison of designs and experimental verification. , 2010, Journal of magnetic resonance.
[7] P. Glover,et al. A horn antenna improves the transmit field homogeneity in the human brain using the travelling wave technique , 2010 .
[8] Christopher M Collins,et al. Numerical field calculations considering the human subject for engineering and safety assurance in MRI , 2009, NMR in biomedicine.
[9] Robert Turner,et al. Fast MRI coil analysis based on 3-D electromagnetic and RF circuit co-simulation. , 2009, Journal of magnetic resonance.
[10] Klaas P. Pruessmann,et al. Travelling-wave nuclear magnetic resonance , 2009, Nature.
[11] P. Glover,et al. A Comparison of a Patch Antenna to an End-fire Helix Antenna for use in Travelling Wave MRI , 2009 .
[12] D. Sodickson,et al. Contribution of the inherent traveling wave in 7T to large FOV imaging , 2009 .
[13] Yi Wang,et al. Quantitative MR susceptibility mapping using piece‐wise constant regularized inversion of the magnetic field , 2008, Magnetic resonance in medicine.
[14] J. Hand. Modelling the interaction of electromagnetic fields (10 MHz–10 GHz) with the human body: methods and applications , 2008, Physics in medicine and biology.
[15] G. Metzger,et al. Local B1+ shimming for prostate imaging with transceiver arrays at 7T based on subject‐dependent transmit phase measurements , 2008, Magnetic resonance in medicine.
[16] Dirk Diehl,et al. Evaluation of MR-Induced Hot Spots for Different Temporal SAR Modes Using a Time-Dependent Finite Difference Method With Explicit Temperature Gradient Treatment , 2007, IEEE Transactions on Biomedical Engineering.
[17] Zhi-Pei Liang,et al. A noniterative method to design large‐tip‐angle multidimensional spatially‐selective radio frequency pulses for parallel transmission , 2007, Magnetic resonance in medicine.
[18] R.P. Kleihorst,et al. Large-Scale Simulations Including a Human-Body Model for MRI , 2007, 2007 IEEE/MTT-S International Microwave Symposium.
[19] Jan J W Lagendijk,et al. Simultaneous B 1+ homogenization and specific absorption rate hotspot suppression using a magnetic resonance phased array transmit coil , 2007, Magnetic resonance in medicine.
[20] Michael B. Smith,et al. Array‐optimized composite pulse for excellent whole‐brain homogeneity in high‐field MRI , 2007, Magnetic resonance in medicine.
[21] T. Ibrahim,et al. Proposed radiofrequency phased‐array excitation scheme for homogenous and localized 7‐Tesla whole‐body imaging based on full‐wave numerical simulations , 2007, Magnetic resonance in medicine.
[22] M. B. Smith,et al. RF Shimming Considering Both Excitation Homogeneity and SAR , 2007 .
[23] I. Graesslin,et al. Real-time SAR Monitoring to ensure Patient Safety for Parallel Transmission Systems , 2007 .
[24] T. Ibrahim,et al. A Whole-Body 7 Tesla RF Excitation Scheme with Much Improved B1+ Field Homogeneity and Local/Global SARs over Quadrature Excitation , 2007 .
[25] Daniel K. Sodickson,et al. Electrodynamic constraints on minimum SAR in parallel excitation , 2007 .
[26] X. Wu,et al. SAR Reduction in Transmit SENSE Using Adapted Excitation k-Space Trajectories , 2007 .
[27] L. Wald,et al. PULSE DESIGN METHODS FOR REDUCTION OF SPECIFIC ABSORPTION RATE IN PARALLEL RF EXCITATION , 2007 .
[28] V. K. Goyal,et al. PULSES WITH OPTIMAL SPECIFIC ABSORPTION RATE ( SAR ) CHARACTERISTICS AND EXPLORING EXCITATION FIDELITY , SAR AND PULSE DURATION TRADEOFFS , 2007 .
[29] W. Kainz,et al. Evaluations of Specific Absorption Rate and Temperature Increase Within Pregnant Female Models in Magnetic Resonance Imaging Birdcage Coils , 2006, IEEE Transactions on Microwave Theory and Techniques.
[30] Peter Andersen,et al. 9.4T human MRI: Preliminary results , 2006, Magnetic resonance in medicine.
[31] Michael B. Smith,et al. Exploring the limits of RF shimming for high‐field MRI of the human head , 2006, Magnetic resonance in medicine.
[32] K. Uğurbil,et al. Manipulation of image intensity distribution at 7.0 T: Passive RF shimming and focusing with dielectric materials , 2006, Journal of magnetic resonance imaging : JMRI.
