JP6037658B2 - Neutron generator - Google Patents
Neutron generator Download PDFInfo
- Publication number
- JP6037658B2 JP6037658B2 JP2012118986A JP2012118986A JP6037658B2 JP 6037658 B2 JP6037658 B2 JP 6037658B2 JP 2012118986 A JP2012118986 A JP 2012118986A JP 2012118986 A JP2012118986 A JP 2012118986A JP 6037658 B2 JP6037658 B2 JP 6037658B2
- Authority
- JP
- Japan
- Prior art keywords
- neutron generator
- beam duct
- orifice plate
- duct
- liquid metal
- 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.)
- Active
Links
Landscapes
- Particle Accelerators (AREA)
Description
本発明は、液体金属に陽子ビームを照射して中性子を発生させる中性子発生装置に関するものである。 The present invention relates to a neutron generator for generating neutrons by irradiating a liquid metal with a proton beam.
現在、ホウ素中性子捕捉療法(Boron neutron capture therapy; BNCT)が癌細胞を選択的に殺傷できる技術として注目されている。BNCTでは、ターゲットとして液体リチウム等の液体金属を用い、このターゲットに陽子を照射することで中性子を発生させる中性子発生装置が用いられる。このような中性子発生装置として特許文献1に記載された技術が知られている。 Currently, boron neutron capture therapy (BNCT) is attracting attention as a technology that can selectively kill cancer cells. In BNCT, a liquid metal such as liquid lithium is used as a target, and a neutron generator that generates neutrons by irradiating the target with protons is used. As such a neutron generator, the technique described in Patent Document 1 is known.
図6は、従来の中性子発生装置の一例を示す構成図である。この中性子発生装置500は、液体リチウムを流す反応槽502に対してビームダクト503を接続した構成である。反応槽502の内部には湾曲したバックウォール501が形成され、その上部に設けたノズル511から液体リチウムを噴出してその遠心力でバックウォール501に液体リチウム膜のターゲットTを形成する。ビームダクト503内には、所定径の入射孔508を有する3枚のオリフィス板507が設けられる。真空ポンプ505は、オリフィス板507で区画された空間531毎に設けられる。 FIG. 6 is a block diagram showing an example of a conventional neutron generator. This neutron generator 500 has a configuration in which a beam duct 503 is connected to a reaction tank 502 in which liquid lithium is passed. A curved back wall 501 is formed inside the reaction tank 502, and liquid lithium is ejected from a nozzle 511 provided on the upper portion of the reaction tank 502, and the target T of the liquid lithium film is formed on the back wall 501 by the centrifugal force. In the beam duct 503, three orifice plates 507 having an incident hole 508 having a predetermined diameter are provided. The vacuum pump 505 is provided for each space 531 partitioned by the orifice plate 507.
係る構成によれば、オリフィス板507による排気抵抗により反応槽502内の真空度がビームダクト503内より低くなるので、ターゲットTの沸点温度が上昇する。これにより、反応槽502内の真空度が高くなる事を防止できる為、液体リチウムが沸騰し難くなり、蒸発した液体リチウムがビームダクト503を通じて加速器に流れ込むのを防止できる。 According to such a configuration, the degree of vacuum in the reaction tank 502 becomes lower than that in the beam duct 503 due to the exhaust resistance by the orifice plate 507, so that the boiling point temperature of the target T rises. As a result, the degree of vacuum in the reaction vessel 502 can be prevented from becoming high, so that liquid lithium is less likely to boil, and evaporated liquid lithium can be prevented from flowing into the accelerator through the beam duct 503.
しかしながら、従来の中性子発生装置500では、陽子ビームBの径が大きくなると、これに伴いオリフィス板507の入射孔508の径を大きくしなければならない。このため、反応槽502とビームダクト503との間のコンダクタンスを小さくできず、反応槽502及びビームダクト503の真空度の設定が上手くできないという問題点がある。この発明はかかる問題点を解決するためになされたものである。 However, in the conventional neutron generator 500, when the diameter of the proton beam B increases, the diameter of the entrance hole 508 of the orifice plate 507 must be increased accordingly. For this reason, there is a problem that the conductance between the reaction tank 502 and the beam duct 503 cannot be reduced, and the vacuum degree of the reaction tank 502 and the beam duct 503 cannot be set well. The present invention has been made to solve such problems.
