JPH0642878B2 - Magnetic resonance imaging equipment - Google Patents

Magnetic resonance imaging equipment

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Publication number
JPH0642878B2
JPH0642878B2 JP1094874A JP9487489A JPH0642878B2 JP H0642878 B2 JPH0642878 B2 JP H0642878B2 JP 1094874 A JP1094874 A JP 1094874A JP 9487489 A JP9487489 A JP 9487489A JP H0642878 B2 JPH0642878 B2 JP H0642878B2
Authority
JP
Japan
Prior art keywords
light emitting
light
magnetic field
resonance imaging
magnetic resonance
Prior art date
Legal status (The legal status 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 status listed.)
Expired - Lifetime
Application number
JP1094874A
Other languages
Japanese (ja)
Other versions
JPH02274231A (en
Inventor
基司 原頭
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Toshiba Corp
Original Assignee
Tokyo Shibaura Electric Co Ltd
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 Tokyo Shibaura Electric Co Ltd filed Critical Tokyo Shibaura Electric Co Ltd
Priority to JP1094874A priority Critical patent/JPH0642878B2/en
Publication of JPH02274231A publication Critical patent/JPH02274231A/en
Publication of JPH0642878B2 publication Critical patent/JPH0642878B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】 [発明の目的] (産業上の利用分野) 本発明は、静磁場発生手段,傾斜磁場発生手段,励起用
磁場の送信及び励起信号の受信を行う手段を装備すると
共に被検者配置空間を設け、該空間内に前記各手段によ
って磁場を発生させるようにした磁気共鳴イメージング
装置に関する。
DETAILED DESCRIPTION OF THE INVENTION (Industrial field of application) The present invention is equipped with static magnetic field generating means, gradient magnetic field generating means, means for transmitting an excitation magnetic field and receiving an excitation signal, and The present invention relates to a magnetic resonance imaging apparatus in which a subject placement space is provided and a magnetic field is generated in the space by each of the means.

(従来の技術) 磁気共鳴(MR:magnetic resonance)現象は、静磁場
中に置かれた零でないスピン及び磁気モーメントを持つ
原子核が特定の周波数の電磁波のみを共鳴的に吸収・放
出する現象であり、この原子核は下記式に示す角周波数
ω(ω=2πν,ν;ラーモア周波数)で共鳴
する。
(Prior Art) A magnetic resonance (MR) phenomenon is a phenomenon in which an atomic nucleus having a non-zero spin and a magnetic moment placed in a static magnetic field resonantly absorbs and emits an electromagnetic wave of a specific frequency. , This nucleus resonates at an angular frequency ω 00 = 2πν 0 , ν 0 ; Larmor frequency) shown in the following formula.

ω=γH ここで、γは原子核の種類に固有の磁気回転比であり、
また、Hは静磁場強度である。
ω 0 = γH 0 where γ is the gyromagnetic ratio peculiar to the type of nucleus,
H 0 is the static magnetic field strength.

以上の原理を利用して生体診断を行う装置は、上述の共
鳴吸収の後に誘起される上記と同じ周波数の電磁波(磁
気共鳴信号:エコー信号やFID信号)を信号処理し
て、原子核密度,縦緩和時定数T1,横緩和時定数T
2,流れ、化学シフト等の情報が反映された診断情報例
えば被検体のスライス像等を無侵襲で得るようにしてい
る。
A device for performing a biomedical diagnosis using the above principle performs signal processing of electromagnetic waves (magnetic resonance signals: echo signals and FID signals) of the same frequency as that induced after the above-mentioned resonance absorption, to obtain nuclear density, longitudinal Relaxation time constant T1, lateral relaxation time constant T
2. Diagnostic information in which information such as flow and chemical shift is reflected, for example, a slice image of a subject is obtained non-invasively.

