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JP5224461B2 - Method for producing contrast medium - Google Patents
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JP5224461B2 - Method for producing contrast medium - Google Patents

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JP5224461B2
JP5224461B2 JP2009021568A JP2009021568A JP5224461B2 JP 5224461 B2 JP5224461 B2 JP 5224461B2 JP 2009021568 A JP2009021568 A JP 2009021568A JP 2009021568 A JP2009021568 A JP 2009021568A JP 5224461 B2 JP5224461 B2 JP 5224461B2
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nuclear spin
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polarization
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radicals
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高之 熊田
洋平 能田
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Description

本発明は、NMR(核磁気共鳴:Nuclear Magnetic Resonance)を用いた生体診断や有機化学の分子構造解析などにおいて、被分析試料のNMR信号検出感度の向上に有効な方法等に関する。より具体的には、紫外線を用いた有機ラジカル種の製造方法、並びに該有機ラジカル種にさらに動的核スピン偏極(Dynamic Nuclear Polarization: 以下必要に応じてDNPと呼ぶ)を行ってNMR信号検出感度を向上させた造影剤の製造方法及びその製造方法によって製造される造影剤に関する。   The present invention relates to a method effective for improving NMR signal detection sensitivity of a sample to be analyzed in biodiagnosis using NMR (Nuclear Magnetic Resonance), molecular structure analysis of organic chemistry, and the like. More specifically, a method for producing an organic radical species using ultraviolet rays, and an NMR signal detection by further performing dynamic nuclear polarization (hereinafter referred to as DNP if necessary) on the organic radical species. The present invention relates to a method for producing a contrast agent with improved sensitivity and a contrast agent produced by the method.

NMRは、磁気モーメントを有する原子核を含んだ被測定試料を数テスラの強磁場中に置き、これに共鳴条件を満足する周波数の電磁波を加えたときに生じる共鳴現象を言う。原子核の磁気モーメントを核スピンと呼び、NMRでは該核スピンのエネルギー吸収・放出過程を観測する。通常は、共鳴周波数の電磁波を停止した直後の核スピン放出エネルギーをサーチコイルで電気信号として検出し、検出された電気信号をNMR信号と呼ぶ。NMRは、生体診断や分子構造解析などにおいて有用とされているが、NMR信号の検出感度が低いといった本質的な欠点を有しているため、NMR信号の検出感度向上に関する種々の技術開発が行われている。   NMR refers to a resonance phenomenon that occurs when a sample to be measured containing nuclei having a magnetic moment is placed in a strong magnetic field of several Tesla and an electromagnetic wave having a frequency satisfying the resonance condition is applied thereto. The magnetic moment of a nucleus is called a nuclear spin, and NMR observes the energy absorption and emission processes of the nuclear spin. Normally, the nuclear spin emission energy immediately after stopping the electromagnetic wave having the resonance frequency is detected as an electric signal by a search coil, and the detected electric signal is called an NMR signal. Although NMR is considered useful for biodiagnosis and molecular structure analysis, it has the inherent disadvantage of low NMR signal detection sensitivity, and various technological developments related to improving NMR signal detection sensitivity have been conducted. It has been broken.

技術開発の主なものとしては、
1)更なる強磁場化
2)NMR信号検出回路の低ノイズ化
3)動的核スピン偏極方法の採用
が挙げられ、本発明は、3)動的核スピン偏極方法に関するものである。
動的核スピン偏極方法は、電子スピンを有するラジカル種に強磁場及びマイクロ波を加えて、電子スピン偏極を核スピン偏極に移行させることにより、NMR信号の強度を高めるものである。
The main technological developments are:
1) Further strong magnetic field
2) Low noise in NMR signal detection circuit
3) Adoption of dynamic nuclear spin polarization method is mentioned, and the present invention relates to 3) dynamic nuclear spin polarization method.
The dynamic nuclear spin polarization method increases the intensity of an NMR signal by applying a strong magnetic field and microwaves to a radical species having electron spin to shift the electron spin polarization to nuclear spin polarization.