第1の発明に係る中性子発生装置は、陽子ビームを液体金属ターゲットに対して照射して核反応により中性子を発生させる中性子発生装置であって、液体金属ターゲットと陽子ビームとが反応する領域を区画形成する反応槽と、反応槽に接続され且つ輸送されてきた陽子ビームを反応槽内に導くビームダクトと、ビームダクトの周囲に設けた前記陽子ビームを集束させる電磁石と、ビームダクトと反応槽との間に設けられると共に輸送されてきた陽子ビームの径より小さな径であって且つ前記電磁石により集束した集束部を通過し得る大きさを有する入射孔を設けたオリフィス板と、反応槽及びビームダクトに接続した真空ポンプとを備えたことを特徴とする。 A neutron generator according to a first invention is a neutron generator for generating a neutron by a nuclear reaction by irradiating a proton beam to a liquid metal target, and divides a region where the liquid metal target and the proton beam react A reaction vessel to be formed, a beam duct connected to and transported to the reaction vessel to guide the proton beam into the reaction vessel, an electromagnet for focusing the proton beam provided around the beam duct, a beam duct and a reaction vessel, An orifice plate provided with an entrance hole having a size smaller than the diameter of the proton beam which has been provided and transported and which can pass through the focusing portion focused by the electromagnet, and the reaction vessel and beam duct And a vacuum pump connected to.
本発明の中性子発生装置は、陽子ビームを電磁石で集束させ、その集束部が通過し得る径の入射孔を有するオリフィス板により反応槽とビームダクトとを仕切るため、反応槽とビームダクトとの間のコンダクタンスを小さくできる。このため、反応槽及びビームダクトの真空度の設定の自由度を高めることができる。なお、前記入射孔には、孔のみならず管状パイプにより形成する場合も含まれる。また、前記入射孔の径は、当該入射孔が円形である場合には直径、楕円形である場合には短径、長方形である場合には短辺長、多角形の場合には内接円の直径を意味するものとする。 In the neutron generator of the present invention, a proton beam is focused by an electromagnet, and the reaction vessel and the beam duct are partitioned by an orifice plate having an incident hole having a diameter through which the focusing portion can pass. The conductance can be reduced. For this reason, the freedom degree of the setting of the vacuum degree of a reaction tank and a beam duct can be raised. The incident hole includes not only the hole but also a tubular pipe. The diameter of the incident hole is a diameter when the incident hole is circular, a short diameter when it is elliptical, a short side length when it is rectangular, and an inscribed circle when it is polygonal. Means the diameter of.
また、上記発明において、更に、反応槽又はビームダクトに真空ポンプを接続するのが好ましい。 Moreover, in the said invention, it is further preferable to connect a vacuum pump to a reaction tank or a beam duct.
ビームダクトに真空ポンプを接続することでビームダクトと反応槽との間に十分な差圧が確保できる。特に、前記真空ポンプを反応槽に接続した場合、オリフィス板の入射孔の付近に液体金属が付着し難くなる。 By connecting a vacuum pump to the beam duct, a sufficient differential pressure can be secured between the beam duct and the reaction vessel. In particular, when the vacuum pump is connected to the reaction vessel, it becomes difficult for liquid metal to adhere to the vicinity of the entrance hole of the orifice plate.
また、上記発明において、更に、前記オリフィス板をビームダクト内に複数設け、当該オリフィス板で区画した空間の一部又は全部に前記真空ポンプを設けるのが好ましい。 In the above invention, it is preferable that a plurality of the orifice plates are further provided in the beam duct, and the vacuum pump is provided in a part or all of the space defined by the orifice plates.
反応槽とビームダクトとの間にオリフィス板による空間を形成することで、当該反応槽とビームダクトとの間でより自由に真空度を設定できるようになる。 By forming a space by the orifice plate between the reaction tank and the beam duct, it becomes possible to set the degree of vacuum more freely between the reaction tank and the beam duct.
また、上記発明において、更に、前記オリフィス板の入射孔の径を、前記電磁石により集束させた集束部の形状に合わせて設定するのが好ましい。 In the above invention, it is preferable that the diameter of the entrance hole of the orifice plate is set in accordance with the shape of the converging part that is converged by the electromagnet.
集束部の形状に合わせるとは、陽子ビームの集束部は電磁石により左右に末広がりの円錐形状となるので、入射孔の径を各オリフィス板の位置において係る陽子ビームが通過し得る寸法とすることである。これにより、陽子ビームの通過に必要な寸法のみをオリフィスとできるので、反応槽とビームダクトとの間のコンダクタンスをより小さくでき、真空度設定の自由度が向上する。 Matching with the shape of the converging part means that the converging part of the proton beam has a conical shape that spreads to the left and right by the electromagnet. is there. Thereby, only the dimension necessary for the passage of the proton beam can be used as the orifice, so that the conductance between the reaction vessel and the beam duct can be further reduced, and the degree of freedom in setting the degree of vacuum is improved.
