Nuclear magnetic resonance probe

Claim 2

In an NMR probe system of the type comprising substantially electromagnetically orthogonal RF transmitter and receiver coils, a balancing coil adjacent and electromagnetically coupled to the transmitter coil as well as in RF signal transfer relationship with the receiver coil, and electrical trimmers of RF amplitude and phase associated with the transmitter coil, whereby adjustment of said trimmers enables in operation an RF voltage to be set up in the balancing coil that is of the correct phase and amplitude for substantially cancelling any spurious RF voltage in the receiver coil due to stray induction effects.

Claim 3

In an NMR probe system of the type comprising substantially electromagnetically orthogonal RF transmitter and receiver coils, the said transmitter coil being divided into two halves, a balancing coil intermediate between said halves that is in RF signal transfer relationship with the receiver coil and electromagnetically coupled to both of said halves so that RF voltages of opposite phase are induced therein from one and other of said halves, and electrical trimmers of RF amplitude and phase associated with each transmitter half, whereby adjustment of said trimmers enables in operation a dominant RF voltage to be set up in the balancing coil that is of the correct phase and amplitude substantially to cancel any spurious RF voltage in the receiver coil due to stray induction effects.

Claim 4

In an NMR probe system of the type comprising substantially electromagnetically orthogonal RF transmitter and receiver coils, the said transmitter coil being divided into two halves, a balancing coil intermediate between said halves that is in RF signal transfer relationship with the receiver coil and electromagnetically coupled to both of said halves so that RF voltages of opposite phase are induced therein from one and other of said halves, and electrical trimmers of RF amplitude and phase associated with each transmitter half, whereby adjustment of said trimmers enables in operation a dominant RF voltage to be set up in the balancing coil that is of the correct phase and amplitude substantially to cancel any spurious RF voltage in the receiver coil due to stray induction effects.

Claim 5

In an NMR probe system of the type comprising substantially electromagnetically orthogonal RF transmitter and receiver coils, the said transmitter coil being divided into two halves, a balancing coil similarly divided into two halves with the half of one coil intermediate between the two halves of the other coil and electromagnetically coupled thereto so that RF voltages of opposite phase are induced in each balancing coil half from one and other transmitter half, the two balancing coil halves being connected so that the dominant induced RF voltage in one half aids the dominant induced RF voltage in the other half and the connected halves being in RF signal transfer relationship with the receiver coil, and electrical trimmers of RF phase and amplitude associated with each transmitter coil half, whereby adjustment of said trimmers enables in operation dominant RF voltages to be set up in the balancing coil halves which together provide the correct phase and amplitude substantially to cancel any spurious RF voltage in the receiver coil due to stray induction effects.

Claim 6

In an NMR probe system of the type comprising substantially electromagnetically orthogonal RF transmitter and receiver coils, the said transmitter coil being divided into two halves, a balancing coil similarly divided into two halves with the half of one coil intermediate between the two halves of the other coil and electromagnetically coupled thereto so that RF voltages of opposite phase are induced in each balancing coil half from one and other transmitter half, the two balancing coil halves being connected so that the dominant induced RF voltage in one half aids the dominant induced RF voltage in the other half and the connected halves being in RF signal transfer relationship with the receiver coil, and electrical trimmers of RF phase and amplitude associated with each transmitter coil half, whereby adjustment of said trimmers enables in operation dominant RF voltages to be set up in the balancing coil halves which together provide the correct phase and amplitude substantially to cancel any spurious RF voltage in the receiver coil due to stray induction effects.

Claim 7

The system of claim 3, wherein the two transmitter halves are spaced on a substantially common electromagnetic axis.

Claim 8

The system of claim 4, wherein the balancing coil halves are spaced on a substantially common electromagnetic axis that is substantially orthogonal to the electromagnetic axis of the transmitter halves.

Claim 9

The system of claim 5, wherein the electromagnetic coupling between the transmitter and balancing coil halves is mainly confined to adjacent rectilinear portions of the coil halves which in the operational attitude of the probe extend substantially at right angles to the axis of the NMR polarizing field.

Claim 10

The system of claim 6, wherein the coil halves are of generally rectangular shape and the said rectilinear portions represent the long sides of the coil halves.

Claim 11

The probe system of claim 7, wherein the coil halves comprise a single turn.

Claim 12

The system of claim 3, wherein the two halves of the transmitter coil are adapted for parallel feed from a source of RF potential.

Claim 13

The system of claim 9, wherein the amplitude trimmers are variable resistors and the phase trimmers are variable capacitors, a variable resistor and variable capacitor being placed in parallel with each transmitter coil half.

Claim 14

The system of claim 10, wherein the trimmers are devices that alter in value in response to electrical energization thus enabling remote control of amplitude and phase by purely electrical means.

Claim 15

The system of claim 11, wherein the amplitude trimmers are P.I.N. diodes and the phase trimmers are Varicaps.