WO1997046895A1 - Antenna system for nmr and mri apparatus - Google Patents

Antenna system for nmr and mri apparatus Download PDF

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Publication number
WO1997046895A1
WO1997046895A1 PCT/US1997/009420 US9709420W WO9746895A1 WO 1997046895 A1 WO1997046895 A1 WO 1997046895A1 US 9709420 W US9709420 W US 9709420W WO 9746895 A1 WO9746895 A1 WO 9746895A1
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WIPO (PCT)
Prior art keywords
circuit
switching position
antenna system
signal
coupled
Prior art date
Application number
PCT/US1997/009420
Other languages
French (fr)
Inventor
Samuel Roznitsky
Original Assignee
Samuel Roznitsky
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Samuel Roznitsky filed Critical Samuel Roznitsky
Priority to IL12695997A priority Critical patent/IL126959A0/en
Priority to JP10500734A priority patent/JP2000514670A/en
Priority to BR9709291A priority patent/BR9709291A/en
Priority to AU31519/97A priority patent/AU3151997A/en
Priority to GB9826523A priority patent/GB2331587B/en
Publication of WO1997046895A1 publication Critical patent/WO1997046895A1/en

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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00Arrangements or instruments for measuring magnetic variables
    • G01R33/20Arrangements or instruments for measuring magnetic variables involving magnetic resonance
    • G01R33/28Details of apparatus provided for in groups G01R33/44 - G01R33/64
    • G01R33/32Excitation or detection systems, e.g. using radio frequency signals
    • G01R33/36Electrical details, e.g. matching or coupling of the coil to the receiver
    • G01R33/3642Mutual coupling or decoupling of multiple coils, e.g. decoupling of a receive coil from a transmission coil, or intentional coupling of RF coils, e.g. for RF magnetic field amplification
    • G01R33/3657Decoupling of multiple RF coils wherein the multiple RF coils do not have the same function in MR, e.g. decoupling of a transmission coil from a receive coil