(実施の形態1)
図1は、この発明の実施の形態1にかかる中性子発生装置を示す構成図である。この中性子発生装置100は、ターゲット形成部1が内設され且つ液体金属ターゲットTと陽子ビームBとが反応する領域を区画形成する反応槽2と、反応槽2に対して接続され且つ加速器(図示省略)から輸送される陽子ビームBを前記反応槽2に導くビームダクト3と、ビームダクト3の周囲に設けた電磁石4と、ビームダクト3及び反応槽2に設けた真空ポンプ5,6とを有する。
(Embodiment 1)
FIG. 1 is a block diagram showing a neutron generator according to Embodiment 1 of the present invention. The neutron generator 100 includes a reaction tank 2 in which a target forming unit 1 is provided and a region in which a liquid metal target T and a proton beam B react with each other, and is connected to the reaction tank 2 and an accelerator (illustrated). A beam duct 3 for guiding the proton beam B transported from the reaction tank 2 to the reaction tank 2, an electromagnet 4 provided around the beam duct 3, and vacuum pumps 5 and 6 provided in the beam duct 3 and the reaction tank 2. Have.
ターゲット形成部1は、陽子ビームBの照射領域を横切るように液体金属を平面的に噴射するノズル11と、噴射された液体金属を受けるディフューザからなる受け部12とから構成される。ターゲット形成部1は、配管を介してクエンチタンク、電磁ポンプ、熱交換器と接続され全体として液体金属ループを構成している(いずれも図示省略)。液体金属は、例えば液体リチウムである。なお、ターゲット形成部1は、図4に示したような湾曲したバックウォール上に液体リチウムを流す構造であっても良い(図示省略)。 The target forming unit 1 includes a nozzle 11 that ejects a liquid metal in a plane so as to cross the irradiation region of the proton beam B, and a receiving unit 12 that includes a diffuser that receives the ejected liquid metal. The target forming unit 1 is connected to a quench tank, an electromagnetic pump, and a heat exchanger via a pipe and constitutes a liquid metal loop as a whole (all not shown). The liquid metal is, for example, liquid lithium. Note that the target forming unit 1 may have a structure in which liquid lithium flows on a curved back wall as shown in FIG. 4 (not shown).
ビームダクト3の端部3aには、円形の入射孔8を設けたオリフィス板7が設けられている。オリフィス板7は、フェライト鋼或いはステンレス鋼等である。オリフィス板7の入射孔8の直径は、陽子ビームBを集束させたときの集束部Bsの最小径(陽子ビームが最もくびれた部分の径)より若干大きく設定する。また、オリフィス板7の厚さを大きくすることで反応槽2とビームダクト3との間のコンダクタンスを更に小さくできる。 At the end 3a of the beam duct 3, an orifice plate 7 provided with a circular incident hole 8 is provided. The orifice plate 7 is made of ferritic steel or stainless steel. The diameter of the entrance hole 8 of the orifice plate 7 is set slightly larger than the minimum diameter of the converging part Bs when converging the proton beam B (the diameter of the part where the proton beam is most constricted). Further, the conductance between the reaction vessel 2 and the beam duct 3 can be further reduced by increasing the thickness of the orifice plate 7.
前記電磁石4は、例えば四重極電磁石から構成する。陽子ビームBを曲げる手段としては、電磁石4の他、公知の物を用いることができる。前記真空ポンプ5,6には、ターボ分子ポンプ、イオンポンプ等を用いる。 The electromagnet 4 is composed of, for example, a quadrupole electromagnet. As means for bending the proton beam B, a known object can be used in addition to the electromagnet 4. As the vacuum pumps 5 and 6, a turbo molecular pump, an ion pump or the like is used.
この中性子発生装置100では、陽子ビームBを電磁石4により集束させ、陽子ビームBに集束部Bsを形成させる。この集束部Bsは、オリフィス板7の入射孔8の位置が最小径となるように調整される。入射孔8を通過した陽子ビームBは末広がりの円錐状に進んで液体金属ターゲットTに照射され、当該液体金属ターゲットTの背後に中性子を発生させる。液体金属ターゲットTに照射される際の陽子ビームBのフラックス量は、液体金属が蒸発しない程度に抑える。このため、集束部Bsの最小径に近い部分が液体金属ターゲットTに照射されないように、入射孔8と電磁石4との距離と前記入射孔8と液体金属ターゲットTとの距離とは、略同じとするのが好ましい。 In this neutron generator 100, the proton beam B is focused by the electromagnet 4 to form a focusing portion Bs in the proton beam B. The converging portion Bs is adjusted so that the position of the incident hole 8 of the orifice plate 7 has a minimum diameter. The proton beam B that has passed through the incident hole 8 travels in a conical shape spreading toward the end, and is irradiated onto the liquid metal target T, and neutrons are generated behind the liquid metal target T. The flux amount of the proton beam B when irradiating the liquid metal target T is suppressed to such an extent that the liquid metal does not evaporate. For this reason, the distance between the incident hole 8 and the electromagnet 4 and the distance between the incident hole 8 and the liquid metal target T are substantially the same so that the portion near the minimum diameter of the converging part Bs is not irradiated onto the liquid metal target T. Is preferable.