そして、磁気共鳴による診断情報の収集は、静磁場中に
配置した被検体の全部位を励起し且つ信号収集すること
ができるものであるが、装置構成上の制約やイメージン
グ像の臨床上の要請から、実際の装置としては特定部位
に対する励起とその信号収集を行うようにしている。
Further, the collection of diagnostic information by magnetic resonance is capable of exciting all the parts of the subject placed in a static magnetic field and collecting signals, but there are restrictions on the device configuration and clinical demands for imaging images. Therefore, in an actual device, excitation and signal acquisition of a specific part are performed.

このような磁気共鳴イメージング装置では、静磁場発生
手段としては超電導磁石,常電導磁石,永久磁石のいず
れか単体若しくはその組合せが用いられている。そし
て、静磁場発生手段により発生される静磁場領域の一部
分が診断可能領域であって被検体者が配置され且つイメ
ージング可能領域となりうる。これは、診断可能領域の
静磁場領域としては、磁気共鳴現象の原理から必然的
に、数千〜数万ガウスの高強度磁場であってその磁場均
一性が数ppmである必要があるためである。
In such a magnetic resonance imaging apparatus, any one of a superconducting magnet, a normal conducting magnet, and a permanent magnet or a combination thereof is used as the static magnetic field generating means. Then, a part of the static magnetic field region generated by the static magnetic field generation means can be a diagnostic possible region where the subject is placed and can be imaged. This is because the static magnetic field region of the diagnosable region is necessarily a high-intensity magnetic field of several thousand to tens of thousands of Gauss and its magnetic field homogeneity is several ppm because of the principle of the magnetic resonance phenomenon. is there.

従って、超電導磁石,常電導磁石,永久磁石のいずれか
単体若しくはその組合せからなる静磁場発生手段は、寸
法で言うと数メートルであり、重量で言うと数トン〜十
数トン以上に及ぶものとなっている。
Therefore, the static magnetic field generating means composed of any one of a superconducting magnet, a normal conducting magnet, and a permanent magnet or a combination thereof is several meters in terms of dimensions and several tons to over ten tons in terms of weight. Has become.

例えば、超電導磁石からなる静磁場発生手段は、二重円
筒体の両開口が閉塞されてなる容器内に、超電導線及び
冷媒を収容したものであり、その内筒空間の軸方向中間
位置に、磁場均一性が数ppmの高強度磁場を生成するよ
うになっている。そして、内筒空間の軸方向長さは、2
メートル程度となっている。つまり、被検者は、この軸
方向長さ2メートルの内筒空間に、その軸方向に沿って
導入される。そして、該内筒空間における前記磁場均一
性が数ppmの高強度磁場が生成される軸方向中間位置に
在る被検者の部位が、イメージング可能領域となる。
For example, the static magnetic field generating means consisting of a superconducting magnet is one in which a superconducting wire and a refrigerant are contained in a container in which both openings of a double cylindrical body are closed, and an axial intermediate position of the inner cylindrical space thereof, It is designed to generate a high intensity magnetic field with magnetic field homogeneity of several ppm. The axial length of the inner cylinder space is 2
It is about meters. That is, the subject is introduced along the axial direction into the inner cylindrical space having a length of 2 meters in the axial direction. The region of the subject at the axially intermediate position where the high-intensity magnetic field with the magnetic field homogeneity of several ppm in the inner cylindrical space is generated is the imageable region.

(発明が解決しようとする課題) 上述の例は、静磁場発生手段として超電導磁石からなる
ものであるが、他のものについても、被検者導入空間は
メートル単位の長さとなっている。この長さは、断層像
映像化装置として良く比較されるX線CTスキャナ装置
と比べると、非常に長いものとなっている。これは、前
述したように、必要な磁場を得るため等の理由からであ
る。
(Problems to be Solved by the Invention) In the above example, a superconducting magnet is used as the static magnetic field generating means, but in other cases as well, the subject introduction space has a length in meters. This length is extremely long as compared with an X-ray CT scanner device that is often compared as a tomographic image visualization device. This is because, for example, the necessary magnetic field is obtained as described above.