動的核スピン偏極を行うためには、試料中にラジカルが1019spins/cm3程度存在しなくてはならない。従来までに
A.トリチルラジカルやニトロキシラジカルなどの安定ラジカルを混入する、
B.電子線照射により極低温固体試料中にラジカルを発生させる(非特許文献1及び2を参照)、
C.ペンタセンなどの光励起スピン三重項を用いる(非特許文献3を参照)
手法が報告されている。また、動的核スピン偏極を行うための装置としては、オックスフォードインスツルメンツ社のハイパーセンス(HyperSense:登録商標)が知られている(非特許文献4を参照)。
In order to perform dynamic nuclear spin polarization, there must be about 10 19 spins / cm 3 of radicals in the sample. Until now
A. Incorporating stable radicals such as trityl radicals and nitroxy radicals,
B. Generate radicals in a cryogenic solid sample by electron beam irradiation (see Non-Patent Documents 1 and 2),
Uses photoexcited spin triplet such as C. pentacene (see Non-Patent Document 3)
Methods have been reported. As a device for performing dynamic nuclear spin polarization, HyperSense (registered trademark) of Oxford Instruments is known (see Non-Patent Document 4).

D.G.Crabb et al. Phys. Rev. Lett. 64, 2627(1990)D.G.Crabb et al. Phys. Rev. Lett. 64, 2627 (1990) S. T. Goertz et al. Nucl. Inst. Meth. A 526, 43 (2004)S. T. Goertz et al. Nucl. Inst. Meth. A 526, 43 (2004) M.Iinuma et al. Phys. Rev. Lett. 84,171(2000)M.Iinuma et al. Phys. Rev. Lett. 84,171 (2000) Oxford Instruments Molecular Biotools Ltd.のHyperSense(登録商標)のカタログ(Hyp/01/A/0306)Catalog of HyperSense (registered trademark) of Oxford Instruments Molecular Biotools Ltd. (Hyp / 01 / A / 0306) E. R. McCarney and S. Han, J. Mag. Res. 190,307(2008)E. R. McCarney and S. Han, J. Mag. Res. 190,307 (2008) J. H Ardenkjaer-Larsen et al. Appl. Phys. Sci.100,10158(2003)J. H Ardenkjaer-Larsen et al. Appl. Phys. Sci. 100, 10158 (2003)

DNP法は、試料中に混入した電子スピンから核スピンへ偏極移動することで、電子スピンと同等の核スピン偏極度を得る手法である。室温、3.5テスラの磁場下における水素核スピンの偏極度はわずか10-4%程度であるが、DNP法を極低温下で用いれば、原理的には100%近くまで引き上げることができる。NMRの信号強度は核スピン偏極度に比例する。核スピン緩和時間より早く、DNP装置中で得られた高核スピン偏極状態の極低温の試料を融解して、NMR装置に移送し測定すれば、原理的に信号強度が6ケタ高いNMR信号を得ることができる。 The DNP method is a technique for obtaining a nuclear spin polarization equivalent to an electron spin by performing a polarization transfer from an electron spin mixed in a sample to a nuclear spin. The polarization degree of hydrogen nuclear spins at room temperature under a magnetic field of 3.5 Tesla is only about 10 -4 %. However, if the DNP method is used at an extremely low temperature, it can be raised to nearly 100% in principle. The NMR signal intensity is proportional to the nuclear spin polarization. An NMR signal whose signal intensity is 6 digits higher in principle if the cryogenic sample in the high nuclear spin polarization state obtained in the DNP apparatus is melted, transferred to the NMR apparatus, and measured before the nuclear spin relaxation time. Can be obtained.

前に戻って、前述のA.は、最も容易に試料中にラジカルを導入できる手法であり、DNP実験に一般に用いられてきた手法であるが、次の二つの問題点があった。
安定ラジカルは試料融解後も残存し、核スピン偏極度の減少を促進するため、安定ラジカルを混入した試料では、造影剤としての効果を長時間維持することができない。
動物のNMR測定を行なう上での、安定ラジカルの毒性。
Returning to the previous section, the above-mentioned A. is a technique that can introduce radicals most easily into a sample, and is a technique that has been generally used in DNP experiments, but has the following two problems.
Since stable radicals remain even after the sample is melted and promotes a decrease in the degree of nuclear spin polarization, a sample mixed with stable radicals cannot maintain the effect as a contrast agent for a long time.
Toxicity of stable radicals in animal NMR measurements.

この問題を解決するため、安定ラジカルをエアロゲルに付着させることで、偏極溶液からラジカルを分離する研究(非特許文献5を参照)もあるが、その最大偏極度は室温熱平衡時の値の僅か40倍程度であり、B.の手法を用いたこれまでの報告値(>10000, 非特許文献6を参照)よりはるかに低い。   In order to solve this problem, there is a study (see Non-Patent Document 5) that separates radicals from a polarized solution by attaching stable radicals to the airgel. However, the maximum degree of polarization is slightly less than that at room temperature thermal equilibrium. It is about 40 times, which is much lower than the reported value using the method of B. (> 10000, see Non-Patent Document 6).

