Double-Tuned Birdcage Radio Frequency Coil for 7 T MRI: Optimization, Construction and Workbench Validation

Author:

Retico Alessandra1ORCID,Maggiorelli Francesca123,Giovannetti Giulio4ORCID,Boskamp Eddy5,Robb Fraser6,Fantasia Marco7,Galante Angelo789ORCID,Alecci Marcello789ORCID,Tiberi Gianluigi1011,Tosetti Michela312

Affiliation:

1. Pisa Division, National Institute for Nuclear Physics (INFN), 56127 Pisa, Italy

2. Department of Physical Sciences, Earth and Environment (DSFTA), University of Siena, 53100 Siena, Italy

3. Imago7 Foundation, 56128 Pisa, Italy

4. Institute of Clinical Physiology, National Research Council (CNR), 56124 Pisa, Italy

5. Hyperfine Research Inc., Guilford, CT 06437, USA

6. GE Healthcare Inc., Aurora, OH 44202, USA

7. Department of Life, Health & Environmental Sciences (MESVA), University of L’Aquila, 67100 L’Aquila, Italy

8. Gran Sasso National Laboratory, INFN, 67100 L’Aquila, Italy

9. SPIN-CNR, c/o Department of Physical and Chemical Science, University of L’Aquila, 67100 L’Aquila, Italy

10. School of Engineering, London South Bank University, London SE1 0AA, UK

11. Umbria Bioengineering Technologies (UBT) Srl, 06081 Perugia, Italy

12. IRCCS Stella Maris Foundation, 56128 Pisa, Italy

Abstract

The aim of the present study is the optimization, construction, and workbench validation of a double-tuned 1H- 23Na volume radio frequency (RF) coil suitable for human head imaging at 7 T, based on the birdcage geometry. The birdcage-like design which is considered is the four-ring model, in which two standard birdcage-like structures with the same diameters are nested along the longitudinal axis. Simulations based on Maxwell’s equations are performed to evaluate the RF magnetic field homogeneity and the RF coil efficiency varying the coil geometrical parameters. The RF magnetic field homogeneity is evaluated both on the transverse (z = 0) and longitudinal (y = 0) planes without performing the impedance matching procedure, so that the RF coil symmetry is not perturbed by the matching network. The RF coil efficiency is instead dependent on the effective coil input RF power, and it is evaluated after matching the coil, so that the reflected power is minimized, assuming that the stimulation power is totally delivered to the RF coil. Considering the simulation results and the target application, the useful RF coil geometrical parameters are fixed. The four-ring model, which showed the best performances, has been built and tested on a workbench, using a cylindrical phantom filled with a 0.05 M saline solution as load. This provides the first example of a four-ring realization intended 1H- 23Na for human head imaging at 7 T.

Funder

Italian National Institute for Nuclear Physics

Publisher

MDPI AG

Subject

Electrical and Electronic Engineering,Computer Networks and Communications,Hardware and Architecture,Signal Processing,Control and Systems Engineering

Reference41 articles.

1. An efficient, highly homogeneous radiofrequency coil for whole-body NMR imaging at 1.5 T;Hayes;J. Magn. Reson.,1985

2. The theory of the bird-cage resonator;Tropp;J. Magn. Reson.,1989

3. Resonant Modes of the Birdcage Coil;Leifer;J. Magn. Reson.,1997

4. Mutual inductance in the bird-cage resonator;Tropp;J. Magn. Reson.,1997

5. Mispelter, J., Lupu, M., and Briguet, A. (2015). NMR Probeheads for Biophysical and Biomedical Experiments: Theoretical Principles & Practical Guidelines, Imperial College Press. [2nd ed.].

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