WO2005122890A1 - Mr装置用ボリュームコイル - Google Patents
Mr装置用ボリュームコイル Download PDFInfo
- Publication number
- WO2005122890A1 WO2005122890A1 PCT/JP2005/011040 JP2005011040W WO2005122890A1 WO 2005122890 A1 WO2005122890 A1 WO 2005122890A1 JP 2005011040 W JP2005011040 W JP 2005011040W WO 2005122890 A1 WO2005122890 A1 WO 2005122890A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- conductive
- coil
- volume coil
- radio wave
- wave shield
- Prior art date
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R33/00—Arrangements or instruments for measuring magnetic variables
- G01R33/20—Arrangements or instruments for measuring magnetic variables involving magnetic resonance
- G01R33/28—Details of apparatus provided for in groups G01R33/44 - G01R33/64
- G01R33/32—Excitation or detection systems, e.g. using radio frequency signals
- G01R33/34—Constructional details, e.g. resonators, specially adapted to MR
- G01R33/34046—Volume type coils, e.g. bird-cage coils; Quadrature bird-cage coils; Circularly polarised coils
Definitions
- the present invention relates to an RF coil for an MR device for transmitting or receiving an RF (radio frequency) radio wave for measuring an echo signal of MRI (magnetic resonance imaging) or MRS (magnetic resonance spectroscopy), and in particular, The present invention relates to a volume coil for an MR device used for imaging the head of a subject and the like.
- a magnetic resonance diagnostic apparatus that performs MRI and MRS measurements applies a static magnetic field having a uniform intensity in an examination area and converts an RF radio wave polarized in a plane orthogonal to the direction of the static magnetic field into a magnetic field.
- This device irradiates the nucleus to be detected, receives the RF radio waves emitted by the nucleus excited by the nucleus, and processes the signal.
- MRI Magnetic Resonance Imaging
- MRS Magnetic Resonance Statroscopy
- the V ⁇ deviation method also uses a gradient magnetic field generator to limit the examination area or to specify where signals are being emitted.
- the MRI device and the MRS device have exactly the same hardware configuration, and differ only in the signal processing format including the imaging process.
- RF coils are used to transmit and receive RF waves with these devices.
- a shield is provided between the RF coil and the gradient magnetic field generator to prevent leakage of electromagnetic waves to the outside of the RF coil and reception of external electromagnetic waves. (For example, see Patent Documents 1 and 2)
- the frequency of the RF radio wave transmitted and received by the RF coil increases in proportion to the strength of the static magnetic field. For example, when the static magnetic field strength exceeds 3T (Tesla), the magnetic resonance frequency of hydrogen atoms becomes 120 MHz or higher, and the RF coil used at that time irradiates a large amount of electromagnetic waves to the outside and causes loss of transmission power and This causes deterioration of the SN ratio of the received signal. Therefore, it is even more important to shield the outer surface of the RF coil to prevent radio waves from escaping to the outside during transmission, and to suppress the mixing of noise radio waves from outside during reception.
- 3T 3T
- a conductor such as a copper foil, a thin plate, or a copper plate is wound around the outer surface of the RF coil as a shield, and the electric power is supplied to the outside. Magnetic wave leakage and reception of external electromagnetic waves have been prevented.
- coil decoupling or detuning is required for imaging in an environment where a plurality of coils coexist. (Temporarily defeating the function of the coil by cutting or breaking the resonance condition) is provided.
- the RF coil is tuned to resonate at a specific frequency determined by the measured nuclei and the magnetic field strength. If you want to transmit with a volume coil and receive with a different surface coil, the force that places the two coils close together If these two resonant circuits are magnetically coupled to each other, the resonance characteristics will deteriorate. For this reason, it is necessary to cut off the circuit of the receiving coil at the time of transmission and cut off the circuit of the transmitting coil at the time of reception so that a plurality of coils do not work at the same time. This switching is performed by the blocking circuit.
- the RF shield attached to the inside of the gradient coil is divided into a plurality of copper foils, a diode is interposed between the copper foils, and the copper foils are blocked.
- a switch control circuit that is DC-connected and RF-separated by a circuit is provided, and by changing the polarity of the DC bias voltage from the switch control circuit, the diode is actively controlled to transmit RF signals and receive NMR signals.
- the RF shield performance can be improved and overcurrent due to the gradient magnetic field can be reduced.