A.の安定ラジカルとは異なり、B.の手法によって極低温固体試料中に生成したラジカルは、融解とともに消失するため、A.の手法に比べ造影剤としての効果が長続きし、ラジカルの毒性も考慮する必要がない。しかし、
電子線は磁場下では曲がってしまうため、動的核スピン偏極装置を消磁するか、一定距離以上離れた場所で試料を照射しなくてはならない。照射後の試料は、極低温環境を維持したまま動的核スピン偏極装置に搬送しなくてはならない。
さらに、電子線は物質透過性が低いため、極低温の試料を容器から取り出して照射しなくてはならない。
放射線防護などの対策が必要になる。
などと、電子線照射実験は大変煩雑であるため、本手法はほとんど用いられてこなかった。
Unlike the stable radical of A., the radical generated in the cryogenic solid sample by the method of B. disappears with melting, so the effect as a contrast agent lasts longer than the method of A. There is no need to consider. But,
Since an electron beam bends in a magnetic field, the dynamic nuclear spin polarization device must be demagnetized or the sample must be irradiated at a location more than a certain distance away. The irradiated sample must be transported to a dynamic nuclear spin polarization device while maintaining a cryogenic environment.
Furthermore, since the electron beam has a low material permeability, a very low temperature sample must be taken out from the container and irradiated.
Measures such as radiation protection are required.
Since the electron beam irradiation experiment is very complicated, this method has hardly been used.

C.はペンタセンの有機溶媒に対する溶解度が低いこと、レーザー光を入射するにあたって、固体試料でありながら高い透明度を要することから、ナフタレン結晶など非常に限られた媒質でしか用いることができない。   C. can be used only in very limited media such as naphthalene crystals because pentacene has a low solubility in organic solvents and requires high transparency even though it is a solid sample when laser light is incident.

本発明の目的は、有機ラジカル製造が容易な有機ラジカル種の製造方法、並びに、毒性が低く、造影作用が持続する、動的核スピン偏極法を用いた造影剤の製造方法とその製造方法によって製造される造影剤を提供することにある。   An object of the present invention is to provide a method for producing an organic radical species that is easy to produce organic radicals, and a method for producing a contrast agent using a dynamic nuclear spin polarization method that has low toxicity and maintains a contrast effect. It is in providing the contrast agent manufactured by this.

前述の目的を達成するため、本発明の一つの観点に係る有機ラジカル種の製造方法においては、有機溶媒中に微量の光解離性分子を添加し、極低温下で紫外線を照射し、多数の有機ラジカルを発生させるようにしている。また、有機溶媒中に添加される前記光解離性分子の量は、0.1〜1wt%である。   In order to achieve the aforementioned object, in the method for producing an organic radical species according to one aspect of the present invention, a small amount of photodissociable molecules are added to an organic solvent, irradiated with ultraviolet rays at an extremely low temperature, An organic radical is generated. The amount of the photolabile molecule added to the organic solvent is 0.1 to 1 wt%.

また、本発明の他の観点に係る造影剤の製造方法においては、光解離性分子を混入した極低温有機溶媒に、紫外線を照射して生成した有機ラジカルを用いて動的核スピン偏極を行なっている。   In addition, in the method for producing a contrast agent according to another aspect of the present invention, dynamic nuclear spin polarization is performed using an organic radical generated by irradiating ultraviolet light to a cryogenic organic solvent mixed with a photolabile molecule. Is doing.

有機溶媒中に微量の光解離性分子を添加しておき、極低温下で紫外線を照射することで、分子解離とその副次反応が誘発される。この現象を利用して、動的核スピン偏極に用いる大量のラジカルを作ることができる。電子線と異なり紫外線は、線源が小さく放射線防護の必要がない。特に波長200nm以上の紫外線は、空気中の酸素のオゾン化を引き起こさないため、取り扱いが容易で安全性が高い。また、磁場によって曲げられることはなく、試料セルに石英等を用いれば、試料をセルから取り出すことなく照射できる。また、光ファイバを用い、動的核スピン偏極装置中心の試料部まで容易に紫外光を導くこともできる。   Molecular dissociation and its side reactions are induced by adding a small amount of photodissociable molecules in an organic solvent and irradiating ultraviolet rays at an extremely low temperature. Using this phenomenon, a large amount of radicals used for dynamic nuclear spin polarization can be produced. Unlike electron beams, ultraviolet rays are small and do not require radiation protection. In particular, ultraviolet rays having a wavelength of 200 nm or more are easy to handle and highly safe because they do not cause ozonization of oxygen in the air. In addition, if the sample cell is made of quartz or the like without being bent by the magnetic field, the sample can be irradiated without being taken out of the cell. In addition, it is possible to easily guide ultraviolet light to the sample portion at the center of the dynamic nuclear spin polarization apparatus using an optical fiber.

