Jiaming Cui1, Chenhao Sun1, Dheyaa Alkandari1, and Steven Wright1
1Electrical& Computer Engineering, Texas A&M University, College Station, TX, United States
Synopsis
This abstract reports
a switchable coil element which uses “forced
current excitation”. The coil consists of three aligned rungs,
with a total length of 37 cm. Any one or
more of three rungs can be easily selected to provide a
variable length or position field-of-view.
The forced current approach ensures equal current on the selected rungs
to give a uniform field distribution along the length of
the field-of-view. Bench measurements demonstrate the expected efficiency
improvement when only a single rung is selected and the uniform field
pattern.
Target Audience
Researchers and practitioners interested in RF coils
for high-field MRI.Introduction
Spine imaging at 7T is
of high interest due to the high intrinsic signal-to-noise ratio (SNR)
and its diagnostic potential [1]. The large field of
view (FOV) requires a long RF coil for surveying the spine. At lower field a
body coil can be used for transmission with an array for reception. Most 7T
system does not have a body coil. Additionally, at 7T it may be desirable to
tailor the RF coil length such that only the desired portion of spine, e.g.
cervical, thoracic or lumbar zone is excited while redundant power
decomposition is avoided. Qi et al has reported a segmented coil design at 7T
where the FOV can be adjusted to a certain degree [3]. However the design does
not allow the user to select the FOV near the edge of the coil. Here we report
a switchable length rung design using a very straightforward design, force
current excitation, which can provide uniform field distribution as well as
enhanced flexibility for varying the FOV. This concept has been demonstrated previously
with a switchable unilateral/bilateral 7T breast coil [4]. In this work, the
design is scaled to three elements on a 37 cm long rung intended for use in a spine
coil. Methods
Forced
Current Excitation uses odd multiples of ¼ wavelength transmission lines to
excite coil elements and guarantee equal current delivery to different elements
despite mutual coupling [5]. The other ends of the transmission lines are
connected to the common voltage point, which can be upgraded to a PIN diode
switching circuit to activate or detune each coil element [4]. Three short
current rungs, 11cm each and with 2 cm gap between them, are aligned in the z
direction to form a 37 cm long spine coil. Each rung is segmented every 2cm
with a 33pF capacitor. A ground plane, serving as the current return path, lies
1.2 cm beneath each current rung. The rungs are fed from the side with ¾
wavelength coax cables with very low loss semi-rigid cable (EZ form-141). Three
DC signals are generated from a power supply module to control the switching
circuit: a +15V bias activates the
corresponding rung, while a -15V bias detunes it.
With
the ability to enable or detune each of the three elements, the coil is
equipped with eight different operating modes in total. Depending on the region
of interest, the user can pick from any of the eight modes for imaging. The
coil was tested on bench in four modes. With the same input power applied, the
efficiency of the coil in the four modes were measured using a shielded probe
and a network analyzer. The measurement was taken along z direction with 1cm
resolution, at 4cm away from the coil in the y direction at 298 MHz, which is
the larmor frequency at 7T. Results and discussion
The
four modes being tested are left coil only (mode 1), middle coil only (mode 2),
right coilonly (mode 3) and all coils (mode 4). The B1 maps were plotted
together and scaled to the global maximum. Mode 4 demonstrate uniform
excitation across a large FOV, which means equal current is achieved at each
rung. Modes 1-3 demonstrate higher power efficiency in the corresponding area.
The efficiency of mode 1-3 is 3.5-4 dB higher than that of mode 4, in the
corresponding region. Additional modes, with two of the three rungs excited were
possible but not presented.
This
work uses current rung as the basic element, however this method can be used
for any type of coil element. In addition, the coil structure can be divided
into more elements (more than three) if smaller FOV and higher B1 efficiency
is required. Conclusion
Forced-current excitation is used to excite a three-element
spine coil. It is also configured such that each small coil segment can be
activated or detuned through electronic control, giving flexible FOV variation.
A large FOV gives large coverage while a smaller FOV allows more focused RF power,
potentially important in some applications requiring either low whole-body SAR
or localized high B1 values. In addition, when multiple elements are activated,
the FCE method ensures uniform current delivery to the different element and
prevents mode splits due to coupling. This work also proves the scalability of
the ‘FCE+variable FOV’ concept. This ‘extendable rung’ design will be used as
the element in a two element spine array in the future.Acknowledgements
This work was supported in part by grants from the National Institutes of Health (R21HL120064 ) and the Cancer Prevention and Research Institute of Texas (RP15046 or RP160847). References
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