- a volume coil for an MR device used for imaging a head or the like of a subject is a cylindrical coil having an opening into which a head is inserted. It is formed of a cavity.
- the cylindrical cavity is composed of an outer surface, an inner surface, and both end surfaces.
- 16 axially extending elements are arranged between the inner surface and the outer surface of the cavity.
- the outer surface of this coil is covered with a cylindrical shield having a diameter of 34 cm and a height of 22 cm (see Non-Patent Document 1, page 541).
- Patent Document 1 JP-A-7-39539
- Patent Document 2 Japanese Patent Application Laid-Open No. 8-252234
- Patent Document 3 JP-A-62-112542
- Patent Document 4 JP-A-5-113473
- Non-Patent Document 1 Brian A. Baertlein et al. “Theoretical Model for an MRI Radio Frequenc y Resonator” IEEE TRANSACTION ON BIOMEDICAL ENGINEERING. VOL.47. N 0.4. APRIL 2000
- the subject is forced to feel a blockage because the outside of the RF coil is blocked with a conductor. This was particularly noticeable in the case of a volume coil used for inspection of the head and the like.
- fMRI magnetic resonance imaging
- decoupling and detuning of the coil may be performed.In the case of an RF coil having a resonance frequency exceeding 120 MHz, the electric current flowing through the coil is distributed on the copper foil or copper plate of the shield, and the circuit of the coil is electrically connected. I could't cut it.
- An object of the present invention is to reduce the feeling of obstruction of a subject and to facilitate experiments such as fMRI, and to additionally enable decoupling of a coil.
- a volume coil for an MR device used for transmitting and receiving RF radio waves
- the volume coil includes a plurality of conductive rods and has a radio wave shield wound on an outer surface.
- the conductive segment has a transparent structure.
- a featured volume coil for an MR device is provided.
- One of the conductive rods corresponds to one of the conductive segments, one closed current path including each conductive rod is provided, and a blocking circuit is inserted into the closed current path.
- the conductive segment corresponding to one end of the closed current path may be electrically connected.
- the capacitor may be configured by overlapping a part of adjacent conductive segments with a dielectric interposed therebetween.
- the radio wave shield is preferably covered with a transparent insulating structure.
- the insulating structure may be configured to hold the radio wave shield.
- the conductive segment having the see-through structure may be a conductive segment made of a transparent conductive material, a conductive segment having a mesh pattern, or a conductive segment having a perforated pattern. ,.
- the conductive segment of the radio wave shield has a structure that can be seen through, the outside can be seen and the effect of reducing the feeling of obstruction of the subject can be obtained.
- the light stimulation is easily performed in experiments such as fMRI, the effect can be obtained.
- the capacitor cuts the conductive segment DC for each conductive rod of the volume coil in order to suppress the generation of eddy current caused by the switching of the gradient magnetic field, but connects it for high frequency. Therefore, it is possible to effectively block electromagnetic waves.
- one of the conductive rods corresponds to one of the conductive segments, and one closed current path including each conductive rod is provided, and a blocking circuit is inserted into the closed current path. Then, the conductive segment corresponding to one end of the closed current path is electrically connected, so that the function of decoupling ⁇ detuning can be easily realized.
- FIG. 1 shows a simple configuration of an MR device to which the volume coil of the present invention can be applied.
- This MR device includes a static magnetic field coil 11 for applying a static magnetic field having a uniform intensity to an examination area, a gradient magnetic field coil 12 for limiting an examination area or specifying a place where a signal is emitted, and an RF radio wave. Irradiates the nuclei to be inspected and emits the nuclei excited by the nuclei.
- a gradient magnetic field generator 14 for generating a magnetic field, an RF transmitter / receiver 15 for driving the volume coil 13 to transmit and receive RF radio waves, and amplifying a signal of the radio wave received by the volume coil 13;
- a controller 16 that controls the gradient magnetic field generator 14 and the RF transceiver 15 so that the coil 12 and the volume coil 13 operate in a predetermined operation sequence, and a signal that processes the RF radio signal received from the RF transceiver 15
- a processing device 17 is provided.
- FIG. 2 is a schematic perspective view showing a part of the volume coil 21 of the present invention.
- the volume coil 21 has a cylindrical shape so that the head of the subject can be disposed therein, and extends in the axial direction between the two conductive end rings 22a and 22b.
- eight conductive rods 23 are shown, and the number of conductive rods is eight, but another number may be used. For example, it may be 16.