上述の造影剤の製造において、好適には、有機溶媒として0.1〜1重量パーセント(wt%)のフェノールを光解離性分子として含有するブタノールが使用される。   In the production of the contrast agent described above, butanol containing 0.1 to 1 weight percent (wt%) phenol as a photolabile molecule is preferably used as the organic solvent.

また、造影剤の製造にあたっては、前記光解離性分子を含む前記有機溶媒を動的核スピン偏極装置内に置き、紫外線透過型光ファイバを介して紫外線を前記有機溶媒に導くことにより、紫外線照射と動的核スピン偏極を同一個所にて行うことで、融解を防ぎながら低温固体試料を紫外線照射部から動的核スピン偏極装置に搬送するわずらわしさを避けることができる。   Further, in the production of a contrast agent, the organic solvent containing the photolabile molecule is placed in a dynamic nuclear spin polarization device, and ultraviolet rays are guided to the organic solvent via an ultraviolet transmission optical fiber. By performing irradiation and dynamic nuclear spin polarization at the same location, it is possible to avoid the hassle of transporting a low-temperature solid sample from the ultraviolet irradiation section to the dynamic nuclear spin polarization apparatus while preventing melting.

本発明のさらに他の観点に係る造影剤は、微量の光解離性分子を混入した極低温有機溶媒に、紫外線を照射して生成した有機ラジカルを用いて動的核スピン偏極を行うことにより、極めて簡単な設備で製造できる。紫外線分解により極低温試料中に生じたラジカルは、一般に反応性が高く、解凍直後に他のラジカルとの再結合反応などを通じて瞬時に消失して、反応性・毒性の低い分子になる。したがって、これまで安定ラジカルを用いた手法で問題となっていた、毒性や解凍後の脱偏極の問題が解決される。   The contrast agent according to still another aspect of the present invention is to perform dynamic nuclear spin polarization using an organic radical generated by irradiating ultraviolet light to a cryogenic organic solvent mixed with a trace amount of photolabile molecules. Can be manufactured with extremely simple equipment. The radical generated in the cryogenic sample by ultraviolet decomposition is generally highly reactive, and immediately disappears through a recombination reaction with another radical immediately after thawing to become a molecule having low reactivity and toxicity. Therefore, the problem of toxicity and depolarization after thawing, which has been a problem with the technique using stable radicals, is solved.

本発明によれば、前述のA.の手法と同程度の手間で、これまで煩雑なB.の手法でしか得られなかった、溶融時に消失するために核スピンの脱偏極や動物試料に対し害を与えることのないラジカルを、大量に発生させることができる。したがって、本発明によれば、NMR信号検出感度が極めて高い造影剤を得ることができる。   According to the present invention, with the same degree of effort as the method of A. described above, it has been obtained only by the complicated method of B. A large amount of radicals that do not cause harm can be generated. Therefore, according to the present invention, a contrast agent having extremely high NMR signal detection sensitivity can be obtained.

本発明の一実施形態に係る動的核スピン偏極を行うことによる造影剤の製造方法を実施するための装置の概略説明図である。It is a schematic explanatory drawing of the apparatus for enforcing the manufacturing method of the contrast agent by performing dynamic nuclear spin polarization concerning one embodiment of the present invention. 紫外線によるラジカルの発生と動的核スピン偏極を検証するための実験装置の概略説明図である。It is a schematic explanatory drawing of the experimental apparatus for verifying the generation of radicals by ultraviolet rays and the dynamic nuclear spin polarization. 実験によって得られた結果を示す図であって、本発明の造影剤を用いて動的核スピン偏極を起こす前(熱平衡時)と後(核スピン偏極時)のNMR信号の強度変化を説明するための図である。It is a figure which shows the result obtained by experiment, Comprising: The intensity | strength change of the NMR signal before (at the time of thermal equilibrium) and after (at the time of nuclear spin polarization) which raise | generates dynamic nuclear spin polarization using the contrast agent of this invention is shown. It is a figure for demonstrating. 電子スピン法により決定した、77Kブタノール/フェノール(0.1 wt.%)試料中におけるラジカル濃度と紫外線照射時間との相関を示す図である。It is a figure which shows the correlation with the radical concentration and ultraviolet irradiation time in a 77K butanol / phenol (0.1 wt.%) Sample determined by the electron spin method. ブタノール/フェノール(0.3 wt.%)試料への紫外線照射時間と、4.2 K熱平衡時のNMR信号強度に対する4.2K偏極時のNMR信号強度の関係を示す図である。It is a figure which shows the ultraviolet signal irradiation time to a butanol / phenol (0.3 wt.%) Sample, and the relationship of the NMR signal intensity at the time of 4.2K polarization with respect to the NMR signal intensity at the time of 4.2 K thermal equilibrium. フェノール濃度と、4.2 K熱平衡時のNMR信号強度に対する1.5K偏極時のNMR信号強度の比との関係を示す図である。It is a figure which shows the relationship between a phenol concentration and the ratio of the NMR signal intensity at the time of 1.5K polarization with respect to the NMR signal intensity at the time of 4.2 K thermal equilibrium.