Definitions

  • the present invention is directed to transmission and reception antennas for use in a nuclear magnetic resonance (NMR) apparatus and in a magnetic resonance imaging (MRI) apparatus, for calculating spectra or generating images of an examination subject or object.
  • NMR nuclear magnetic resonance
  • MRI magnetic resonance imaging
  • Nuclear magnetic resonance is the effect of a resonant rotating or alternating magnetic field, imposed at right angles to a static field, to perturb the orientation of nuclear magnetic moments.
  • Magnetic resonance imaging is the development of nuclear magnetic resonance (NMR) techniques for obtaining a diagnostic scan of a subject such as a human or animal body.
  • NMR nuclear magnetic resonance
  • the patient or examination subject is placed in a strong magnetic field. This magnetic field induces a net magnetization of the nuclei in the subject.
  • a short radio frequency pulse (RF pulse) is applied at the Larmor frequency of the precessing nuclei which, in turn, emit an RF signal of the same frequency. This is detected and gives a
  • fingerprint of the environment of the nucleus being studied. This information is one-dimensional but is converted into a two-dimensional anatomical image by adding a gradient to the applied magnetic field which results in a frequency modulation of the -emitted RF signal. A series of such measurements is analyzed by computer to generate the image .
  • a strong magnetic field aligns the nuclei of the subject or object to be studied along the field direction.
  • the conditions of efficient energy absorption require that the RF fields of the transmitter and receiver antennas be orthogonal to the static magnetic field.
  • the simultaneous condition of negligibly low interaction between the receiver and transmitter antennas for minimal mutual distortion of their RF fields and for the prevention of high transmitter power to be applied to the receiver, in part also means that the RF fields of the transmitter and receiver antennas must be orthogonal even though transmission and reception do not coincide in time. Acceptable switching time between the two is of the order of about ten microseconds.
  • a radio frequency (RF) transmitter 4 transmits a signal to a transmitter antenna 2.
  • the signal which is absorbed and subsequently re-emitted by the examination body or subject (patient) 5 is then picked up by a receiver antenna 1 and fed to a radio frequency (RF) receiver 3.
  • the examination body or subject 5 which is being scanned is within the RF fields of both the transmitter and receiver antennas 2,1.
  • the transmitter antenna 2 and receiver antenna 1 are optimized for their respective tasks and are tuned by variable capacitors 6 and 7. Normally, the single, fixed in place transmitter antenna 2 is big enough to encompass the largest part of a body or subject 5 to be scanned. Significantly smaller reception antennas 1, specialized for different body parts, are separately connected and used.
  • Magnet poles 8 and 9 are shown located above and below the patient (body or subject 5) , respectively.
  • the resulting low electromagnetic coupling between the transmitter antenna 2 and receiver antenna 1 assures low field distortion and allows utilization of speedy and efficient electronic tuning for the receiver antenna 1.
  • the required transmitting power is high and manual tuning of the transmitter antenna 2 by a variable capacitor 6 is employed, for no known electronically controlled semiconductor device may withstand the incident power.
  • FIG. 2 represents another prior art apparatus using a single antenna 10 which is alternatively switched by switch 14 between the RF signal transmitter 12 and RF signal receiver 13.
  • the antenna 10 is tuned by a variable capacitor 11.
  • the transmitter power requirement is significantly lower as compared to the embodiment of Fig. 1.
  • the antenna 10 is not limited to a single orientation but may be multi-orientable.
  • the antenna 10 also does not put a large constraint on the size of the magnet gap.
  • An object of the present invention is to provide a unique antenna circuitry for use in NMR and MRI apparatus wherein a single antenna utilizing a plurality of interacting inductance coils is positioned so as to enclose the object or subject to be scanned in its transmitting and receiving RF fields.
  • a further object is to provide an antenna which can be electronically tuned through a varactor (an electronically controlled variable capacitor) , which needs only low transmitter power, which is small and is multi-orientable, and which has high sensitivity at reception.
  • an antenna system comprises at least two electromagnetically coupled resonant circuits.
  • the inductance coils in each resonant circuit is comprised of a coil producing an RF (radio frequency) field fully or partially enclosing the examination object or subject.
  • the combined RF field which is a result of interaction between the resonant circuits, excites the nuclei of the full volume of interest and subsequently intercepts the signal emitted by those nuclei as they relax from their higher energy state.
  • One of the resonant circuits is connected to a transmitter through a first switch device which, in its closed position, forwards the transmitter power to the antenna during the transmitting RF pulse.
  • Another resonant circuit is connected to the receiver.
  • This second resonant circuit incorporates a tuning varactor and a second switch device. The second switch device shorts, during transmission, the part of the resonant circuit which includes the varactor and the receiver input, thus protecting them from the excessive power during transmission.
  • the combined resonant frequency of the antenna during transmission is controlled by a variable capacitor in the first resonant circuit .
  • antenna bandwidth at transmission can be artificially widened, making the antenna substantially indifferent to load variations at the expense of somewhat higher transmitter power requirements.
  • reception bandwidth is not influenced and retains its prior high selectivity properties.
  • the first and second switch devices are easily implemented by using a pair of oppositely interconnected diodes for each connectivity link.
  • Application of transmitter power causes the diodes to conduct, effectively shorting them (i.e., effectively closing the switch) and allowing the power to proceed or pass through.
  • Removal of transmitter power brings the diodes back into a high impedance nonconductive state (i.e., switch open) .
  • the antenna can be positioned at a multitude of orientations in a NMR or MRI apparatus as long as its electrical axis remains perpendicular to the static magnetic field. This property makes it particularly suitable for kinematic orthopaedic examinations.
  • the antenna system of the present invention is fail ⁇ safe.
  • Nonpermissible and unintended high levels of RF power are avoided by the inherent features of low required power and by automatic detuning of the antenna in a case of a single or plural components failure.
  • Those skilled in the art will understand that the principles presented herein allow antenna implementation in a multitude ways which depend on particular application specific requirements: such as Larmor frequency, examination subject or object, magnet field orientation. It will also be clear that a multitude of components can be used instead of those described, for example: any type of variable capacitor can be used in place of a varactor, a set of capacitors can be used in place of any single capacitor, (the same with respect to the varactor) , and an electronically controlled switch can be used in place of a pair of oppositely interconnected diodes. Because the level of transmitted power is low and readily available, the bandwidth of the antenna at transmission may be artificially widened, which means a wide frequency range, and the system seldom requires transmission frequency tuning.
  • Fig. 1 is a schematic representation of a conventional nuclear magnetic resonance (NMR) or magnetic resonance imaging (MRI) apparatus of a type comprising separate transmission and reception antenna systems.
  • NMR nuclear magnetic resonance
  • MRI magnetic resonance imaging
  • Fig. 2 is a schematic representation of a conventional NMR or MRI apparatus having one antenna system.
  • Fig. 3 is an electrical schematic of the antenna system of the present invention.
  • Fig. 3A is a partial schematic showing a modification of the embodiment of Fig. 3.
  • Figs. 3B and 3C are partial schematic views showing diode switches replacing the switches shown schematically in Fig. 3.
  • Fig. 4 is a schematic representation of the antenna system of Fig. 3.
  • Figs. 5A-5D show modified receiver-side configurations of the antenna system of the present invention. DETAILED DESCRIPTION OF THE DRAWINGS
  • the apparatus of the present invention comprises an antenna 15, which may be electronically tuned, needs low transmitter power, is small in size and is multi-orientable, has high sensitivity at reception and is inherently fail-safe.
  • the magnets shown in Figs. 1 and 2) for producing a static magnetic field are not shown in Fig. 3 for ease of illustration.
  • the antenna 15 comprises at least two electromagnetically coupled resonant circuits 27, 28.
  • the inductance coil 16, 17 in each resonant circuit 27, 28 produces an RF field enclosing the examination object (not shown, but see Fig. 1) sometimes somewhat inadequately.
  • the electromagnetic interaction 24 between the resonant circuits 27, 28 results in a combined RF field, which excites the nuclei of the full volume of interest and also intercepts the signal emitted by those nuclei as they relax from their higher energy state.
