CN108181663B - Atomic interference gravity acceleration measuring device based on pyramid-like structure - Google Patents
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Abstract
本发明公开了一种基于二维交叉光栅的类金字塔结构型原子干涉重力加速度测量装置,包括真空腔、扩束筒、二维交叉光栅以及用于产生分离式金字塔结构的反射镜组件;所述扩束筒用来引入真空系统的单根光纤,所述二维交叉光栅位于扩束筒与反射镜组件之间;所述反射镜组件由上至下依次分为:MOT区、干涉区和探测区;所述MOT区内包括四个第一反射镜,探测区的下方设置有第二反光镜。本发明具有整体体积小、鲁棒性强、成本低、测量精度高等优点。
The invention discloses a pyramid structure-like atomic interference gravitational acceleration measurement device based on a two-dimensional cross grating, which includes a vacuum cavity, a beam expander, a two-dimensional cross grating and a reflector assembly for producing a separated pyramid structure; The beam expander is used to introduce a single optical fiber of the vacuum system. The two-dimensional cross grating is located between the beam expander and the mirror assembly; the mirror assembly is divided into: MOT area, interference area and detection area from top to bottom. area; the MOT area includes four first reflectors, and a second reflector is arranged below the detection area. The invention has the advantages of small overall volume, strong robustness, low cost, high measurement accuracy and the like.
Description
技术领域technical field
本发明主要涉及到原子干涉仪领域,特指一种基于二维交叉光栅的类金字塔结构型原子干涉重力加速度测量装置。The invention mainly relates to the field of atomic interferometers, in particular to a pyramid-like structure atomic interference gravitational acceleration measurement device based on a two-dimensional cross grating.
背景技术Background technique
自迈克尔逊干涉仪发明以来,根据光波的衍射、干涉特性构建的干涉计量仪器因其极高的测量精度和灵敏度而广泛应用于基础科学研究、生产实践、航天航空、地质探矿和国防工业等众多领域。在实践中,人们逐渐认识到采用波长更短的波进行干涉可以提高测量精度,因此于1952年构建了电子干涉仪,1962年构建了中子干涉仪,直到20世纪70年代,人们才开始构思原子干涉仪。原子干涉仪,即以原子物质波代替经典光波作为干涉媒介,用原子光学器件代替经典光学器件来实现分束、反射、合束过程而构成的干涉仪。Since the invention of the Michelson interferometer, interferometric instruments constructed based on the diffraction and interference characteristics of light waves have been widely used in basic scientific research, production practice, aerospace, geological prospecting, and national defense industries due to their extremely high measurement accuracy and sensitivity. field. In practice, people gradually realized that the use of shorter wavelength waves for interference can improve measurement accuracy, so an electronic interferometer was built in 1952, and a neutron interferometer was built in 1962. It was not until the 1970s that people began to conceive Atom interferometer. An atomic interferometer is an interferometer composed of atomic matter waves instead of classical light waves as the interference medium, and atomic optical devices instead of classical optical devices to achieve beam splitting, reflection, and beam combining processes.
相比于其他干涉媒介,原子干涉仪具有以下优势:①由于原子质量远大于光子、中子及电子,相应的物质波波长更短,因此可以获得更高的测量精度和灵敏度。理论分析表明,原子干涉陀螺仪的灵敏度比相同回路面积的He-Ne激光陀螺仪高1011倍,原子加速度仪比现有加速度计的灵敏度高1017倍。②因为原子具有丰富的内部能级,可以利用电磁场对其进行精密操控,因而原子干涉仪可以提供更广泛的基础研究与应用。③原子显电中性,受杂散电场干扰小,且原子间不存在库伦相互作用,因此可以获得优于电子干涉仪的测量精度。④此外,激光冷却原子技术的发展使得高通量的冷或超冷原子束较易获得,因而原子干涉仪的构造要比中子干涉仪简单和便宜。Compared with other interference media, atomic interferometer has the following advantages: ① Since the mass of atoms is much larger than that of photons, neutrons and electrons, the corresponding matter wave wavelength is shorter, so higher measurement accuracy and sensitivity can be obtained. Theoretical analysis shows that the sensitivity of the atomic interference gyroscope is 10 11 times higher than that of the He-Ne laser gyroscope with the same loop area, and the sensitivity of the atomic accelerometer is 10 17 times higher than that of the existing accelerometers. ②Because atoms have rich internal energy levels and can be precisely manipulated by electromagnetic fields, atomic interferometers can provide a wider range of basic research and applications. ③ Atoms are electrically neutral, less disturbed by stray electric fields, and there is no Coulomb interaction between atoms, so the measurement accuracy can be better than that of electronic interferometers. ④In addition, the development of laser cooling atom technology makes it easier to obtain high-throughput cold or ultracold atomic beams, so the construction of atomic interferometers is simpler and cheaper than neutron interferometers.
