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United States Patent 5,339,032
Konishi August 16, 1994
Magnetic resonance imaging apparatus

Abstract

In a magnetic resonance imaging apparatus, a radiofrequency shielding body, which is disposed between the gradient magnetic field generating coils and the radio-frequency coil for interrupting electromagnetic coupling between the gradient magnetic field generating coils and the radio-frequency coil due to the radio-frequency pulse applied to the radio-frequency coil, is formed of a conductive material having a thickness less than the skin depth defined by 1/.sqroot. .pi. fo .mu. .sigma. where .pi. stands for the ratio of the circumference of a circle to its diameter, of stands for the Larmor frequency of atomic nuclei of an imaging object, .mu. stands for the conductivity of the conductive material and .sigma. stands for the magnetic permeability of the conductive material.

Inventors: Konishi; Mineyuki (Ootawara, JP)
Assignee: Kabushiki Kaisha Toshiba (Kawasaki, JP)
Appl. No.: 618386
Filed: November 27, 1990
Foreign Application Priority Data
Nov 28, 1989[JP]1-308547

Intern'l Class: G01V 003/00
Field of Search: 324/300,318,322,307,319 336/84 C,84 M,84 R

References Cited
U.S. Patent Documents
4642569Feb., 1987Hayes et al.324/318.
4871969Oct., 1989Roemer et al.324/300.
4879515Nov., 1989Roemer et al.324/318.
4924184May., 1990Yoda324/318.
4980641Dec., 1990Breneman et al.324/318.
Foreign Patent Documents
0151726Aug., 1985EP.
3445724Jun., 1985DE.
3621107Jan., 1987DE.
63-290554Nov., 1988JP.

Primary Examiner: Arana; Louis
Attorney, Agent or Firm: Limbach & Limbach
Claims


What is claimed is:

1. In a magnetic resonance imaging apparatus comprising:

static magnetic field generating means for generating a static magnetic field along the direction of a first axis;

gradient magnetic field generating coil means for generating gradient magnetic fields along the direction of said first axis and the directions of second and third axes orthogonal to said first axis;

a radio-frequency coil means for transmitting or receiving electromagnetic waves from a direction other than the direction of said first axis; and

a radio-frequency shielding body disposed between said gradient magnetic field generating coil means and said radio-frequency coil means and having a thickness along the directions of said second and third axes,

the improvement wherein said radio-frequency shielding body is formed of a conductive material having a thickness less than approximately 1/.sqroot. .pi. fo .sigma. .mu.

where: .pi. is a constant equal to the ratio of the circumference of a circle to its diameter;

fo is the Larmor frequency of the atomic nuclei of an imaging object;

.sigma. is the conductivity of the conductive material; and

.mu. is the magnetic permeability of the conductive material; and is arranged to interrupt electromagnetic coupling between said gradient magnetic field generating coil means and said radio-frequency coil means resulting from a radio-frequency pulse applied to said radio-frequency coil means and reduce a time constant of eddy currents generated in the surface of said gradient magnetic field coil means.

2. A magnetic resonance imaging apparatus according to claim 1, in which said radio-frequency shielding body is disposed close to the radio-frequency coil side of said gradient magnetic field generating coil means.

3. A magnetic resonance imaging apparatus according to claim 2, in which said radio-frequency shielding body has a shape similar to that of said gradient magnetic field generating coil means.

4. A magnetic resonance imaging apparatus according to claim 1, in which said radio-frequency shielding body has a sectional structure in which a conductive layer is formed on a sheet of insulating material.

5. A magnetic resonance imaging apparatus according to claim 1, in which said radio-frequency shielding body has a sectional structure in which an organic fiber textile is plated with a metal.

6. A magnetic resonance imaging apparatus according to claim 5, in which said organic fiber is made of polyester.

7. A magnetic resonance imaging apparatus according to claim 5, in which said metal is copper.

8. A magnetic resonance imaging apparatus according to claim 1, in which said radio-frequency coil means is a whole-body transmit and receive coil which is disposed coaxially with said gradient magnetic field generating coil means.

9. A magnetic resonance imaging apparatus according to claim 1, in which said radio-frequency coil means is a transmit and/or receive coil which is disposed inside said gradient magnetic field coil means with a space between them.