[33] Stuart Crozier,et al. Multiple‐acquisition parallel imaging combined with a transceive array for the amelioration of high‐field RF distortion: A modeling study , 2006 .
[34] J. Hajnal,et al. Prediction of specific absorption rate in mother and fetus associated with MRI examinations during pregnancy , 2006, Magnetic resonance in medicine.
[35] W. Kainz,et al. MRI‐induced heating of selected thin wire metallic implants – laboratory and computational studies – findings and new questions raised , 2006, Minimally invasive therapy & allied technologies : MITAT : official journal of the Society for Minimally Invasive Therapy.
[36] Steen Moeller,et al. B1 destructive interferences and spatial phase patterns at 7 T with a head transceiver array coil , 2005, Magnetic resonance in medicine.
[37] Michael B. Smith,et al. Combination of optimized transmit arrays and some receive array reconstruction methods can yield homogeneous images at very high frequencies , 2005, Magnetic resonance in medicine.
[38] Stuart Crozier,et al. Focused, eight‐element transceive phased array coil for parallel magnetic resonance imaging of the chest—Theoretical considerations , 2005, Magnetic resonance in medicine.
[39] C. Collins,et al. Calculations ofB1 distribution, specific energy absorption rate, and intrinsic signal-to-noise ratio for a body-size birdcage coil loaded with different human subjects at 64 and 128 MHz , 2005, Applied magnetic resonance.
[40] Michael B. Smith,et al. Central brightening due to constructive interference with, without, and despite dielectric resonance , 2005, Journal of magnetic resonance imaging : JMRI.
[41] K. Uğurbil,et al. Parallel imaging performance as a function of field strength—An experimental investigation using electrodynamic scaling , 2004, Magnetic resonance in medicine.
[42] P. Boesiger,et al. Electrodynamics and ultimate SNR in parallel MR imaging , 2004, Magnetic resonance in medicine.
[43] Mark S. Mirotznik,et al. Numerical evaluation of heating of the human head due to magnetic resonance imaging , 2004, IEEE Transactions on Biomedical Engineering.
[44] R. Mallozzi,et al. Radiofrequency power deposition utilizing thermal imaging , 2004, Magnetic resonance in medicine.
[45] K. Uğurbil,et al. Temperature and SAR calculations for a human head within volume and surface coils at 64 and 300 MHz , 2004, Journal of magnetic resonance imaging : JMRI.
[46] J. Belliveau,et al. Metallic electrodes and leads in simultaneous EEG‐MRI: Specific absorption rate (SAR) simulation studies , 2004, Bioelectromagnetics.
[47] J. Tropp,et al. Image brightening in samples of high dielectric constant. , 2004, Journal of magnetic resonance.
[48] Z. Zhai,et al. Numerical Evaluation of B1-field and SAR for Heterogeneous and Homogeneous Body Model , 2004 .
[49] Michael B. Smith,et al. Spatial resolution of numerical models of man and calculated specific absorption rate using the FDTD method: A study at 64 MHz in a magnetic resonance imaging coil , 2003, Journal of magnetic resonance imaging : JMRI.
[50] Rolf Schuhmann,et al. A uniformly stable conformal FDTD‐method in Cartesian grids , 2003 .
[51] P. Börnert,et al. Transmit SENSE , 2003, Magnetic resonance in medicine.
[52] R. C. Susil,et al. RF heating due to conductive wires during MRI depends on the phase distribution of the transmit field , 2002, Magnetic resonance in medicine.
[53] Robin M Heidemann,et al. Generalized autocalibrating partially parallel acquisitions (GRAPPA) , 2002, Magnetic resonance in medicine.
[54] Christopher M Collins,et al. Numerical calculations of the static magnetic field in three-dimensional multi-tissue models of the human head. , 2002, Magnetic resonance imaging.
[55] K. Uğurbil,et al. Different excitation and reception distributions with a single‐loop transmit‐receive surface coil near a head‐sized spherical phantom at 300 MHz , 2002, Magnetic resonance in medicine.
[56] James A Bankson,et al. Simulation‐based investigation of partially parallel imaging with a linear array at high accelerations , 2002, Magnetic resonance in medicine.
[57] A. Borthakur,et al. Fast MRI of RF heating via phase difference mapping , 2002, Magnetic resonance in medicine.
[58] T. Ibrahim,et al. Effect of RF coil excitation on field inhomogeneity at ultra high fields: a field optimized TEM resonator. , 2001, Magnetic resonance imaging.
