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CN101569848B - Real-time precious gas polarization generator and delivery box of polarized precious gas - Google Patents

Real-time precious gas polarization generator and delivery box of polarized precious gas Download PDF

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Publication number
CN101569848B
CN101569848B CN 200810096620 CN200810096620A CN101569848B CN 101569848 B CN101569848 B CN 101569848B CN 200810096620 CN200810096620 CN 200810096620 CN 200810096620 A CN200810096620 A CN 200810096620A CN 101569848 B CN101569848 B CN 101569848B
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noble gas
real
polarization
cavity
unit
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CN101569848A (en
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张烈铮
陈政宏
蔡依蒨
汪瑞民
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TMIT TECHNOLOGY Inc
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Abstract

A real-time noble gas polarization generator comprises a cavity, a heat preservation unit, a base bottle, a heating source and an excitation unit, wherein the cavity is provided with an upper cover and a lower cover which are composed of high-permeability substances, and a first magnet unit and a second magnet unit which have the same magnetic field direction and are used for generating a magnetic field; the heat preservation unit is positioned in the cavity and is provided with a furnace space for keeping the temperature within a preset range; the base bottle is positioned in the space of the furnace body and is used for filling noble gas; the heating source is used for providing heat to the furnace body space so as to maintain the temperature of the base bottle within a preset range; the exciting unit is used for generating a polarized laser beam with a specific wavelength and the same direction as the magnetic field direction of the magnetic field space to pass through the base bottle so as to polarize the noble gas in the base bottle.

Description

实时贵重气体偏极化产生器及偏极化贵重气体的传送箱Real-time precious gas polarization generator and delivery box of polarized precious gas

技术领域 technical field

本发明涉及一种贵重气体偏极化产生器,具体地说,是一种实时(InSitu)贵重气体偏极化产生器。  The invention relates to a noble gas polarization generator, specifically, a real-time (InSitu) noble gas polarization generator. the

背景技术 Background technique

偏极化贵重气体(polarized noble gases)已广泛应用于物理实验、中子束研究、材料科学以及医疗应用上,例如在核磁显影的相关应用上,偏极化贵重气体偏极化信号的强度是传统偏极化的氢1(1H)偏极化信号的10,000倍以上,这使得医疗及材料科学等的应用上出现了一个原来无法达到的崭新领域。而在中子束相关研究方面,偏极化的氦3(3He)气体可以非常有效地过滤中子,达到使中子偏极的目的,且不会限制中子束的能量与动量。  Polarized noble gases (polarized noble gases) have been widely used in physical experiments, neutron beam research, material science, and medical applications. The hydrogen 1 ( 1 H) polarization signal of traditional polarization is more than 10,000 times, which makes a new field of medical and material science applications appear that cannot be achieved before. In terms of research on neutron beams, polarized helium 3 ( 3 He) gas can filter neutrons very effectively to achieve the purpose of polarizing neutrons without limiting the energy and momentum of neutron beams.

偏极化贵重气体可以由光学激化核自旋交换法(SEOP)所制备。例如氦3的光学激化核自旋交换法,包括铷的共价电子由光学激化到单一基态的自旋状态形成偏极化,以及偏极化的铷共价电子与氦3原子碰撞产生自旋偏极的转移。图1是已知的利用光学激化核自旋交换法的贵重气体偏极化产生器100的示意图,其包括一组直径约为1米的亥姆霍兹(Helmholtz)线圈110及111,一保温炉112位于亥姆霍兹线圈110及111之间,基瓶114位于保温炉112中,其内装填铷120、氦3、氦4以及氮气,一加热与温控单元118经热传输路径128连接保温炉112以控制基瓶114的温度,使铷120蒸发为气态,一波长为794.7nm且功率为30W的激光124产生激光光束130通过偏极装置126产生圆偏极激光光束132通过基瓶114停止于激光停止单元122,以及一核磁共振线圈(NMR coil)116位于基瓶114的附近以发送与接收射频(RF)信号,检测基瓶114中氦3的偏极化。亥姆霍兹线圈110及111用以通大电流(约8安培)产生磁场,其磁力线的分布如 图2所示,图2是已知的贵重气体偏极化产生器的亥姆霍兹线圈磁力线的分布图,在中心位置134形成均匀磁场空间,其磁场B0的强度约为25.6高斯(Gauss)。  Polarized noble gases can be prepared by optically excited nuclear spin exchange (SEOP). For example, the optically excited nuclear spin exchange method of helium 3 includes that the covalent electrons of rubidium are optically excited to a single ground state spin state to form polarization, and the polarized rubidium covalent electrons collide with helium 3 atoms to generate spin Bias transfer. 1 is a schematic diagram of a known noble gas polarization generator 100 using optically excited nuclear spin exchange method, which includes a group of Helmholtz (Helmholtz) coils 110 and 111 with a diameter of about 1 meter. The furnace 112 is located between the Helmholtz coils 110 and 111, the base bottle 114 is located in the holding furnace 112, and filled with rubidium 120, helium 3, helium 4 and nitrogen, and a heating and temperature control unit 118 is connected via a heat transfer path 128 The holding furnace 112 is used to control the temperature of the base bottle 114, so that rubidium 120 evaporates into a gaseous state, and a laser 124 with a wavelength of 794.7nm and a power of 30W generates a laser beam 130 and passes through a polarizing device 126 to generate a circularly polarized laser beam 132, which passes through the base bottle 114 Stopping at the laser stop unit 122 , and an NMR coil 116 is located near the vial 114 to send and receive radio frequency (RF) signals to detect the polarization of He3 in the vial 114 . The Helmholtz coils 110 and 111 are used to pass a large current (about 8 amperes) to generate a magnetic field, and the distribution of the magnetic force lines is shown in Figure 2, which is a Helmholtz coil of a known noble gas polarization generator In the distribution diagram of the magnetic field lines, a uniform magnetic field space is formed at the central position 134, and the intensity of the magnetic field B 0 is about 25.6 Gauss (Gauss).

参考图1,在铷120的光学激化过程中,由于794.7nm的圆偏极激光光束132相当于铷120的D1跃迁线,且圆偏极光只能驱动电子的自旋状态从 m j = - 1 2 m j = + 1 2 的跃迁,因此激光光束132驱动铷120的电子从  m j = - 1 2 的基态跃迁至 