10. A magnetic resonance imaging apparatus according to claim 1, in which said radio-frequency coil means comprises a whole-body transmit and receive coil which is disposed coaxially with said gradient magnetic field generating coil means and a transmit and/or receive coil which is disposed inside said gradient magnetic field coil means with a space between them.

11. A magnetic resonance imaging apparatus according to claim 1, in which said static magnetic field generating means comprises an electromagnet for generating a static magnetic field horizontally.

12. A magnetic resonance imaging apparatus according to claim 1, in which said static magnetic field generating means comprises an electromagnet for generating a static magnetic field vertically.

13. A magnetic resonance imaging apparatus according to claim 1, in which said static magnetic field generating means comprises a permanent magnet for generating a static magnetic field horizontally.

14. A magnetic resonance imaging apparatus according to claim 1, in which said static magnetic field generating means comprises a permanent magnet for generating a static magnetic field vertically.

15. In a magnetic resonance imaging apparatus comprising a static magnetic field generating coil for generating a static magnetic field which is applied to a subject under examination, gradient magnetic field generating coils for generating gradient magnetic fields used to obtain information on the position of a body portion of the subject in which magnetic resonance signals are induced, a radio-frequency coil responsive to application of a radio-frequency pulse thereto for transmitting a radio-frequency magnetic field adapted to induce the magnetic resonance signals and for detecting the induced magnetic resonance signals and a radio-frequency shielding body disposed between said gradient magnetic field generating coils and said radio-frequency coil for interrupting electromagnetic coupling between said gradient magnetic field generating coils and said radio-frequency coil due to said radio-frequency pulse applied to said radio-frequency coil,

the improvement wherein said radio-frequency shielding body is formed of a conductive material having a thickness less than the skin depth defined by 1/.sqroot. .pi. fo .sigma. .mu. where .pi. stands for the ratio of the circumference of a circle to its diameter, fo stands for the Lamor frequency of atomic nuclei of an imaging object, .sigma. stands for the conductivity of said conductive material and .mu. stands for the magnetic permeability of said conductive material.
Description


BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to a magnetic resonance imaging apparatus employing nuclear magnetic resonance (NMR) phenomena and, more particularly, to a magnetic resonance imaging apparatus with an improved radio-frequency shielding body.

2. Description of the Related Art

The nuclear magnetic resonance is a phenomenon in which atomic nuclei placed in magnetic fields absorb electromagnetic energy at specific frequencies and then emit the energy as electromagnetic waves. A diagnostic apparatus employing the phenomenon senses electromagnetic waves emitted by the atomic nuclei, protons in particular, and processes received signals to obtain diagnostic information of a subject under examination, such as a tomographic image, which contains the atomic nucleus density (the proton density in particular), the longitudinal spin-lattice relaxation time T1, the transversal spin-lattice relaxation time T2, flow, chemical shifts and so on.

The magnetic resonance imaging apparatus for obtaining cross-sectional NMR images of a subject under examination is provided with gradient magnetic field forming coils for forming gradient magnetic fields which serve to obtain position information of a body portion in which magnetic resonance signals are induced and a radio-frequency coil responsive to application of a radio-frequency pulse thereto for radiating a radio-frequency magnetic field serving to induce the magnetic resonance signals in the body portion and detecting the induced magnetic resonance signals. Between the gradient magnetic field forming coils and the radio-frequency coil is disposed a radio-frequency shielding body for interrupting electromagnetic coupling between the gradient magnetic field forming coils and the radio-frequency coil due to the radio-frequency pulse applied to the radio-frequency coil.

The radio-frequency shielding body is generally formed of metallic foil made of a good conductor such as copper. However, eddy currents will be induced in the surface of the radio-frequency shielding body by time-varying gradient magnetic fields formed by the gradient magnetic field forming coils. A problem arises due to the eddy currents in that the rising and falling characteristics of the gradient magnetic fields are deteriorated. As a result, resulting cross-sectional NMR images will have poor quality.

In order to solve the problem with the radio-frequency shielding body, an approach has been proposed in Japanese Unexamined Patent Publication No. 60-177249 according to which metallic foil consisting of first and second conductive regions separated by a relatively narrow nonconductive region, such as a slit, is used to form the radio-frequency shielding body.

