An asymmetrical whole-body birdcage RF coil without RF shield for hyperpolarized Xe lung MR imaging at 1.5 T.

Purpose: This study describes the development and testing of an asymmetrical xenon-129 ( Xe) birdcage radiofrequency (RF) coil for Xe lung ventilation imaging at 1.5 Tesla, which allows proton ( H) system body coil transmit-receive functionality.

Methods: The Xe RF coil is a whole-body asymmetrical elliptical birdcage constructed without an outer RF shield to enable H imaging.

Impact of a parallel magnetic field on radiation dose beneath thin copper and aluminum foils.

Purpose: The RF coils for magnetic resonance image guided radiotherapy (MRIgRT) may be constructed using thin and/or low-density conductors, along with thinner enclosure materials. This work measures the surface dose increases for lightweight conductors and enclosure materials in a magnetic field parallel to a 6 MV photon beam.

Methods: Aluminum and copper foils (9-127 μm thick), as well as samples of polyimide (17 μm) and polyester (127 μm) films are positioned atop a polystyrene phantom.

How thin can you go? Performance of thin copper and aluminum RF coil conductors.

Purpose: To evaluate the impact of emerging conductor technology on RF coils. Performance and resulting image quality of thin or alternate conductors (eg, aluminum instead of copper) and thicknesses (9-600 μm) are compared in terms of SNR.

Methods: Eight prototype RF coils (15 cm × 15 cm square loops) were constructed and bench-tested to measure quality factor.

Optimal-permittivity Dielectric Liners for a 4.7T Transceiver Array.

Placing dielectric pads adjacent to the imaging region is an effective method to increase the signal locally and also increase the radio frequency magnetic field homogeneity in magnetic resonance imaging. The use of local high permittivity pads is becoming more common, and this work focuses on the effect of larger dielectric pads on the transmit/receive performance of an array (e.g.

The noise factor of receiver coil matching networks in MRI.

In typical MRI applications the dominant noise sources in the received signal are the sample, the coil loop and the preamplifier. We hypothesize that in some cases (e.g.