Figure RE-S2008100966204D00025
m j = + 1 2 的激态,之后铷120的电子衰退到 m j = - 1 2 m j = + 1 2 的基态( 
Figure RE-S2008100966204D00029
),然而任何回到 
Figure RE-S2008100966204D000210
m j = - 1 2 的电子会被圆偏极激光光束132重新激化,最后铷120的电子都被激化到  m j = + 1 2 的基态( 
Figure RE-S2008100966204D000213
),产生偏极化的铷,此过程典型上需花费数毫秒的时间。在铷-氦3的自旋交换与氦的超偏极化的过程中,通过超精细费米接触的交互作用,氦3的原子核与偏极化铷的电子自旋交互作用以转移偏极化铷的自旋状态到氦3上,使氦3产生超偏极化,此过程需要铷电子的波函数与氦3的原子核紧密重迭,且交互作用随原子间的距离以指数般的变化,因此只有少部分的碰撞产生足够地重迭导致铷与氦3的自旋交换,相对于铷120在基瓶114中偏极化稳态的达成约需数毫秒,氦3偏极化的发生需要小时这样的数量级,因此,氦3的光学激化核自旋交换法偏好使用加热的基瓶114,以增加偏极化铷的密度,进而增加铷-氦3自旋交换的机率。  Referring to Fig. 1, in the process of optical excitation of Rubidium 120, since the 794.7nm circularly polarized laser beam 132 is equivalent to the D1 transition line of Rubidium 120, and the circularly polarized light can only drive the spin state of electrons from m j = - 1 2 arrive m j = + 1 2 transition, so the laser beam 132 drives the electrons of the rubidium 120 from and m j = - 1 2 ground state transition to
Figure RE-S2008100966204D00025
and m j = + 1 2 excited state, after which the electrons of Rubidium 120 decay to m j = - 1 2 and m j = + 1 2 ground state (
Figure RE-S2008100966204D00029
), however any returns
Figure RE-S2008100966204D000210
and m j = - 1 2 The electrons of the rubidium 120 will be re-excited by the circularly polarized laser beam 132, and finally the electrons of the rubidium 120 will be excited to m j = + 1 2 ground state (
Figure RE-S2008100966204D000213
), producing polarized rubidium, which typically takes a few milliseconds. During the spin exchange of rubidium-helium 3 and the hyperpolarization of helium, through the interaction of hyperfine Fermi contacts, the nucleus of helium 3 interacts with the electron spin of polarized rubidium to transfer the polarization The spin state of rubidium is transferred to helium 3, which makes helium 3 hyperpolarized. This process requires the wave function of rubidium electrons to overlap closely with the nucleus of helium 3, and the interaction changes exponentially with the distance between atoms. Therefore, only a small number of collisions produce enough overlap to cause the spin exchange of rubidium and helium 3. Compared with the realization of the polarization steady state of rubidium 120 in the base bottle 114, which takes about several milliseconds, the occurrence of helium 3 polarization requires Therefore, the optically excited nuclear spin exchange method of helium 3 prefers to use a heated base bottle 114 to increase the density of polarized rubidium, thereby increasing the probability of rubidium-helium 3 spin exchange.

图3是以核磁共振线圈检测氦3偏极化的示意图,以所述核磁共振线圈116检测基瓶114中氦3偏极化,核磁共振线圈116位于均匀磁场B0 中,为一独立的脉冲式的核磁共振系统,其包括发射与接收线圈210及220分别位于基瓶114的两端。发射与接收线圈210及220发射频率与氦3在 磁场B0进动(regression)频率相同的RF信号使氦3达到小角度的倾角,并接收返回的RF信号,以检测基瓶114中氦3的偏极化。由于氦3在磁场B0的进动频率与磁场B0的大小成正比,因此不稳定的磁场会影响检测结果。此外,偏极化的氦3与不均匀磁场的交互作用是造成氦3去偏极化的主要原因之一,所以不均匀的磁场导致偏极化后氦3的存放时间或弛缓时间(relaxation time)T1减小,加速偏极化氦3的衰减。  Fig. 3 is the schematic diagram that detects the polarization of helium 3 with nuclear magnetic resonance coil, detects the polarization of helium 3 in base bottle 114 with described nuclear magnetic resonance coil 116, and nuclear magnetic resonance coil 116 is located in uniform magnetic field B 0 , is an independent pulse A type of NMR system, which includes transmitting and receiving coils 210 and 220 respectively located at two ends of the base bottle 114 . Transmitting and receiving coils 210 and 220 transmit RF signals with the same frequency as the helium 3 in the magnetic field B 0 precession (regression) frequency to make the helium 3 reach a small angle of inclination, and receive the returned RF signal to detect the helium 3 in the base bottle 114 of polarization. Since the precession frequency of Helium 3 in the magnetic field B 0 is proportional to the magnitude of the magnetic field B 0 , the unstable magnetic field will affect the detection results. In addition, the interaction between polarized He3 and the inhomogeneous magnetic field is one of the main reasons for the depolarization of He3, so the inhomogeneous magnetic field leads to the storage time or relaxation time of He3 after polarization. ) T1 decreases, accelerating the decay of polarized helium 3 .

由于在氦3偏极化的过程需要磁场B0,使铷原子能阶分裂以及使偏极化的铷与偏极化的氦-3有遵循的方向,此外,氦3偏极之后必须置于均匀磁场中以避免氦3的去偏极化,而且氦-3的偏极检测需要稳定的磁场,因此,一个稳定均匀的磁场空间在偏极化贵重气体上是相当重要的。  Since the process of helium 3 polarization requires a magnetic field B 0 , the energy levels of rubidium atoms are split and the polarized rubidium and polarized helium-3 follow directions. In addition, helium 3 must be placed in a uniform The depolarization of helium-3 is avoided in the magnetic field, and the polarized detection of helium-3 requires a stable magnetic field. Therefore, a stable and uniform magnetic field space is very important for polarizing the noble gas.

然而,如图1所示,已知的贵重气体偏极化产生器100通过在直径约为1米的亥姆霍兹线圈110及111上通大电流(约8安培)以产生均匀度((最大值-最小值)/平均值)小于10-4的稳定均匀磁场空间,因此需要稳定的电源供应器与周围温度的控制,以避免因电流或温度的改变而影响磁场的稳定性,所需的设备成本及偏极化氦3的制造成本均较高。此外,由于亥姆霍兹线圈110及111所产生的磁场会受到周围电气产品、电磁场及铁磁性物质的影响,很难在开放的系统中产生均匀的磁场,因此需在亥姆霍兹线圈110及111外围加上金属屏蔽,以避免外围环境的电磁干扰。但是亥姆霍兹线圈110及111与金属屏蔽的体积庞大且重量过重,不适于移动,因此传统上若要运送偏极化后的氦3气体到使用地点时,需先将基瓶114从亥姆霍兹线圈110及111取出,再放入一具有均匀磁场及有屏蔽效果的传送箱(例如螺线管或永久磁铁箱)后加以运送。参考图1及图2所示,图2是已知的贵重气体偏极化产生器的亥姆霍兹线圈磁力线的分布图,当基瓶114从亥姆霍兹线圈110及111取出时,会经过不均匀磁场A或B,使得氦3的偏极化受到影响。即使关闭亥姆霍兹线圈110及111产生的磁场以消除不均匀磁场A及B,但此时仅剩地球磁场,且地球磁场太小,偏极化的氦3易受到外界的电磁干扰,造成氦3偏极化的衰减。  However, as shown in FIG. 1, a known noble gas polarization generator 100 generates a uniformity (( Maximum value - minimum value)/average value) is less than 10 -4 in a stable and uniform magnetic field space, so a stable power supply and ambient temperature control are required to avoid affecting the stability of the magnetic field due to changes in current or temperature. The equipment cost and the manufacturing cost of polarized helium 3 are relatively high. In addition, since the magnetic fields generated by the Helmholtz coils 110 and 111 will be affected by surrounding electrical products, electromagnetic fields and ferromagnetic substances, it is difficult to generate a uniform magnetic field in an open system. And 111 peripheral with metal shielding to avoid electromagnetic interference from the external environment. However, the Helmholtz coils 110 and 111 and the metal shielding are bulky and heavy, and are not suitable for moving. Therefore, traditionally, if the polarized helium 3 gas is to be transported to the place of use, the base bottle 114 needs to be removed from the The Helmholtz coils 110 and 111 are taken out, put into a transfer box (such as a solenoid box or a permanent magnet box) with a uniform magnetic field and a shielding effect, and then transported. Referring to Fig. 1 and Fig. 2, Fig. 2 is a distribution diagram of the Helmholtz coil magnetic field lines of a known noble gas polarization generator, when the base bottle 114 is taken out from the Helmholtz coils 110 and 111, it will After the inhomogeneous magnetic field A or B, the polarization of helium 3 is affected. Even if the magnetic fields generated by the Helmholtz coils 110 and 111 are turned off to eliminate the inhomogeneous magnetic fields A and B, only the earth's magnetic field is left at this time, and the earth's magnetic field is too small, and the polarized helium 3 is susceptible to external electromagnetic interference, causing Attenuation of He-3 polarization.