  • the first resonance circuit 27 has a first variable capacitance 23, the variation in capacitance of which causes a shift in the resonant frequency of the first resonant circuit 27, and also of the resonance frequency of the combined resonant circuits 27, 28.
  • the first capacitance 23 is connected in parallel to the first inductance coil 16.
  • the resonant circuit 27 comprising the first inductance coil 16 and first capacitance 23 is connected through a switch 18 to a source of RF transmitting power 20.
  • the switch 18 is shown schematically as a mechanical switch in Figs. 3 and 4 for ease of description, but is preferably implemented as an electronic switch, as described later.
  • the switch 18 is in a closed position when the transmitter RF power is delivered to the antenna 15, allowing the power to excite the nuclei in the examination object. At other times the switch 18 is open, as shown in Figs. 3 and 4. _
  • the second resonant circuit 28 is comprised of the second inductance coil 17 connected in series with a varactor 22 which serves as a variable capacitance, an auxiliary inductance 26 and a fixed second capacitance 25.
  • the second capacitance 25 may be made variable, as desired. Varying the varactor capacitance 22 causes a shift in the resonant frequency of the combined resonant circuit (comprising resonant circuits 27 and 28) .
  • a receiver 21 picks up the signal emitted by the examination body (object, patient) by being connected to the second resonant circuit 28 in parallel with the varactor 22.
  • a switch 19 is coupled to short out the inductance coil 26, varactor 22 and receiver 21, and is operated synchronously with the switch 18. That is, both switches 18 and 19 are closed when transmitting RF power is delivered; and both switches 18 and 19 are open at other times (as shown in Fig. 3) .
  • the switch 19 is shown schematically in Figs. 3 and 4 as a mechanical switch for ease of description, but is preferably implemented as an electronic switch, as described later.
  • the second resonant circuit 28 When the switch 19 is closed, the second resonant circuit 28 is transformed to effectively be comprised of two elements : the second inductance coil 17 and the second capacitance 25, and the resonant frequency of the transformed second resonant circuit 28 is such that the combined resonant frequency of the antenna 15 matches the frequency of the RF transmitting source 20, which is the examination object's Larmor frequency.
  • the necessary tuning is provided by means of varying the first variable capacitance 23 or, if desired, by varying the capacitance of the second capacitance 25.
  • the RF power from transmitter 20 is thus properly delivered into the examination object.
  • the shorting switch 19 (which is closed) prevents the power from reaching the varactor 22 and receiver 21, hence protecting them from destruction due to high power levels at transmission.
  • the RF power source (transmitter) 20 is disconnected from the antenna.15, the varactor capacitance 22 is a part of the second resonant circuit 28 and is set to define the resonant frequency of the combined resonant circuits 27, 28 to match the Larmor frequency of the relaxing nuclei.
  • the signal from the second resonant circuit 28 is fed to the RF signal receiver 21.
  • the inductance of the auxiliary inductance coil 26 is chosen in such a way as to maintain the resonant frequency range through switching transformations of the second resonant circuit 28.
  • the second resonance circuit 28 can also be used in a detuned mode during transmission, if the spacial positioning of the second inductance coil 17 and its interaction with the first resonant circuit 27 is such that the RF transmitting field flux maintains its proper shape and coverage. As explained later (see Figs. 5A-D) , omission of the auxiliary inductance 26 alone or together with the capacitance 25 is then possible, as well as different modifications of the second resonant circuit 28.
  • the first and second inductance coils 16, 17 comprising the antenna 15 are positioned in close proximity to each other and, as such, they normally have a level of electromagnetic coupling between them of about a few percent.
  • Varactor 22 provides accurate and speedy tuning of the antenna 15 at reception, which is essential for optimal extraction of the signal from background noise at varying load conditions.
  • the antenna 15 can be made substantially indifferent to load variations by using an ohmic resistance R (preferably less than 1 ohm) (see Fig. 3A) on the transmitter side of the first switch 18, which effectively widens the combined resonant circuits' bandwidth.
  • R preferably less than 1 ohm
  • the not-shown parts of the system of Fig. 3A are the same as shown in Fig. 3.
  • This approach of Fig. 3A which widens the bandwidth, avoids the necessity of antenna tuning with replacement of examination objects (patients) , at the expense of slightly higher transmitter RF power.
  • the increase in RF power is negligible for most applications, as the initial RF power requirements are low because of the proximity of the antenna 15 to the examination object.
  • the antenna 15 retains its high selectivity properties.
  • the series resistor R of Fig. 3A could be placed in parallel with the output of RF transmitter 20, to achieve similar results. In this case, the resistance of the parallel resistor must be large.
  • the antenna 15 can be positioned at a multitude of orientations in an MRI or NMR apparatus as long as its electrical axis remains perpendicular to the static magnetic field orientation. It is, therefore, particularly suitable for kinematic orthopaedic examinations.
  • the antenna 15 of the present invention is fail-safe: unintended or excessive RF power delivery is avoided by automatic detuning of the antenna in the case of antenna component failure.
  • the two resonant circuits 27, 28 interact to produce a combined tuning effect, if one component fails, the whole system is detuned, and the delivered power drops, thus preventing damage to the object or patient under examination.
  • the system also has low initial power requirements because the antennas are configured for the desired use, and lower power is thus used in many cases, thereby making the antenna system even more fail-safe.
  • Fig. 3B shows a simple implementation of the switches 18 as respective pairs of oppositely interconnected diodes
  • Fig. 3C shows a simple implementation of the switch 19 as a pair of oppositely interconnected diodes.
  • Such diode switches are shown, for example, in U. S. Patent No. 4,975,644 (Fig. 8) .
  • Other electronic switching arrangements could be used; see for example U. S. Patent No. 5,144,244. In operation, the diode switching arrangement of Figs. 3B and 3C is automatic.
  • the high power output of the transmitter when the transmitter is turned on to transmit an RF signal, the high power output of the transmitter, during the positive half cycle of the AC RF signal, causes the diode connected in the forward direction to conduct, and the diode connected in the reverse direction does not conduct.
  • the diode connected in the reverse direction conducts and the diode connected in the forward direction does not conduct.
  • Each pair of diodes operates in a similar manner.
  • the stray signals in the system are not sufficient to cause the diodes to conduct, even in their respective forward directions, thereby effectively isolating the transmitter 20 from the resonant circuits during times when the transmitter 20 is turned off.
  • the RF signals passing through the diodes in Fig. 3C are sufficiently large to cause the diodes to conduct in their respective forward directions
  • the transmitter 20 When the transmitter 20 is turned off, the signals flowing through the circuit are sufficiently low that the diodes 19 are not turned on, even in their forward directions, thereby appearing as an open circuit and permitting the received signals to be forwarded to the RF signal receiver 21.
  • two or more series connected diodes can be used in place of each diode shown in Figs. 3B and 3C, for example as shown in Fig. 8 of U. S. Patent No. 4,975,644.
  • the potential implementations of the antenna of the present invention are numerous and application driven.
  • the Larmor frequency, the nature of the examination object and magnetic field orientation will prescribe the specified antenna's shape, size and components. It will also be clear that a multitude of components can be used instead of those specifically described.
  • a pair of parallel and oppositely interconnected diodes can be used in place of each switching pole 18, 19, a set of capacitors including stray capacitance can be used in place of any single capacitor, and any type and number of variable capacitors can be used in place of varactor 22.
  • standard consideration should be given to stray reactances and to impedance matching of the transmitter 20 and receiver 21.
  • the impedance matching circuitry is presumed to be integral parts of the RF signal transmitter 20, and RF signal receiver 21, respectively.
  • the system could be configured so that (I) during transmission the resonant circuit 28 is tuned to the transmitter frequency, or (II) during transmission the resonant circuit 28 is detuned with respect to the transmitter frequency.
  • the conditions I and II are shown in Figs. 5A-5D. In each case, switch 19 is closed during transmission. In Figs. 5A and 5D, the conditions I and II are determined by the values of the components of the circuit. In Fig. 5A, the switches 19', which are connected in series with inductance 26' , close (during the respective positive and negative half cycles) during transmission due to the high transmission power level. Only receiver-side circuits are shown in Figs. 5A-5D. The transmission side is as shown in Figs. 3 and/or 4 (and/or as modified by Figs. 3A or 3B) .