本発明は(電子線照射法で作られるような、極低温固体中でのみ安定で、融解と同時に瞬時に消失するラジカルを、紫外線分解法を用いて極めて容易に作成し、動的核スピン偏極に用いられるようにしたものである。放射線と異なり、紫外線の吸光係数及び分解確率は、分子の形状に強く依存する。本発明の一実施形態では、偏極試料に紫外線分解しやすいフェノールを光解離性分子として混入させている。   The present invention makes it very easy to create radicals that are stable only in cryogenic solids, such as those produced by electron beam irradiation, and that disappear instantaneously upon melting, using the ultraviolet decomposition method. Unlike radiation, the extinction coefficient and decomposition probability of ultraviolet light strongly depend on the shape of the molecule.In one embodiment of the present invention, phenol that is susceptible to ultraviolet decomposition is applied to a polarized sample. It is mixed as a photolabile molecule.

光解離性分子には、光ファイバ、石英窓、大気に対して透過性の高い波長の紫外線で分解し、水素原子を発生させるものがよい。ほとんどの有機物の炭素‐水素間結合の結合力は、水素分子の水素‐水素間の結合力より小さいため、紫外線照射によって生成した水素原子は有機溶媒から水素原子を引き抜き、炭素の部位に不対電子を持つラジカルを作る。炭素部位に不対電子を持つラジカルは、電子スピン共鳴のg値の異方性が小さく、強磁場電子スピン共鳴スペクトルの線幅が細いため、動的核スピン偏極を引き起こしやすい。   The photolabile molecule is preferably an optical fiber, a quartz window, or a molecule that decomposes with ultraviolet rays having a wavelength that is highly permeable to the atmosphere to generate hydrogen atoms. Since the bonding force of carbon-hydrogen bonds of most organic substances is smaller than the hydrogen-hydrogen bonding force of hydrogen molecules, hydrogen atoms generated by ultraviolet irradiation draw hydrogen atoms from organic solvents and unpair with carbon sites. Create radicals with electrons. A radical having an unpaired electron at a carbon site is likely to cause dynamic nuclear spin polarization because the g-value anisotropy of electron spin resonance is small and the line width of the strong magnetic field electron spin resonance spectrum is narrow.

以下図面を参照して、本発明の一実施形態について詳細に説明する。図1は、本発明の一実施形態に係る動的核スピン偏極を行うことによる造影剤の製造方法を実施するための装置の概略説明図である。図1において、20がNMR装置であり、19はマイクロ波発生装置、11が動的核スピン偏極装置、そして12、13が紫外線発生装置である。また、14は紫外線透過型光ファイバ、15は偏極用コイル、16は試料、17は偏極試料輸送管、18は偏極試料輸送管17の先端に取り付けた、生体内に造影剤を注入するための作業器具である。   Hereinafter, an embodiment of the present invention will be described in detail with reference to the drawings. FIG. 1 is a schematic explanatory diagram of an apparatus for carrying out a method for producing a contrast agent by performing dynamic nuclear spin polarization according to an embodiment of the present invention. In FIG. 1, 20 is an NMR apparatus, 19 is a microwave generator, 11 is a dynamic nuclear spin polarization apparatus, and 12 and 13 are ultraviolet generators. In addition, 14 is an ultraviolet transmission optical fiber, 15 is a polarization coil, 16 is a sample, 17 is a polarized sample transport tube, 18 is attached to the tip of the polarized sample transport tube 17, and a contrast agent is injected into the living body. It is a work implement to do.