Other techniques have been proposed in Japanese Unexamined Patent Publication No. 62-334. That is to say, a metal cylinder, which forms a radio-frequency shielding body, is provided with a lengthwise slit so as to decrease eddy currents by confining them locally or a metal cylinder is formed of plural pieces of metallic foil connected by insulating materials or dielectric materials so as to reduce impedance of a radio-frequency shielding body to a radio-frequency pulse and to thereby reduce undesirable electromagnetic coupling between the gradient magnetic field coils and the radio-frequency coil.

However, such a radio-frequency shielding body is complex in structure and costly because of the provision of the metallic foil with a slit or interposition of a insulating material or dielectric material between pieces of metallic foil.

According to still another proposal in Japanese Unexamined Patent Publication No. 63-290554, the radio-frequency shielding body is formed of a metal cylinder made of copper foil having a thickens not less than the skin depth. The skin depth is the depth in the direction to the center of the cylinder at which the amplitude of electromagnetic waves decays to 1/e (e=2.718 . . , the base of the natural logarithm). More specifically, when electromagnetic waves with the Larmor frequency of protons penetrate into a cylinder made of some metal by a depth of .delta. in the direction to the center of the cylinder, if the amplitude of all the electromagnetic waves decays to 1/e at the depth .delta., then the skin depth is defined as .delta..

In the case of a radio-frequency shielding body with a thickness less than the skin depth, the time constant of eddy currents can be made small so that the time it takes for eddy currents to dissipate is effectively shortened. However, the technique disclosed in the Publication, which is directed to a radio-frequency shielding body made of a metal cylinder, implies that it is impossible to make a radio-frequency shielding body having a thickness less than the skin depth.

As described above, the conventional radio-frequency shielding bodies are complex in structure and costly.

SUMMARY OF THE INVENTION

It is therefore an object of the present invention to provide a magnetic resonance imaging apparatus which is provided with a radio-frequency shielding body which is simple in construction and sufficiently interrupts electromagnetic coupling between gradient magnetic field forming coils and a radio-frequency coil due to a radio-frequency pulse applied to the radio-frequency coil so as not to deteriorate the rising and falling characteristics of gradient magnetic fields.

The object of the present invention is attained by the following magnetic resonance imaging apparatus.

In a magnetic resonance imaging apparatus comprising:

static magnetic field generating means for generating a static magnetic field along the direction of a first axis;

gradient magnetic field generating coil means for generating gradient magnetic fields along the direction of said first axis and the directions of second and third axes orthogonal to said first axis;

a radio-frequency coil means for transmitting or receiving electromagnetic waves from a direction other than the direction of said first axis; and

a radio-frequency shielding body disposed between said gradient magnetic field generating coil means and said radio-frequency coil means and having a thickness along the directions of said second and third axes,

the improvement wherein said radio-frequency shielding body being arranged to interrupt electromagnetic coupling between said gradient magnetic field generating coil means and said radio-frequency coil means resulting from a radio-frequency pulse applied to said radio-frequency coil means and reduce a time constant of eddy currents generated in the surface of said gradient magnetic field coil means.

Also, the object of the present invention is attained by the following magnetic resonance imaging apparatus.

In a magnetic resonance imaging apparatus comprising a static magnetic field generating coil for generating a static magnetic field which is applied to a subject under examination, gradient magnetic field generating coils for generating gradient magnetic fields used to obtain information on the position of a body portion of the subject in which magnetic resonance signals are induced, a radio-frequency coil responsive to application of a radio-frequency pulse thereto for transmitting a radio-frequency magnetic field adapted to induce the magnetic resonance signals and for detecting the induced magnetic resonance signals and a radio-frequency shielding body disposed between said gradient magnetic field generating coils and said radio-frequency coil for interrupting electromagnetic coupling between said gradient magnetic field generating coils and said radio-frequency coil due to said radio-frequency pulse applied to said radio-frequency coil,

the improvement wherein said radio-frequency shielding body is formed of a conductive material having a thickness less than the skin depth defined by 1/.sqroot. .pi. fo .mu. .sigma. where .pi. stands for the ratio of the circumference of a circle to its diameter, of stands for the Larmor frequency of atomic nuclei of an imaging object, .sigma. stands for the conductivity of said conductive material and .mu. stands for the magnetic permeability of said conductive material.

