JP2006258779A - Rectangular type resonator for electron spin resonance - Google Patents

Rectangular type resonator for electron spin resonance Download PDF

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JP2006258779A
JP2006258779A JP2005116230A JP2005116230A JP2006258779A JP 2006258779 A JP2006258779 A JP 2006258779A JP 2005116230 A JP2005116230 A JP 2005116230A JP 2005116230 A JP2005116230 A JP 2005116230A JP 2006258779 A JP2006258779 A JP 2006258779A
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resonator
magnetic field
microwave
cut
wall surface
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Hiroaki Oya
博昭 大矢
Morihisa Yamashita
盛久 山下
Takuo Shiraishi
卓夫 白石
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Keycom Corp
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Abstract

<P>PROBLEM TO BE SOLVED: To obtain a rectangular type resonator which enables high-sensitivity measurement of electron spin resonance, has a high Q-value, and introduces an external modulated magnetic field. <P>SOLUTION: This resonator is a TE<SB>102</SB>rectangular type resonator, has at least one cut line in the direction parallel to the flow of current formed in the direction of energy propagation of a microwave, and has neither a cut line nor a connecting part in the direction perpendicular to this, in a wall surface made up of an electric conductor. The resonator is composed of its lower part 31 and its upper part 32 which separate in the direction of the cut line. At the wall surface through which an AC magnetic field is intended to be guided into the resonator from outside, a conductor thickness is not larger than 0.3 mm, and a cut line whose width is between 1 mm and 5 mm is formed. Moreover, the quantity of reflection of an electromagnetic wave from the resonator can be adjusted in this resonator, by inserting two conductors or more at fixed intervals in a direction of vertically piercing the wall of the longitudinal diameter part of a waveguide being connected to the resonator, and adjusting the insertion length of these conductors. <P>COPYRIGHT: (C)2006,JPO&NCIPI

Description

マイクロ波を利用する計測技術に関わる発明であり、特に電子スピン共鳴装置において小型で高感度な計測を実現する共振器を提供するものである。  The present invention relates to a measurement technique using a microwave, and particularly to provide a resonator that realizes a small and highly sensitive measurement in an electron spin resonance apparatus.

電子スピン共鳴信号の観察は、磁場中に置かれた試料にマイクロ波を照射し電子スピン共鳴現象に起因するマイクロ波の吸収を検出する。この時僅かなマイクロ波の吸収を効率よく検出するために共振器を用いる。一般的に、共振器内に設置された試料に照射されたマイクロ波の反射が最小になるように共振器を調整し、磁場掃引によって生じるマイクロ波の吸収による反射の増加を検出する方式が取られている。この時、電気的雑音を軽減するために主磁場に加えて100kHz程度の周波数の変調磁場を印加し、この100kHzで変調されている信号のみを検出することにより感度の向上を図っている。  In the observation of the electron spin resonance signal, a sample placed in a magnetic field is irradiated with microwaves to detect absorption of the microwaves caused by the electron spin resonance phenomenon. At this time, a resonator is used to efficiently detect slight microwave absorption. Generally, a method is adopted in which the resonator is adjusted so that the reflection of the microwave irradiated to the sample placed in the resonator is minimized, and the increase in reflection due to the absorption of the microwave caused by the magnetic field sweep is detected. It has been. At this time, in order to reduce electrical noise, a modulation magnetic field having a frequency of about 100 kHz is applied in addition to the main magnetic field, and the sensitivity is improved by detecting only the signal modulated at 100 kHz.

電子スピン共嗚に用いられる共振器には複数のタイプがあるが、一般的にはTE011円筒型共振器とTE102矩形型共振器である。円筒型共振器は良好な共振特性(Q値=100,000以上)を有するが、磁場方向の幅が比較的大きいとともに水溶液試料を測定する場合はQ値が大きく低下する。一方、矩形型共振器は測定に必要な磁場を与えるマグネットに挟まれる部分の共振器の幅を狭くすることが出来るため、比較的容易に磁場供給マグネットが製作し易い。しかし、Q値が低く高感度測定に適していない。There are a plurality of types of resonators used for electron spin symbiosis. Generally, a TE 011 cylindrical resonator and a TE 102 rectangular resonator are used. Although the cylindrical resonator has good resonance characteristics (Q value = 100,000 or more), the width in the magnetic field direction is relatively large and the Q value is greatly reduced when measuring an aqueous solution sample. On the other hand, the rectangular resonator can narrow the width of the resonator sandwiched between the magnets that provide a magnetic field necessary for measurement, and therefore it is relatively easy to manufacture a magnetic field supply magnet. However, the Q value is low and it is not suitable for high sensitivity measurement.