前記反応槽2及びビームダクト3内は、それぞれに接続した真空ポンプ5,6により所定の真空度になるまで差動排気される。この中性子発生装置100では、陽子ビームBを集束させてオリフィス板7の入射孔8を通過させるので、入射孔8を、前記加速器から輸送されてきた集束前の陽子ビームBの径よりも小径とすることができる。このため、反応槽2及びビームダクト3の間のコンダクタンスが小さくなり、反応槽2及びビームダクト3の間で十分な差圧を確保できるようになる。 The inside of the reaction vessel 2 and the beam duct 3 is differentially evacuated until a predetermined degree of vacuum is obtained by vacuum pumps 5 and 6 connected thereto. In this neutron generator 100, the proton beam B is focused and passed through the entrance hole 8 of the orifice plate 7. Therefore, the entrance hole 8 has a diameter smaller than the diameter of the unfocused proton beam B transported from the accelerator. can do. For this reason, the conductance between the reaction tank 2 and the beam duct 3 is reduced, and a sufficient differential pressure can be secured between the reaction tank 2 and the beam duct 3.
差動排気により反応槽2内の圧力を高く設定することで液体金属の沸点温度を高くできる。例えば、反応槽2内の圧力は、1×104Torr程度に設定し、ビームダクト3内の圧力は、1×106Torr程度に設定し得る。このため、陽子ビームBを照射することによる液体金属の蒸発が抑制される。また、液体金属が蒸発してもオリフィス板7の入射孔8が十分小さいので液体金属の蒸気がビームダクト3に流れ込み難い。なお、前記オリフィス板7の入射孔8の形状は円形に限定されず、例えば楕円形等でも良い。楕円形の場合、短径が集束部Bsの最小径より若干大きくなるように設定する。長方形の場合、短辺長(便宜的に径という)が集束部Bsの最小径より若干大きくなるように設定する。三角形、5角以上の多角形の場合、内接円の直径が集束部Bsの最小径より若干大きくなるように設定する。また、真空ポンプ5とは別に真空ポンプ6を設けることで入射孔8の周囲に蒸発した液体金属が付着するのを防止できる。 The boiling point temperature of the liquid metal can be increased by setting the pressure in the reaction tank 2 high by differential exhaust. For example, the pressure in the reaction vessel 2 can be set to about 1 × 10 4 Torr, and the pressure in the beam duct 3 can be set to about 1 × 10 6 Torr. For this reason, evaporation of the liquid metal due to irradiation with the proton beam B is suppressed. Further, even if the liquid metal evaporates, the entrance hole 8 of the orifice plate 7 is sufficiently small so that the liquid metal vapor does not easily flow into the beam duct 3. The shape of the entrance hole 8 of the orifice plate 7 is not limited to a circle, and may be an ellipse, for example. In the case of an ellipse, the minor axis is set to be slightly larger than the minimum diameter of the converging part Bs. In the case of a rectangle, the short side length (referred to as a diameter for convenience) is set to be slightly larger than the minimum diameter of the converging part Bs. In the case of a triangle of five or more polygons, the diameter of the inscribed circle is set to be slightly larger than the minimum diameter of the converging part Bs. Further, by providing the vacuum pump 6 separately from the vacuum pump 5, it is possible to prevent the evaporated liquid metal from adhering around the entrance hole 8.
なお、図2(a)に示すように、入射孔8に直管状のオリフィスパイプ9を設けることで、コンダクタンスを更に小さくできる。オリフィスパイプ9の長さ及び内径は、電磁石4で形成する陽子ビームBの集束部Bsの形状に基づき決定する。また、図2(b)に示すように、オリフィスパイプ10は、陽子ビームBの集束部Bsの形状に合わせて、両側がラッパ形状となる筒状体としても良い。このようにすれば、コンダクタンスを更に小さくできる。 As shown in FIG. 2A, the conductance can be further reduced by providing a straight tubular orifice pipe 9 in the incident hole 8. The length and inner diameter of the orifice pipe 9 are determined based on the shape of the converging part Bs of the proton beam B formed by the electromagnet 4. Further, as shown in FIG. 2B, the orifice pipe 10 may be a cylindrical body having both sides of a trumpet shape in accordance with the shape of the converging part Bs of the proton beam B. In this way, conductance can be further reduced.