此种先对贵重气体偏极化再运送使用的方式,为非实时的应用,除了偏极化贵重气体取出后有信号折损的问题而造成运送的困扰外,更有使用 时间的限制(受限于迟缓时间),若能同步对贵重气体进行偏极及使用,则可同时解决运送的困扰及使用时间的限制,一般称此种能当场制造及使用的设备为实时化(InSitu)设备。  This method of first polarizing the precious gas and then transporting it for use is a non-real-time application. In addition to the problem of signal loss after the polarized precious gas is taken out, which causes troubles in transportation, there is also a limit on the use time (subject to limited to delay time), if the precious gas can be biased and used simultaneously, it can solve the problem of transportation and the limitation of use time at the same time. Generally, this kind of equipment that can be manufactured and used on the spot is called real-time (InSitu) equipment. the

因此已知的为非实时的贵重气体偏极化再运送使用的方式存在着上述种种不便和问题。  Therefore, there are above-mentioned inconveniences and problems in the known methods for non-real-time precious gas polarization re-transportation. the

发明内容 Contents of the invention

本发明的目的,在于提出一种体积小且具有磁场屏蔽的实时贵重气体偏极化产生器。  The object of the present invention is to propose a real-time precious gas polarization generator with small volume and magnetic field shielding. the

本发明的另一目的,在于提出一种易于运送的实时贵重气体偏极化产生器。  Another object of the present invention is to provide a real-time precious gas polarization generator that is easy to transport. the

本发明的又一目的,在于提出一种便携式实时贵重气体偏极化产生器。  Another object of the present invention is to provide a portable real-time precious gas polarization generator. the

本发明的再一目的,在于提出一种降低成本的实时贵重气体偏极化产生器。  Another object of the present invention is to provide a real-time precious gas polarization generator with reduced cost. the

为实现上述目的,本发明的技术解决方案是:  For realizing the above object, technical solution of the present invention is:

一种实时贵重气体偏极化产生器,包括一腔体,一保温单元,一基瓶,一加热源和一激化单元,其特征在于:  A real-time precious gas polarization generator, comprising a cavity, a heat preservation unit, a base bottle, a heating source and an excitation unit, characterized in that:

所述腔体具有由高导磁率物质所构成的上盖与下盖,以及磁场方向相同的第一及第二磁铁单元用以产生一磁场,所述第一及第二磁铁单元分别连接至所述上盖与所述下盖的两侧,所述上盖及所述下盖相对所述腔体的中心部份为等距以引导所述磁场在所述腔体内部产生一均匀的磁场空间,并形成屏蔽效应;  The cavity has an upper cover and a lower cover made of a material with high magnetic permeability, and first and second magnet units with the same magnetic field direction to generate a magnetic field, and the first and second magnet units are respectively connected to the On both sides of the upper cover and the lower cover, the upper cover and the lower cover are equidistant from the central part of the cavity so as to guide the magnetic field to generate a uniform magnetic field space inside the cavity , and form a shielding effect;

所述保温单元位于所述腔体内,且具有一炉体空间以将温度保持在一预定的范围之内;  The heat preservation unit is located in the cavity and has a furnace space to keep the temperature within a predetermined range;

所述基瓶,位于所述炉体空间中,用以装填贵重气体;  The base bottle is located in the space of the furnace body and is used for filling precious gas;

所述加热源,用以提供热至所述炉体空间中以维持所述基瓶的温度在所述预定的范围内;  The heating source is used to provide heat to the furnace space to maintain the temperature of the base bottle within the predetermined range;

所述激化单元,用以产生一特定波长且与所述磁场空间的磁场方向相同的偏极化激光光束通过所述基瓶,以偏极化所述基瓶内的贵重气体。 The excitation unit is used to generate a polarized laser beam with a specific wavelength and the same direction as the magnetic field in the magnetic field space to pass through the base bottle to polarize the noble gas in the base bottle.

前述的实时贵重气体偏极化产生器,其中所述偏极化激光光束包括圆偏极激光光束。  The aforementioned real-time noble gas polarization generator, wherein the polarized laser beam includes a circularly polarized laser beam. the

前述的实时贵重气体偏极化产生器,其中所述上盖具有第一及第二延伸边盖,所述下盖具有第三及第四延伸边盖,所述第一磁铁单元位于所述第一及第三延伸边盖之间,以及所述第二磁铁单元位于所述第二及第四延伸边盖之间。  The aforementioned real-time noble gas polarization generator, wherein the upper cover has first and second extended side covers, the lower cover has third and fourth extended side covers, and the first magnet unit is located at the second Between the first and third extension side covers, and the second magnet unit is located between the second and fourth extension side covers. the

前述的实时贵重气体偏极化产生器,其中所述第一及第二磁铁单元包括:  The aforementioned real-time precious gas polarization generator, wherein the first and second magnet units include:

一第一永久磁铁;  a first permanent magnet;

一第二永久磁铁;  a second permanent magnet;

一侧壁,所述侧壁由所述高导磁率物质构成,且位于所述第一及第二永久磁铁之间,以串接所述第一及第二永久磁铁;  A side wall, the side wall is made of the high magnetic permeability material, and is located between the first and second permanent magnets, so as to connect the first and second permanent magnets in series;

前述的实时贵重气体偏极化产生器,其中所述侧壁具有第一及第二延伸边盖分别接合所述第一及第二永久磁铁。  In the aforementioned real-time noble gas polarization generator, wherein the side wall has first and second extended side covers respectively engaging with the first and second permanent magnets. the

前述的实时贵重气体偏极化产生器,其中所述高导磁率物质包括镍铁合金。  The aforementioned real-time noble gas polarization generator, wherein the high magnetic permeability material includes nickel-iron alloy. the

前述的实时贵重气体偏极化产生器,其中所述保温单元由玻璃、硅酸钙板或具保温效果的材料构成。  The aforementioned real-time precious gas polarization generator, wherein the heat preservation unit is made of glass, calcium silicate board or materials with heat preservation effect. the

前述的实时贵重气体偏极化产生器,其中所述加热源包括一连接至加热气枪的石英管或可以提供恒定热风或热物质的管路或装置。  In the aforementioned real-time noble gas polarization generator, the heating source includes a quartz tube connected to a heating gun or a pipeline or device that can provide constant hot air or hot material. the

前述的实时贵重气体偏极化产生器,其中所述激化单元包括:  The aforementioned real-time precious gas polarization generator, wherein the excitation unit includes:

一激光,位于所述腔体外,用以产生一激光光束;  A laser, located outside the cavity, for generating a laser beam;

一反射单元,位于所述腔体内,用以反射所述激光光束,使所述激光光束通过所述基瓶;  A reflection unit, located in the cavity, used to reflect the laser beam, so that the laser beam passes through the base bottle;

一偏极单元,位于所述激光与所述基瓶之间,以偏极所述激光光束。  A polarizing unit is located between the laser and the base bottle to polarize the laser beam. the

前述的实时贵重气体偏极化产生器,其中所述反射单元包括反射镜或棱镜。  The aforementioned real-time noble gas polarization generator, wherein the reflection unit includes a reflection mirror or a prism. the

前述的实时贵重气体偏极化产生器,其中所述激化单元包括:  The aforementioned real-time precious gas polarization generator, wherein the excitation unit includes:

一激光,位于所述腔体外,用以产生一激光光束;  A laser, located outside the cavity, for generating a laser beam;

一反射单元,位于所述腔体内,用以反射与偏极所述激光光束,使所述激光光束通过所述基瓶。  A reflection unit, located in the cavity, is used to reflect and polarize the laser beam, and make the laser beam pass through the base bottle. the