原子干涉仪是以原子物质波代替经典光波作为干涉媒介,用原子光学器件代替经典光学器件来实现分束、反射、合束过程而构成的物质波干涉系统,可实现角速度、加速度、时频基准、重力/重力梯度的高灵敏度测量。理论分析表明,原子干涉绝对重力仪可使现有绝对重力仪的灵敏度至少提高3个量级,因此冷原子干涉重力仪器是目前绝对重力仪和重力梯度仪领域中的研究热点,有望为未来高精度地球重力场的探测和重力场模型的建立带来革命性的影响。冷原子干涉重力仪的基本流程为:首先,利用六束光的3维磁光阱技术将大量碱金属(如铷Rb或铯Cs)原子囚禁并冷却至μK量级,使得常温状态下以超音速运动的原子速度降低至1mm/s以下;其次,将冷却后的原子团置于重力场中做自由落体运动,并与相位相干的激光脉冲相互作用,对原子波包进行分束、反射、合束等相干操控,并实现原子干涉;最后,对原子团末态进行探测,利用荧光收集或吸收成像法获得原子干涉条纹,拟合出重力加速度引起的相移,实现绝对重力加速度的精确测量。冷原子干涉重力仪的基本流程与重力仪类似,通过上下两个具有一定距离差的原子干涉重力仪测量结果做差,得到重力测量结果。The atomic interferometer is a matter-wave interference system composed of atomic matter waves instead of classical light waves as the interference medium, and atomic optical devices instead of classical optical devices to realize beam splitting, reflection, and beam combining processes. It can realize angular velocity, acceleration, and time-frequency reference. , High sensitivity measurement of gravity/gravity gradient. Theoretical analysis shows that the atomic interference absolute gravimeter can increase the sensitivity of the existing absolute gravimeter by at least 3 orders of magnitude. Therefore, the cold atom interference gravimeter is a research hotspot in the field of absolute gravimeter and gravity gradient The detection of the Earth's gravity field and the establishment of the gravity field model have brought revolutionary impact. The basic process of the cold atom interference gravimeter is as follows: first, a large number of alkali metal (such as rubidium Rb or cesium Cs) atoms are imprisoned and cooled to the μK level by using the 3-dimensional magneto-optical trap technology of six beams of light, so that The speed of the atoms moving at the speed of sound is reduced to below 1mm/s; secondly, the cooled atomic clusters are placed in the gravitational field for free fall, and interact with phase-coherent laser pulses to split, reflect, and combine the atomic wave packets. Beam and other coherent manipulation, and achieve atomic interference; finally, detect the final state of atomic groups, use fluorescence collection or absorption imaging to obtain atomic interference fringes, and fit the phase shift caused by gravitational acceleration to achieve accurate measurement of absolute gravitational acceleration. The basic process of the cold atom interference gravimeter is similar to that of the gravimeter. The gravity measurement result is obtained by making difference between the measurement results of the upper and lower atomic interference gravimeters with a certain distance difference.
目前,原子干涉重力仪的主要方案是通过三个维度的六束光形成磁光阱(Magnetic-optic traps,简记为MOT),囚禁和冷却原子团,再对原子团进行速度选择和态选择,最后进行拉曼干涉过程。磁光阱的六束激光需要在真空腔上安装六个扩束筒,光路部分需要大量的光学器件,这就不可避免的使得系统体积增加。At present, the main scheme of atomic interference gravimeter is to form magneto-optic traps (Magnetic-optic traps, abbreviated as MOT) through six beams of light in three dimensions, trap and cool atomic groups, and then perform speed selection and state selection on atomic groups, and finally Perform Raman interferometry. The six laser beams of the magneto-optical trap need to install six beam expanders on the vacuum cavity, and a large number of optical devices are required in the optical path, which inevitably increases the volume of the system.