このように磁気共鳴イメージング装置では、被検者導入
空間はメートル単位の長さとなっているので、その中は
薄暗くなっている。しかもその中に被検者が入ると、一
層暗くなってしまう。また、磁気共鳴イメージング装置
のスキャン時間は数分〜数十分にも及ぶため、この長い
スキャン時間の間にわたって暗い空間に置かれる被検者
は、不安感をもってしまう。
As described above, in the magnetic resonance imaging apparatus, the subject introduction space has a length of a unit of meter, so that the inside thereof is dim. Moreover, when the subject enters the area, it becomes even darker. In addition, since the scan time of the magnetic resonance imaging apparatus extends from several minutes to several tens of minutes, the subject placed in a dark space during this long scan time feels uneasy.

そこで本発明の目的は、被検者に不安感を与えないよう
にした磁気共鳴イメージング装置を提供することにあ
る。
Therefore, an object of the present invention is to provide a magnetic resonance imaging apparatus that does not give a subject anxiety.

[発明の構成] (課題を解決するための手段) 本発明は上記課題を解決し且つ目的を達成するために次
のような手段を講じた構成としている。すなわち、請求
項1にかかる発明は、静磁場発生手段,傾斜磁場発生手
段,励起用磁場の送信及び誘起信号の受信を行う手段を
装備すると共に被検者配置空間を設け、該空間内に前記
各手段によって磁場を発生させるようにした磁気共鳴イ
メージング装置において、プラスチック光ファイバの複
数を条状に形成したもののクラッド部分を傷付けてなる
発光手段を、前記空間内に配置すると共に、当該発光手
段に光を導入する手段を設けたことを特徴とし、また、
請求項2にかかる発明は、前記発光手段を着色してなる
ことを特徴とし、さらに、請求項3にかかる発明は、前
記発光手段の面に、反射部材及び拡散部材の少なくとも
一方を配置することを特徴とし、また、請求項4にかか
る発明は、前記発光手段を、反射部材と拡散部材との間
に挟んでなることを特徴とする。
[Structure of the Invention] (Means for Solving the Problems) The present invention has a structure in which the following means are provided in order to solve the above problems and achieve the object. That is, the invention according to claim 1 is equipped with a static magnetic field generation means, a gradient magnetic field generation means, a means for transmitting an excitation magnetic field and a reception of an induction signal, and also provides a subject placement space in which the space is provided. In a magnetic resonance imaging apparatus configured to generate a magnetic field by each means, a light emitting means formed by scratching a clad portion of a plurality of plastic optical fibers formed in a strip shape is arranged in the space and Characterized in that it is provided with means for introducing light,
The invention according to claim 2 is characterized in that the light emitting means is colored, and the invention according to claim 3 is characterized in that at least one of a reflecting member and a diffusing member is arranged on the surface of the light emitting means. The invention according to claim 4 is characterized in that the light emitting means is sandwiched between a reflecting member and a diffusing member.

(作用) このような請求項1にかかる発明の構成によれば、被検
者配置空間に配置された発光手段のクラッド部分から、
スポット照明でなく面状照明となり得る側面漏光が得ら
れ、前記空間を明るくすることができる上、発光手段
は、条状であるので、設置スペースは小さくて済み、被
検者配置空間を狭めない。また、請求項2にかかる発明
によれば、前記発光手段を例えば乳白色に着色すると、
被検者の気分を和らげる乳白色の面状照明光となるので
好ましい。さらに、請求項3にかかる発明によれば、前
記発光手段の面に、反射部材及び拡散部材の少なくとも
一方を配置するので、漏光指向性を改善することができ
る。また、請求項4にかかる発明によれば、前記発光手
段を、反射部材と拡散部材との間に挟んでなるので、漏
光指向性を請求項3にかかる発明のものよりも一層改善
することができる。
(Operation) According to the configuration of the invention according to claim 1 as described above, from the clad portion of the light emitting means arranged in the subject arrangement space,
Side light leakage that can be planar illumination instead of spot illumination can be obtained, and the space can be made brighter. Moreover, since the light emitting means is strip-shaped, the installation space can be small, and the subject placement space is not narrowed. . According to the invention of claim 2, when the light emitting means is colored, for example, milky white,
This is preferable because it provides a milky white planar illumination light that softens the subject's mood. Further, according to the invention of claim 3, since at least one of the reflecting member and the diffusing member is arranged on the surface of the light emitting means, it is possible to improve the light leakage directivity. Further, according to the invention of claim 4, since the light emitting means is sandwiched between the reflecting member and the diffusing member, the light leakage directivity can be further improved as compared with the invention of claim 3. it can.