Abstract

An antenna system for use in an NMR or MRI apparatus which includes a radio frequency (RF) signal transmitter (20) and a radio frequency (RF) signal receiver (21). The antenna system includes at least first and second electromagnetically coupled resonant circuits, the first resonant circuit comprising a first inductance coil (16) producing a first electromagnetic field flux vector, and the second resonant circuit comprising a second inductance coil (17) producing a second electromagnetic field flux vector, the first electromagnetic field flux vector having a component parallel to the second electromagnetic field flux vector. A switch system (18, 19) is coupled to the first and second resonant circuits. The switch system has a first switching position for coupling the first resonant circuit to an output of the RF signal transmitter and preventing a signal from the second resonant circuit from being fed to an input of said RF signal receiver, and a second switching position for permitting an RF signal from the second resonant circuit to be fed to an input of the RF signal receiver and disconnecting the first resonant circuit from the output of the RF signal transmitter.

Description

TITLE
ANTENNA SYSTEM FOR NMR AND MRI APPARATUS
CROSS REFERENCE TO RELATED APPLICATION
This is a Continuation-in-Part of my prior application Serial No. 08/656,766, the entire contents of which are incorporated herein by reference.
BACKGROUND OF THE INVENTION
1. FIELD OF THE INVENTION
The present invention is directed to transmission and reception antennas for use in a nuclear magnetic resonance (NMR) apparatus and in a magnetic resonance imaging (MRI) apparatus, for calculating spectra or generating images of an examination subject or object.
2. DESCRIPTION OF THE PRIOR ART
Nuclear magnetic resonance (NMR) is the effect of a resonant rotating or alternating magnetic field, imposed at right angles to a static field, to perturb the orientation of nuclear magnetic moments.
Magnetic resonance imaging (MRI) is the development of nuclear magnetic resonance (NMR) techniques for obtaining a diagnostic scan of a subject such as a human or animal body. The patient or examination subject is placed in a strong magnetic field. This magnetic field induces a net magnetization of the nuclei in the subject. A short radio frequency pulse (RF pulse) is applied at the Larmor frequency of the precessing nuclei which, in turn, emit an RF signal of the same frequency. This is detected and gives a
"fingerprint" of the environment of the nucleus being studied. This information is one-dimensional but is converted into a two-dimensional anatomical image by adding a gradient to the applied magnetic field which results in a frequency modulation of the -emitted RF signal. A series of such measurements is analyzed by computer to generate the image .
In an NMR apparatus, as well as in an MRI apparatus, a strong magnetic field aligns the nuclei of the subject or object to be studied along the field direction. A radio frequency field delivered through a transmitter antenna, also known as the transmitter coil, brings the nuclei to a higher energy state. A receiver antenna, also referred to as a receiver coil, intercepts the signal emitted by the object (patient) as its nuclei precess or relax from the higher energy state.
The conditions of efficient energy absorption require that the RF fields of the transmitter and receiver antennas be orthogonal to the static magnetic field. The simultaneous condition of negligibly low interaction between the receiver and transmitter antennas for minimal mutual distortion of their RF fields and for the prevention of high transmitter power to be applied to the receiver, in part also means that the RF fields of the transmitter and receiver antennas must be orthogonal even though transmission and reception do not coincide in time. Acceptable switching time between the two is of the order of about ten microseconds.
As represented by Fig. 1, which shows the prior art, a radio frequency (RF) transmitter 4 transmits a signal to a transmitter antenna 2. The signal which is absorbed and subsequently re-emitted by the examination body or subject (patient) 5 is then picked up by a receiver antenna 1 and fed to a radio frequency (RF) receiver 3. The examination body or subject 5 which is being scanned is within the RF fields of both the transmitter and receiver antennas 2,1. The transmitter antenna 2 and receiver antenna 1 are optimized for their respective tasks and are tuned by variable capacitors 6 and 7. Normally, the single, fixed in place transmitter antenna 2 is big enough to encompass the largest part of a body or subject 5 to be scanned. Significantly smaller reception antennas 1, specialized for different body parts, are separately connected and used. Magnet poles 8 and 9 are shown located above and below the patient (body or subject 5) , respectively.
Because of the orthogonal arrangement and spatial separations of the transmitter antenna 2 and receiver antenna 1, the resulting low electromagnetic coupling between the transmitter antenna 2 and receiver antenna 1 assures low field distortion and allows utilization of speedy and efficient electronic tuning for the receiver antenna 1. The required transmitting power is high and manual tuning of the transmitter antenna 2 by a variable capacitor 6 is employed, for no known electronically controlled semiconductor device may withstand the incident power.
Another limitation of the prior art apparatus is that the magnet gap between magnet poles 8 and 9 should be large enough to receive the two separate antennas 1, 2 therebetween, which is not always possible or cost efficient.
These prior art types of devices are described, for example, in U.S. Patent Nos. 4,926,126; 4,975,644; 5,144,244; and 5,256,972, the entire contents of which are incorporated herein by reference.
Figure 2 represents another prior art apparatus using a single antenna 10 which is alternatively switched by switch 14 between the RF signal transmitter 12 and RF signal receiver 13. The antenna 10 is tuned by a variable capacitor 11.
In the case of Fig. 2, the transmitter power requirement is significantly lower as compared to the embodiment of Fig. 1. The antenna 10 is not limited to a single orientation but may be multi-orientable. The antenna 10 also does not put a large constraint on the size of the magnet gap. These prior art types of devices are described, for example, in U.S. Patent Nos. 4,901,022 and 5,166,617, the entire contents of which are incorporated herein by reference. However, even though the transmitter power is lower in the embodiment of Fig. 2, the transmitter power requirement is still so high as to prevent simple implementation of electronic antenna tuning.
SUMMARY OF THE INVENTION An object of the present invention is to provide a unique antenna circuitry for use in NMR and MRI apparatus wherein a single antenna utilizing a plurality of interacting inductance coils is positioned so as to enclose the object or subject to be scanned in its transmitting and receiving RF fields. A further object is to provide an antenna which can be electronically tuned through a varactor (an electronically controlled variable capacitor) , which needs only low transmitter power, which is small and is multi-orientable, and which has high sensitivity at reception. According to the invention, an antenna system comprises at least two electromagnetically coupled resonant circuits. The inductance coils in each resonant circuit is comprised of a coil producing an RF (radio frequency) field fully or partially enclosing the examination object or subject. The combined RF field, which is a result of interaction between the resonant circuits, excites the nuclei of the full volume of interest and subsequently intercepts the signal emitted by those nuclei as they relax from their higher energy state.
As proximately positioned coils normally have a level of electromagnetic coupling of a few percent only, this low level of interaction leads to a frequency response curve of the combined resonant circuit which approximates a multiplication of separate frequency response curves for each resonant circuit. This, in turn, contributes to higher selectivity and sensitivity of the antenna at reception, as compared to a single resonant circuit .
One of the resonant circuits is connected to a transmitter through a first switch device which, in its closed position, forwards the transmitter power to the antenna during the transmitting RF pulse. Another resonant circuit is connected to the receiver. This second resonant circuit incorporates a tuning varactor and a second switch device. The second switch device shorts, during transmission, the part of the resonant circuit which includes the varactor and the receiver input, thus protecting them from the excessive power during transmission. The combined resonant frequency of the antenna during transmission is controlled by a variable capacitor in the first resonant circuit .
At the time of reception, all switch devices are open, causing the transmitter to be disconnected from the antenna, while the receiver input is freed to pick up a signal, and the varactor is used to control the combined resonant frequency.
Since the antenna is located in the very proximity to the examination object, transmitting power requirements are minimal. By using an ohmic resistance on the transmitter side of the first switch device, antenna bandwidth at transmission can be artificially widened, making the antenna substantially indifferent to load variations at the expense of somewhat higher transmitter power requirements. Thus, the reception bandwidth is not influenced and retains its prior high selectivity properties.
The first and second switch devices are easily implemented by using a pair of oppositely interconnected diodes for each connectivity link. Application of transmitter power causes the diodes to conduct, effectively shorting them (i.e., effectively closing the switch) and allowing the power to proceed or pass through. Removal of transmitter power brings the diodes back into a high impedance nonconductive state (i.e., switch open) . The antenna can be positioned at a multitude of orientations in a NMR or MRI apparatus as long as its electrical axis remains perpendicular to the static magnetic field. This property makes it particularly suitable for kinematic orthopaedic examinations. The antenna system of the present invention is fail¬ safe. Nonpermissible and unintended high levels of RF power are avoided by the inherent features of low required power and by automatic detuning of the antenna in a case of a single or plural components failure. _ Those skilled in the art will understand that the principles presented herein allow antenna implementation in a multitude ways which depend on particular application specific requirements: such as Larmor frequency, examination subject or object, magnet field orientation. It will also be clear that a multitude of components can be used instead of those described, for example: any type of variable capacitor can be used in place of a varactor, a set of capacitors can be used in place of any single capacitor, (the same with respect to the varactor) , and an electronically controlled switch can be used in place of a pair of oppositely interconnected diodes. Because the level of transmitted power is low and readily available, the bandwidth of the antenna at transmission may be artificially widened, which means a wide frequency range, and the system seldom requires transmission frequency tuning.
BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a schematic representation of a conventional nuclear magnetic resonance (NMR) or magnetic resonance imaging (MRI) apparatus of a type comprising separate transmission and reception antenna systems.
Fig. 2 is a schematic representation of a conventional NMR or MRI apparatus having one antenna system.
Fig. 3 is an electrical schematic of the antenna system of the present invention.