また、上記実施の形態1に係る中性子発生装置の別の例として、図3に示すように、ビームダクト3の周囲に冷却手段50を設けても良い。換言すれば、少なくともビームダクト3の加速器とオリフィス板7との間に冷却手段50を設ける。冷却手段50は、例えばビームダクト3の外周面に管を巻き付けて内部に冷却水を通す構成としても良いし、ペルチェ素子等の簡単な構造の冷却装置としても良い。 As another example of the neutron generator according to the first embodiment, a cooling unit 50 may be provided around the beam duct 3 as shown in FIG. In other words, the cooling means 50 is provided at least between the accelerator of the beam duct 3 and the orifice plate 7. The cooling means 50 may be configured, for example, such that a tube is wound around the outer peripheral surface of the beam duct 3 and cooling water is passed through the inside, or a cooling device having a simple structure such as a Peltier element.
蒸発した液体金属は温度が低いほど表面に吸着する傾向にあるので、ビームダクト3に冷却手段50を設けて当該ビームダクト3の内面に積極的に吸着させる。これにより、入射孔8の周囲に蒸発した液体金属が付着して口径が小さくなるのを防止できる。蒸発して入射孔8を通過した液体金属の蒸気は、当該冷却手段50により冷却されたビームダクト3の部分に吸着される。これにより、加速器側に蒸発した液体金属が移動するのを防止できる。 Since the evaporated liquid metal tends to be adsorbed on the surface as the temperature is lower, the cooling means 50 is provided in the beam duct 3 and is actively adsorbed on the inner surface of the beam duct 3. Thereby, it can prevent that the liquid metal which evaporated near the entrance hole 8 adheres, and a diameter becomes small. The vapor of the liquid metal that has evaporated and passed through the incident hole 8 is adsorbed by the beam duct 3 cooled by the cooling means 50. Thereby, it is possible to prevent the evaporated liquid metal from moving to the accelerator side.
また、オリフィス板7を加熱するためのヒーター等の加熱手段を当該オリフィス板7に設け、液体金属の付着を防止するようにしても良い(図示省略)。更に、設計条件から、オリフィス板7とビームダクト3との間に温度差を設け、ビームダクト3の温度がオリフィス板7より低くなるようにしても良い。 Further, heating means such as a heater for heating the orifice plate 7 may be provided on the orifice plate 7 to prevent the liquid metal from adhering (not shown). Furthermore, a temperature difference may be provided between the orifice plate 7 and the beam duct 3 based on design conditions so that the temperature of the beam duct 3 is lower than that of the orifice plate 7.
(実施の形態2)
図4は、この発明の実施の形態2に係る中性子発生装置を示す構成図である。この中性子発生装置200は、実施の形態1と略同じ構成であるが、ビームダクト3にオリフィス板71,72,73を複数設け、各オリフィス板71,72,73で区画される空間31,32,ビームダクト3にそれぞれ真空ポンプ51,52,53を設けた点が異なる。
(Embodiment 2)
FIG. 4 is a block diagram showing a neutron generator according to Embodiment 2 of the present invention. The neutron generator 200 has substantially the same configuration as that of the first embodiment, but a plurality of orifice plates 71, 72, 73 are provided in the beam duct 3, and spaces 31, 32 partitioned by the orifice plates 71, 72, 73 are provided. The difference is that vacuum pumps 51, 52, 53 are provided in the beam duct 3, respectively.
オリフィス板71,72,73の入射孔81,82,83は、陽子ビームBを集束させたときの集束部Bsの両末広がり形状に合わせて設定する。中央のオリフィス板72の入射孔82は、集束部Bsの最小ビーム径を形成する部分に位置するので、当該ビーム径より若干大きく設定する。左右側のオリフィス板71,73の入射孔81,83は、当該オリフィス板71,73を設置した位置において陽子ビームBが通過できる径とする。即ち、中央のオリフィス板72の入射孔82の径が左右のオリフィス板71,73の入射孔81,83の径より小さくなるので、反応槽2とビームダクト3との間のコンダクタンスが更に小さくなる。 The incident holes 81, 82, 83 of the orifice plates 71, 72, 73 are set according to the shape of both ends of the converging part Bs when the proton beam B is converged. Since the entrance hole 82 of the central orifice plate 72 is located in a portion where the minimum beam diameter of the converging portion Bs is formed, it is set slightly larger than the beam diameter. The incident holes 81 and 83 of the left and right orifice plates 71 and 73 have a diameter through which the proton beam B can pass at the position where the orifice plates 71 and 73 are installed. That is, since the diameter of the entrance hole 82 of the central orifice plate 72 is smaller than the diameter of the entrance holes 81 and 83 of the left and right orifice plates 71 and 73, the conductance between the reaction tank 2 and the beam duct 3 is further reduced. .