紫外線透過型光ファイバ14は、水銀ランプやレーザーから成る紫外線発生装置12、13と動的核スピン偏極装置11の試料16間に設けれ、紫外線発生装置12、13で発生された紫外線を偏極試料に導くようになっている。試料16内の偏極試料にはフェノールなどの光解離性分子が少量混入されている。極低温に冷やされた試料に紫外線を照射し、ラジカルを生成した後に、マイクロ波発生装置19によって生じたマイクロ波を照射することで、同一箇所にて動的核スピン偏極を行う。動的核スピン偏極した試料は、安定ラジカルを用いた偏極試料と同様に、例えば熱湯を用いるなどして瞬時に融解した後、輸送管17を通じて瞬時にNMR装置20(またはNMR装置)まで移送する。ここで、動的核スピン偏極装置11、そこからNMR装置20まで延びている輸送管17、輸送管17の先端に設けられた作業器具18等はいずれも従来のNMR診断で使用されている装置、器具と同一の構造を有する。
<実験例>
The UV transmissive optical fiber 14 is provided between the UV generators 12 and 13 made of a mercury lamp or a laser and the sample 16 of the dynamic nuclear spin polarization device 11, and polarizes the UV generated by the UV generators 12 and 13. It leads to the pole sample. The polarized sample in the sample 16 is mixed with a small amount of photolabile molecules such as phenol. A sample cooled to a very low temperature is irradiated with ultraviolet rays to generate radicals, and then irradiated with microwaves generated by the microwave generator 19, thereby performing dynamic nuclear spin polarization at the same location. The dynamic nuclear spin-polarized sample, like the polarized sample using stable radicals, is instantly melted by using, for example, hot water, and then instantaneously reaches the NMR apparatus 20 (or NMR apparatus) through the transport tube 17. Transport. Here, the dynamic nuclear spin polarization device 11, the transport tube 17 extending from the dynamic nuclear spin polarization device 11 to the NMR device 20, and the work tool 18 provided at the tip of the transport tube 17 are all used in conventional NMR diagnosis. It has the same structure as the device and instrument.
<Experimental example>

本発明に係る造影剤の製造方法を検証するため、検証実験では、動的核スピン偏極装置11とは別の装置(容器)を用いて紫外線照射を行った後、動的核スピン偏極装置11に試料を移し替えて動的核スピン偏極を行った。図2は、紫外線によるラジカルの発生と動的核スピン偏極を検証するための実験装置の概略説明図である。図中、図1と同一符号は実質的に同一の機能を有する構成体を示し、21は石英製液体窒素用デュワー、22はガラス製液体ヘリウム用デュワーであり、各デュワーは従来のものを使用し、それぞれ独立して設置した。また、核スピン偏極度の測定は、核スピン偏極度測定用NMR装置23を用いて行った。   In order to verify the method for producing a contrast agent according to the present invention, in a verification experiment, after performing ultraviolet irradiation using an apparatus (container) different from the dynamic nuclear spin polarization apparatus 11, dynamic nuclear spin polarization is performed. The sample was transferred to the apparatus 11 for dynamic nuclear spin polarization. FIG. 2 is a schematic explanatory diagram of an experimental apparatus for verifying generation of radicals by ultraviolet rays and dynamic nuclear spin polarization. In the figure, the same reference numerals as those in FIG. 1 denote components having substantially the same function, 21 is a quartz liquid nitrogen dewar, 22 is a glass liquid helium dewar, and each dewar uses a conventional one. And installed independently. The nuclear spin polarization was measured using the NMR apparatus 23 for measuring nuclear spin polarization.

77Kの液体窒素で満たされた石英デュワー21中に、フェノールを含むブタノール試料を挿入し、固化した。固化後にデュワー21の外から水銀キセノンランプによる紫外線(三永電気SUPERCURE-352S、中心波長365nm, 5000mW)を1時間程度照射し、ブタノールのラジカルを1019 spins/cm3程度発生させた。室温中とは異なり、77Kではブタノールのラジカルは消滅しない。照射後、試料を液体ヘリウムで満たされた動的核スピン偏極装置11に手早く(10秒以内に)移し、4.2K、1.18テスラ下における熱平衡状態の水素のNMR信号を測定したのち、液体ヘリウムを減圧することで試料を1.5Kまで冷却し、マイクロ波照射(33.2 GHz、50 mW)により動的核スピン偏極を行った。 A butanol sample containing phenol was inserted into a quartz dewar 21 filled with 77K liquid nitrogen and solidified. After solidification, ultraviolet rays (Minaga Electric SUPERCURE-352S, central wavelength 365 nm, 5000 mW) from a mercury xenon lamp were irradiated from outside Dewar 21 for about 1 hour to generate about 10 19 spins / cm 3 of butanol radicals. Unlike at room temperature, butanol radicals do not disappear at 77K. After irradiation, the sample was quickly transferred (within 10 seconds) to the dynamic nuclear spin polarization device 11 filled with liquid helium, and after measuring the NMR signal of hydrogen in thermal equilibrium under 4.2K, 1.18 Tesla, liquid helium The sample was cooled to 1.5K by depressurizing and dynamic nuclear spin polarization was performed by microwave irradiation (33.2 GHz, 50 mW).