- FIG. 3 is a schematic perspective view of the volume coil 31 of the present invention, and illustrates the relationship between the volume coil 21 of FIG. 2 and the radio wave shield 32 wound on the outer surface thereof.
- the radio wave shield 32 is composed of eight sets of conductive segments 33 (only three sets of conductive segments 33a, 33b, and 33c are shown) arranged so as to cover the cylindrical outer surface of the volume coil 21.
- Each conductive segment has a mesh pattern composed of a wire extending in the axial direction of the volume coil and a wire orthogonal to the wire, and corresponds to each conductive rod 23 of the volume coil 21.
- the length of the conductive segment 33 in the axial direction is longer than the length of the conductive pad 23 in the axial direction.Each end of each conductive segment extends beyond both ends of the volume coil to the center of the end rings 22a and 22b. Each of the conductive rods 23 is bent inward by the opposing force and is electrically connected to both ends of the corresponding conductive rod 23.
- a capacitor 34 (only three capacitors 34a, 34b, and 34c are shown) is connected between the conductive 'conductive segment and the other conductive' seg- ments. Is cut off in a DC manner, and the eddy current generated by the gradient coil is suppressed from flowing to the radio wave shield.
- the mesh pattern of the conductive segments is made of conductive wire or narrow tape. Also, all intersections of the wires are electrically connected. The larger the aperture ratio of the mesh pattern is, the better the transparency and the feeling of obstruction are reduced. It is preferred. However, considering the shielding performance, the width of the mesh putter opening is 1 mn! The size of the opening is exaggerated in the drawings of the present application. Also, three capacitors are shown in the figure. Any number of capacitors can be used as long as the effect of suppressing the force eddy current can be obtained.
- the volume coil of the present invention When the volume coil of the present invention is used for humans or animals, parts that may cause electric shock, such as the outside of the radio wave shield 32 and the inside of the volume coil in which the subject enters, are made of transparent insulating material such as acrylic pipe material It is necessary to cover it with a conductive structure and secure electrical safety. If the radio wave shield 32 is made of, for example, stamped aluminum sheet and the strength of the structure alone is not sufficient, this transparent insulating structure is attached to the outside or inside of the volume coil and held. The shortage can be compensated.
- the mounting method does not limit the method, such as screwing and pasting.
- FIG. 4 is an expanded view of a part of the radio wave shield as shown in FIG. 3, in which only two conductive segments 43a and 43b are shown. These two conductive segments are connected to each other by three capacitors 44a, 44b, and 44c.
- broken lines 45a and 45b show two end rings 22a and 22b as shown in FIG. 3, and portions of the conductive segments extending above and below the broken lines are shown in FIG. This is an expansion of the bent part in 3.
- 23a and 23b indicate both end portions of two conductive rods 23 corresponding to the conductive segments 43a and 43b, respectively.
- FIG. 5 and FIG. 6 are developed views showing two conductive segments similar to FIG. 4, and show another example of the mesh pattern.
- the conductive segment in FIG. 5 has a pattern formed by a plurality of parallel wires obliquely intersecting the wires extending in the axial direction of the volume coil from left and right.
- the conductive segment in Fig. 6 has a rhombic mesh pattern formed by a plurality of parallel wires that extend diagonally and cross each other at right and left directions with respect to the axial direction of the wire that extends in the axial direction of the volume coil. are doing.
- Each of the two conductive segments shown in Figs. 5 and 6, respectively, is connected by three capacitors and both ends are connected to the corresponding conductive rods, similarly to the conductive segment in Fig. 4. Is electrically connected to
- FIG. 7 shows a radio wave shield according to still another embodiment of the present invention. Net shown in Figure 7
- the eye pattern is similar to the mesh pattern shown in FIG. 4, except that each conductive segment, together with each corresponding conductive rod, forms one current circuit. That is, in the mesh pattern of FIG. 7, the wires 76a and 76b extending in the axial direction at the left and right ends of the two conductive segments 73a and 73b respectively correspond to the center wire among a plurality of wires orthogonal to the wire. It is electrically connected only to 77a and 77b.
- connection between each of the conductive segments 73a and 73b and the corresponding conductive rod 23 is also achieved by connecting the ends 23a and 23b of each conductive rod only to both ends of the wires 76a and 76b. .
- one closed current path including each of the wires 76a and 76b and each conductive rod is provided, and the conductive segment corresponding to one end of the closed current path is electrically connected.