真空ポンプ51,52,53は、反応槽2、第1オリフィス板71と第2オリフィス板72で区画した第1空間31、第2オリフィス板72と第3オリフィス板73で区画した第2空間32、及び、ビームダクト3にそれぞれ接続される。 The vacuum pumps 51, 52, and 53 are the reaction tank 2, the first space 31 defined by the first orifice plate 71 and the second orifice plate 72, and the second space 32 defined by the second orifice plate 72 and the third orifice plate 73. , And the beam duct 3, respectively.
この中性子発生装置では、反応槽2、第1空間31、第2空間32、ビームダクト3の間で段階的に圧力差が生じることになり、反応槽2の真空度をビームダクト3の真空度より低くできる。また、液体金属が蒸発しても第1空間31、第2空間32によりビームダクト3に流れ込む蒸気を抑えることができる。このため加速器に液体金属の蒸気が流れ込むことを十分に防止できる。 In this neutron generator, a pressure difference is generated in stages between the reaction tank 2, the first space 31, the second space 32, and the beam duct 3, and the degree of vacuum in the reaction tank 2 is set to the degree of vacuum in the beam duct 3. Can be lower. Further, even if the liquid metal evaporates, the vapor flowing into the beam duct 3 by the first space 31 and the second space 32 can be suppressed. For this reason, it is possible to sufficiently prevent the liquid metal vapor from flowing into the accelerator.
なお、左右側のオリフィス板71,73の一方を省略しても良い(図示省略)。その場合、ビームダクト3と反応槽2との間には1つの空間が形成される。また、真空ポンプ51,52,53,6のいずれかを省略しても良い。例えば、第1空間31、第2空間32の全てに設けた真空ポンプ51,52のいずれか一方を省略して一部の空間のみに真空ポンプを設けても良い。 One of the left and right orifice plates 71 and 73 may be omitted (not shown). In that case, one space is formed between the beam duct 3 and the reaction vessel 2. Further, any one of the vacuum pumps 51, 52, 53, 6 may be omitted. For example, one of the vacuum pumps 51 and 52 provided in all of the first space 31 and the second space 32 may be omitted, and the vacuum pump may be provided only in a part of the spaces.
また、上記実施の形態2に係る中性子発生装置200において、冷却手段60を、ビームダクト3の外側であって第1空間31の周囲に設けても良い。これにより、第1空間内31に侵入した蒸発した液体金属を、当該第1空間31内で効果的にトラップできる。第1空間31は、オリフィス板71,72により区画されているため金属蒸気が抜け難く且つ第1空間31のビームダクト3の内面が冷却されているため当該内面に蒸発金属が吸着し易くなる。これにより、液体金属の蒸気が第1空間31を抜けてビームダクト内3に侵入し難くなる。なお、冷却手段60は、例えばビームダクト3の外周面に管を巻き付けて内部に冷却水を通す構成としても良いし、ペルチェ素子等の簡単な構造の冷却装置としても良い。また、当該冷却手段60は、ビームダクト3の外側であって第2空間32の周囲に設けても良い(図示省略)。この場合、液体金属の蒸気は第2空間32内でトラップされる。更に、前記冷却手段60は、ビームダクト3の外周の全長に渡って設けても良い(図示省略)。 In the neutron generator 200 according to the second embodiment, the cooling unit 60 may be provided outside the beam duct 3 and around the first space 31. As a result, the evaporated liquid metal that has entered the first space 31 can be effectively trapped in the first space 31. Since the first space 31 is partitioned by the orifice plates 71 and 72, it is difficult for the metal vapor to escape, and the inner surface of the beam duct 3 in the first space 31 is cooled, so that the evaporated metal is easily adsorbed on the inner surface. This makes it difficult for the liquid metal vapor to enter the beam duct 3 through the first space 31. The cooling means 60 may be configured, for example, by winding a tube around the outer peripheral surface of the beam duct 3 and allowing cooling water to pass therethrough, or a cooling device having a simple structure such as a Peltier element. The cooling means 60 may be provided outside the beam duct 3 and around the second space 32 (not shown). In this case, the liquid metal vapor is trapped in the second space 32. Furthermore, the cooling means 60 may be provided over the entire outer circumference of the beam duct 3 (not shown).