(実施例) 以下本発明にかかる磁気共鳴イメージング装置の一実施
例を、第1図及び第2図を参照して説明する。
(Embodiment) An embodiment of the magnetic resonance imaging apparatus according to the present invention will be described below with reference to FIGS. 1 and 2.

第1図は本実施例の磁気共鳴イメージング装置の要部で
ある、例えば超電導磁石からなる静磁場発生手段及びこ
の静磁場発生手段に配置される発光手段の構成を示す斜
視図、第2図〜第4図は同実施例の発光手段の詳細を示
すものであって、第2図は発光手段としてのプラスチッ
ク光ファイバのリボン又はテープの斜視図、第3図
(a)はプラスチック光ファイバのリボン又はテープの
側面漏光の発生を、リボン又はテープの伸長方向から見
た図、第3図(b)は同プラスチック光ファイバのリボ
ン又はテープの側面漏光の発生を、リボン又はテープの
端面方向から見た図、第4図は漏光指向性を改善するた
めにプラスチック光ファイバのリボン又はテープの面に
反射板,拡散板を貼着してなる発光手段を示す図であ
る。
FIG. 1 is a perspective view showing a configuration of a main part of the magnetic resonance imaging apparatus of this embodiment, for example, a static magnetic field generating means composed of a superconducting magnet and a light emitting means arranged in the static magnetic field generating means, and FIGS. FIG. 4 shows the details of the light emitting means of the embodiment, FIG. 2 is a perspective view of a plastic optical fiber ribbon or tape as the light emitting means, and FIG. 3 (a) is a plastic optical fiber ribbon. FIG. 3B is a view showing the occurrence of side light leakage from the side of the ribbon or tape, and FIG. 3B shows the occurrence of side light leakage from the ribbon or tape of the plastic optical fiber as seen from the end face direction of the ribbon or tape. 4 and FIG. 4 are views showing a light emitting means in which a reflecting plate and a diffusing plate are attached to the surface of a ribbon or tape of a plastic optical fiber in order to improve the light leakage directivity.

第1図に示すように、例えば超電導電磁石からなる静磁
場発生手段は、二重円筒体の両開口が閉塞されてなる容
器10内に、図示しない超電導線及び冷媒を収容したも
のであり、その内筒空間11の軸方向中間位置に、磁場
均一性が数ppmの高強度磁場を生成するようになってい
る。そして、内筒空間11の軸方向長さは、2メートル
程度となっている。つまり、図示しない被検者は、この
軸方向長さ2メートルの内筒空間11に、その軸方向に
沿って導入される。そして、該内筒空間11における前
記磁場均一性が数ppmの高強度磁場が生成される軸方向
中間位置に在る図示しない被検者の部位が、イメージン
グ可能領域となる。
As shown in FIG. 1, the static magnetic field generating means composed of, for example, a superconducting electromagnet is a container 10 in which both openings of a double cylinder are closed, and contains a superconducting wire and a refrigerant (not shown). A high-intensity magnetic field with magnetic field homogeneity of several ppm is generated at an axially intermediate position of the inner cylindrical space 11. The axial length of the inner cylindrical space 11 is about 2 meters. That is, a subject (not shown) is introduced into the inner cylindrical space 11 having a length of 2 meters in the axial direction along the axial direction. Then, a portion of the subject (not shown) located at an intermediate position in the axial direction where a high-intensity magnetic field having a magnetic field homogeneity of several ppm is generated in the inner cylindrical space 11 becomes an imageable region.