矩形型共振器に関する先行技術として、特開2004−286757では電子スピン共鳴測定のための外部変調磁場が共振器内部に導入されやすい形状を提案しているが、マイクロ波のエネルギー伝搬方向に形成される電流の流れに直交する方向に接続部を有する構造であるため高いQ値は得られない。
特開2004−286757号公報
As a prior art related to a rectangular resonator, Japanese Patent Application Laid-Open No. 2004-286757 proposes a shape in which an external modulation magnetic field for electron spin resonance measurement is easily introduced into the resonator, but is formed in the direction of microwave energy propagation. A high Q value cannot be obtained because it has a connection portion in a direction orthogonal to the current flow.
JP 2004-286757 A

円筒型共振器は高いQ値を示し高感度な電子スピン共鳴測定を可能にするが、最も一般的なXバンド周波数帯のマイクロ波を用いた測定では少なくとも50X50mm以上の共振空間を必要とするため、電磁石は約60mm以上のポールピース間隔で330mT程度の磁場を供給する能力が必要となる。このため電磁石部分が大きくなり、現在市販されている装置ではサイズ400(w)X500(D)X500(H)mm以上、重量100kg以上である。なお、測定感度を低下させるとこなくポールピース間を狭くすることが可能であれば、装置の小型化・低コスト化が実現される。この発明は、この課題を解決するために小型化に適した矩形型共振器において、高いQ値を有し実用的な高感度電子スピン共鳴測定を可能とする構造を提案するものである。  The cylindrical resonator has a high Q value and enables highly sensitive electron spin resonance measurement. However, measurement using a microwave in the most common X band frequency band requires a resonance space of at least 50 × 50 mm or more. The electromagnet needs to be capable of supplying a magnetic field of about 330 mT with a pole piece interval of about 60 mm or more. For this reason, an electromagnet part becomes large and the apparatus currently marketed is size 400 (w) X500 (D) X500 (H) mm or more and the weight of 100 kg or more. If the gap between the pole pieces can be reduced without reducing the measurement sensitivity, the apparatus can be reduced in size and cost. In order to solve this problem, the present invention proposes a structure having a high Q value and enabling practical high-sensitivity electron spin resonance measurement in a rectangular resonator suitable for miniaturization.

本発明が提案する共振器は、TE102矩形型共振器であって、電気導体からなる壁面において、マイクロ波のエネルギー伝搬方向に形成される電流の流れに平行な方向に少なくとも1つ以上の切れ目が有り、しかもこれに直交する方向には切れ目および接続部が無いことを特徴とする。The resonator proposed by the present invention is a TE 102 rectangular resonator, and has at least one cut line in a direction parallel to a current flow formed in a direction of microwave energy propagation on a wall surface made of an electric conductor. In addition, there is no cut and no connection portion in a direction orthogonal to this.

さらに、本発明の共振器において、外部から交流磁界を共振器内に導入しようとする少なくともその壁面の導体厚さが0.3mm以下であることを特徴とする。  Furthermore, in the resonator according to the present invention, the conductor thickness of at least the wall surface of the AC magnetic field to be introduced into the resonator from the outside is 0.3 mm or less.

加えて、本発明の共振器において、外部から交流磁界を共振器内に導入しようとする、少なくともその壁面の導体の切れ目において、切れ目の幅が1mmから5mmの間であることを特徴とする。  In addition, the resonator according to the present invention is characterized in that the width of the cut is between 1 mm and 5 mm at least in the cut of the conductor on the wall surface to introduce an AC magnetic field into the resonator from the outside.

さらに加えて、上記の共振器において、共振器に接続している導波管の長径部分の壁を垂直に突き抜ける方向に一定間隔を置いて2本以上の導体を挿入し、この導体の挿入長を調整することにより、共振器からの電磁波の反射量を調整できることを特徴とする。  In addition, in the above resonator, two or more conductors are inserted at a predetermined interval in a direction perpendicularly penetrating the wall of the long diameter portion of the waveguide connected to the resonator, and the insertion length of the conductors The amount of reflection of the electromagnetic wave from the resonator can be adjusted by adjusting.

電界方向に一体の導電体から成ることによって良好な共振特性(高いQ値)が得られる。この構造は製作が容易であり、低コスト化に寄与する。さらに側面にスリットを設けることで外部変調磁場が内部に導入される。この時、スリットは前記の電界を切断しない方向に設けられるためQ値の低下は抑制される。この共振器のマイクロ波の結合調整は、接続するHコーナー導波管に設けたスタブによって比較的容易に行われる。  Good resonance characteristics (high Q value) can be obtained by comprising an integral conductor in the electric field direction. This structure is easy to manufacture and contributes to cost reduction. Furthermore, an external modulation magnetic field is introduced inside by providing a slit on the side surface. At this time, since the slit is provided in a direction not cutting the electric field, a decrease in the Q value is suppressed. The coupling adjustment of the microwave of the resonator is relatively easily performed by a stub provided in the H corner waveguide to be connected.