- Blocking circuits 78a and 78b are inserted into the wires 76a and 76b forming the closed current path, respectively.
- the blocking circuits 78a and 78b have a circuit configuration as shown in FIG. That is, a PIN diode 81 is combined with a resonance circuit using lumped components including an inductance L and a capacitance C.
- the resonance frequency of this resonance circuit is the same as the resonance frequency of the volume coil.
- the operation of the blocking circuit is to control the opening and closing of the coil resonance circuit by applying a forward or reverse bias voltage to both ends of the PIN diode 81.
- the radio wave shield including such a blocking circuit is useful when dedicated volume coils are used for transmission and reception of RF radio waves, respectively. In other words, it is useful when a volume coil is used as a transmitting RF coil and a surface coil is used as a receiving RF coil.
- FIG. 9 shows a volume coil 91 and a radio wave shield 92 wound around the outer surface of the volume coil 91.
- the radio wave shield 92 has a plurality of conductive segments 93 and a plurality of capacitors 94 connected therebetween.
- the ends 93a and 93b of one axial wire of each conductive segment 93 are connected to the volume coil 91 in the same manner as the radio shield 32 in FIG. It is electrically connected to both ends 95a and 95b of the plurality of conductive rods 95.
- two surface coils 96 are arranged inside the volume coil 91.
- the radio wave shield 92 is actually provided with a blocking circuit as shown in FIG. 7, but is not shown in FIG. Also, another blocking circuit is provided in the surface coil 96, but is not shown in FIG.
- FIG. 10 briefly shows an imaging sequence when imaging is performed by a gradient echo method in an MR apparatus using a volume coil as a transmitting RF coil and a surface coil as a receiving RF coil.
- Figure 10 shows the timing of the blocking of the surface coil and the volume coil, the timing of the generation of the RF transmission pulse, and the timing of the generation of each of the gradient magnetic field X, gradient magnetic field Y and gradient magnetic field Z by the gradient magnetic field coil. The relationship between and is briefly shown.
- the volume coil is unblocked and active, while the surface coil is blocked and the coil circuit is disconnected. Is inoperative.
- the surface coil When the object is irradiated with the RF electric wave from the volume coil, the surface coil receives the echo signal generated by the measurement site force of the object specified by the gradient magnetic field X, the gradient magnetic field Y, and the gradient magnetic field Z.
- the surface coil is adjusted so that the surface coil is not blocked at the center of the echo so that the echo signal is effectively received by the surface coil.
- the radio wave shield including the blocking circuit as shown in FIG. 7 is used when the volume coil is used exclusively for transmission or reception without being used for both transmission and reception.
- Radio shields that do not include a blocking circuit as shown in Fig. 6 to Fig. 6 are useful when a volume coil is used for both transmission and reception.
- FIG. 11 shows a mesh pattern of a radio shield including the same blocking circuits 78a and 78b as in FIG. 7, and illustrates an example of a method of forming a capacitor using conductive segments.
- the difference from the mesh pattern of FIG. 7 is that the capacitor 4 is formed by overlapping the ends of the adjacent conductive segments 73a and 73b with a dielectric therebetween.
- Capacitors are generally capable of using a commercially available small-capacitance capacitor that allows only high frequencies to pass. It can be realized in stages. Such a capacitor can be used for a radio wave shield that does not include a blocking circuit as shown in FIGS. 3 to 6 that can be used only for a radio wave shield that includes a blocking circuit as in the mesh pattern in FIG.
- the mesh pattern is not limited to the shape shown in the drawings of the present application, but may be any as long as a predetermined shielding effect can be achieved and an effect of reducing the feeling of obstruction of the subject by providing transparency can be obtained.
- Other grid patterns can be used.
- the conductive segment may have a perforated pattern instead of the mesh pattern.
- This perforation pattern is made by punching a sheet material or the like.
- the shape is not particularly limited to a circle or a square.
- the formation of the mesh pattern or the perforated pattern does not need to be entirely uniform.
- the conductive segments can be made of a transparent conductive material.
- the volume coil of the present invention can be used for an MR device using one RF coil for both transmission and reception and an MR device using two RF coils for transmission only and reception only, respectively. Also, it can be used for MR devices having a magnetic field strength of 3T or more.
- FIG. 1 is a diagram showing a simple configuration of an MR device to which a volume coil according to the present invention can be applied.
- FIG. 2 is a schematic perspective view of a part of a volume coil according to the present invention.
