We present a numerical investigation of the RF fields generated inside a human head by single and dual-row loop arrays. For a uniform circular polarization (CP) mode excitation, a dual-row array has no advantage for human brain excitation. Significant improvement of B1+ homogeneity with a simultaneous increase of coverage in the axial direction can be obtained by using a dual-row array together with a static RF shim: that is, excitation of both rows separately in CP mode, while providing the upper row elements with a +90 phase shift relative to axially adjacent lower row elements. For this case the excitation efficiency over the entire brain remains practically unaffected, and the improved B1+ coverage results in a relatively smaller amount...
Purpose: Optimisation of transmit array performance is crucial in ultra-high-field MRI scanners such...
We investigated how performance trade-off depends on dual-row transmit array geometry, position of a...
The well known transmit field inhomogeneity at ultra high field strengths, caused by the shorter RF ...
We present a numerical investigation of the RF fields generated inside a human head by single and du...
Objective: To provide a numerical and experimental investigation of the static RF shimming capabi...
We evaluated how magnetic resonance imaging robustness depends on dual-row transmit array geometry, ...
Important issues in designing radiofrequency (RF) coils for human head imaging at ultra-high field (...
Transmit elements arranged in multiple rows are beneficial in extending longitudinal coverage and ac...
Purpose: Arranging transmit array elements in multiple rows provides an additional degree of freedo...
We evaluated and compared the performances of two simulated radiofrequency (RF) dual-row transmit ar...
We investigated how cerebrospinal fluid (CSF) simulated as a single electrically connected object an...
Dielectric resonance effects and radio-frequency (RF) power deposition have become challenging issue...
Purpose: To improve the homogeneity of transmit volume coils at high magnetic fields (≥4 T). Due to ...
PURPOSE: To design, construct and validate radiofrequency (RF) transmit and receive phased array coi...
Simultaneous investigation of electrophysiology and fMRI in non-human primates presents several chal...
Purpose: Optimisation of transmit array performance is crucial in ultra-high-field MRI scanners such...
We investigated how performance trade-off depends on dual-row transmit array geometry, position of a...
The well known transmit field inhomogeneity at ultra high field strengths, caused by the shorter RF ...
We present a numerical investigation of the RF fields generated inside a human head by single and du...
Objective: To provide a numerical and experimental investigation of the static RF shimming capabi...
We evaluated how magnetic resonance imaging robustness depends on dual-row transmit array geometry, ...
Important issues in designing radiofrequency (RF) coils for human head imaging at ultra-high field (...
Transmit elements arranged in multiple rows are beneficial in extending longitudinal coverage and ac...
Purpose: Arranging transmit array elements in multiple rows provides an additional degree of freedo...
We evaluated and compared the performances of two simulated radiofrequency (RF) dual-row transmit ar...
We investigated how cerebrospinal fluid (CSF) simulated as a single electrically connected object an...
Dielectric resonance effects and radio-frequency (RF) power deposition have become challenging issue...
Purpose: To improve the homogeneity of transmit volume coils at high magnetic fields (≥4 T). Due to ...
PURPOSE: To design, construct and validate radiofrequency (RF) transmit and receive phased array coi...
Simultaneous investigation of electrophysiology and fMRI in non-human primates presents several chal...
Purpose: Optimisation of transmit array performance is crucial in ultra-high-field MRI scanners such...
We investigated how performance trade-off depends on dual-row transmit array geometry, position of a...
The well known transmit field inhomogeneity at ultra high field strengths, caused by the shorter RF ...