Fig. 3A is a partial schematic showing a modification of the embodiment of Fig. 3. Figs. 3B and 3C are partial schematic views showing diode switches replacing the switches shown schematically in Fig. 3.
Fig. 4 is a schematic representation of the antenna system of Fig. 3. Figs. 5A-5D show modified receiver-side configurations of the antenna system of the present invention. DETAILED DESCRIPTION OF THE DRAWINGS
The apparatus of the present invention, represented in Figs. 3 and 4, comprises an antenna 15, which may be electronically tuned, needs low transmitter power, is small in size and is multi-orientable, has high sensitivity at reception and is inherently fail-safe. The magnets (shown in Figs. 1 and 2) for producing a static magnetic field are not shown in Fig. 3 for ease of illustration. The antenna 15 comprises at least two electromagnetically coupled resonant circuits 27, 28. The inductance coil 16, 17 in each resonant circuit 27, 28 produces an RF field enclosing the examination object (not shown, but see Fig. 1) sometimes somewhat inadequately. The electromagnetic interaction 24 between the resonant circuits 27, 28 results in a combined RF field, which excites the nuclei of the full volume of interest and also intercepts the signal emitted by those nuclei as they relax from their higher energy state.
The first resonance circuit 27 has a first variable capacitance 23, the variation in capacitance of which causes a shift in the resonant frequency of the first resonant circuit 27, and also of the resonance frequency of the combined resonant circuits 27, 28. The first capacitance 23 is connected in parallel to the first inductance coil 16. The resonant circuit 27 comprising the first inductance coil 16 and first capacitance 23 is connected through a switch 18 to a source of RF transmitting power 20. The switch 18 is shown schematically as a mechanical switch in Figs. 3 and 4 for ease of description, but is preferably implemented as an electronic switch, as described later. The switch 18 is in a closed position when the transmitter RF power is delivered to the antenna 15, allowing the power to excite the nuclei in the examination object. At other times the switch 18 is open, as shown in Figs. 3 and 4. _ The second resonant circuit 28 is comprised of the second inductance coil 17 connected in series with a varactor 22 which serves as a variable capacitance, an auxiliary inductance 26 and a fixed second capacitance 25. The second capacitance 25 may be made variable, as desired. Varying the varactor capacitance 22 causes a shift in the resonant frequency of the combined resonant circuit (comprising resonant circuits 27 and 28) . A receiver 21 picks up the signal emitted by the examination body (object, patient) by being connected to the second resonant circuit 28 in parallel with the varactor 22. A switch 19 is coupled to short out the inductance coil 26, varactor 22 and receiver 21, and is operated synchronously with the switch 18. That is, both switches 18 and 19 are closed when transmitting RF power is delivered; and both switches 18 and 19 are open at other times (as shown in Fig. 3) . The switch 19 is shown schematically in Figs. 3 and 4 as a mechanical switch for ease of description, but is preferably implemented as an electronic switch, as described later.
When the switch 19 is closed, the second resonant circuit 28 is transformed to effectively be comprised of two elements : the second inductance coil 17 and the second capacitance 25, and the resonant frequency of the transformed second resonant circuit 28 is such that the combined resonant frequency of the antenna 15 matches the frequency of the RF transmitting source 20, which is the examination object's Larmor frequency. The necessary tuning is provided by means of varying the first variable capacitance 23 or, if desired, by varying the capacitance of the second capacitance 25. The RF power from transmitter 20 is thus properly delivered into the examination object. At the same time, during RF power transmission, the shorting switch 19 (which is closed) prevents the power from reaching the varactor 22 and receiver 21, hence protecting them from destruction due to high power levels at transmission.
At reception, when both of the switches 18, 19 are open, the RF power source (transmitter) 20 is disconnected from the antenna.15, the varactor capacitance 22 is a part of the second resonant circuit 28 and is set to define the resonant frequency of the combined resonant circuits 27, 28 to match the Larmor frequency of the relaxing nuclei. The signal from the second resonant circuit 28 is fed to the RF signal receiver 21. The inductance of the auxiliary inductance coil 26 is chosen in such a way as to maintain the resonant frequency range through switching transformations of the second resonant circuit 28. The second resonance circuit 28 can also be used in a detuned mode during transmission, if the spacial positioning of the second inductance coil 17 and its interaction with the first resonant circuit 27 is such that the RF transmitting field flux maintains its proper shape and coverage. As explained later (see Figs. 5A-D) , omission of the auxiliary inductance 26 alone or together with the capacitance 25 is then possible, as well as different modifications of the second resonant circuit 28. The first and second inductance coils 16, 17 comprising the antenna 15 are positioned in close proximity to each other and, as such, they normally have a level of electromagnetic coupling between them of about a few percent. This low level of interaction leads to a frequency response curve of the combined resonant circuits 27, 28 which approximates a multiplication of the frequency response curves of each member circuit 27, 28. The result is higher selectivity and sensitivity of the antenna 15 as compared to an antenna having only a single resonant circuit. Varactor 22 provides accurate and speedy tuning of the antenna 15 at reception, which is essential for optimal extraction of the signal from background noise at varying load conditions.
At transmission, the antenna 15 can be made substantially indifferent to load variations by using an ohmic resistance R (preferably less than 1 ohm) (see Fig. 3A) on the transmitter side of the first switch 18, which effectively widens the combined resonant circuits' bandwidth. The not-shown parts of the system of Fig. 3A are the same as shown in Fig. 3. This approach of Fig. 3A, which widens the bandwidth, avoids the necessity of antenna tuning with replacement of examination objects (patients) , at the expense of slightly higher transmitter RF power. The increase in RF power is negligible for most applications, as the initial RF power requirements are low because of the proximity of the antenna 15 to the examination object. At reception, the antenna 15 retains its high selectivity properties. The series resistor R of Fig. 3A could be placed in parallel with the output of RF transmitter 20, to achieve similar results. In this case, the resistance of the parallel resistor must be large. The antenna 15 can be positioned at a multitude of orientations in an MRI or NMR apparatus as long as its electrical axis remains perpendicular to the static magnetic field orientation. It is, therefore, particularly suitable for kinematic orthopaedic examinations. The antenna 15 of the present invention is fail-safe: unintended or excessive RF power delivery is avoided by automatic detuning of the antenna in the case of antenna component failure. Since the two resonant circuits 27, 28 interact to produce a combined tuning effect, if one component fails, the whole system is detuned, and the delivered power drops, thus preventing damage to the object or patient under examination. The system also has low initial power requirements because the antennas are configured for the desired use, and lower power is thus used in many cases, thereby making the antenna system even more fail-safe.
Fig. 3B shows a simple implementation of the switches 18 as respective pairs of oppositely interconnected diodes, and Fig. 3C shows a simple implementation of the switch 19 as a pair of oppositely interconnected diodes. Such diode switches are shown, for example, in U. S. Patent No. 4,975,644 (Fig. 8) . Other electronic switching arrangements could be used; see for example U. S. Patent No. 5,144,244. In operation, the diode switching arrangement of Figs. 3B and 3C is automatic. That is, when the transmitter is turned on to transmit an RF signal, the high power output of the transmitter, during the positive half cycle of the AC RF signal, causes the diode connected in the forward direction to conduct, and the diode connected in the reverse direction does not conduct. During the negative half cycle of the AC RF signal, the diode connected in the reverse direction conducts and the diode connected in the forward direction does not conduct. Each pair of diodes operates in a similar manner. When the transmitter 20 is turned off, the stray signals in the system are not sufficient to cause the diodes to conduct, even in their respective forward directions, thereby effectively isolating the transmitter 20 from the resonant circuits during times when the transmitter 20 is turned off. Similarly, at the receiver side, when the transmitter 20 is turned on, the RF signals passing through the diodes in Fig. 3C are sufficiently large to cause the diodes to conduct in their respective forward directions
(during the positive and negative half cycles, respectively) to effectively short out the input of the receiver 21. When the transmitter 20 is turned off, the signals flowing through the circuit are sufficiently low that the diodes 19 are not turned on, even in their forward directions, thereby appearing as an open circuit and permitting the received signals to be forwarded to the RF signal receiver 21.
If higher threshold switching voltages are required, two or more series connected diodes can be used in place of each diode shown in Figs. 3B and 3C, for example as shown in Fig. 8 of U. S. Patent No. 4,975,644.
Those skilled in the art will recognize that the potential implementations of the antenna of the present invention are numerous and application driven. The Larmor frequency, the nature of the examination object and magnetic field orientation will prescribe the specified antenna's shape, size and components. It will also be clear that a multitude of components can be used instead of those specifically described. For example, as mentioned above, a pair of parallel and oppositely interconnected diodes (or other electronic switching arrangements) can be used in place of each switching pole 18, 19, a set of capacitors including stray capacitance can be used in place of any single capacitor, and any type and number of variable capacitors can be used in place of varactor 22. Also, standard consideration should be given to stray reactances and to impedance matching of the transmitter 20 and receiver 21. The impedance matching circuitry is presumed to be integral parts of the RF signal transmitter 20, and RF signal receiver 21, respectively.
The system could be configured so that (I) during transmission the resonant circuit 28 is tuned to the transmitter frequency, or (II) during transmission the resonant circuit 28 is detuned with respect to the transmitter frequency. The conditions I and II are shown in Figs. 5A-5D. In each case, switch 19 is closed during transmission. In Figs. 5A and 5D, the conditions I and II are determined by the values of the components of the circuit. In Fig. 5A, the switches 19', which are connected in series with inductance 26' , close (during the respective positive and negative half cycles) during transmission due to the high transmission power level. Only receiver-side circuits are shown in Figs. 5A-5D. The transmission side is as shown in Figs. 3 and/or 4 (and/or as modified by Figs. 3A or 3B) .
It will be appreciated that the instant specification is set forth by way of illustration and not limitation, and that various modifications and changes may be made without departing from the spirit and scope of the present invention.