With the magnetic resonance imaging apparatus of the present invention, since the radio-frequency shielding body is formed of a conductive material having a thickness less than 1/.sqroot. .pi. fo .mu. .sigma. the time constant of eddy currents induced in the surface of the radio-frequency shielding body in accordance with variations in the gradient magnetic fields with time can be made small and thus the eddy currents decay quickly. As a result, the rising and falling characteristics of the gradient magnetic fields will become abrupt, whereby good tomographic images are obtained. More specifically, the time constant of the eddy currents induced in the radio-frequency shielding body is in inverse proportion to the resistance of the radio-frequency shielding body, while the resistance is in proportion to the thickness of the radio-frequency shielding body. Therefore, the time constant of the eddy currents can be made small by decreasing the thickness of the radio-frequency shielding body.

Additional objects and advantages of the invention will be set forth in the description which follows, and in part will be obvious from the description, or may be learned by practice of the invention. The objects and advantages of the invention may be realized and obtained by means of the instrumentalities and combinations particularly pointed out in the appended claims.

BRIEF DESCRIPTION OF THE DRAWINGS

The accompanying drawings, which are incorporated in and constitute a part of the specification, illustrate presently preferred embodiments of the invention, and together with the general description given above and the detailed description of the preferred embodiments given below, serve to explain the principles of the invention.

FIG. 1 is a diagrammatic representation of a magnetic resonance imaging apparatus of the present invention;

FIG. 2 is a cross-sectional view illustrating a radio-frequency shielding coil of the present invention;

FIG. 3 is a sectional view taken along the line III--III of FIG. 2;

FIG. 4 is a sectional view of a radio-frequency shielding body according to another embodiment of the present invention; and

FIG. 5 is a sectional view of a radio-frequency shielding body according to still another embodiment of the present invention.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

Hereinafter the embodiments of the present invention will be described with reference to the drawings. FIG. 1 is a graphical representation of a nuclear magnetic resonance imaging apparatus embodying the present invention.

As illustrated in FIG. 1, the magnetic resonance imaging apparatus, which is generally indicated at 10, includes gradient magnetic field forming coils 12 for forming gradient magnetic fields adapted to acquire information on the position of a body portion of a subject under examination 100 in which magnetic resonance signals are induced and a radio-frequency coil 13 responsive to application of a radio-frequency pulse thereto for radiating to the subject a radio-frequency magnetic field adapted to induce the magnetic resonance signals and for detecting the induced magnetic resonance signals. More specifically, with the lengthwise axis of the subject under examination 100 taken as the Z axis and the axes orthogonal to the Z axis taken as the X and Y axes, the gradient magnetic field forming coils 12 comprise a X-axis gradient magnetic field forming coil 12a for forming a gradient magnetic field in the X-axis direction, a Y-axis gradient magnetic field forming coil 12b for forming a gradient magnetic field in the Y-axis direction and a Z-axis gradient magnetic field forming coil 12c for forming a gradient magnetic field in the Z-axis direction. The gradient magnetic field forming coils 12a, 12b and 12c are connected to an X-axis gradient magnetic field power supply 14a, a Y-axis gradient magnetic field power supply 14b and a Z-axis gradient magnetic field power supply 14c, respectively. The radio-frequency coil 13 is connected to a transmit circuit system 15 and a receive circuit system 16.

The apparatus 10 is further provided with a sequencer 17 for practicing an imaging pulse sequence and a computer system 18 for controlling all of the power supplies 14a, 14b and 14c, the transmit circuit system 15, the receive circuit system 16 and the sequencer and processing the detected NMR signals. Signals processed by the computer system 18 are displayed on a display 19. The apparatus is provided with a static magnetic field forming coil (refer to FIG. 2) for applying a static magnetic field to the subject 100 in the Z-axis direction and a power supply (not shown) for supplying the static magnetic field forming coil with current as well.