前述的实时贵重气体偏极化产生器,其中更包括一绝热层,位于所述腔体与所述保温单元之间。  The aforementioned real-time noble gas polarization generator further includes a heat insulating layer located between the cavity and the heat preservation unit. the

前述的实时贵重气体偏极化产生器,其中所述绝热层包括热传递装置。  The aforementioned real-time noble gas polarization generator, wherein the thermal insulation layer includes a heat transfer device. the

前述的实时贵重气体偏极化产生器,其中所述热传递装置包括玻璃管,其中通过控温的气体。  The aforementioned real-time noble gas polarization generator, wherein the heat transfer device includes a glass tube through which temperature-controlled gas passes. the

前述的实时贵重气体偏极化产生器,其中更包括一隔热垫,位于所述绝热层与所述保温单元之间。  The aforementioned real-time noble gas polarization generator further includes a thermal insulation pad located between the thermal insulation layer and the thermal insulation unit. the

前述的实时贵重气体偏极化产生器,其中更包括一核磁共振线圈,位于所述基瓶附近,用以发射与接收射频信号,以检测所述贵重气体的偏极化程度。  The aforementioned real-time noble gas polarization generator further includes a nuclear magnetic resonance coil located near the base bottle for transmitting and receiving radio frequency signals to detect the polarization degree of the noble gas. the

一种偏极化贵重气体的传送箱,包括一腔体和一基瓶,其特征在于:  A transmission box for polarized noble gas, including a cavity and a base bottle, characterized in that:

所述腔体具有由高导磁率物质所构成的上盖与下盖,以及磁场方向相同的第一及第二磁铁单元用以产生一磁场,所述第一及第二磁铁单元分别连接至所述上盖与所述下盖的两侧,所述上盖及所述下盖相对所述腔体的中心部份为等距以引导所述磁场在所述腔体内部产生一均匀的磁场空间,并形成屏蔽效应;  The cavity has an upper cover and a lower cover made of a material with high magnetic permeability, and first and second magnet units with the same magnetic field direction to generate a magnetic field, and the first and second magnet units are respectively connected to the On both sides of the upper cover and the lower cover, the upper cover and the lower cover are equidistant from the central part of the cavity so as to guide the magnetic field to generate a uniform magnetic field space inside the cavity , and form a shielding effect;

所述基瓶位于所述腔体中,且内部具有偏极化贵重气体。  The base bottle is located in the cavity and has polarized noble gas inside. the

前述的偏极化贵重气体的传送箱,其中所述上盖具有第一及第二延伸边盖,所述下盖具有第三及第四延伸边盖,所述第一磁铁单元位于所述第一及第三延伸边盖之间,以及所述第二磁铁单元位于所述第二及第四延伸边盖之间。  In the aforementioned transfer box for polarized noble gas, the upper cover has first and second extended side covers, the lower cover has third and fourth extended side covers, and the first magnet unit is located at the second Between the first and third extension side covers, and the second magnet unit is located between the second and fourth extension side covers. the

前述的偏极化贵重气体的传送箱,其中所述第一及第二磁铁单元包括:  The aforementioned transfer box for polarized noble gas, wherein the first and second magnet units include:

一第一永久磁铁;  a first permanent magnet;

一第二永久磁铁;  a second permanent magnet;

一侧壁,所述侧壁由所述高导磁率物质构成,且位于所述第一及第二永久磁铁之间,以串接所述第一及第二永久磁铁;  A side wall, the side wall is made of the high magnetic permeability material, and is located between the first and second permanent magnets, so as to connect the first and second permanent magnets in series;

前述的偏极化贵重气体的传送箱,其中所述侧壁具有第一及第二延伸边盖分别接合所述第一及第二永久磁铁。  In the aforementioned transfer box for polarized noble gas, wherein the side wall has first and second extended side covers respectively engaging with the first and second permanent magnets. the

前述的偏极化贵重气体的传送箱,其中所述高导磁率物质包括镍铁合金。  In the aforementioned transfer box for polarized noble gas, the high magnetic permeability material includes nickel-iron alloy. the

前述的偏极化贵重气体的传送箱,其中更包括一防碰撞装置位于所述腔体与所述基瓶之间。  The aforementioned transfer box for polarized noble gas further includes an anti-collision device located between the cavity and the base bottle. the

前述的偏极化贵重气体的传送箱,其中更包括一核磁共振线圈,位于所述基瓶附近,用以发射与接收射频信号,以检测所述偏极化贵重气体的偏极化程度。  The aforementioned transfer box for the polarized noble gas further includes a nuclear magnetic resonance coil located near the base bottle for transmitting and receiving radio frequency signals to detect the degree of polarization of the polarized noble gas. the

采用上述技术方案后,本发明的实时贵重气体偏极化产生器及偏极化贵重气体的传送箱具有以下优点:  After adopting the above technical scheme, the real-time precious gas polarization generator and the transmission box of the polarized precious gas of the present invention have the following advantages:

1.大幅降低贵重气体偏极化产生器的体积与重量,使贵重气体偏极化产生器成为便携式装置,可在需要偏极化贵重气体的场合实时产生偏极化贵重气体。  1. Significantly reduce the volume and weight of the precious gas polarization generator, making the precious gas polarization generator a portable device, which can generate polarized precious gas in real time when polarized precious gas is required. the

2.直接以所述腔体为传送箱,避免偏极化的贵重气体因经不均匀磁场或外界干扰而造成贵重气体偏极化的衰减,增加运送的安全性。  2. The cavity is directly used as the transfer box to avoid the attenuation of the polarization of the polarized precious gas due to an uneven magnetic field or external interference, thereby increasing the safety of transportation. the

附图说明 Description of drawings

图1是已知的贵重气体偏极化产生器的示意图;  Fig. 1 is the schematic diagram of known precious gas polarization generator;

图2是已知的贵重气体偏极化产生器的亥姆霍兹线圈磁力线的分布图;  Fig. 2 is the distribution figure of the Helmholtz coil magnetic field line of known noble gas polarization generator;

图3是以核磁共振线圈检测氦3偏极化的示意图;  Fig. 3 is the schematic diagram that detects helium 3 polarization with nuclear magnetic resonance coil;

图4是本发明的实时贵重气体偏极化产生器的示意图;  Fig. 4 is the schematic diagram of the real-time precious gas polarization generator of the present invention;

图5是本发明的实时贵重气体偏极化产生器的侧视图;  Fig. 5 is the side view of the real-time precious gas polarization generator of the present invention;

图6是本发明的实时贵重气体偏极化产生器中的腔体的示意图;  Fig. 6 is the schematic diagram of the cavity in the real-time precious gas polarization generator of the present invention;

图7是本发明的实时贵重气体偏极化产生器中的腔体的正视图;  Fig. 7 is the front view of the cavity in the real-time precious gas polarization generator of the present invention;

图8是腔体中水平磁场的分布图;  Figure 8 is a distribution diagram of the horizontal magnetic field in the cavity;

图9是极化后的氦3基瓶放入本发明的腔体中的弛缓现象检测图;  Fig. 9 is the detection figure of the relaxation phenomenon that the polarized helium 3 base bottle is put into the cavity of the present invention;

图10是偏极化后的氦3基瓶放入已知外围无金属屏蔽的亥姆霍兹线圈中的弛缓现象检测图;  Fig. 10 is the detection diagram of the relaxation phenomenon when the polarized helium 3 base bottle is placed in the known peripheral Helmholtz coil without metal shielding;

图11是偏极化氦3在运送前的自由感应衰变信号图;  Figure 11 is a free induction decay signal diagram of polarized helium 3 before delivery;

图12是偏极化氦3经运送后的自由感应衰变信号图。  Fig. 12 is a diagram of the free induction decay signal of polarized helium 3 after transport. the