Claims

CLAIMS :
1. An antenna system for use in a nuclear magnetic resonance or magnetic resonance imaging apparatus which includes a radio frequency (RF) signal transmitter and a radio frequency (RF) signal receiver, the antenna system comprising: at least first and second electromagnetically coupled resonant circuits; said first resonant circuit comprising a first inductance coil producing a first electromagnetic field flux vector; said second resonant circuit comprising a second inductance coil producing a second electromagnetic field flux vector; said first and second inductance coils being electromagnetically coupled such that the first electromagnetic field flux vector has a component parallel to the second electromagnetic field flux vector; and a switch system coupled to said first resonant circuit and to said second resonant circuit, said switch system having: a first switching position for coupling said first resonant circuit to an output of said RF signal transmitter and for preventing a signal from said second resonant circuit from being fed to an input of said RF signal receiver, and a second switching position for permitting an RF signal from said second resonant circuit to be fed to an input of said RF signal receiver and for disconnecting said first resonant circuit from the output of said RF signal transmitter; and wherein: at least said first inductance coil produces an electromagnetic field flux enclosing an examination object therewithin, which electromagnetic field flux is used to irradiate the examination object, when said switch system is in the first switching position; and an electromagnetic field flux produced by a signal emitted by the examination object's relaxing nuclei is picked up by said electromagnetically coupled inductance coils and is fed to said RF signal receiver via said second resonant circuit, when said switch system is in the second switching position.
2. The antenna system of claim 1, wherein: said first resonant circuit comprises at least a first capacitance connected in parallel with said first inductance coil, and comprising together with said first inductance coil the first resonant circuit, and wherein at least said first capacitance is used for frequency tuning of the antenna system at least during transmission; and said switch system includes at least one first switching element connecting said first resonant circuit to said RF signal transmitter output in said first switching position and disconnecting said first resonant circuit from said RF signal transmitter output in said second switching position.
3. The antenna system of claim 2, wherein said first capacitance comprises a variable capacitor element .
4. The antenna system of claim 2, wherein: said second resonant circuit comprises: a variable capacitance element, coupled for frequency tuning of the antenna circuitry and for feeding an RF signal to an input of said RF receiver; a second capacitance; and an auxiliary inductance for roughly matching an impedance of said second capacitance; said second capacitance, said variable capacitance element and said auxiliary inductance being coupled together and being further coupled to said second inductance coil; and said switch system includes a second switching element coupled to selectively short out at least said variable capacitance element and said RF receiver input, and for electrically removing at least said variable capacitance element, and said RF receiver input from said second resonance circuit, in said first switching position, and said second switching element being electrically open and having no electrical effect in said second switching position.
5. The antenna circuitry of claim 4, wherein said variable capacitance element comprises at least one varactor.
6. The antenna system of claim 4, wherein said first capacitance comprises a variable capacitor element.
7. The antenna system of claim 1, wherein: said second resonant circuit comprises: a variable capacitance element, coupled for frequency tuning of the antenna circuitry and for feeding an RF signal to an input of said RF receiver; a second capacitance; and an auxiliary inductance for roughly matching an impedance of said second capacitance; said second capacitance, said variable capacitance element and said auxiliary inductance being coupled together and being further coupled to said second inductance coil; and said switch system includes a second switching element coupled to selectively short out at least said variable capacitance element and said RF receiver input, and for electrically removing at least said variable capacitance element, and said RF receiver input from said second resonance circuit, in said first switching position, and said second switching element being electrically open and having no electrical effect in said second switching position.
8. The antenna circuitry of claim 7, wherein said variable capacitance element comprises at least one varactor. 9. The antenna system of claim 7, wherein said first resonant circuit comprises a capacitor element connected to said first inductance coil .
10. The antenna system of claim 7, wherein said second capacitance, said variable capacitance element and said auxiliary inductance are connected in a series connection.
11. The antenna system of claim 10, wherein said series connection is serially connected with said second inductance coil .
12. The antenna system of claim 7, wherein said auxiliary inductance is connected in series with a switch device, the series connection being connected in parallel with said second capacitance.
13. The antenna system of claim 1, wherein said switch system comprises: at least a first pair of opposite polarity, parallel connected, diodes coupled to an output of said RF signal transmitter; and at least a second pair of opposite polarity, parallel connected, diodes coupled across the input of said RF signal receiver.
14. The antenna system of claim 1, further comprising a resistance coupled to an output of said RF signal transmitter.
15. The antenna system of claim 1, wherein: said second resonant circuit comprises: a variable capacitance element, coupled for frequency tuning of the antenna circuitry and for feeding an RF signal to an input of said RF receiver; a second capacitance; and said second capacitance and said variable capacitance element being connected to said second inductance coil; and said switch system includes a second switching element coupled to selectively short out said variable capacitance element and said RF receiver input, and for electrically removing at least said variable capacitance element, and said RF receiver input from said second resonance circuit, in said first switching position, and said second switching element being electrically open and having no electrical effect in said second switching position.
16. The antenna circuitry of claim 15, wherein said variable capacitance element comprises a varactor.
17. The antenna system of claim 15, wherein said first resonant circuit comprises a capacitor element connected to said first inductance coil.
18. The antenna system of claim 1, wherein: said second resonant circuit comprises: a variable capacitance element, coupled for frequency tuning of the antenna circuitry and for feeding an RF signal to an input of said RF receiver; said variable capacitance element being coupled to said second inductance coil; and said switch system includes a second switching element coupled to selectively short out said variable capacitance element and said RF receiver input, and for electrically removing said variable capacitance element and said RF receiver input from said second resonance circuit, in said first switching position, and said second switching element being electrically open and having no electrical effect in said second switching position.
19. The antenna circuitry of claim 18, wherein said variable capacitance element comprises a varactor. 20. The antenna system of claim 18, wherein said first resonant circuit comprises a capacitor element connected to said first inductance coil.
21. A method of operating an antenna system in a nuclear magnetic resonance or magnetic resonance imaging apparatus which includes a radio frequency (RF) signal transmitter and a radio frequency (RF) signal receiver, the method comprising: providing at least first and second electromagnetically coupled resonant circuits; said first resonant circuit comprising a first inductance coil producing a first electromagnetic field flux vector; said second resonant circuit comprising a second inductance coil producing a second electromagnetic field flux vector; causing said first and second inductance coils to be electromagnetically coupled such that the first electromagnetic field flux vector has a component parallel to the second electromagnetic field flux vector; and switching said first resonant circuit and said second resonant circuit with a switch system such that : when said switch system is in a first switching position, said first resonant circuit is coupled to an output of said RF signal transmitter, and a signal from said second resonant circuit is prevented from being fed to an input of said RF signal receiver, and when said switch system is in a second switching position, an RF signal from said second resonant circuit is fed to an input of said RF signal receiver and said first resonant circuit is disconnected from the output of said RF signal transmitter; and wherein: at. least said first inductance coil produces an electromagnetic field flux enclosing an examination object therewithin, which electromagnetic field flux is used to irradiate the examination object, when said switch system is in the first switching position; and an electromagnetic field flux produced by a signal emitted by the examination object's relaxing nuclei is picked up by said electromagnetically coupled inductance coils and is fed to said RF signal receiver via said second resonant circuit, when said switch system is in the second switching position.
22. The method of claim 21, wherein: the frequency response of said first and second resonant circuits is set independently and separately in the first and second switching positions.
23. The method of claim 21, wherein the antenna system is positioned at any angle orthogonal to a static magnetic field of the apparatus.
24. The method of claim 21, comprising maintaining said first and second resonant circuits tuned to the object's Larmor frequency when said switch system is in said first switching position.
25. The method of claim 21, comprising detuning said second resonant circuit from the object's Larmor frequency when said switch system is in said first switching position.
26. The method of claim 21, wherein said first and second resonant circuits are tuned to the object's Larmor frequency when said switch system is in said second switching position. AMENDED CLAIMS
[received by the International Bureau on 21 November 1997 (21.11.97); original claims 1, 2, 4, 7, 9, 13, 15, 17, 18,
20-22 and 24-26 amended; new claims 27-35 added; remaining claims unchanged (10 pages)]
1. An antenna system for use in a nuclear magnetic resonance or magnetic resonance imaging apparatus which includes a radio frequency (RF) signal transmitter and a radio frequency (RF) signal receiver, the antenna system comprising: at least first and second electromagnetically coupled circuits; said first circuit comprising a first inductance coil producing a first electromagnetic field flux vector; said second circuit comprising a second inductance coil producing a second electromagnetic field flux vector ; said first and second inductance coils being electromagnetically coupled such that the first electromagnetic field flux vector has a component interacting with a component of the second electromagnetic field flux vector; and a switch system coupled to said first circuit and to said second circuit, said switch system having: a first switching position for coupling said first circuit to an output of said RF signal transmitter and for preventing a damaging level of signal from said second circuit from being fed to an input of said RF signal receiver, and a second switching position for permitting an RF signal from said second circuit to be fed to an input of said RF signal receiver and for decoupling said first circuit from the output of said RF signal transmitter; and wherein: said antenna system produces an electromagnetic field flux enclosing an examination object therewithin, which electromagnetic field flux is used to irradiate the examination object, when said switch system is in the first switching position; and an electromagnetic field flux produced by a signal emitted by the examination object's relaxing nuclei is picked up by said electromagnetically coupled inductance coils and is fed to said RF signal receiver ia said second circuit, when said switch system is in the second switching position.
2. The antenna system of claim 1, wherein: said first circuit comprises at least a first capacitance connected in parallel with said first inductance coil, and comprising together with said first inductance coil the first circuit, and wherein at least said first capacitance is used for frequency tuning of the antenna system at least during transmission; and said switch system includes at least one first switching element coupling said first circuit to said RF signal transmitter output in said first switching position and decoupling said first circuit from said RF signal transmitter output in said second switching position.