動的核スピン偏極の状態を核スピン偏極度測定用NMR装置23で測定した結果を図3に示す。図3は、紫外線照射したブタノール/フェノール(0.3 wt%)資料中における水素原子核のNMR信号強度を示している。図3において、縦軸(図示せず)のNMR信号強度(arb.)は核スピン偏極度に比例する。4.2K熱平衡時と動的核スピン偏極時の信号強度比から、偏極度が最大で約50倍になっていることがわかる。図3に示すように、NMR信号の強度は4.2Kの熱平衡信号に対して、4.2K動的偏極時には14倍に、1.5K動的偏極時には48倍の絶対偏極度1.3%に達した。この値は、1.l8Tesla室温における熱平衡時の偏極度4 x 10-4%の3000倍以上である。超電導マグネットを用い、より高い磁場で同様の実験を行えばより高い絶対偏極度が得られると考えられる。 FIG. 3 shows the result of measuring the state of dynamic nuclear spin polarization with the NMR device 23 for measuring nuclear spin polarization. FIG. 3 shows the NMR signal intensity of hydrogen nuclei in butanol / phenol (0.3 wt%) material irradiated with ultraviolet rays. In FIG. 3, the NMR signal intensity (arb.) On the vertical axis (not shown) is proportional to the nuclear spin polarization. From the signal intensity ratio between 4.2K thermal equilibrium and dynamic nuclear spin polarization, it is clear that the degree of polarization is up to about 50 times. As shown in FIG. 3, the intensity of the NMR signal reached 14% for 4.2K dynamic polarization and 48% for 1.5K dynamic polarization with respect to the 4.2K thermal equilibrium signal. . This value is more than 3000 times the degree of polarization 4 × 10 −4 % at 1.l8 Tesla room temperature thermal equilibrium. It is considered that a higher absolute polarization can be obtained if a similar experiment is performed with a higher magnetic field using a superconducting magnet.

図4に電子スピン共鳴法で決定した、ブタノール/フェノール試料中のラジカル濃度と紫外線照射時間の関係を示した。フェノール添加量1 wt%の試料中では、照射時間20分で、一旦ラジカル濃度が飽和するが、試料を回転すると再び濃度の増加がみられた。本結果から、1 wt%もフェノールを添加すると、紫外線が内径3.2ミリメートルの試料を透過せずに、表面のみで光解離反応が起き、試料全体を均一に偏極できていないことがわかる。   FIG. 4 shows the relationship between the radical concentration in the butanol / phenol sample and the ultraviolet irradiation time determined by the electron spin resonance method. In the sample with 1 wt% of phenol added, the radical concentration once saturated after 20 minutes of irradiation, but the concentration increased again when the sample was rotated. From this result, it can be seen that when 1 wt% of phenol is added, the ultraviolet light does not pass through the sample having an inner diameter of 3.2 millimeters and the photodissociation reaction occurs only on the surface, and the entire sample cannot be polarized uniformly.

図5にNMR信号の増幅率(arb.)と紫外線照射時間(hour)との関係を示す。図5において、横軸は、ブタノール/フェノール(0.3 wt%)試料への紫外線照射時間(時)を示し、縦軸は、4.2 K熱平衡時のNMR信号強度に対する4.2K偏極時のNMR信号強度比(倍)を示している。実験は、0.5時間照射、1時間照射及び2時間照射の3回行った。その結果、1時間照射した試料で最も高い偏極度が得られた。   FIG. 5 shows the relationship between the amplification factor (arb.) Of the NMR signal and the ultraviolet irradiation time (hour). In FIG. 5, the horizontal axis represents the time of ultraviolet irradiation (hours) on the butanol / phenol (0.3 wt%) sample, and the vertical axis represents the NMR signal intensity at 4.2 K polarization relative to the NMR signal intensity at 4.2 K thermal equilibrium. The ratio (times) is shown. The experiment was performed three times: 0.5 hour irradiation, 1 hour irradiation, and 2 hour irradiation. As a result, the highest degree of polarization was obtained with the sample irradiated for 1 hour.