以上のように本発明を用いることで、共振特性の良好な矩形型共振器が実現する。これによって、現状の測定感度を低下させることなく、装置全体の小型化・低コスト化が可能となる。  By using the present invention as described above, a rectangular resonator having good resonance characteristics is realized. As a result, the entire apparatus can be reduced in size and cost without reducing the current measurement sensitivity.

以下に本発明の実施例について述べる。  Examples of the present invention will be described below.

図1に一般的な矩形型共振器11を示した。マイクロ波は導波管を経て、マイクロ波導入口12から共振器内に導入され、共振状態では共振器11内にマイクロ波磁界14を形成する。この時、マイクロ波電界は磁界に垂直方向に形成される。電子スピン共鳴測定を行う時には、試料挿入口から鉛直方向に試料が挿入されるため、測定に際しての共振特性(Q値)に影響を与える電界はエネルギー伝搬方向15に沿った向きに壁面に形成される電界である。図2に示した切れ目面21に沿って接続面または切れ目(スリット)を設けることで、マイクロ波電界を遮断することをなくQ値の高い共振器を得ることが可能となる。図2では上下面の中間に切れ目面を描いている。切れ目面の位置は共振器内の上下壁の中間であることが望ましく、そこからずれるに従ってQ値の低下を招く。しかしながら、共振器を用いた測定に求められる感度の許容範囲であれば、厳密に中間位置である必要はない。  FIG. 1 shows a general rectangular resonator 11. The microwave is introduced into the resonator from the microwave inlet 12 through the waveguide, and forms a microwave magnetic field 14 in the resonator 11 in the resonance state. At this time, the microwave electric field is formed in a direction perpendicular to the magnetic field. When performing electron spin resonance measurement, the sample is inserted in the vertical direction from the sample insertion port, so that an electric field that affects the resonance characteristics (Q value) at the time of measurement is formed on the wall surface in the direction along the energy propagation direction 15. Electric field. By providing a connection surface or a cut (slit) along the cut surface 21 shown in FIG. 2, a resonator having a high Q value can be obtained without blocking the microwave electric field. In FIG. 2, a cut surface is drawn between the upper and lower surfaces. The position of the cut surface is preferably in the middle of the upper and lower walls in the resonator, and the Q value is lowered as the distance is shifted. However, if the sensitivity is within the allowable range required for the measurement using the resonator, it is not necessary to be strictly at the intermediate position.

図3には図2に示した切れ目面21に対応する位置を接続面33とする共振器下部31と共振器上部32を示した。接続面33の固定は機械的なもので充分である。側面または前後面にネジ穴を開け金属板に固定してよいし、上下から挟み込んでもよい。  FIG. 3 shows a resonator lower portion 31 and a resonator upper portion 32 having a connection surface 33 at a position corresponding to the cut surface 21 shown in FIG. The connection surface 33 may be fixed mechanically. Screw holes may be made on the side or front and back surfaces and fixed to the metal plate, or may be sandwiched from above and below.

図4は、外部変調磁場を導入するために側面部に設けたスリット41を示した。外部から印加する変調磁場を積極的に共振器11内部に導入するために、前述の切れ目をスリット41として複数個設けてある。スリット41は図2に示した切れ目面21に平行で幅は1mmから5mmの間であることが必要であるが、スリット41の数は任意である。スリット41の数が多くなり開口幅が大きくなると、外部変調磁場は内部に導入され易くなるが共振器のQ値は低下する。設計に際して、変調磁場の大きさとQ値のトレイドオフを考えなければならない。  FIG. 4 shows a slit 41 provided on the side surface for introducing an external modulation magnetic field. In order to positively introduce a modulation magnetic field applied from the outside into the resonator 11, a plurality of the aforementioned cuts are provided as the slits 41. The slits 41 are required to be parallel to the cut surface 21 shown in FIG. 2 and have a width between 1 mm and 5 mm, but the number of slits 41 is arbitrary. When the number of slits 41 increases and the opening width increases, the external modulation magnetic field is easily introduced inside, but the Q value of the resonator decreases. In designing, the magnitude of the modulation magnetic field and the trade-off of the Q value must be considered.

図5に共振器にHコーナー導波管52を接続した様子を示した。ここでは、共振器下部31と共振器上部32は、固定板51と導波管端に設けられたフランジによって固定されている。Hコーナー導波管52のコーナー部中央に設置したスタブ53の出し入れによって、共振器のマイクロ波結合を調整する。  FIG. 5 shows a state in which the H corner waveguide 52 is connected to the resonator. Here, the resonator lower portion 31 and the resonator upper portion 32 are fixed by a fixing plate 51 and a flange provided at the waveguide end. The microwave coupling of the resonator is adjusted by inserting and removing the stub 53 installed at the center of the corner portion of the H corner waveguide 52.