发明内容Contents of the invention
本发明要解决的技术问题就在于:针对现有技术存在的技术问题,本发明提供一种整体体积小、鲁棒性强、成本低、测量精度高的基于二维交叉光栅的类金字塔结构型原子干涉重力加速度测量装置。The technical problem to be solved by the present invention is that: aiming at the technical problems existing in the prior art, the present invention provides a pyramid-like structure type based on two-dimensional intersecting grating with small overall volume, strong robustness, low cost and high measurement accuracy. Atom interference gravitational acceleration measurement device.
为解决上述技术问题,本发明采用以下技术方案:In order to solve the problems of the technologies described above, the present invention adopts the following technical solutions:
一种基于二维交叉光栅的类金字塔结构型原子干涉重力加速度测量装置,包括真空腔、扩束筒、二维交叉光栅以及用于产生分离式金字塔结构的反射镜组件;所述扩束筒用来引入真空系统的单根光纤,所述二维交叉光栅位于扩束筒与反射镜组件之间;所述反射镜组件由上至下依次分为:MOT区、干涉区和探测区;所述MOT区内包括四个第一反射镜,探测区的下方设置有第二反射镜。A kind of pyramidal structure-like atom interference gravitational acceleration measurement device based on two-dimensional cross grating, including vacuum chamber, beam expander, two-dimensional cross grating and reflector assembly for producing separated pyramid structure; the beam expander is used To introduce a single optical fiber into the vacuum system, the two-dimensional cross grating is located between the beam expander and the mirror assembly; the mirror assembly is divided into: MOT area, interference area and detection area from top to bottom; The MOT area includes four first reflection mirrors, and the second reflection mirror is arranged under the detection area.
作为本发明装置的进一步改进:一束冷却光由所述扩束筒引入,经过二维交叉光栅后分为五束光。As a further improvement of the device of the present invention: a beam of cooling light is introduced by the beam expander, and is divided into five beams after passing through a two-dimensional cross grating.
作为本发明装置的进一步改进:所述五束光的特性相同的。As a further improvement of the device of the present invention: the characteristics of the five beams of light are the same.
作为本发明装置的进一步改进:所述MOT区中,所述四个第一反射镜位于所述真空腔的腔体四面,且处于水平方向。As a further improvement of the device of the present invention: in the MOT area, the four first mirrors are located on four sides of the vacuum chamber and are in a horizontal direction.
作为本发明装置的进一步改进:经四个所述第一反射镜和一个第二反射镜后,形成三对相互正交的囚禁光及泵浦光,构成磁光阱,实现原子团的冷却和囚禁。As a further improvement of the device of the present invention: after the four first reflectors and one second reflector, three pairs of mutually orthogonal trapping light and pump light are formed to form a magneto-optical trap to realize the cooling and trapping of atomic groups .
作为本发明装置的进一步改进:所述真空腔采用变频干式涡旋泵、涡轮式分子泵和复合泵三级真空泵来实现系统所需的超高真空环境。As a further improvement of the device of the present invention: the vacuum chamber adopts a three-stage vacuum pump of frequency conversion dry scroll pump, turbo molecular pump and compound pump to realize the ultra-high vacuum environment required by the system.
作为本发明装置的进一步改进:所述扩束筒引入的光束包括冷却光、回泵光、探测光和拉曼光的扩束。As a further improvement of the device of the present invention: the beam introduced by the beam expander includes expanded beams of cooling light, back pumping light, probe light and Raman light.
作为本发明装置的进一步改进:所述光束中两束拉曼光的频率差为6.8GHz,一团经过冷却后的原子团,经过态制备后处于磁不敏感的状态而后对原子团施加π/2、π和π/2三束光脉冲,实现原子团的分束与合束,构建了一个原子干涉仪。As a further improvement of the device of the present invention: the frequency difference between the two beams of Raman light in the light beam is 6.8 GHz, a group of atomic groups after cooling is in a magnetically insensitive state after state preparation, and then the atomic groups are applied π/2, The three light pulses of π and π/2 realize the beam splitting and combining of atomic groups, and construct an atomic interferometer.
作为本发明装置的进一步改进:通过探测光配合回泵光的作用,分别测得处于两基态超精细能级上的原子布居数,并最终得到跃迁概率以及重力加速度值。As a further improvement of the device of the present invention: through the combination of the detection light and the pump light, the population numbers of atoms in the two ground state hyperfine energy levels are respectively measured, and finally the transition probability and the acceleration of gravity are obtained.