また、プラスチック光ファイバの複数を条状に形成す
る、例えばリボン又はテープしたもののクラッド部分を
傷付けてなる例えば2本の発光手段12を、前記空間内
11に配置すると共に、この2本の発光手段12に光を
導入するため、発光手段12の受光端部に接続されたラ
イトガイド15を介し、当該ライトガイド15の受光端
部にそれぞれ光源13を設けている。この場合、図示で
は、一つの発光手段12,ライトガイド15の両受光端
部にそれぞれ光源13を設け、合計で4つの光源13を
用いている。また、符号14は、被検者配置空間となる
内筒空間11に出入れされる被検者載置用天板である。
Further, for example, two light emitting means 12 formed by forming a plurality of plastic optical fibers in a strip shape, for example, which is formed by damaging the clad portion of a ribbon or tape, are arranged in the space 11, and the two light emitting means are provided. In order to introduce light into the light guide 12, light sources 13 are provided at the light receiving ends of the light guides 15 via the light guides 15 connected to the light receiving ends. In this case, in the figure, light sources 13 are provided at both light receiving ends of one light emitting means 12 and one light guide 15, and a total of four light sources 13 are used. Further, reference numeral 14 is a subject-mounting top plate that is put in and taken out from the inner cylindrical space 11 that is a subject placement space.

ここで、発光手段12の詳細を第2図〜第4図を参照し
て説明する。第2図に示すように、発光手段12は、プ
ラスチック光ファイバの多数本を平行に配列加工するこ
とでリボン又はテープのような条状に形成できる。
Details of the light emitting means 12 will be described with reference to FIGS. As shown in FIG. 2, the light emitting means 12 can be formed in a strip shape such as a ribbon or a tape by arranging a plurality of plastic optical fibers in parallel.

ここで、プラスチック光ファイバの1本を、符号12a
で示し、当該1本のプラスチック光ファイバにおける側
面漏光の発生を、第3図(a)ではリボン又はテープの
伸長方向から、第3図(b)ではリボン又はテープの端
面方向から見た状況で説明する。すなわち、プラスチッ
ク光ファイバ12aは、コア12a1とクラッド12a
2とからなり、そして、クラッド12a2の表面の一部
を粗面加工することにより、粗面加工された面で光が散
乱,反射角の変化が生じ、外部に漏光が出て、プラスチ
ック光ファイバ12aの側面から漏光が得られることが
知られている。
Here, one of the plastic optical fibers is denoted by reference numeral 12a.
In Fig. 3 (a), the occurrence of side light leakage in the one plastic optical fiber is seen from the extending direction of the ribbon or tape, and in Fig. 3 (b) from the end face direction of the ribbon or tape. explain. That is, the plastic optical fiber 12a includes a core 12a1 and a clad 12a.
2 and by roughening a part of the surface of the clad 12a2, light is scattered on the roughened surface and the reflection angle is changed, so that light leaks to the outside and the plastic optical fiber It is known that light leakage can be obtained from the side surface of 12a.

また、偏光指向性を向上するために、第4図に示すよう
に、プラスチック光ファイバ12a上に反射板16と拡
散シート17とを配置する構成を採用することができ
る。ここで、反射板16としては、白色板やアルミニウ
ム板(箔)を用いることができ、この反射板16を設け
ることにより、拡散効果の改善が図られ、よって偏光を
効率的にし得る。また、拡散シート17としては、セロ
ハン等を用いることができる。この拡散シート17を設
けることにより、拡散効果が図られ、よって出射光量を
より均一にし得る。
Further, in order to improve the polarization directivity, as shown in FIG. 4, it is possible to adopt a configuration in which the reflection plate 16 and the diffusion sheet 17 are arranged on the plastic optical fiber 12a. Here, a white plate or an aluminum plate (foil) can be used as the reflection plate 16. By providing the reflection plate 16, the diffusion effect can be improved, and thus the polarization can be made efficient. Further, cellophane or the like can be used as the diffusion sheet 17. By providing this diffusing sheet 17, a diffusing effect is achieved, and thus the amount of emitted light can be made more uniform.