具体实施方式 Detailed ways

以下结合实施例及其附图对本发明作更进一步说明。  The present invention will be further described below in conjunction with embodiment and accompanying drawing. the

现请参阅图4和图5,图4是本发明的实时贵重气体偏极化产生器的示意图,图5是本发明的实时贵重气体偏极化产生器的侧视图,如图所示,所述实时贵重气体偏极化产生器300包括一腔体310,其内具有一均匀的磁场空间,所述腔体310对所述磁场空间形成屏蔽效应,一保温单元(例如保温炉)324位于腔体310内,其具有一炉体空间325以将温度保持在预定的范围之内,一绝热层320位于腔体310与保温单元324之间,一基瓶328位于炉体空间325中,基瓶328中装填贵重气体(例如氦3或氙129)、碱金属(例如铷)以及缓冲气体(例如氮气),一加热源332连接炉体空间325以维持基瓶328的温度在所述预定的范围之内,使基瓶328中的碱金属蒸发为气态,一隔热垫330位于绝热层320与保温单元324之间以进一步阻绝热的传递,一激光336提供一激光光束334,一反射单元(例如反射镜或棱镜)322位于腔体310内,例如保温单元324的上方,用以反射激光光束334以形成与所述磁场空间的磁场方向相同的激光路径通过基瓶328,一偏极装置338位于激光336与基瓶328之间的激光路径上,例如在激光336的前方或在反射单元322与基瓶328之间,以偏极化激光光束334,使进入基瓶328的激光光束为偏极化激光光束,以偏极基瓶328中的碱金属,例 如将碱金属的共价电子激化到单一基态的自旋状态,偏极化的碱金属共价电子与贵重气体原子的原子核碰撞产生自旋偏极的转移,形成偏极化的贵重气体,以及一核磁共振线圈326位于基瓶328附近,用以发射与接收RF信号,以检测基瓶328中贵重气体的偏极化。在本实施例中,激光336、反射单元322以及偏极装置338构成一激化单元,用以产生一特定波长且与所述磁场空间的磁场方向相同的偏极化激光光束,以偏极化基瓶328内的贵重气体,保温单元324由玻璃、硅酸钙板或任何具保温效果的材料构成,以保持炉体空间325的温度在所述预定范围内,加热源332包括可以提供恒定热风或热物质来加热基瓶328的管路或装置,例如一连接至加热气枪的石英管,以及绝热层320由绝热物质或可将热带走的热传递装置所构成,例如在腔体310内壁上围绕玻璃管并在所述玻璃管中通过控温的气体,以有效带走外散的热,形成均匀的温度分布,避免因不均匀的温度分布导致腔体310内部磁场空间的均匀度劣化,影响偏极化的效率。在不同的实施例中,激化单元中的偏极装置338包括偏极板(例如 

Figure RE-S2008100966204D00091
λ波板)或由分光镜与 
Figure RE-S2008100966204D00092
λ波板组成的圆偏极装置,以产生圆偏极激光光束进入基瓶328偏极其中的碱金属。在另一实施例中,激化单元包括激光336以及具有偏极激光光束334功能的反射单元322,因而省略偏极装置338。  Referring now to Fig. 4 and Fig. 5, Fig. 4 is a schematic diagram of the real-time noble gas polarization generator of the present invention, and Fig. 5 is a side view of the real-time noble gas polarization generator of the present invention, as shown in the figure, the The real-time precious gas polarization generator 300 includes a cavity 310, which has a uniform magnetic field space, and the cavity 310 forms a shielding effect on the magnetic field space, and a heat preservation unit (such as a heat preservation furnace) 324 is located in the cavity In the body 310, it has a furnace body space 325 to keep the temperature within a predetermined range, a heat insulating layer 320 is located between the cavity 310 and the heat preservation unit 324, a base bottle 328 is located in the furnace body space 325, and the base bottle 328 is filled with precious gas (such as helium 3 or xenon 129), alkali metal (such as rubidium) and buffer gas (such as nitrogen), and a heating source 332 is connected to the furnace body space 325 to maintain the temperature of the base bottle 328 in the predetermined range Inside, the alkali metal in the base bottle 328 is evaporated into a gaseous state, a thermal insulation pad 330 is located between the thermal insulation layer 320 and the heat preservation unit 324 to further block the transmission of heat, a laser 336 provides a laser beam 334, and a reflection unit ( For example reflective mirror or prism) 322 is positioned in cavity 310, for example the top of heat preservation unit 324, in order to reflect laser beam 334 to form the same laser path with the magnetic field direction of described magnetic field space to pass base bottle 328, a polarizing device 338 On the laser path between the laser 336 and the base bottle 328, for example, in front of the laser 336 or between the reflection unit 322 and the base bottle 328, the laser beam 334 is polarized so that the laser beam entering the base bottle 328 is polarized. The polarized laser beam is used to polarize the alkali metal in the base bottle 328, for example, to excite the covalent electrons of the alkali metal to the spin state of a single ground state, and the polarized alkali metal covalent electrons collide with the nuclei of the noble gas atoms to generate The transfer of spin polarization forms polarized noble gas, and a nuclear magnetic resonance coil 326 is located near the base bottle 328 for transmitting and receiving RF signals to detect the polarization of the noble gas in the base bottle 328 . In this embodiment, the laser 336, the reflective unit 322 and the polarizing device 338 form an excitation unit, which is used to generate a polarized laser beam with a specific wavelength and the same direction as the magnetic field in the magnetic field space. The precious gas in the bottle 328, the heat preservation unit 324 is made of glass, calcium silicate plate or any material with heat preservation effect, to keep the temperature of the furnace body space 325 within the predetermined range, the heating source 332 includes a constant hot blast or Hot material heats the pipeline or device of base bottle 328, such as a quartz tube connected to the heating air gun, and the heat insulating layer 320 is made of heat insulating material or heat transfer device that can take heat away, such as surrounding on the cavity 310 inner wall The glass tube and the temperature-controlled gas pass through the glass tube to effectively take away the heat dissipated to form a uniform temperature distribution, so as to avoid the deterioration of the uniformity of the magnetic field space inside the cavity 310 due to the uneven temperature distribution, which affects Polarization efficiency. In various embodiments, the polarizing means 338 in the excitation unit comprises a polarizing plate (e.g.
Figure RE-S2008100966204D00091
λ wave plate) or by beam splitter and
Figure RE-S2008100966204D00092
A circular polarizing device composed of a λ wave plate is used to generate a circularly polarized laser beam and enter the base bottle 328 to polarize the alkali metal therein. In another embodiment, the excitation unit includes a laser 336 and a reflection unit 322 functioning as a polarized laser beam 334 , thus omitting the polarizing device 338 .

