The present invention relates to imaging systems and more particularly, relates to coil decoupling schemes between various coil elements to offer improved performance and results.
Specialized RF coils for application-specific imaging modalities are common in the field of magnetic resonance imaging (MRI). In particular, for the magnetic resonance imaging of the female breast in horizontal and vertical clinical MR instruments a number of single and multi-loop RF coil concepts for single channel, quadrature, and phased array configurations have been devised by a number of inventors. Examples of these systems are described in U.S. Pat. No. 7,084,631 (Qu et al., Aug. 1, 2006), U.S. Pat. No. 6,850,065 (Fujita et al., Feb. 1, 2005), U.S. Pat. No. 6,493,572 (Su et al., Dec. 10, 2002), U.S. Pat. No. 6,377,836 (Arakawa et al., Apr. 23, 2002), U.S. Pat. No. 6,163,717 (Su, Dec. 19, 2000), U.S. Pat. No. 6,023,166 (Eydelnan, Feb. 8, 2000), and U.S. Pat. No. 5,699,802 (Duerr, Dec. 23, 1997), each of which is hereby incorporated by reference in its entirety.
Often the individual loops or coil elements are laid out in planar and orthogonal planes with respect to the main magnet in the clinical MR instrument. For example, in
In a multi-channel receiver system, the MR signal obtained by a multi-loop breast coil system can be configured such that each loop or coil element is selectively tuned to the resonance frequency of the MR instruments, while the remaining loops, or coil elements, are detuned. As a result, by tuning and detuning individual coil elements, parallel MR imaging is accomplished which enables high resolution imaging of selective regions of interest and concomitantly more rapid image formation.
Unfortunately, when connecting each of the loops, or coil elements, to a receiving channel of the MR instrument, coupling between the tuned and detuned loops can occur. This is due to the fact that the signal received by one loop is also received by neighboring loops, despite detuning measures that involve preamplifier detuning. The coupling is most prominent for the orthogonal loop in the center of the configuration and its adjacently positioned planar loops. There is therefore a perceived need for a coil construction that offers provides improves coil decoupling schemes between various coil elements to offer improved performance and results.
A multi-loop RF coil according to one embodiment of the present invention includes a plurality of channels and is formed of a plurality of coil elements. The coil includes a pair of coil elements that overlap with one another as part of a geometric decoupling scheme between the pair of coil elements.
In another embodiment, an RF coil that has a plurality of channels includes a plurality of coil elements and a hybrid decoupling scheme between the coil elements that is a combination of geometric and capacitive decoupling.
In another embodiment, a multi-loop RF coil that has a plurality of channels that includes a plurality of coil elements. A first pair of coils that are disposed in one plane overlap with one another as part of a geometric decoupling scheme between the first pair of coils. In addition, one vertical coil is partially decoupled from the first pair of coils by a bridge over the overlapping portions of the first pair of coils.
a-g are schematic illustrations of the 7-channel coil system showing current flow in each of the seven channels; and
The RF coil 100 has the following loop (or channel) assignments: coil 110 represents the upper right channel, coil 120 represents the upper left channel, coil 130 represents the lower right channel, coil 140 represents the lower left channel, coil 150 represents the vertical right channel, coil 160 represents the vertical middle channel, and coil 170 represents the vertical left channel.
Moreover, each coil element shown in
Capacitive decoupling is used between the vertical middle loop 160 and the lower right loop 130 and lower left loop 140. At the same time, the vertical middle loop 160 is only partially decoupled from the upper right loop 110 and upper left loop 120 by a bridge over the two overlapping segments of the lower right loop 130 and lower left loop 140. Partial decoupling is sufficient in this case, because preamplifier decoupling (using low input impedance preamplifier) is additionally used for each loop as seen in
More particularly, in
1. Coil 1 (coil 110)-Coil 2 (coil 120)
2. Coil 1 (coil 110)-Coil 6 (coil 160)
3. Coil 2 (coil 120)-Coil 6 (coil 160)
4. Coil 1 (coil 110)-Coil 5 (coil 150)
5. Coil 2 (coil 120)-Coil 7 (coil 170)
6. Coil 3 (coil 130)-Coil 5 (coil 150)
7. Coil 4 (coil 140)-Coil 7 (coil 170)
Tuning capacitors for respective coils are indicated by “C tune x,” where x is the coil number. For example, “C tune 1” refers to a tuning capacitor for coil 1. Similarly, matching capacitors are indicated by “C match x,” where x is the coil number. For example, “C match 1” refers to a matching capacitor for coil 1.
However, unlike previous capacitive decoupling attempts reported in the literature, an inductive decoupling is used for coils 3 and 4 (coils 130, 140) by creating an overlap of the conductive coil structures. As shown in
In the illustrated embodiment, the coil 4 lies over coil 3; however, the opposite can be true in that coil 3 can lie over coil 4.
As already mentioned above, Coil 6 (coil 160) features a bridge 162 that is positioned below the plane where Coils 3 and 4 (coils 130, 140) are located. Even though the pairs Coil 3-Coil 6 (coils 130, 160) and Coil 4-Coil 6 (coils 140, 160) are not capacitively decoupled, the bridge 162 helps to decrease the amount of coupling.
The effectiveness of the disclosed geometric as well as the associated electrical decoupling is demonstrated in
As can be seen in
According to reciprocity principle, the sensitivity of a particular coil to the radiation from the biological load is proportional to the magnetic field of the coil, if the latter is driven by an external voltage source. The magnetic B1 field of these coils can be calculated, provided that the coils take the same amount of input power. The signal-to-noise (SNR) of a coil is proportional to B1/√{square root over (P)}, where P is input power. Finally, the squares of magnetic fields of the seven coils can be added according to the formula:
The resulting field is shown in
The present application claims the benefit of U.S. patent application Ser. No. 60/979,362, filed Oct. 11, 2007, which is hereby incorporated by reference in its entirety.
Number | Date | Country | |
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60979362 | Oct 2007 | US |