もちろん、反射板16及び拡散シート17のうち少なく
とも一方をプラスチック光ファイバ12a上に配置して
も、ある程度の漏光指向性の向上を図り得る。
Of course, even if at least one of the reflection plate 16 and the diffusion sheet 17 is arranged on the plastic optical fiber 12a, the light leakage directivity can be improved to some extent.

このように本実施例によれば、被検者配置空間11に配
置された発光手段12の側面であるクラッド部分から、
スポット照明でなく面状照明となり得る側面漏光が得ら
れ、空間11を明るくすることができる上、発光手段1
2は、リボン又はテープのように条状であるので、設置
スペースは小さくて済み、被検者配置空間11を狭める
ことがなく有利となる。
As described above, according to the present embodiment, from the clad portion which is the side surface of the light emitting means 12 arranged in the subject arrangement space 11,
Side light leakage that can be planar illumination instead of spot illumination is obtained, and the space 11 can be made brighter and the light emitting means 1 can be used.
Since 2 is a strip shape like a ribbon or tape, the installation space can be small, which is advantageous without narrowing the subject placement space 11.

また、発光手段12を例えば乳白色に着色すると、被検
者の気分を和らげる乳白色の面状照明光となるので好ま
しい。同じ効果は、光源13の色を乳白色とすることに
より得られる。
Further, it is preferable to color the light emitting means 12 into, for example, milky white because it becomes milky white planar illumination light that softens the subject's mood. The same effect is obtained by making the color of the light source 13 milky white.

さらに、発光手段12の面に、反射板16及び拡散シー
ト17の少なくとも一方を配置するので、漏光指向性を
改善することができる。
Further, since at least one of the reflection plate 16 and the diffusion sheet 17 is arranged on the surface of the light emitting means 12, the light leakage directivity can be improved.

また、発光手段12を、反射板16と拡散シート17と
の間に挟んでなるので、漏光指向性を前述のものよりも
一層改善することができる。
Further, since the light emitting means 12 is sandwiched between the reflection plate 16 and the diffusion sheet 17, the light leakage directivity can be further improved as compared with the above.

もちろん、被検者配置空間11は磁場生成空間であっ
て、ノイズの混入が有ってはならない所であるが、発光
手段12は非電気要素であるので、ノイズを引込んだ
り、ノイズ発生源となったりしない。また、磁場を乱す
ことも無く、磁場により発光手段12等の動作が異常を
きたすこともない。
Of course, the subject arrangement space 11 is a magnetic field generation space and should not be mixed with noise. However, since the light emitting means 12 is a non-electrical element, it draws in noise or a noise generation source. It does not become. Further, the magnetic field is not disturbed, and the operation of the light emitting means 12 and the like does not become abnormal due to the magnetic field.

[発明の効果] このように請求項1にかかる発明では、静磁場発生手
段,傾斜磁場発生手段,励起用磁場の送信及び誘起信号
の受信を行う手段を装備すると共に被検者配置空間を設
け、該空間内に前記各手段によって磁場を発生させるよ
うにした磁気共鳴イメージング装置において、プラスチ
ック光ファイバの複数を条状に形成したもののクラッド
部分を傷付けてなる発光手段を、前記空間内に配置する
と共に、当該発光手段に光を導入する手段を設けたこと
により、被検者配置空間に配置された発光手段のクラッ
ド部分から、スポット照明でなく面状照明となり得る側
面偏光が得られ、前記区間を明るくすることができる
上、発光手段は、条状であるので、設置スペースは小さ
くて済み、被検者配置空間を狭めな句することができ
る。
As described above, in the invention according to claim 1, the static magnetic field generating means, the gradient magnetic field generating means, the means for transmitting the excitation magnetic field and the means for receiving the induced signal are provided, and the subject arrangement space is provided. In a magnetic resonance imaging apparatus in which a magnetic field is generated in each of the means in the space, a light emitting means formed by damaging a clad portion of a plurality of plastic optical fibers formed in a stripe shape is arranged in the space. At the same time, by providing a means for introducing light to the light emitting means, side-polarized light that can be planar illumination instead of spot illumination is obtained from the clad portion of the light emitting means disposed in the subject placement space, and the section In addition, since the light emitting means is strip-shaped, the installation space can be small, and the subject placement space can be narrowed.