図6はフェノール濃度と、4.2 K熱平衡時のNMR信号強度に対する1.5K偏極時のNMR信号強度の比との関係を示す図である。図6から、フェノール濃度0.1 wt%でも33倍もの偏極の増大が得られるが、フェノール濃度0.3〜1 wt%では、50倍近い偏極の増大を示すことがわかる。   FIG. 6 is a graph showing the relationship between the phenol concentration and the ratio of the NMR signal intensity at 1.5 K polarization to the NMR signal intensity at 4.2 K thermal equilibrium. From FIG. 6, it can be seen that even when the phenol concentration is 0.1 wt%, a 33-fold increase in polarization is obtained, but at a phenol concentration of 0.3 to 1 wt%, the polarization increase is nearly 50 times.

ブタノールラジカルのような一般のラジカルは、試料を融解すると同時にラジカル同士の再結合により瞬時に消失することがよく知られている。図2の装置を用いて実証した紫外線分解法を用いた動的核スピン偏極を図1の装置で行えば、今まで以上に高い偏極度を維持したまま液体NMRや画像診断測定が行える。   It is well known that general radicals such as butanol radicals disappear instantaneously due to recombination of radicals at the same time as the sample is melted. If dynamic nuclear spin polarization using the ultraviolet decomposition method demonstrated using the apparatus of FIG. 2 is performed with the apparatus of FIG. 1, liquid NMR and diagnostic imaging measurements can be performed while maintaining a higher degree of polarization than before.

本発明は以上の実施形態に限定されるものではなく、本発明の技術的思想の範囲を逸脱しない限り、あらゆる変形が本願の請求項に含まれるものと解釈すべきである。例えば、前述の実験例においては、光解離性分子としてフェノールを、有機溶媒としてブタノールを用いているが、これらの物質や組合せに限定されるものではなく、本発明の精神を逸脱しない限り他の物質や組合せを用いても良い。例えば、ヨウ化水素などの光解離性の高いハロゲン化物も利用可能であると考えられる。また、上述の実施形態では、本発明についてNMRを対象にして説明しているが、これに限らず同様の原理を用いる装置、例えばMRIなどにも適用可能である。   The present invention is not limited to the above embodiments, and all modifications should be construed as being included in the claims of the present application without departing from the scope of the technical idea of the present invention. For example, in the above-described experimental examples, phenol is used as a photolabile molecule and butanol is used as an organic solvent. However, the present invention is not limited to these substances and combinations, and other substances may be used without departing from the spirit of the present invention. Substances and combinations may be used. For example, it is considered that halides having high photodissociation properties such as hydrogen iodide can be used. In the above-described embodiment, the present invention has been described with respect to NMR. However, the present invention is not limited to this, and the present invention can be applied to an apparatus using the same principle, for example, MRI.

11 動的核スピン偏極装置
12、13 紫外線発生装置
14 紫外線透過型光ファイバ
15 偏極用コイル
16 試料
16’移送後の試料
17 偏極試料輸送管
18 生体内に造影剤を注入するための作業器具
19 マイクロ波発生装置
20 NMR装置
21 液体窒素用デュワー
22 液体ヘリウム用デュワー
23 核スピン偏極度測定用NMR装置
DESCRIPTION OF SYMBOLS 11 Dynamic nuclear spin polarization apparatus 12, 13 Ultraviolet generator 14 Ultraviolet transmission type optical fiber 15 Polarization coil 16 Sample 16 'Sample after transfer 16' Polarized sample transport pipe 18 For injecting contrast agent into living body Work tool 19 Microwave generator 20 NMR device 21 Dewar for liquid nitrogen 22 Dewar for liquid helium 23 NMR device for nuclear spin polarization measurement

Claims (2)

0.3wt%のフェノールを光解離性分子として含有するブタノールに、極低温下で紫外線を照射してブタノールラジカルを生成し、生成されたブタノールラジカルにマイクロ波を照射して動的核スピン偏極を行うことを特徴とする造影剤の製造方法。Butanol containing 0.3 wt% phenol as a photolabile molecule is irradiated with ultraviolet rays at extremely low temperatures to generate butanol radicals, and the generated butanol radicals are irradiated with microwaves to perform dynamic nuclear spin polarization. A method for producing a contrast agent. 請求項1に記載の造影剤の製造方法において、前記ブタノールラジカルの生成と前記動的核スピン偏極を同一の装置にて行うことを特徴とする造影剤の製造方法。The method for producing a contrast agent according to claim 1, wherein the butanol radical generation and the dynamic nuclear spin polarization are performed in the same apparatus.
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