在本发明的一实施例中,反射单元322、绝热层320及隔热垫330是可拆解的,在贵重气体被偏极化后,拆除反射单元322、绝热层320及隔热垫330,并加装富有弹性的防碰撞装置(例如适当形状大小的泡棉)置于基瓶328、保温单元324与腔体310之间,以固定基瓶328避免碰撞,并使用腔体310作为运送箱,将偏极化的贵重气体运送到需要的地方。在本发明的另一实施例中,拆除反射单元322、保温单元324、绝热层320及隔 热垫330,保留基瓶328在腔体310中,并加装富有弹性的防碰撞装置(例如适当形状大小的泡棉)置于基瓶328与腔体310之间,以固定基瓶328避免碰撞,并使用腔体310作为运送箱。在本发明的又一实施例中,拆除反射单元322及隔热垫330,并加装富有弹性的防碰撞装置(例如适当形状大小的泡棉)置于基瓶328、保温单元324与绝热层320(如绝热物质)之间,以固定基瓶328避免碰撞,并使用腔体310作为运送箱。由于腔体310具有均匀磁场以及屏蔽效果,因此偏极化的贵重气体在运送的过程中,不会受到不均匀磁场或外界电磁干扰的影响,而造成偏极化贵重气体的衰减。  In an embodiment of the present invention, the reflection unit 322, the heat insulation layer 320 and the heat insulation pad 330 are detachable, and after the noble gas is polarized, the reflection unit 322, the heat insulation layer 320 and the heat insulation pad 330 are removed, And add elastic anti-collision devices (such as foam of appropriate shape and size) to place between the base bottle 328, the heat preservation unit 324 and the cavity 310, to fix the base bottle 328 to avoid collisions, and use the cavity 310 as a transport box , to transport the polarized precious gas to where it is needed. In another embodiment of the present invention, the reflection unit 322, the heat preservation unit 324, the heat insulation layer 320 and the heat insulation pad 330 are removed, the base bottle 328 is kept in the cavity 310, and a flexible anti-collision device (such as a suitable The shape and size of the foam) is placed between the base bottle 328 and the cavity 310 to fix the base bottle 328 to avoid collisions, and the cavity 310 is used as a transport case. In yet another embodiment of the present invention, the reflection unit 322 and the heat insulation pad 330 are removed, and an elastic anti-collision device (such as foam of appropriate shape and size) is installed on the base bottle 328, the heat preservation unit 324 and the heat insulation layer. 320 (such as heat insulating material), avoid collision with fixed base bottle 328, and use cavity 310 as transport case. Since the cavity 310 has a uniform magnetic field and a shielding effect, the polarized noble gas will not be affected by an uneven magnetic field or external electromagnetic interference during transportation, which will cause attenuation of the polarized noble gas. the

在本发明的不同的实施例中,实时贵重气体偏极化产生器300的重量小(例如小于十公斤)且体积小型化,可将其搬运到需要偏极化贵重气体的场合实时产生偏极化的贵重气体。此小型化的贵重气体偏极化产生器成为便携式装置,增加使用上的弹性及便利性。此外,在使用空间被限制的情况下,可持续实时的对贵重气体加以偏极,无须将基瓶328取出,免除受限于偏极化贵重气体弛缓时间T1的问题。例如在中子束的相关研究上,以偏极化贵重气体作为自旋过滤器时,弛缓时间T1决定自旋过滤器可应用的时间,通过持续实时的对贵重气体加以偏极化,可使中子束的研究不会因已达弛缓时间T1而暂停,具有优越的操作性。  In different embodiments of the present invention, the real-time precious gas polarization generator 300 has a small weight (for example, less than ten kilograms) and a miniaturized volume, and can be transported to occasions that require polarized precious gas to generate polarization in real time. liquefied noble gases. The miniaturized precious gas polarization generator becomes a portable device, increasing flexibility and convenience in use. In addition, under the condition that the use space is limited, the noble gas can be continuously polarized in real time without taking out the base bottle 328 , and the problem of being limited by the relaxation time T1 of the polarized noble gas is avoided. For example, in the related research of neutron beams, when the polarized noble gas is used as the spin filter, the relaxation time T1 determines the applicable time of the spin filter. By continuously polarizing the noble gas in real time, the The research of the neutron beam will not be suspended because the relaxation time T1 has been reached, which has excellent operability. the

现请参阅图6和图7,图6是本发明的实时贵重气体偏极化产生器中的腔体的示意图,图7是本发明的实时贵重气体偏极化产生器中的腔体的正视图,如图所示,在一实施例中,所述腔体310包括由高导磁率物质(μ-metal),例如镍铁合金,构成的上盖342与下盖344,二者相对腔体310的中心部份为等距,例如具有相同的尺寸,以及磁铁单元370及372分别连接在上盖342与下盖344的两侧之间,作为产生磁场的磁力源,磁铁单元370包括永久磁铁316及318,以及一位于永久磁铁316及318之间的侧壁348,用以串接永久磁铁316及318,磁铁单元372包括永久磁铁312及314,以及一位于永久磁铁312及314之间的侧壁346,用以串接永久磁铁312及314。其中,磁铁单元370及372的磁场方向相同,例如永久磁铁312-318的N极方向374均向上,以及侧壁346及348由高导磁率物质构成。优选侧壁348具有延伸边盖358与360分别接合永久磁铁316及 318,以将其串接在一起,侧壁346具有延伸边盖354及356分别接合永久磁铁312及314,以将其串接在一起,上盖342具有延伸边盖350及352,下盖344具有延伸边盖362及364,磁铁单元370位于延伸边盖352与364之间,磁铁单元372位于延伸边盖350与362之间。永久磁铁312-318的磁力线经侧壁346与348、上盖342以及下盖344的引导,在腔体310内部形成磁场方向为上下方向(本实施例为向下)的均匀磁场空间,其水平磁场的分布如图8所示,其显示腔体310中在水平距离8公分至28公分之间具有均匀的磁场B0’,其磁场大小约为1.2E-3特斯拉(Tesla),且在水平距离13公分至23公分之间的磁场均匀度小于10-4,已达到贵重气体偏极化时所需的磁场均匀度的要求,因此可作为提供贵重气体偏极化时所需的稳定均匀磁场。此外,由于腔体310由高导磁率物质构成,因此自动形成屏蔽效应。在一实施例中,调整所述均匀磁场B0’的强度为10高斯,以和维持中子偏极化的标准导向磁场(guide field)的数量级一致。在另一实施例中,永久磁铁312-318与接合区域350-364经由黏着剂黏合在一起,或者经由如螺丝或夹钳等机械结构接合在一起。在不同的实施例中,可通过调整磁铁单元370与372中侧壁及永久磁铁的数量,产生所需的磁场空间,例如磁铁单元370与372可以各为单独一个永久磁铁直接连至上盖342与下盖344,或二个以上的永久磁铁经由多个侧壁串接在一起,再与上盖342与下盖344连接。  Referring now to Fig. 6 and Fig. 7, Fig. 6 is a schematic diagram of the chamber in the real-time noble gas polarization generator of the present invention, and Fig. 7 is a front view of the chamber in the real-time noble gas polarization generator of the present invention As shown in the figure, in one embodiment, the cavity 310 includes an upper cover 342 and a lower cover 344 made of high magnetic permeability material (μ-metal), such as nickel-iron alloy, the two are opposite to the cavity 310 The central part is equidistant, for example has the same size, and the magnet units 370 and 372 are respectively connected between the two sides of the upper cover 342 and the lower cover 344, as a magnetic source for generating a magnetic field, the magnet unit 370 includes a permanent magnet 316 and 318, and a side wall 348 between the permanent magnets 316 and 318, in order to connect the permanent magnets 316 and 318 in series, the magnet unit 372 includes the permanent magnets 312 and 314, and a side wall between the permanent magnets 312 and 314 The wall 346 is used for connecting the permanent magnets 312 and 314 in series. The magnetic field directions of the magnet units 370 and 372 are the same, for example, the N-pole directions 374 of the permanent magnets 312-318 are all upward, and the side walls 346 and 348 are made of high magnetic permeability materials. Preferably side wall 348 has extended side covers 358 and 360 respectively engaging permanent magnets 316 and 318 to connect them in series, and side wall 346 has extended side covers 354 and 356 respectively engaging permanent magnets 312 and 314 to connect them in series Together, the upper cover 342 has extension side covers 350 and 352, the lower cover 344 has extension side covers 362 and 364, the magnet unit 370 is located between the extension side covers 352 and 364, and the magnet unit 372 is located between the extension side covers 350 and 362 . The magnetic field lines of the permanent magnets 312-318 are guided by the side walls 346 and 348, the upper cover 342 and the lower cover 344, forming a uniform magnetic field space in which the magnetic field direction is the up-down direction (downward in this embodiment) inside the cavity 310, and its horizontal The distribution of the magnetic field is shown in Figure 8, which shows that there is a uniform magnetic field B 0 ' between the horizontal distance of 8 cm and 28 cm in the cavity 310, and its magnetic field size is about 1.2E-3 Tesla (Tesla), and The uniformity of the magnetic field between the horizontal distance of 13 cm and 23 cm is less than 10 -4 , which has met the requirements of the magnetic field uniformity required for the polarization of the noble gas, so it can be used to provide the stability required for the polarization of the noble gas uniform magnetic field. In addition, since the cavity 310 is made of a material with high magnetic permeability, a shielding effect is automatically formed. In one embodiment, the strength of the uniform magnetic field B 0 ′ is adjusted to be 10 Gauss, which is consistent with the magnitude of a standard guide field for maintaining neutron polarization. In another embodiment, the permanent magnets 312-318 and the bonding areas 350-364 are bonded together via adhesives, or bonded together via mechanical structures such as screws or clamps. In different embodiments, the required magnetic field space can be generated by adjusting the number of side walls and permanent magnets in the magnet units 370 and 372. For example, the magnet units 370 and 372 can each be a single permanent magnet directly connected to the upper cover 342 and The lower cover 344 , or more than two permanent magnets are connected in series via a plurality of side walls, and then connected with the upper cover 342 and the lower cover 344 .