3. The antenna system of claim 2, wherein said first capacitance comprises a variable capacitor element.
4. The antenna system of claim 2, wherein: said second circuit comprises: a variable capacitance element, coupled for frequency tuning of the antenna circuitry; a second capacitance; and an auxiliary inductance for roughly matching an impedance of said second capacitance; said second capacitance, said variable capacitance element and said auxiliary inductance being coupled together and being further coupled to said second inductance coil; and said switch system includes a second switching element coupled to selectively short out at least said variable capacitance element and said RF receiver input, and for electrically removing at least said variable capacitance element and said RF receiver input from said second circuit, in said first switching position, and said second switching element being electrically open and having substantially no electrical effect in said second switching position.
5. The antenna circuitry of claim 4, wherein said variable capacitance element comprises at least one varactor.
6. The antenna system of claim , wherein said first capacitance comprises a variable capacitor element.
7. The antenna system of claim 1, wherein: said second circuit comprises: a variable capacitance element, coupled for frequency tuning of the antenna circuitry; a second capacitance; and an auxiliary inductance for roughly matching an impedance of said second capacitance; said second capacitance, said variable capacitance element and said auxiliary inductance being coupled together and being further coupled to said second inductance coil; and said switch system includes a second switching element coupled to selectively short out at least said variable capacitance element and said RF receiver input, and for electrically removing at least said variable capacitance element and said RF receiver input from said second circuit, in said first switching position, and said second switching element being electrically open and having substantially no electrical effect in said second switching position.
8. The antenna circuitry of claim 7, wherein said variable capacitance element comprises at least one varactor.
9. The antenna system of claim 7, wherein said first circuit comprises a capacitor element connected to said first inductance coil.
10. The antenna system of claim 7, wherein said second capacitance, said variable capacitance element and said auxiliary inductance are connected in a series connection.
11. The antenna system of claim 10, wherein said series connection is serially connected with said second inductance coil.
12. The antenna system of claim 7, wherein said auxiliary inductance is connected in series with a switch device, the series connection being connected in parallel with said second capacitance.
13. The antenna system of claim 1, wherein said switch system comprises: at least a first pair of opposite polarity, parallel connected, diodes coupled to an output of said RF signal transmitter; and at least a second pair of opposite polarity, parallel connected, diodes coupled across an input of said RF signal receiver.
14. The antenna system of claim 1, further comprising a resistance coupled to an output of said RF signal transmitter.
15. The antenna system of claim 1, wherein: said second circuit comprises: a variable capacitance element, coupled for frequency tuning of the antenna circuitry; a second capacitance; and said second capacitance and said variable capacitance element being connected to said second inductance coil; and said switch system includes a second switching element coupled to selectively short out at least said variable capacitance element and said RF receiver input, and for electrically removing at least said variable capacitance element and said RF receiver input from said second circuit, in said first switching position, and said second switching element being electrically open and having substantially no electrical effect in said second switching position.
16. The antenna circuitry of claim 15, wherein said variable capacitance element comprises a varactor.
17. The antenna system of claim 15, wherein said first circuit comprises a capacitor element connected to said first inductance coil.
18. The antenna system of claim 1, wherein: said second circuit comprises: a variable capacitance element, coupled for frequency tuning of the antenna circuitry; said variable capacitance element being coupled to said second inductance coil; and said switch system includes a second switching element coupled to selectively short out at least said variable capacitance element and said RF receiver input, and for electrically removing said variable capacitance element and said RF receiver input from said second circuit, in said first switching position, and said second switching element being electrically open and having substantially no electrical effect in said second switching position.
19. The antenna circuitry of claim 18, wherein said variable capacitance element comprises a varactor.
20. The antenna system of claim 18, wherein said first circuit comprises a capacitor element connected to said first inductance coil.
21. A method of operating an antenna system in a nuclear magnetic resonance or magnetic resonance imaging apparatus which includes a radio frequency (RF) signal transmitter and a radio frequency (RF) signal receiver, the method comprising: providing at least first and second electromagnetically coupled circuits; said first circuit comprising a first inductance coil producing a first electromagnetic field flux vector; said second circuit comprising a second inductance coil producing a second electromagnetic field flux vector; causing said first and second inductance coils to be electromagnetically coupled such that the first electromagnetic field flux vector has a component interacting with a component of the second electromagnetic field flux vector; and switching said first circuit and said second circuit with a switch system such that: when said switch system is in a first switching position, said first circuit is coupled to an output of said RF signal transmitter, and a damaging level of signal from said second circuit is prevented from being fed to an input of said RF signal receiver, and when said switch system is in a second switching position, an RF signal from said second circuit is fed to an input of said RF signal receiver and said first circuit is decoupled from an output of said RF signal transmitter; and wherein: said antenna system produces an electromagnetic field flux enclosing an examination object therewithin, which electromagnetic field flux is used to irradiate the examination object, when said switch system is in the first switching position; and an electromagnetic field flux produced by a signal emitted by the examination object's relaxing nuclei is picked up by said electromagnetically coupled inductance coils and is fed to said RF signal receiver via said second circuit, when said switch system is in the second switching position.
22. The method of claim 21, wherein: the frequency response and the electromagnetic field flux of said antenna system is set independently and separately in the first and second switching positions.
23. The method of claim 21, wherein the antenna system is positioned at any angle orthogonal to a static magnetic field of the apparatus.
24. The method of claim 21, comprising maintaining said antenna system tuned to the object's Larmor frequency when said switch system is in said first switching position.
25. The method of claim 21, comprising detuning said second circuit from the object's Larmor frequency when said switch system is in said first switching position.
26. The method of claim 21, wherein said antenna system is tuned to the object's Larmor frequency when said switch system is in said second switching position.
27. An antenna system for use in a nuclear magnetic resonance αr magnetic resonance imaging apparatus which includes a radio frequency (RF) signal transmitter and a radio frequency (RF) signal receiver, the antenna system comprising: at least one circuit, including an inductance coil, for producing an electromagnetic field flux vector; and a switch system coupled to said at least one circuit, said switch system having: a first switching position for coupling said at least one circuit to an output of said RF signal transmitter and for preventing a damaging level of signal from said at least one circuit from being fed to an input of said RF signal receiver, and a second switching position for permitting an RF signal from said at least one circuit to be fed to an input of said RF signal receiver and for decoupling said at least one circuit from the output of said RF signal transmitter; and wherein: said antenna system produces an electromagnetic field flux enclosing an examination object therewithin, which electromagnetic field flux is used to irradiate the examination object, when said switch system is in the first switching position; and an electromagnetic field flux produced by a signal emitted by the examination object's relaxing nuclei is picked up by said at least one circuit and is fed to said RF signal receiver, when said switch system is in the second switching position.
28. The antenna system of claim 27, wherein: said at least one circuit comprises at least a first capacitance connected in parallel with said inductance coil, and wherein at least said first capacitance is used for frequency tuning of the antenna system at least during transmission; and said switch system includes at least one first switching element coupling said at least one circuit to said RF signal transmitter output in said first switching position and decoupling said at least one circuit from said RF signal transmitter output in said second switching position.
29. The antenna system of claim 28, wherein said first capacitance comprises a variable capacitor element.
30. The antenna system of claim 28, wherein: said at least one circuit further comprises a second capacitance, said second capacitance comprising a variable capacitance element coupled to said inductance coil for frequency tuning at least during reception when said switch system is in the second switching position; and said switch system includes a second switching element coupled to selectively effectively short out at least said variable capacitance element and said RF receiver input, and for thereby electrically removing at least said variable capacitance element and said RF receiver input from said at least one circuit when said switch system is in the first switching position, and said second switching element being electrically open and having substantially no electrical effect when said switch system is in said second switching position.
31. A method of operating an antenna system in a nuclear magnetic resonance or magnetic resonance imaging apparatus which includes a radio frequency (RF) signal transmitter and a radio frequency (RF) signal receiver, the method comprising: providing at least one circuit including an inductance coil, for producing an electromagnetic field flux vector; and switching said at least one circuit with a switch system such that: when said switch system is in a first switching position, said at least one circuit is coupled to an output of said RF signal transmitter, and a damaging level of signal from said at least one circuit is prevented from being fed to an input of said RF signal receiver, and when said switch system is in a second switching position, an RF signal from said at least one circuit is fed to an input of said RF signal receiver and said at least one circuit is decoupled from an output of said RF signal transmitter; and wherein: said antenna system produces an electromagnetic field flux enclosing an examination object therewithin, which electromagnetic field flux is used to irradiate the examination object, when said switch system is in the first switching position; and an electromagnetic field flux produced by a signal emitted by the examination object's relaxing nuclei is picked up by said at least one circuit and is fed to said RF signal receiver when said switch system is in the second switching position.
32. The method of claim 31, comprising frequency tuning the antenna system with a capacitance coupled to said inductance coil.
33. The method of claim 32, wherein said capacitance comprises a variable capacitance for frequency tuning the antenna system.
34. The method of claim 32, comprising maintaining said antenna system tuned to the object's Larmor frequency when said switch system is in said first switching position.
35. The method of claim 32, wherein said antenna system is tuned to the object's Larmor frequency when said switch system is in said second switching position.
PCT/US1997/009420 1996-06-03 1997-05-29 Antenna system for nmr and mri apparatus WO1997046895A1 (en)