また、請求項2にかかる発明では、前記発光手段を着色
してなるので、前記発光手段を例えば乳白色に着色する
と、被検者の気分を和らげる乳白色の面状照明光となる
ので、臨床上好ましいものとなる。
Further, in the invention according to claim 2, since the light emitting means is colored, when the light emitting means is colored, for example, milky white, it becomes a milky white planar illumination light that softens the subject, which is clinically preferable. Will be things.

さらに、請求項3にかかる発明では、前記発光手段の面
に、反射部材及び拡散部材の少なくとも一方を配置して
いるので、漏光指向性を改善することができる。
Further, in the invention according to claim 3, since at least one of the reflecting member and the diffusing member is arranged on the surface of the light emitting means, it is possible to improve the light leakage directivity.

また、請求項4にかかる発明では、前記発光手段を、反
射部材と拡散部材との間に挟んでなるので、漏光指向性
を請求項3にかかる発明のものよりも一層改善すること
ができる。
In the invention according to claim 4, since the light emitting means is sandwiched between the reflecting member and the diffusing member, it is possible to further improve the light leakage directivity as compared with the invention according to claim 3.

よって、本発明によれば、被検者に不安感を与えないよ
うにした磁気共鳴イメージング装置を提供できるもので
ある。
Therefore, according to the present invention, it is possible to provide a magnetic resonance imaging apparatus that does not give the subject a sense of anxiety.

【図面の簡単な説明】[Brief description of drawings]

第1図は本発明にかかる磁気共鳴イメージング装置の一
実施例の要部である例えば超電導磁石からなる静磁場発
生手段及びこの静磁場発生手段に配置される発光手段の
構成を示す斜視図、第2図〜第4図は同実施例の発光手
段の詳細を示すものであって、第2図は発光手段として
プラスチック光ファイバのリボン又はテープの斜視図、
第3図(a)はプラスチック光ファイバのリボン又はテ
ープの側面漏光の発生を、リボン又はテープの伸長方向
から見た図、第3図(b)は同プラスチック光ファイバ
のリボン又はテープの側面漏光の発生を、リボン又はテ
ープの端面方向から見た図、第4図は漏光指向性を改善
するためにプラスチック光ファイバのリボン又はテープ
の面に反射板,拡散板を貼着してなる発光手段を示す図
である。 10……容器、11……内筒空間11、12……発光手
段、13……光源、14……被検者載置用天板、15…
…ライトガイド、16……反射板、17……拡散シー
ト。
FIG. 1 is a perspective view showing a configuration of a static magnetic field generating means, which is a main part of an embodiment of a magnetic resonance imaging apparatus according to the present invention, for example, a superconducting magnet, and a light emitting means arranged in the static magnetic field generating means. 2 to 4 show the details of the light emitting means of the same embodiment, and FIG. 2 is a perspective view of a ribbon or tape of a plastic optical fiber as the light emitting means,
FIG. 3 (a) is a diagram showing the occurrence of side light leakage of a ribbon or tape of a plastic optical fiber as seen from the extending direction of the ribbon or tape, and FIG. 3 (b) is a side light leakage of the ribbon or tape of the same plastic optical fiber. FIG. 4 is a view of the generation of light from the direction of the end surface of the ribbon or tape, and FIG. 4 is a light emitting means in which a reflecting plate and a diffusing plate are attached to the surface of the ribbon or tape of the plastic optical fiber to improve the light leakage directivity. FIG. 10 ... Container, 11 ... Inner cylindrical space 11, 12 ... Light emitting means, 13 ... Light source, 14 ... Subject mounting top plate, 15 ...
… Light guide, 16 …… Reflector, 17 …… Diffusion sheet.