现参照图5,以产生偏极化氦3为例说明,其中,如图7所示,所述腔体3 10通过永久磁铁与高导磁率物质形成均匀磁场,且高导磁率物质构成自然的屏蔽以阻绝外界的干扰。基瓶328中装填铷、氦3、氦4及氮气,以及反射单元322为一反射镜。热经由加热源332提供至炉体空间325以维持基瓶328的温度,使铷蒸发为气态,激光336产生波长为794.7nm的激光光束334经偏极装置338后提供偏极化波长794.7nm的激光光束,经反射单元322后形成与磁场B0’方向相同的激光路径通过基瓶328,将铷激化到单一基态的自旋状态,氦3的原子核与铷碰撞产生自旋偏移的转移,形成偏极化的氦3。由于腔体3 10通过永久磁铁与高导磁率物质形成均匀磁场,因此不需要稳定的电源供应器提供大电流以产生均匀的磁场,除了 大幅减少贵重气体偏极化产生器300的体积及重量外,更有效降低设备成本与偏极化氦3的制造成本。  Now referring to FIG. 5, it is illustrated by taking the generation of polarized helium 3 as an example, wherein, as shown in FIG. Shield to block outside interference. The base bottle 328 is filled with rubidium, helium-3, helium-4 and nitrogen, and the reflection unit 322 is a reflection mirror. The heat is supplied to the furnace body space 325 via the heating source 332 to maintain the temperature of the base bottle 328, and the rubidium is evaporated into a gaseous state, and the laser beam 336 generates a laser beam 334 with a wavelength of 794.7nm and provides a polarized wavelength of 794.7nm after passing through the polarizing device 338. The laser beam passes through the reflection unit 322 to form a laser path in the same direction as the magnetic field B 0 ′, passes through the base bottle 328, and excites the rubidium to a single ground spin state, and the collision of the nucleus of the helium 3 with the rubidium produces a spin offset transfer, Polarized helium 3 is formed. Since the cavity 310 forms a uniform magnetic field through permanent magnets and high-permeability materials, it does not require a stable power supply to provide a large current to generate a uniform magnetic field. In addition to greatly reducing the volume and weight of the precious gas polarization generator 300 , to more effectively reduce the equipment cost and the manufacturing cost of polarized helium 3 .

再请参阅图9和图10,图9是极化后的氦3基瓶放入本发明的腔体中的弛缓现象检测图,图10是偏极化后的氦3基瓶放入已知外围无金属屏蔽的亥姆霍兹线圈中的弛缓现象检测图,它们分别为在压力为1大气压下,将偏极化氦3基瓶放入本发明的腔体以及已知外围无金属屏蔽的亥姆霍兹线圈中的弛缓现象检测图。以一直径为5公分,高为6公分的基瓶为例,将偏极化氦3置于本发明具有均匀磁场的腔体中的弛缓检测结果如图9所示,其弛缓时间T1约为24.75小时。而将偏极化后的氦3置于习知外围无金属屏蔽的亥姆霍兹线圈所产生的磁场中的弛缓检测结果如图10所示,其弛缓时间T1约为17.5小时,显示本发明能提供更好的防护以减缓偏极化氦3的衰减。  Please refer to Fig. 9 and Fig. 10 again, Fig. 9 is that the helium 3 base bottle after the polarization is put into the relaxation phenomenon detection figure in the cavity of the present invention, Fig. 10 is that the helium 3 base bottle after the polarization is put into known The relaxation phenomenon detection diagram in the Helmholtz coil without metal shielding on the periphery, they are respectively under the pressure of 1 atmosphere, the polarized helium 3 base bottle is put into the cavity of the present invention and the known non-metal shielding on the periphery Diagram of detection of relaxation phenomena in a Helmholtz coil. Taking a base bottle with a diameter of 5 cm and a height of 6 cm as an example, the relaxation detection results of placing polarized helium 3 in the cavity with a uniform magnetic field of the present invention are shown in Figure 9, and the relaxation time T1 is about 24.75 hours. And place the helium after the polarization 3 in the magnetic field that the Helmholtz coil of the conventional periphery produces without metal shielding and relax detection result as shown in Figure 10, and its relaxation time T1 is about 17.5 hours, shows the present invention Can provide better protection to slow down the decay of polarized He-3. the

最后请参阅图11和图12,图11是偏极化氦3在运送前的自由感应衰变(Free Induction Decay;FID)信号图,图12是偏极化氦3经运送后(例如以本发明的腔体作为传送箱,由汽车从实验室运送至数公里外的办公室)的的自由感应衰变信号图,如图所示,所述偏极化氦3的FID信号在运送前与运送后的FID信号峰值几乎没有改变,显示在形成偏极化氦3后,直接以本发明的腔体作为传送箱将偏极化氦3运送至使用地点,例如中子炉或医院等地方,可避免因偏极化氦3从偏极化设备取出后的信号折损等问题。  Please refer to Fig. 11 and Fig. 12 at last, Fig. 11 is the free induction decay (Free Induction Decay; FID) signal figure of polarized helium 3 before transporting, Fig. 12 is polarized helium 3 after transporting (for example according to the present invention The free induction decay signal diagram of the cavity as a transport box, which is transported by car from the laboratory to the office several kilometers away), as shown in the figure, the FID signal of the polarized helium 3 before and after transport The peak value of the FID signal hardly changes, which shows that after the polarized helium 3 is formed, the cavity of the present invention is directly used as a delivery box to transport the polarized helium 3 to the place of use, such as a neutron furnace or a hospital, etc. Problems such as signal loss after the polarized helium 3 is taken out from the polarized device. the

以上实施例仅供说明本发明之用,而非对本发明的限制,有关技术领域的技术人员,在不脱离本发明的精神和范围的情况下,还可以作出各种变换或变化。因此,所有等同的技术方案也应该属于本发明的范畴,应由各权利要求限定。  The above embodiments are only for illustrating the present invention, rather than limiting the present invention. Those skilled in the relevant technical field can also make various transformations or changes without departing from the spirit and scope of the present invention. Therefore, all equivalent technical solutions should also belong to the category of the present invention and should be defined by each claim. the