与现有技术相比,本发明的优点在于:Compared with the prior art, the present invention has the advantages of:
1、本发明的基于二维交叉光栅的类金字塔结构型原子干涉重力加速度测量装置,系统整体体积小,由于只需要一束光进入真空腔,激光模块省去了大量的光学器件,真空模块省略了水平方向四束光的扩束筒,从而缩小了真空模块和激光模块的体积。1. The pyramid-like structure atomic interference gravitational acceleration measurement device based on the two-dimensional cross grating of the present invention has a small overall system volume, and since only one beam of light is required to enter the vacuum cavity, the laser module saves a large number of optical devices, and the vacuum module omits A beam expander tube with four beams in the horizontal direction is provided, thereby reducing the volume of the vacuum module and the laser module.
2.本发明的基于二维交叉光栅的类金字塔结构型原子干涉重力加速度测量装置,鲁棒性强,系统调试中只需要保证引入真空腔的光纤功率稳定即可,易于实现。由于系统结构简单、调节变量少,在长时间工作时,出错概率低。2. The pyramid-like atomic interference gravitational acceleration measurement device based on the two-dimensional cross grating of the present invention has strong robustness, and only needs to ensure the stability of the optical fiber power introduced into the vacuum cavity during system debugging, which is easy to implement. Due to the simple structure of the system and few adjustment variables, the error probability is low when working for a long time.
3.本发明的基于二维交叉光栅的类金字塔结构型原子干涉重力加速度测量装置,成本低,该方案与经典的六束光方案相比,节约了大量光学器件,从而降低了总体成本。3. The pyramid-like atomic interference gravitational acceleration measurement device based on the two-dimensional cross grating of the present invention has low cost. Compared with the classic six-beam solution, this solution saves a large number of optical devices, thereby reducing the overall cost.
附图说明Description of drawings
图1是本发明装置的主视结构原理示意图。Fig. 1 is a schematic diagram of the front view structure of the device of the present invention.
图2是本发明装置的侧视结构原理示意图。Fig. 2 is a schematic diagram of the side view structure of the device of the present invention.
图3是本发明装置的立体结构原理示意图。Fig. 3 is a schematic diagram of the three-dimensional structure principle of the device of the present invention.
图4是本发明在具体应用实例中的详细流程示意图。Fig. 4 is a detailed flow diagram of the present invention in a specific application example.
图例说明:illustration:
1、真空腔;2、扩束筒;3、二维交叉光栅;4、MOT区;5、第一干涉区;6、第二反射镜;7、探测区;8、第一反射镜;9、复合泵。1. Vacuum chamber; 2. Beam expander; 3. Two-dimensional cross grating; 4. MOT area; 5. First interference area; 6. Second mirror; 7. Detection area; 8. First mirror; 9 , Compound pump.
具体实施方式Detailed ways
以下将结合说明书附图和具体实施例对本发明做进一步详细说明。The present invention will be further described in detail below in conjunction with the accompanying drawings and specific embodiments.
如图1、图2和图3所示,本发明的基于二维交叉光栅的类金字塔结构型原子干涉重力测量装置采用二维交叉光栅3进行分束,形成的类金字塔磁光阱的设计方案。具体来说就是,整个真空系统只需要从上往下的一束光,通过二维交叉光栅3分束为五束特性相同的光,通过水平方向的四个反射镜和最下面的反射镜形成三对相互正交的囚禁光及泵浦光,构成磁光阱,实现原子团的冷却和囚禁,取代传统六束光方案。As shown in Fig. 1, Fig. 2 and Fig. 3, the quasi-pyramid structure type atomic interference gravity measurement device based on two-dimensional cross grating of the present invention adopts two-dimensional cross grating 3 to carry out beam splitting, the design scheme of the quasi-pyramid magneto-optical trap formed . Specifically, the entire vacuum system only needs one beam of light from top to bottom, which is divided into five beams of light with the same characteristics through the two-dimensional cross grating 3, and is formed by four mirrors in the horizontal direction and the bottom mirror. Three pairs of orthogonal confinement light and pump light form a magneto-optical trap to realize the cooling and confinement of atomic groups, replacing the traditional six-beam light scheme.
