The present invention relates to an apparatus for measuring the neuro-magnetic field generated around a human head by the current flowing in the nerves of the brain when it works, approximately one hundred million times as small as the magnetic field of the earth, and a method for operating the same.
A SQUID (Superconducting Quantum Interference Device) immersed in a liquid helium bath can work as a sensor for magnetic fields at a very low temperature to detect such a weak magnetic field. Thus, the observation of the dynamics of the neural network of the brain is enabled. So, diagnosis can be made of the function of the brain (such as memory, learning, attention and other mental acts) and of some brain disorders (attention deficit hyperactivity disorder, learning disabilities, autism or schizophrenia).
The present inventor developed a low temperature type system of neuro-magnetic field sensors in which a SQUID can be used while being immersed in a liquid helium bath. The instrument has been practically used.
Referring to
The lower part of the liquid-Helium dewar 13 defines a head accommodating area 131 to accommodate the head of a patient under inspection. The liquid-Helium dewar 13 has a plurality of SQUID magnetic sensors 15 therein. The SQUID magnetic sensors 15 are fixedly arranged on a support block 20 around the head accommodating area 131. The liquid-Helium dewar 13 is filled with liquid Helium of cryogenic temperature.
The vacuum structure 11 for thermal insulation is supported by the horizontal shafts on the four legs. It has a non-magnetic chair 17 placed in its lower opening. The top cover 14 of magnetic material is put on the top of the vacuum structure 11 for thermal insulation, effectively preventing invasion both of the geomagnetism and the electromagnetic wave from the top.
The conventional MEG apparatus is described in the following documents: (Patent Document)
Patent Application Public Disclosure No. 10-313135; and (Non-Patent Document)
“Whole-Head-Type SQUID System in a Superconducting Magnetic Shield of High Critical-Temperature Superconductor”, by Hiroshi Ohta, “Ceramics 35” (2000), No. 2. Extra Edition. Titled “Brain and Ceramics; Ceramics Useful in Illustrating the Functions of the Brain, Making the Diagnosis of the Brain Disorders and Carrying out Required Treatments”, and
“Nanometer SNS Junctions and Their Application to SQUIDs”, by Hiroshi Ohta et al, “PHISICA C” 352 (2001), p.p. 186-190
Conventionally it is used to be necessary that the SQUID (MEG) system be completely isolated from the floor of a building to avoid mechanical vibrations. The complete isolation of the SQUID (MagnetoEncephaloGraphy or MEG) system from any mechanical vibrations requires rigid floors of the building usually. Also, an optimum installation site should be chosen to avoid mechanical vibrations from the surroundings such as traffic of automobiles; if not, the MEG system installed in the existing building could not be of practical use. When a building which a MEG system is to be installed in is constructed, the solid underground base of the building needs to be rigid and strong enough to shut off any mechanical vibrations from the surroundings, and accordingly the required foundation work takes much money to build.
Referring to
One object of the present invention is to provide a noise-free MEG apparatus of high-sensitivity. Another object of the present invention is to provide a method of putting such MEG apparatus in operation.
To attain this object, a noise-free MEG system of high-sensitivity according to the present invention is designed to completely isolate the apparatus from the floor on which it is placed in respect of mechanical vibrations, thereby assuring that the apparatus be guaranteed to be free of excursion to the disturbed positions as described with reference to
Also, to attain the above object the magnetic sensors are fastened so as to eliminate any relative displacement between the magnetic sensors and the first cylinder of critical temperature superconductor material, thereby assuring that the magnetic sensors be prevented from traversing across the stationary magnetic fluxes trapped in the inner space of the vacuum structure for thermal insulation (see
The MEG apparatus equipped with the fastening means just described and the mechanical vibration suppressor support above described allows the magnetic sensors and the vacuum structure for thermal insulation to move as a whole in response to any mechanical vibration force from the floor even though it cannot be suppressed by the mechanical vibration suppressor support, thereby keeping the trapped magnetic field stationary with respect to the magnetic sensors. Thus, no noise signals can appear in the magnetic sensors.
The method of putting the MEG apparatus in operation according to the present invention comprises the steps of:
closing both the top and the bottom openings of the vacuum structure of hollow cylinder for thermal insulation with each magnetic member (thereby preventing invasion of the geomagnetism into the inner space of the vacuum structure for thermal insulation); cooling the first cylinder down to around the liquid nitrogen temperature (thereby preventing trapping of the geomagnetism by the high critical temperature superconductor); filling the liquid-Helium dewar with liquid helium or cooling the liquid-Helium dewar by means of thermal conduction to the cryogenic temperature (thereby preventing trapping of the geomagnetism by SQUID magnetic sensors, and hence preventing the adverse effect on the magnetic sensors for their malfunction); and measuring the neuro-magnetic field by the SQUID magnetic sensors.
Referring to
The lower part of the liquid-Helium dewar 13 defines a head accommodating area 131 to accommodate the head of a patient (the subject under inspection). As seen in the drawing, the liquid-Helium dewar 13 has a plurality of SQUID magnetic sensors 15 therein. The magnetic sensors 15 are fixedly arranged around the head accommodating area 131. A superconducting canopy 132 is arranged above the magnetic sensors 15 in the liquid-Helium dewar 13, which is filled with liquid Helium. The superconducting canopy 132 is made of lead, MgB2 or BSCCO.