図6に作製した共振器の共振特性を、マイクロ波周波数に対する吸収率で示した。水溶液の電子スピン共鳴を測定するための石英セルに蒸留水を充填し、これを共振器内に設置して測定した。Q値として4000以上の高い値が得られ、本発明によってコンパクトな矩形型共振器を用いた高感度な電子スピン共鳴測定が可能となったことが確認された。  FIG. 6 shows the resonance characteristics of the manufactured resonator as an absorptance with respect to the microwave frequency. A quartz cell for measuring electron spin resonance of an aqueous solution was filled with distilled water, and this was set in a resonator and measured. A high Q value of 4000 or more was obtained, and it was confirmed that highly sensitive electron spin resonance measurement using a compact rectangular resonator was made possible by the present invention.

一般的な矩形型共振器と、内部に形成されるマイクロ波磁界を示す図である。It is a figure which shows a general rectangular resonator and the microwave magnetic field formed inside. 本発明の切れ目を入れる実施例を示す図である。It is a figure which shows the Example which makes the cut of this invention. 上下2つの部品から成る共振器の構成を示す図である。It is a figure which shows the structure of the resonator which consists of two upper and lower parts. 共振器にスリットを入れる実施例を示す図である。It is a figure which shows the Example which puts a slit in a resonator. 共振器にHコーナー導波管を接続した実施例を示す図である。It is a figure which shows the Example which connected the H corner waveguide to the resonator. 共振器の共振特性をマイクロ波周波数に対する吸収率で示した図である。It is the figure which showed the resonance characteristic of the resonator by the absorption factor with respect to a microwave frequency.

符号の説明Explanation of symbols

11 矩形型共振器
12 マイクロ波導入口
13 試料挿入口
14 マイクロ波磁界
15 エネルギー伝搬方向
21 切れ目面
31 共振器下部
32 共振器上部
33 接続面
41 スリット
51 固定板
52 Hコーナー導波管
DESCRIPTION OF SYMBOLS 11 Rectangular type resonator 12 Microwave introduction port 13 Sample insertion port 14 Microwave magnetic field 15 Energy propagation direction 21 Cut surface 31 Resonator lower part 32 Resonator upper part 33 Connection surface 41 Slit 51 Fixing plate 52 H corner waveguide

Claims (4)

電気導体からなる壁面において、マイクロ波のエネルギー伝搬方向に形成される電流の流れに平行な方向に少なくとも1つ以上の切れ目が有り、しかもこれに直交する方向には切れ目および接続部が無いことを特徴とするTE102矩形型マイクロ波共振器。On the wall surface made of an electrical conductor, there should be at least one cut in the direction parallel to the current flow formed in the microwave energy propagation direction, and there should be no cut and no connection in the direction perpendicular to this. A TE 102 rectangular microwave resonator characterized. 外部から交流磁界を共振器内に導入しようとする少なくともその壁面の導体厚さが0.3mm以下であることを特徴とする請求項1に示す共振器。The resonator according to claim 1, wherein a conductor thickness of at least a wall surface of the AC magnetic field to be introduced into the resonator from the outside is 0.3 mm or less. 外部から交流磁界を共振器内に導入しようとする、少なくともその壁面の導体の切れ目において、切れ目の幅が1mmから5mmの間であることを特徴とする請求項2に示す共振器。3. The resonator according to claim 2, wherein the width of the cut is between 1 mm and 5 mm at least in the cut of the conductor on the wall surface to introduce an AC magnetic field into the resonator from the outside. 共振器に接続している導波管の長径部分の壁を垂直に突き抜ける方向に一定間隔を置いて2本以上の導体を挿入し、この導体の挿入長を調整することにより、共振器からの電磁波の反射量を調整できることを特徴とする請求項1、請求項2、請求項3に示す共振器。By inserting two or more conductors at regular intervals in a direction that penetrates the wall of the long-diameter portion of the waveguide connected to the resonator vertically, and adjusting the insertion length of the conductor, 4. The resonator according to claim 1, wherein the amount of reflection of electromagnetic waves can be adjusted.
JP2005116230A 2005-03-17 2005-03-17 Rectangular type resonator for electron spin resonance Pending JP2006258779A (en)

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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP2273535A3 (en) * 2009-07-10 2011-07-06 LG Electronics Electrodeless lighting system

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP2273535A3 (en) * 2009-07-10 2011-07-06 LG Electronics Electrodeless lighting system
US8508131B2 (en) 2009-07-10 2013-08-13 Lg Electronics Inc. Electrodeless lighting system

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