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】静磁場発生手段と、傾斜磁場発生手段と、
励起用磁場の送信及び誘起信号の受信を行う手段とを備
え、前記各手段によって磁場が生成される被検者配置空
間が設けられた磁気共鳴イメージング装置において、 両端を有し、帯状に形成された複数の光ファイバからな
る光導入部と、前記被検者配置空間内に配設され、前記
光導入部の側面に沿って選択的に複数設けられた漏光部
分を有する発光部とを含む発光手段と、 前記被検者配置空間の外部に設けられ、前記光導入手段
の少なくとも一方端に光を入射する少なくとも1つの光
源と、 を具備することを特徴とする磁気共鳴イメージング装
置。
1. A static magnetic field generating means, a gradient magnetic field generating means,
A magnetic resonance imaging apparatus comprising: a means for transmitting an excitation magnetic field and a means for receiving an induced signal; and a subject placement space in which a magnetic field is generated by each of the means. Light emission including a light introducing part formed of a plurality of optical fibers and a light emitting part having a light leakage part disposed in the subject placement space and selectively provided along the side surface of the light introducing part. A magnetic resonance imaging apparatus comprising: a light source; and a light source that is provided outside the subject placement space and that allows light to enter at least one end of the light introducing unit.
【請求項2】前記発光手段の少なくとも前記発光部が着
色されていることを特徴とする請求項1に記載の磁気共
鳴イメージング装置。
2. The magnetic resonance imaging apparatus according to claim 1, wherein at least the light emitting portion of the light emitting means is colored.
【請求項3】前記発光手段の前記発光部の帯状の面に、
反射部材及び拡散部材の少なくとも一方を配置すること
を特徴とする請求項1に記載の磁気共鳴イメージング装
置。
3. A strip-shaped surface of the light emitting portion of the light emitting means,
The magnetic resonance imaging apparatus according to claim 1, wherein at least one of a reflection member and a diffusion member is arranged.
【請求項4】前記発光手段の前記発光部を、反射部材及
び拡散部材との間に挟んで構成される特徴とする請求項
1に記載の磁気共鳴イメージング装置。
4. The magnetic resonance imaging apparatus according to claim 1, wherein the light emitting portion of the light emitting means is sandwiched between a reflecting member and a diffusing member.
JP1094874A 1989-04-14 1989-04-14 Magnetic resonance imaging equipment Expired - Lifetime JPH0642878B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1094874A JPH0642878B2 (en) 1989-04-14 1989-04-14 Magnetic resonance imaging equipment

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1094874A JPH0642878B2 (en) 1989-04-14 1989-04-14 Magnetic resonance imaging equipment

Publications (2)

Publication Number Publication Date
JPH02274231A JPH02274231A (en) 1990-11-08
JPH0642878B2 true JPH0642878B2 (en) 1994-06-08

Family

ID=14122199

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1094874A Expired - Lifetime JPH0642878B2 (en) 1989-04-14 1989-04-14 Magnetic resonance imaging equipment

Country Status (1)

Country Link
JP (1) JPH0642878B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20150036663A (en) * 2012-08-24 2015-04-07 지멘스 악티엔게젤샤프트 Medical device

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE102008044643A1 (en) * 2008-08-27 2010-03-04 Siemens Aktiengesellschaft Patient table and medical device with a patient table
JP6153835B2 (en) * 2013-09-27 2017-06-28 株式会社日立製作所 Medical imaging device

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS629207U (en) * 1985-07-03 1987-01-20
JPS62280683A (en) * 1986-05-29 1987-12-05 三菱電機株式会社 Nuclear magnetic resonance tomographic device
JPH049681Y2 (en) * 1987-06-05 1992-03-11
JPS6433104U (en) * 1987-08-24 1989-03-01

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20150036663A (en) * 2012-08-24 2015-04-07 지멘스 악티엔게젤샤프트 Medical device

Also Published As

Publication number Publication date
JPH02274231A (en) 1990-11-08

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