The fastening means to prevent the magnetic sensors 15 from moving relative to the first cylinder 111 of high critical temperature superconductor material comprises a first pillow structure 22 to fill the gap between the inner wall of the vacuum structure 11 for thermal insulation and the outer wall of the liquid-Helium dewar 13, and a second pillow structure 21 to fill the gap between the superconducting canopy 132 and the inner wall of the liquid-Helium dewar 13. The second pillow structure 21 is placed next to the lowest end of the liquid-Helium dewar 13. One example of the first pillow structure 22 comprises a pillow 22 and two rails (not shown) laid on the inner wall of the vacuum structure 11 for thermal insulation, so that the pillow 22 can run on the parallel rails with the liquid-Helium dewar 13 laid on when it is pulled up toward the top of the vacuum structure 11 for thermal insulation.
The vacuum structure 11 for thermal insulation is set on the floor via four mechanical vibration-suppressor supports 16 (see
Also, the mechanical vibration-suppressor support 16 includes an up-and-down mechanism 163, which can be conveniently removed when the MEG apparatus (1 ton in weight) is transported.
The top cover 14 is put on the top of the vacuum structure 11 for thermal insulation to effectively prevent invasion of the geomagnetism and the electromagnetic waves from the top. A significant amount of geomagnetic field still invades into the inner space of the vacuum structure 11 for thermal insulation after passing through the top cover 14. A superconducting canopy 132 is placed to protect the SQUID magnetic sensors 15 against the geomagnetic flux which the top cover 14 leaks. In this particular embodiment, the sensor support block 20 has a helmet-like shape to enclose the head of a patient under inspection. The helmet-like shape helps the support block 20 effectively shut off the magnetic field component transverse the axis of the cylinder.
The first pillow structure 22 fills the gap between the inner wall of the vacuum structure 11 for thermal insulation and the outer wall of the liquid-Helium dewar 13, while the second pillow structure 21 fills the gap between the superconducting canopy 132 and the inner wall of the liquid-Helium dewar 13. These pillows 21 and 22 help the liquid-Helium dewar 13 lie stably on the vacuum structure 11 for thermal insulation, thereby preventing any relative displacement between the SQUID magnetic sensors 15 and the first cylinder 111 of high critical temperature superconductor in the vacuum structure 11 for thermal insulation. Thus, even though the least magnitude of mechanical vibration from the floor comes to the MEG apparatus 1, it is assured that the SQUID magnetic sensors 15 and the vacuum structure 11 for thermal insulation (particularly the first cylinder 111) undergo same mechanical vibration (displacement), keeping the static magnetic field in the inner space of the vacuum structure 11 for thermal insulation unchanged relative to the SQUID magnetic sensors 15, and hence causing no noise signals to appear in the magnetic sensors.
The MEG apparatus can be put in operation as follows: First, both of the top and the bottom openings of the vacuum structure 11 for thermal insulation are closed with a magnetic member to prevent invasion of the geomagnetism in the inner space of the vacuum structure 11 for thermal insulation. Then, the first cylinder 111 is cooled down to around the liquid nitrogen temperature (below the superconducting critical temperature, 100 K) by the closed-cycle Helium refrigerator 12, thereby shutting out the surrounding magnetic field. Thus, the SQUID magnetic sensors 15 are guaranteed to be free from being inoperative because of seizures of magnetic flux. The liquid-Helium dewar 13 is filled with liquid helium, letting the SQUID magnetic sensors measure the neuro-magnetic field. As an alternative of the filling of liquid helium the liquid-Helium dewar can be cooled below the superconducting critical temperature by means of thermal conduction.
This is a continuation of prior PCT Patent Application No. PCT/JP2003/000836, filed on Jan. 29, 2003.
Number | Name | Date | Kind |
---|---|---|---|
5081071 | Hirschkoff | Jan 1992 | A |
5406847 | Rowe et al. | Apr 1995 | A |
5418512 | Ohta et al. | May 1995 | A |
6486393 | Matsuba et al. | Nov 2002 | B1 |
6512368 | Tanaka et al. | Jan 2003 | B2 |
7130675 | Ewing et al. | Oct 2006 | B2 |
20020050815 | Suzuki et al. | May 2002 | A1 |
20040002645 | Ewing et al. | Jan 2004 | A1 |
20040049108 | Ardenkjaer-Larsen et al. | Mar 2004 | A1 |
20040106863 | Seki et al. | Jun 2004 | A1 |
20040254443 | Gott et al. | Dec 2004 | A1 |
20050206377 | Romalis et al. | Sep 2005 | A1 |
20080108504 | Matsui et al. | May 2008 | A1 |
Number | Date | Country |
---|---|---|
05-212008 | Aug 1993 | JP |
05-264693 | Oct 1993 | JP |
07-294613 | Nov 1995 | JP |
10-313135 | Nov 1998 | JP |
2001-178695 | Jul 2001 | JP |
2002-315729 | Oct 2002 | JP |
2002-372098 | Dec 2002 | JP |
2003-010142 | Jan 2003 | JP |
WO 2006067828 | Jun 2006 | WO |
Number | Date | Country | |
---|---|---|---|
20050272996 A1 | Dec 2005 | US |
Number | Date | Country | |
---|---|---|---|
Parent | PCT/JP03/000836 | Jan 2003 | US |
Child | 11192514 | US |