As illustrated in FIG. 2, on the inside of the gradient magnetic field forming coils 12 of the apparatus 10 is mounted a cylindrical radio-frequency shielding body 20 adapted for interrupting electromagnetic coupling between the gradient magnetic field forming coils 12 and the radio-frequency coil 13 due to a radio-frequency pulse applied to the radio-frequency coil 13. In FIG. 2, like reference numerals are used to designate corresponding parts to those in FIG. 1. Reference numeral 21 designates the static magnetic field coil adapted to form a static magnetic field along the Z-axis direction of the subject 100 of FIG. 1.

The radio-frequency shielding body 20 for use in the apparatus consists of copper-plated metal which is about 10 .mu.m in thickness and formed on the surface of a base consisting of an organic fiber textile made of, for example, polyester cloth. Since the radio-frequency shielding body 20 is thinner than the skin depth of 30 .mu.m which is represented by 1/.sqroot. .pi. of .mu. .sigma. (where fo=63.874 MHz, the Larmor frequency of protons), the rising and falling characteristics of the gradient magnetic field forming coils 12 will not be deteriorated.

As illustrated in FIG. 3, the radio-frequency shielding body 20 consists of copper layers 20B1 and 20B2 plated on both sides of a base 20A. This structure permits the radio-frequency shielding body 20 of a thickness less than the skin depth to be obtained.

Besides the above embodiment, the radio-frequency shielding body may be formed of a conductive layer formed on the surface of a sheet of insulating material. Also, an evaporated film may be used as the radio-frequency shielding body. In addition, it is desirable that the radio-frequency shielding body 20 have a thickness from 5 to 10 .mu.m which can be manufactured.

Next, another embodiment of the magnetic resonance imaging apparatus of the present invention will be described with reference to FIG. 4. The apparatus shown in FIG. 4 includes a transversal magnetic field forming electromagnet 30 for use as the static magnetic field forming device. As the transversal magnetic field forming electromagnet 30 a desired one may be selected from among various types of electromagnets such as a solenoid coil type magnet, a solenoid coil type superconducting magnet, a Helmholtz type electromagnet, etc. The electromagnet 30 has cylindrical space therein. A static magnetic field Bo is produced in the cylindrical space. A cylindrical gradient magnetic field forming coil 12 is disposed in the cylindrical space. A whole-body transmit and receive radio-frequency coil 31 is disposed inside the cylindrical gradient magnetic field coil 12. Furthermore, a radio-frequency shielding body 32 formed in the shape of a cylinder is disposed between the cylindrical gradient magnetic field coil 12 and the whole-body transmit and receive radio-frequency coil 31. This radio-frequency shielding body 32 is substantially the same as that illustrated in FIG. 2.

Next, still another embodiment of the magnetic resonance imaging apparatus of the present invention will be described with reference to FIG. 5. The apparatus shown in FIG. 5 includes a longitudinal magnetic field forming magnet 40 as the static magnetic field forming device. As the magnet 40 a desired one may be selected from among various types of magnets such as a permanent magnet, an ordinary electromagnet, a superconducting magnet, etc. The magnet 40 has first and second magnetic poles 41 and 42 which face each other and are attached to a yoke 40A. A static magnetic field Bo is formed in the space between the first and second magnetic poles 41 and 42. A gradient magnetic field coil 43 is disposed in the space between the first and second magnetic poles. A whole-body transmit and receive radio-frequency coil 44 is disposed inside the gradient magnetic field coil 43. Furthermore, a radio-frequency shielding body 45 formed in the shape of a cylinder is disposed between the gradient magnetic field coil 43 and the whole-body transmit and receive radio-frequency coil 44. This radio-frequency shielding body 45 is substantially the same as that illustrated in FIG. 2.

As can be seen from the foregoing, according to the present invention, a magnetic resonance imaging apparatus can be provided which is provided with a radio-frequency shielding body that is simple in construction and permits electromagnetic coupling between a gradient magnetic field coil and a radio-frequency coil due to a radio-frequency pulse applied to the radio-frequency coil to be interrupted sufficiently so as not to deteriorate the rising and falling characteristics of gradient magnetic fields.

Additional advantages and modifications will readily occur to those skilled in the art. Therefore, the invention in its broader aspects is not limited to the specific details, and representative devices, shown and described herein. Accordingly, various modifications may be without departing from the spirit or scope of the general inventive concept as defined by the appended claims and their equivalents.

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