- FIG. 3 is a schematic perspective view of a volume coil according to the present invention.
- FIG. 4 is a developed view showing a part of a radio wave shield of a volume coil according to the present invention.
- FIG. 5 is a development view similar to FIG. 4, showing an example of a mesh pattern.
- FIG. 6 is a developed view similar to FIG. 4, showing an example of a mesh pattern.
- FIG. 7 is a developed view showing a part of a radio wave shield of a volume coil according to the present invention including a blocking circuit.
- FIG. 8 is a simple configuration diagram of a blocking circuit.
- FIG. 9 shows a volume coil of the present invention and a surface coil used therewith. It is an exploded perspective view.
- FIG. 10 is a diagram showing an image sequence when the volume coil of the present invention is used together with a surface coil.
- FIG. 11 is a diagram showing another embodiment of the capacitor used for the volume coil of the present invention.
Landscapes
- Physics & Mathematics (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Magnetic Resonance Imaging Apparatus (AREA)
Abstract
Description
Claims
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2004-178544 | 2004-06-16 | ||
JP2004178544A JP2006000295A (ja) | 2004-06-16 | 2004-06-16 | Mr装置用ボリュームコイル |
Publications (1)
Publication Number | Publication Date |
---|---|
WO2005122890A1 true WO2005122890A1 (ja) | 2005-12-29 |
Family
ID=35509394
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/JP2005/011040 WO2005122890A1 (ja) | 2004-06-16 | 2005-06-16 | Mr装置用ボリュームコイル |
Country Status (2)
Country | Link |
---|---|
JP (1) | JP2006000295A (ja) |
WO (1) | WO2005122890A1 (ja) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2007149824A2 (en) * | 2006-06-22 | 2007-12-27 | Koninklijke Philips Electronics, N.V. | Magnetic resonance receive coil array integrated into wall of scanner bore |
US10466318B2 (en) | 2015-03-27 | 2019-11-05 | Koninklijke Philips N.V. | Magnetic resonance volume coil with multiple independent transmit receive channels and method of operation thereof |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH06209918A (ja) * | 1993-01-14 | 1994-08-02 | Hitachi Ltd | 磁気共鳴撮影装置用rfプローブ |
JPH08294477A (ja) * | 1995-01-19 | 1996-11-12 | Univ California | Rfシールド及びその製造方法 |
JP2001145610A (ja) * | 1999-09-07 | 2001-05-29 | Ge Yokogawa Medical Systems Ltd | Rfコイル、rf信号送受信装置および磁気共鳴撮像装置 |
JP2003500133A (ja) * | 1999-05-21 | 2003-01-07 | ザ ゼネラル ホスピタル コーポレーション | 撮像システム用rfコイル |
-
2004
- 2004-06-16 JP JP2004178544A patent/JP2006000295A/ja active Pending
-
2005
- 2005-06-16 WO PCT/JP2005/011040 patent/WO2005122890A1/ja active Application Filing
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH06209918A (ja) * | 1993-01-14 | 1994-08-02 | Hitachi Ltd | 磁気共鳴撮影装置用rfプローブ |
JPH08294477A (ja) * | 1995-01-19 | 1996-11-12 | Univ California | Rfシールド及びその製造方法 |
JP2003500133A (ja) * | 1999-05-21 | 2003-01-07 | ザ ゼネラル ホスピタル コーポレーション | 撮像システム用rfコイル |
JP2001145610A (ja) * | 1999-09-07 | 2001-05-29 | Ge Yokogawa Medical Systems Ltd | Rfコイル、rf信号送受信装置および磁気共鳴撮像装置 |
Non-Patent Citations (3)
Title |
---|
ADRIANY G. ET AL: "A Detuneable TEM Transmit Coil for 4T fMRI and Spectroscopy.", PROCEEDINGS OF THE INTERNATIONAL SOCIETY FOR MAGNETIC RESONANCE IN MEDICINE 8TH SCIENTIFIC MEETINGS AND EXHIBITION., 2000, XP002991362 * |
BROOKERS M.J. ET AL: "The fMRI BOLD Response Co-varies Spatially and Temporally with Electrical Oscilatory Change and a Sustained Electrical Response.", PROCEEDINGS OF THE INTERNATIONAL SOCIETY FOR MAGNETIC RESONANCE IN MEDICINE 12TH SCIENTIFIC MEETINGS AND EXHIBITION., May 2004 (2004-05-01), XP002991364 * |