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JP10500734A JP2000514670A (en) 1996-06-03 1997-05-29 Antenna system for NMR and MRI equipment
BR9709291A BR9709291A (en) 1996-06-03 1997-05-29 Antenna systems and process for operating an antenna system
AU31519/97A AU3151997A (en) 1996-06-03 1997-05-29 Antenna system for nmr and mri apparatus
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Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2012005620A1 (en) * 2010-07-08 2012-01-12 Korotkov Konstantin Georgievich Device for measuring electromagnetic field intensity
WO2021247704A1 (en) * 2020-06-05 2021-12-09 Baker Hughes Oilfield Operations Llc Control of transmitting and receiving antenna properties to reduce electromagnetic coupling

Families Citing this family (45)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5939883A (en) * 1996-07-17 1999-08-17 Fonar Corporation Magnetic resonance imaging excitation and reception methods and apparatus
WO2000050867A2 (en) * 1999-02-22 2000-08-31 Paul Bryant Programmable active microwave ultrafine resonance spectrometer (pamurs) method and systems
US6414488B1 (en) * 2000-03-01 2002-07-02 Koninklijke Philips Electronics N.V. Method and apparatus for decoupling magnetic resonance receive coils
US20030169169A1 (en) * 2000-08-17 2003-09-11 Luc Wuidart Antenna generating an electromagnetic field for transponder
US6552544B2 (en) * 2001-04-05 2003-04-22 Varian, Inc. Detunable coil assembly and method of detuning RF coil for MRI
DE10126338A1 (en) * 2001-05-30 2002-12-12 Siemens Ag High frequency coil arrangement for an NMR imaging device in which both surface and circumferential coils receive the same polarization component
AU2003223429A1 (en) * 2002-04-05 2003-10-27 University Of Rochester Cryogenically cooled phased array rf receiver coil for magnetic resonance imaging
GB0209756D0 (en) 2002-04-29 2002-06-05 Imp College Innovations Ltd Magnetic resonance imaging receive circuit
DE10244173B4 (en) * 2002-09-23 2005-11-03 Siemens Ag Antenna arrangement for a magnetic resonance apparatus, magnetic resonance antenna system, magnetic resonance apparatus and method for coupling two antenna groups
DE10314215B4 (en) * 2003-03-28 2006-11-16 Siemens Ag Magnetic resonance antenna and method for detuning their natural resonance frequency
EP2240792B1 (en) * 2005-03-10 2013-08-21 The University Of Queensland Phased array coil for mri
DE102006029195A1 (en) * 2006-06-26 2008-01-03 Siemens Audiologische Technik Gmbh Transceiver circuit with PIN diodes
CN100495074C (en) * 2006-10-08 2009-06-03 吉林大学 Nuclear magnetic resonance and transient electromagnetic combined instrument and method
DE102006050069B4 (en) * 2006-10-24 2011-07-07 Siemens AG, 80333 Birdcage resonator with coupling rings in addition to the end rings
CN101688906B (en) * 2007-06-19 2013-07-17 皇家飞利浦电子股份有限公司 MRI radio frequency receiver
DE102007047020B4 (en) * 2007-10-01 2012-07-12 Siemens Ag Arrangement for transmitting magnetic resonance signals
EP2414859B1 (en) * 2009-04-02 2019-06-12 Koninklijke Philips N.V. Devices and cabling for use in a multi-resonant magnetic resonance system
US20110136444A1 (en) * 2009-12-09 2011-06-09 Mark Rhodes Transmit and receive antenna
US8542017B2 (en) * 2009-12-21 2013-09-24 Nxp B.V. System and method for measuring the shape of an organ of a patient using a magnetic induction radio sensor integrated in a stretchable strap
US8854042B2 (en) * 2010-08-05 2014-10-07 Life Services, LLC Method and coils for human whole-body imaging at 7 T
WO2012088670A1 (en) * 2010-12-29 2012-07-05 海能达通信股份有限公司 Radio frequency bandpass filter circuit
US8723518B2 (en) 2011-03-18 2014-05-13 Nicole SEIBERLICH Nuclear magnetic resonance (NMR) fingerprinting
US10627468B2 (en) * 2011-03-18 2020-04-21 Case Western Reserve University Nuclear magnetic resonance (NMR) fingerprinting
CN103257331B (en) * 2012-02-16 2016-03-02 上海联影医疗科技有限公司 A kind of double-frequency radio-frequency coil
DE102012206066A1 (en) * 2012-04-13 2013-10-17 Siemens Aktiengesellschaft Detection of unmated local coils in a magnetic resonance tomograph
DE102012209754B4 (en) * 2012-06-12 2016-09-22 Siemens Healthcare Gmbh Coil device for a magnetic resonance tomograph
CN109969007A (en) * 2012-10-19 2019-07-05 韦特里西提公司 External analyte detection in wireless energy transfer system
JP6349320B2 (en) * 2012-11-05 2018-06-27 コーニンクレッカ フィリップス エヌ ヴェKoninklijke Philips N.V. Transmission / reception switching circuit with improved radio frequency separation
DE102013003836A1 (en) * 2012-11-14 2014-05-15 Krohne Ag Measuring system for nuclear magnetic measuring instruments
DE102013006305B4 (en) * 2013-03-19 2015-02-19 Krohne Ag Signal analyzer, in particular for nuclear magnetic flowmeters
US9851420B2 (en) * 2013-08-09 2017-12-26 Schlumberger Technology Corporation Magnetic resonance transmitter
CN107771290B (en) * 2015-04-15 2021-11-05 日本电子株式会社 Magnetically coupled high resolution nuclear magnetic resolution probe and method of use
DE102016214441B3 (en) * 2016-08-04 2017-11-30 Bruker Biospin Gmbh High-frequency interface circuit, high-frequency system and magnetic resonance apparatus with a high-frequency interface circuit
US10386430B2 (en) * 2016-09-21 2019-08-20 Quality Electrodynamics, Llc Single layer magnetic resonance imaging transmit/receive radio frequency coil
US10852373B2 (en) * 2016-09-21 2020-12-01 Quality Electrodynamics, Llc Modulating magnetic resonance imaging transmit field in magnetic resonance fingerprinting using single layer transmit/receive radio frequency coil
US10347973B2 (en) * 2017-02-21 2019-07-09 Nxp B.V. Near-field electromagnetic induction (NFEMI) antenna
US11156682B2 (en) 2017-03-24 2021-10-26 Quality Electrodynamics, Llc Single layer magnetic resonance imaging transmit/receive radio frequency coil for different anatomies
US10976388B2 (en) 2017-03-24 2021-04-13 Quality Electrodynamics, Llc Minimizing intravascular magnetic resonance imaging (MRI) guidewire heating with single layer MRI transmit/receive radio frequency coil
US10649048B2 (en) 2017-04-28 2020-05-12 Quality Electrodynamics, Llc Single layer magnetic resonance imaging (MRI) transmit/receive (TX/RX) radio frequency (RF) coil with integrated shimming
US11193992B2 (en) 2017-05-05 2021-12-07 Quality Electrodynamics, Llc Single layer magnetic resonance imaging (MRI) transmit/receive (Tx/Rx) radio frequency (RF) coil with induced current failsafe protection
US10838028B2 (en) 2017-06-19 2020-11-17 Quality Electrodynamics, Llc Decoupling magnetic resonance imaging (MRI) radio frequency (RF) coil elements with high acceleration factor in parallel transmit (pTx) or receive (Rx) coils using fewer channels
DE102017115807B3 (en) 2017-07-13 2018-08-16 Krohne Ag Nuclear magnetic measuring device
AU2019272580A1 (en) * 2018-05-21 2020-11-12 Hyperfine Operations, Inc. Radio-frequency coil signal chain for a low-field MRI system
GB2580011B (en) * 2018-08-03 2021-11-24 Medical Wireless Sensing Ltd Tunable metamaterial device
CN109444970B (en) * 2019-01-11 2020-06-16 中国科学院成都生物研究所 Ground detection electromagnetic spectrum receiving and transmitting method utilizing visual perception control

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5202634A (en) * 1990-09-29 1993-04-13 Siemens Aktiengesellschaft Double surface coil for a nuclear magnetic resonance apparatus
US5317266A (en) * 1991-11-22 1994-05-31 Siemens Aktiengesellschaft Local antenna with homogeneous sensitivity for a nuclear magnetic resonance imaging apparatus

Family Cites Families (20)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4901022A (en) * 1988-01-05 1990-02-13 Elscint, Ltd. Broadband matching and decoupling network
DE3816831A1 (en) * 1988-05-18 1989-11-30 Philips Patentverwaltung CORE SPIN EXAMINATION DEVICE WITH A HIGH-FREQUENCY COIL ARRANGEMENT
JP2647139B2 (en) * 1988-05-24 1997-08-27 株式会社東芝 Probe head for magnetic resonance equipment
US4975644A (en) * 1989-03-29 1990-12-04 Kabushiki Kaisha Toshiba Coil system for a magnetic resonance imaging system
US5583438A (en) * 1989-04-12 1996-12-10 Fonar Corporation Inductively coupled dedicated RF coils for MRI
US5050605A (en) * 1989-04-12 1991-09-24 Fonar Corporation Magnetic resonance imaging antennas with spiral coils and imaging methods employing the same
DE9012639U1 (en) * 1989-09-18 1990-10-31 Siemens Ag, 8000 Muenchen, De
FI83819C (en) * 1989-11-27 1991-08-26 Instrumentarium Oy SPOL- OCH KOPPLINGSARRANGEMANG.
US5256972A (en) * 1990-01-30 1993-10-26 Elscint, Ltd. Body coil decoupling circuit
US5216367A (en) * 1990-02-21 1993-06-01 Kabushiki Kaisha Toshiba MR imaging apparatus capable of automatically selecting multiple surface coils
US5206639A (en) * 1990-10-25 1993-04-27 Timex Corporation Single antenna dual frequency transponder
US5166617A (en) * 1991-01-11 1992-11-24 Varian Associates, Inc. High power NMR probe
US5321412A (en) * 1991-05-13 1994-06-14 Sensormatic Electronics Corporation Antenna arrangement with reduced coupling between transmit antenna and receive antenna
US5585721A (en) * 1991-06-24 1996-12-17 Fonar Corporation Inductively coupled dedicated RF coils for MRI
US5302901A (en) * 1991-08-26 1994-04-12 U.S. Philips Corporation Magnetic resonance apparatus comprising decoupled receiver coils
US5453692A (en) * 1992-08-06 1995-09-26 Hitachi, Ltd. RF probe for nuclear magnetic resonance imaging (MRI) devices
DE4238831A1 (en) * 1992-11-17 1994-05-19 Siemens Ag HF arrangement for NMR tomography appts - includes surface coil inductively coupled to HF transmission antenna, and electronic switch for damping
US5329233A (en) * 1992-12-10 1994-07-12 General Electric Company Cylindrical local coil for nuclear magnetic resonance imaging
JP3216938B2 (en) * 1993-06-08 2001-10-09 株式会社日立製作所 RF probe for MRI and magnetic resonance imaging apparatus
DE4322352C2 (en) * 1993-07-05 1996-09-05 Siemens Ag High-frequency system of a magnetic resonance imaging system with a galvanically decoupled local coil device

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5202634A (en) * 1990-09-29 1993-04-13 Siemens Aktiengesellschaft Double surface coil for a nuclear magnetic resonance apparatus
US5317266A (en) * 1991-11-22 1994-05-31 Siemens Aktiengesellschaft Local antenna with homogeneous sensitivity for a nuclear magnetic resonance imaging apparatus

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2012005620A1 (en) * 2010-07-08 2012-01-12 Korotkov Konstantin Georgievich Device for measuring electromagnetic field intensity
US9075093B2 (en) 2010-07-08 2015-07-07 Konstantin G. Korotkov Device for measuring electromagnetic field intensity
WO2021247704A1 (en) * 2020-06-05 2021-12-09 Baker Hughes Oilfield Operations Llc Control of transmitting and receiving antenna properties to reduce electromagnetic coupling
GB2611226A (en) * 2020-06-05 2023-03-29 Baker Hughes Oilfield Operations Llc Control of transmitting and receiving antenna properties to reduce electromagnetic coupling

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