组件符号说明  Description of component symbols

100    贵重气体偏极化产生器  100 precious gas polarization generator

110-111亥姆霍兹线圈  110-111 Helmholtz coil

112    保温炉  112 holding furnace

114    基瓶  114 base bottle

116    核磁共振线圈  116 MRI coils

118    加热与温控单元  118 Heating and temperature control unit

120    铷  120 rubidium

122    激光停止单元  122 laser stop unit

124    激光  124 laser

126    偏极装置  126 polarizing device

128    热传输路径  128 heat transfer path

130    激光光束  130 laser beams

132    圆偏极激光光束  132 circularly polarized laser beams

134    中心位置  134 center position

210    发射与接收线圈  210 Transmitting and receiving coils

220    发射与接收线圈  220 Transmitting and receiving coils

300    实时贵重气体偏极化产生器  300 real-time precious gas polarization generator

310    腔体  310 cavity

312-318永久磁铁  312-318 permanent magnet

320    绝热层  320 insulation layer

322    反射单元  322 reflection unit

324    保温单元  324 insulation unit

325    炉体空间  325 furnace body space

326    核磁共振线圈  326 MRI coil

328    基瓶  328 base bottle

330    隔热垫  330 heat insulation pad

332    加热源  332 heating source

334    激光光束  334 laser beam

336    激光  336 laser

338    偏极装置  338 Polarization device

342    上盖  342 cover

344    下盖  344 lower cover

346-348 侧壁  346-348 side wall

350-364 接合区域  350-364 joint area

370-372 磁铁单元  370-372 Magnet unit

374     N极方向  374 N pole direction

376     磁力线  376 magnetic field lines

Claims (24)

1. a real-time noble gas polarization generator comprises a cavity, a heat-insulation unit, and a base bottle, a heating source and intensifies the unit, it is characterized in that:
Described cavity has loam cake and the lower cover that is made of the high permeability material, and identical first and second magnet unit of magnetic direction is in order to produce a magnetic field, described first and second magnet unit is connected to respectively the both sides of described loam cake and described lower cover, the core of described loam cake and the relatively described cavity of described lower cover for equidistantly guiding described magnetic field to produce a uniform magnetic field space in described inside cavity, and formation screen effect;
Described heat-insulation unit is positioned at described cavity, and has a furnace space temperature is remained within the scope of being scheduled to;
Described base bottle is arranged in described furnace space, in order to load noble gas;
Described heating source is in order to provide in the hot extremely described furnace space to keep described basic bottle temperature in described predetermined scope;
The described unit that intensifies passes through described base bottle in order to produce a specific wavelength and the polarization laser beam identical with the magnetic direction of described magnetic field space, with the interior noble gas of the described base bottle of polarization,
Wherein, described high permeability material comprises dilval.
2. real-time noble gas polarization generator as claimed in claim 1 is characterized in that, described polarization laser beam comprises round polar biased laser beam.
3. real-time noble gas polarization generator as claimed in claim 1, it is characterized in that, described loam cake has first and second extension edge lid, described lower cover has the 3rd and the 4th extension edge lid, described the first magnet unit is between the described first and the 3rd extension edge lid, and described the second magnet unit is between the described second and the 4th extension edge lid.
4. real-time noble gas polarization generator as claimed in claim 1 is characterized in that, described first and second magnet unit comprises:
One first permanent magnet;
One second permanent magnet;
One sidewall, described sidewall is made of described high permeability material, and between described first and second permanent magnet, to be connected in series described first and second permanent magnet.
5. real-time noble gas polarization generator as claimed in claim 4 is characterized in that, described sidewall has first and second extension edge lid and engages respectively described first and second permanent magnet.
6. real-time noble gas polarization generator as claimed in claim 1 is characterized in that, described heat-insulation unit is made of the material of tool heat insulation effect.
7. real-time noble gas polarization generator as claimed in claim 6 is characterized in that, described heat-insulation unit is made of glass or calcium silicate board.
8. real-time noble gas polarization generator as claimed in claim 1 is characterized in that, described heating source comprises pipeline or the device that constant hot blast is provided.
9. real-time noble gas polarization generator as claimed in claim 1 is characterized in that, described heating source comprises pipeline or the device that constant hot material is provided.
10. real-time noble gas polarization generator as claimed in claim 1 is characterized in that, described heating source comprises that one is connected to the quartz ampoule of heating air gun.
11. real-time noble gas polarization generator as claimed in claim 1 is characterized in that, the described unit that intensifies comprises:
One laser is positioned at outside the described cavity, in order to produce a laser beam;
One reflector element is positioned at described cavity, in order to reflect described laser beam, makes described laser beam by described base bottle;
One polar biased unit is between described laser and described base bottle, with the described laser beam of polar biased.
12. real-time noble gas polarization generator as claimed in claim 11 is characterized in that described reflector element comprises speculum or prism.
13. real-time noble gas polarization generator as claimed in claim 1 is characterized in that, the described unit that intensifies comprises:
One laser is positioned at outside the described cavity, in order to produce a laser beam;
One reflector element is positioned at described cavity, in order to reflection and the described laser beam of polar biased, makes described laser beam by described base bottle.
14. real-time noble gas polarization generator as claimed in claim 1 is characterized in that, more comprises a heat insulation layer, between described cavity and described heat-insulation unit.
15. real-time noble gas polarization generator as claimed in claim 14 is characterized in that described heat insulation layer comprises heat-transfer arrangement.
16. real-time noble gas polarization generator as claimed in claim 15 is characterized in that described heat-transfer arrangement comprises glass tube, wherein the gas by temperature control.
17. real-time noble gas polarization generator as claimed in claim 14 is characterized in that, more comprises a heat insulating mattress, between described heat insulation layer and described heat-insulation unit.
18. real-time noble gas polarization generator as claimed in claim 1 is characterized in that, more comprises a malcoils, is positioned near the described base bottle, in order to emission and received RF signal, to detect the polarization degree of described noble gas.
19. the carrying case of a polarization noble gas comprises a cavity and a base bottle, it is characterized in that:
Described cavity has loam cake and the lower cover that is made of the high permeability material, and identical first and second magnet unit of magnetic direction is in order to produce a magnetic field, described first and second magnet unit is connected to respectively the both sides of described loam cake and described lower cover, the central part of described loam cake and the relatively described cavity of described lower cover for equidistantly guiding described magnetic field to produce a uniform magnetic field space in described inside cavity, and formation screen effect;
Described base bottle is arranged in described cavity, and inside has the polarization noble gas,
Wherein, described high permeability material comprises dilval.
20. the carrying case of polarization noble gas as claimed in claim 19, it is characterized in that, described loam cake has first and second extension edge lid, described lower cover has the 3rd and the 4th extension edge lid, described the first magnet unit is between the described first and the 3rd extension edge lid, and described the second magnet unit is between the described second and the 4th extension edge lid.
21. the carrying case of polarization noble gas as claimed in claim 19 is characterized in that, described first and second magnet unit comprises:
One first permanent magnet;
One second permanent magnet;
One sidewall, described sidewall is made of described high permeability material, and between described first and second permanent magnet, to be connected in series described first and second permanent magnet;
22. the carrying case of polarization noble gas as claimed in claim 21 is characterized in that, described sidewall has first and second extension edge lid and engages respectively described first and second permanent magnet.
23. the carrying case of polarization noble gas as claimed in claim 19 is characterized in that, comprises that more a collision prevention device is between described cavity and described base bottle.
24. the carrying case of polarization noble gas as claimed in claim 19 is characterized in that, more comprises a malcoils, is positioned near the described base bottle, in order to emission and received RF signal, to detect the polarization degree of described polarization noble gas.
CN 200810096620 2008-04-29 2008-04-29 Real-time precious gas polarization generator and delivery box of polarized precious gas Expired - Fee Related CN101569848B (en)

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