VAUGHAN J. ET AL: "The Head Cradle: An Open Faced, High Performance TEM Coil.", PROCEEDINGS OF THE INTERNATIONAL SOCIETY FOR MAGNETIC RESONANCE IN MEDICINE 9TH SCIENTIFIC MEETINGS AND EXIBITION., 2001, XP002991363 * |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2007149824A2 (en) * | 2006-06-22 | 2007-12-27 | Koninklijke Philips Electronics, N.V. | Magnetic resonance receive coil array integrated into wall of scanner bore |
WO2007149824A3 (en) * | 2006-06-22 | 2008-03-27 | Koninkl Philips Electronics Nv | Magnetic resonance receive coil array integrated into wall of scanner bore |
US10466318B2 (en) | 2015-03-27 | 2019-11-05 | Koninklijke Philips N.V. | Magnetic resonance volume coil with multiple independent transmit receive channels and method of operation thereof |
Also Published As
Publication number | Publication date |
---|---|
JP2006000295A (ja) | 2006-01-05 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US6900636B2 (en) | Transmission and receiving coil for MR apparatus | |
JP4625834B2 (ja) | Rf表面共振器 | |
US8742759B2 (en) | High-frequency coil and magnetic resonance imaging device | |
JP3205385B2 (ja) | 核磁気共鳴断層撮影装置 | |
JP4768627B2 (ja) | 超高磁場(shf)mri用のrfコイル | |
US7973531B2 (en) | Detuning a radio-frequency coil | |
JP3432896B2 (ja) | 核スピントモグラフィ装置の高周波装置 | |
US7414402B2 (en) | Coil apparatus and nuclear magnetic resonance apparatus using the same | |
US20140253122A1 (en) | Mri coil assembly with a radio frequency shield switchable between a blocking state and a transparent state | |
JP4768235B2 (ja) | Rfコイル・アセンブリ | |
EP2351520B1 (en) | Antenna device and magnetic resonance imaging device | |
JPH07265278A (ja) | Rfプローブ | |
US20190310331A1 (en) | Array coil and magnetic resonance imaging apparatus | |
JP2002159471A (ja) | 磁気共鳴画像化装置及びその方法 | |
US7221163B2 (en) | Magnetic resonance system with suppression of capacitive coupling between an RF source and the subject | |
WO2005122890A1 (ja) | Mr装置用ボリュームコイル | |
EP3807666B1 (en) | Sheath wave barrier for magnetic resonance (mr) applications | |
JPH07163547A (ja) | 磁気共鳴装置用の二重共鳴アンテナ装置 | |
JP4494751B2 (ja) | 磁気共鳴撮像装置 | |
US20220326324A1 (en) | Improved birdcage antenna | |
EP4303604A1 (en) | Receiving coil | |
EP3617730A1 (en) | Sheath wave barrier for magnetic resonance (mr) applications | |
JPH08107889A (ja) | 核スピントモグラフィー装置 | |
WO2011135312A2 (en) | Mri rf coil with improved pin diode switch and reduced b1 distortions |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
AK | Designated states |
Kind code of ref document: A1 Designated state(s): AE AG AL AM AT AU AZ BA BB BG BR BW BY BZ CA CH CN CO CR CU CZ DE DK DM DZ EC EE EG ES FI GB GD GE GH GM HR HU ID IL IN IS KE KG KM KP KR KZ LC LK LR LS LT LU LV MA MD MG MK MN MW MX MZ NA NG NI NO NZ OM PG PH PL PT RO RU SC SD SE SG SK SL SM SY TJ TM TN TR TT TZ UA UG US UZ VC VN YU ZA ZM ZW |
|
AL | Designated countries for regional patents |
Kind code of ref document: A1 Designated state(s): GM KE LS MW MZ NA SD SL SZ TZ UG ZM ZW AM AZ BY KG KZ MD RU TJ TM AT BE BG CH CY CZ DE DK EE ES FI FR GB GR HU IE IS IT LT LU MC NL PL PT RO SE SI SK TR BF BJ CF CG CI CM GA GN GQ GW ML MR NE SN TD TG |
|
121 | Ep: the epo has been informed by wipo that ep was designated in this application | ||
NENP | Non-entry into the national phase |
Ref country code: DE |
|
WWW | Wipo information: withdrawn in national office |
Country of ref document: DE |
|
122 | Ep: pct application non-entry in european phase |