(実施の形態3)
また、図5は、実施の形態2に係る中性子発生装置の変形例を示す構成図である。この中性子発生装置250は、実施の形態2に係る中性子発生装置200の第1空間31にガス導入ダクト65を設けて、ガス発生手段66からヘリウム、アルゴン等のLi分子の移動を阻害するガスを導入するようにした構成である。ガスの散乱により第1空間31の圧力が高くなり、オリフィス板71から液体金属の分子が侵入するのを防止できる。これにより、金属蒸気がビームダクト3の電磁石4側に移動し難くなる。また、第2空間32にガス発生手段66を設けることもできる。
(Embodiment 3)
FIG. 5 is a configuration diagram showing a modification of the neutron generator according to the second embodiment. This neutron generator 250 is provided with a gas introduction duct 65 in the first space 31 of the neutron generator 200 according to the second embodiment, and gas that inhibits the movement of Li molecules such as helium and argon from the gas generator 66. This is a configuration to be introduced. The pressure of the first space 31 increases due to gas scattering, and liquid metal molecules can be prevented from entering from the orifice plate 71. This makes it difficult for the metal vapor to move to the electromagnet 4 side of the beam duct 3. Further, the gas generating means 66 can be provided in the second space 32.
このガス導入手段(65,66)と前記冷却手段60を併用すれば、液体金属がビームダクト3の上流や加速器に付着するのをより効果的に防止できる。 If the gas introducing means (65, 66) and the cooling means 60 are used in combination, the liquid metal can be more effectively prevented from adhering to the upstream of the beam duct 3 or the accelerator.
100 中性子発生装置
1 ターゲット形成部
2 反応槽
3 ビームダクト
4 電磁石
5,6 真空ポンプ
7 オリフィス板
8 入射孔
T ターゲット
B 陽子ビーム
Bs 集束部
DESCRIPTION OF SYMBOLS 100 Neutron generator 1 Target formation part 2 Reaction tank 3 Beam duct 4 Electromagnets 5 and 6 Vacuum pump 7 Orifice plate 8 Entrance hole T Target B Proton beam Bs Focusing part
Claims (6)
液体金属ターゲットと陽子ビームとが反応する領域を区画形成する反応槽と、
反応槽に接続され且つ陽子ビームを反応槽内に導くビームダクトと、
ビームダクトの周囲に設けた前記陽子ビームを集束させる電磁石と、
ビームダクトと反応槽との間に設けられると共に集束前の陽子ビームの径より小さな径であって且つ前記電磁石により集束した集束部が通過し得る大きさを有する入射孔を設けたオリフィス板と、
前記オリフィス板と加速器との間であり、かつ、前記ビームダクトの外周面に配置され、前記ビームダクトを冷却する冷却手段と、
を備えたことを特徴とする中性子発生装置。 A neutron generator for generating a neutron by irradiating a liquid metal target with a proton beam transported from an accelerator ,
A reaction vessel that defines a region where the liquid metal target and the proton beam react; and
A beam duct connected to the reaction vessel and guiding the proton beam into the reaction vessel;
An electromagnet for focusing the proton beam provided around the beam duct;
An orifice plate provided between the beam duct and the reaction vessel and provided with an entrance hole having a diameter smaller than the diameter of the proton beam before focusing and having a size through which the focusing portion focused by the electromagnet can pass;
A cooling means disposed between the orifice plate and the accelerator and disposed on an outer peripheral surface of the beam duct for cooling the beam duct;
A neutron generator characterized by comprising:
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2012118986A JP6037658B2 (en) | 2012-05-24 | 2012-05-24 | Neutron generator |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2012118986A JP6037658B2 (en) | 2012-05-24 | 2012-05-24 | Neutron generator |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JP2013246006A JP2013246006A (en) | 2013-12-09 |
| JP6037658B2 true JP6037658B2 (en) | 2016-12-07 |
Family
ID=49845909
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2012118986A Active JP6037658B2 (en) | 2012-05-24 | 2012-05-24 | Neutron generator |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP6037658B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN111683449A (en) * | 2020-05-26 | 2020-09-18 | 中国原子能科学研究院 | A double-layer quartz glass tube-type high-voltage unit for small neutron generators |
Family Cites Families (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS4946398Y1 (en) * | 1969-10-06 | 1974-12-18 | ||
| JPH07249498A (en) * | 1994-01-19 | 1995-09-26 | Ishikawajima Harima Heavy Ind Co Ltd | Neutron generator |
| JP3556804B2 (en) * | 1997-05-20 | 2004-08-25 | 東京エレクトロン株式会社 | Processing device and processing method |
| JP2002318299A (en) * | 2001-04-20 | 2002-10-31 | Ebara Corp | Perticle beam extraction device and boiler device using the device |
-
2012
- 2012-05-24 JP JP2012118986A patent/JP6037658B2/en active Active
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN111683449A (en) * | 2020-05-26 | 2020-09-18 | 中国原子能科学研究院 | A double-layer quartz glass tube-type high-voltage unit for small neutron generators |
| CN111683449B (en) * | 2020-05-26 | 2021-07-20 | 中国原子能科学研究院 | A double-layer quartz glass tube-type high-voltage unit for small neutron generators |