[59] Michael B. Smith,et al. Signal‐to‐noise ratio and absorbed power as functions of main magnetic field strength, and definition of “90°” RF pulse for the head in the birdcage coil , 2001, Magnetic resonance in medicine.
[60] Michael B. Smith,et al. Calculations of B1 distribution, SNR, and SAR for a surface coil adjacent to an anatomically‐accurate human body model , 2001, Magnetic resonance in medicine.
[61] T. Ibrahim,et al. Computational analysis of the high pass birdcage resonator: finite difference time domain simulations for high-field MRI. , 2000, Magnetic resonance imaging.
[62] D. Hoult. The principle of reciprocity in signal strength calculations—a mathematical guide , 2000 .
[63] SAR and Temperature Changes in the Leg Due to an RF Decoupling Coil at Frequencies Between 64 and 213 MHz , 2000, Journal of magnetic resonance imaging : JMRI.
[64] D. Hoult. Sensitivity and Power Deposition in a High‐Field Imaging Experiment , 2000, Journal of magnetic resonance imaging : JMRI.
[65] P. Boesiger,et al. SENSE: Sensitivity encoding for fast MRI , 1999, Magnetic resonance in medicine.
[66] R. W. Lau,et al. Electromagnetic and thermal modeling of SAR and temperature fields in tissue due to an RF decoupling coil , 1999, Magnetic resonance in medicine.
[67] Yu-Chung N. Cheng,et al. Magnetic Resonance Imaging: Physical Principles and Sequence Design , 1999 .
[68] Michael B. Smith,et al. SAR and B1 field distributions in a heterogeneous human head model within a birdcage coil , 1998, Magnetic resonance in medicine.
[69] E. Atalar,et al. Ultimate intrinsic signal‐to‐noise ratio in MRI , 1998, Magnetic resonance in medicine.
[70] W. Manning,et al. Simultaneous acquisition of spatial harmonics (SMASH): Fast imaging with radiofrequency coil arrays , 1997, Magnetic resonance in medicine.
[71] H. Wen,et al. Simulation ofB1Field Distribution and Intrinsic Signal-to-Noise in Cardiac MRI as a Function of Static Magnetic Field , 1997 .
[72] P. Dimbylow. FDTD calculations of the whole-body averaged SAR in an anatomically realistic voxel model of the human body from 1 MHz to 1 GHz. , 1997, Physics in medicine and biology.
[73] R. Balaban,et al. Simulation of B1 field distribution and intrinsic signal-to-noise in cardiac MRI as a function of static magnetic field. , 1997, Journal of magnetic resonance.
[74] S Li,et al. Three‐dimensional mapping of the static magnetic field inside the human head , 1996, Magnetic resonance in medicine.
[75] J. Huisman. The Netherlands , 1996, The Lancet.
[76] C. Gabriel. Compilation of the Dielectric Properties of Body Tissues at RF and Microwave Frequencies. , 1996 .
[77] Magnetic resonance imaging can cause focal heating in a nonuniform phantom , 1993, IEEE Transactions on Biomedical Engineering.
[78] R. Henkelman,et al. RF Current Density Imaging in Homogeneous Media , 1992, Magnetic resonance in medicine.
[79] R. Henkelman,et al. Sensitivity of magnetic-resonance current-density imaging , 1992 .
[80] J W Carlson,et al. Electromagnetic fields of surface coil in vivo NMR at high frequencies , 1991, Magnetic resonance in medicine.
[81] P. Roemer,et al. The NMR phased array , 1990, Magnetic resonance in medicine.
[82] K. Foster,et al. Dielectric properties of tissues and biological materials: a critical review. , 1989, Critical reviews in biomedical engineering.
[83] D. Hoult,et al. The field dependence of NMR imaging. I. Laboratory assessment of signal‐to‐noise ratio and power deposition , 1986, Magnetic resonance in medicine.
[84] W. Edelstein,et al. The intrinsic signal‐to‐noise ratio in NMR imaging , 1986, Magnetic resonance in medicine.
[85] W. Barber,et al. Comparison of linear and circular polarization for magnetic resonance imaging , 1985 .
[86] C N Chen,et al. Quadrature detection in the laboratory frame , 1984, Magnetic resonance in medicine.
[87] O. Gandhi,et al. Electromagnetic Energy Deposition in an Inhomogeneous Block Model of Man for Near-Field Irradiation Conditions , 1980, 1980 IEEE MTT-S International Microwave symposium Digest.
[88] P. Lauterbur,et al. The sensitivity of the zeugmatographic experiment involving human samples , 1979 .
[89] H. Carr,et al. The Principles of Nuclear Magnetism , 1961 .