Also Published As
| Publication number | Publication date |
|---|---|
| JP2013246006A (en) | 2013-12-09 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| Gaillard et al. | Increased laser-accelerated proton energies via direct laser-light-pressure acceleration of electrons in microcone targets | |
| Halfon et al. | High-power liquid-lithium jet target for neutron production | |
| Krygier et al. | On the origin of super-hot electrons from intense laser interactions with solid targets having moderate scale length preformed plasmas | |
| CN103813611B (en) | Compact directional high flux neutron generator | |
| US20100195781A1 (en) | Neutron beam radiation apparatus | |
| CN218830745U (en) | Neutron capture therapy system and target for particle beam generating device | |
| JP2015073783A (en) | Neutron capture therapy device | |
| JP6037658B2 (en) | Neutron generator | |
| JP4980900B2 (en) | Target assembly | |
| CN105788695B (en) | A kind of high-power electron irradiation accelerator X-ray conversion target | |
| JP2013098090A (en) | X-ray radiation device and x-ray radiation method | |
| Compant La Fontaine et al. | Production of multi-MeV Bremsstrahlung x-ray sources by petawatt laser pulses on various targets | |
| Xiao et al. | Guiding and collimation of laser-accelerated proton beams using thin foils followed with a hollow plasma channel | |
| JP6715428B2 (en) | Blanket module and fusion device | |
| Luo et al. | A simulation study of a windowless gas-stripping room in an E//B neutral particle analyzer | |
| Psikal et al. | Hollow target for efficient generation of fast ions by ultrashort laser pulses | |
| JP6997529B2 (en) | Neutron capture therapy device | |
| JPH07249498A (en) | Neutron generator | |
| JP6529059B1 (en) | Electron beam irradiation system | |
| JPH11224798A (en) | Liquid target for neutron generator | |
| CN112309591A (en) | Method and device for realizing low-temperature controllable nuclear fusion by neutron number multiplication | |
| Wang et al. | Guiding and collimating fast electron beam by the quasi-static electromagnetic field array | |
| JP2009278001A (en) | Charged beam lithography system | |
| JP2017069018A (en) | Neutron generation target device and boron neutron capture therapy system | |
| JP3205485U (en) | Combustion improvement device |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| A621 | Written request for application examination |
Free format text: JAPANESE INTERMEDIATE CODE: A621 Effective date: 20150421 |
|
| A521 | Request for written amendment filed |
Free format text: JAPANESE INTERMEDIATE CODE: A821 Effective date: 20150421 |
|
| A977 | Report on retrieval |
Free format text: JAPANESE INTERMEDIATE CODE: A971007 Effective date: 20160317 |
|
| A131 | Notification of reasons for refusal |
Free format text: JAPANESE INTERMEDIATE CODE: A131 Effective date: 20160322 |
|
| A521 | Request for written amendment filed |
Free format text: JAPANESE INTERMEDIATE CODE: A523 Effective date: 20160519 |
|
| TRDD | Decision of grant or rejection written | ||
| A01 | Written decision to grant a patent or to grant a registration (utility model) |
Free format text: JAPANESE INTERMEDIATE CODE: A01 Effective date: 20161004 |
|
| A61 | First payment of annual fees (during grant procedure) |
Free format text: JAPANESE INTERMEDIATE CODE: A61 Effective date: 20161101 |
|
| R150 | Certificate of patent or registration of utility model |
Ref document number: 6037658 Country of ref document: JP Free format text: JAPANESE INTERMEDIATE CODE: R150 |
|
| S531 | Written request for registration of change of domicile |
Free format text: JAPANESE INTERMEDIATE CODE: R313531 |
|
| S533 | Written request for registration of change of name |
Free format text: JAPANESE INTERMEDIATE CODE: R313533 |
|
| R350 | Written notification of registration of transfer |
Free format text: JAPANESE INTERMEDIATE CODE: R350 |
|
| R250 | Receipt of annual fees |
Free format text: JAPANESE INTERMEDIATE CODE: R250 |
|
| R250 | Receipt of annual fees |
Free format text: JAPANESE INTERMEDIATE CODE: R250 |
|
| R250 | Receipt of annual fees |
Free format text: JAPANESE INTERMEDIATE CODE: R250 |
|
| R250 | Receipt of annual fees |
Free format text: JAPANESE INTERMEDIATE CODE: R250 |
|
| R250 | Receipt of annual fees |
Free format text: JAPANESE INTERMEDIATE CODE: R250 |
|
| R250 | Receipt of annual fees |
Free format text: JAPANESE INTERMEDIATE CODE: R250 |
|
| R250 | Receipt of annual fees |
Free format text: JAPANESE INTERMEDIATE CODE: R250 |