本发明的装置具体包括真空腔1、扩束筒2、二维交叉光栅3以及用于产生分离式金字塔结构的反射镜组件。所有器件都安装于真空腔1内,扩束筒2用来引入真空系统的单根光纤,二维交叉光栅3位于扩束筒2与反射镜组件之间。反射镜组件由上至下依次分为:MOT区4、第一干涉区5和探测区7。MOT区4内包括四个第一反射镜8,探测区7的下方设置有第二反射镜6。一束冷却光由扩束筒2引入,经过二维交叉光栅3后分为五束特性相同的光。经四个第一反射镜8和一个第二反射镜6形成三对相互正交的囚禁光及泵浦光,构成磁光阱,实现原子团的冷却和囚禁。The device of the present invention specifically includes a vacuum chamber 1, a beam expander cylinder 2, a two-dimensional cross grating 3 and a mirror assembly for producing a split pyramid structure. All devices are installed in the vacuum chamber 1, the beam expander 2 is used to introduce a single optical fiber of the vacuum system, and the two-dimensional cross grating 3 is located between the beam expander 2 and the mirror assembly. The mirror assembly is divided into: MOT area 4 , first interference area 5 and detection area 7 from top to bottom. The MOT area 4 includes four first reflection mirrors 8 , and the second reflection mirror 6 is arranged under the detection area 7 . A beam of cooling light is introduced by the beam expander tube 2 and divided into five beams of light with the same characteristics after passing through the two-dimensional cross grating 3 . Four first reflectors 8 and one second reflector 6 form three pairs of mutually orthogonal trapping light and pumping light to form a magneto-optical trap to realize cooling and confinement of atomic groups.
在具体应用实例中,在真空腔1的腔体四面各放置一个处于水平方向的第一反射镜8。In a specific application example, a first reflector 8 in a horizontal direction is placed on each of the four sides of the vacuum chamber 1 .
本发明的原子干涉重力仪采用冷原子作为检验介质,其热扩散速率小,有利于增加测量时间,但原子在冷却和囚禁过程中很容易与背景杂散气体发生随机碰撞,从而引起冷原子的寿命和相干时间减小,因此冷原子干涉实验需要在超高真空环境下进行。在具体应用实例中,真空腔1采用玻璃真空腔1,该玻璃真空腔为边长20mm的长方体。作为优选实施例,本发明的真空系统,采用变频干式涡旋泵、涡轮式分子泵和复合泵9(由离子泵与吸气剂组合而成)三级真空泵来实现系统所需的超高真空环境(优于10-8Pa)。The atomic interference gravimeter of the present invention uses cold atoms as the test medium, and its thermal diffusion rate is small, which is beneficial to increase the measurement time, but the atoms are easy to randomly collide with the background stray gas during the cooling and trapping process, thus causing cold atoms The lifetime and coherence time are reduced, so cold atom interference experiments need to be carried out in an ultra-high vacuum environment. In a specific application example, the vacuum chamber 1 adopts a glass vacuum chamber 1, which is a cuboid with a side length of 20 mm. As a preferred embodiment, the vacuum system of the present invention adopts a frequency conversion dry scroll pump, a turbomolecular pump and a compound pump 9 (combined by an ion pump and a getter) three-stage vacuum pump to achieve the ultra-high vacuum required by the system. Vacuum environment (better than 10 -8 Pa).
在具体应用实例中,光纤引入的光包括:冷却光、回泵光、探测光和拉曼光的扩束。两束拉曼光的频率差为6.8GHz。一团经过冷却后的原子团(温度约1μk),经过态制备后处于磁不敏感的状态F=1,mF=0,而后对原子团施加π/2、π和π/2三束光脉冲,实现原子团的分束与合束,构建了一个原子干涉仪。最后,通过探测光配合回泵光的作用,分别测得处于两基态超精细能级上的原子布居数,并最终得到跃迁概率以及重力加速度值。In a specific application example, the light introduced by the optical fiber includes: cooling light, back-pumping light, probe light and beam expansion of Raman light. The frequency difference between the two Raman beams is 6.8GHz. A group of cooled atomic groups (temperature about 1μk) is in a magnetically insensitive state F=1, m F =0 after state preparation, and then three beams of light pulses of π/2, π and π/2 are applied to the atomic group, Realize the beam splitting and combining of atomic groups, and construct an atomic interferometer. Finally, through the combination of probe light and back-pump light, the population numbers of atoms in the two ground state hyperfine energy levels are measured respectively, and the transition probability and the acceleration of gravity are finally obtained.
如图4所示,本发明在具体应用实例中的详细流程为:As shown in Figure 4, the detailed process of the present invention in the specific application example is:
S1:冷原子团的制备。S1: Preparation of cold atomic groups.
首先通过磁光阱、偏振梯度冷却(Polarization Gradient Cooling,简记为PGC)进行前级冷却得到温度约为15μk的冷原子团。Firstly, pre-cooling is performed by magneto-optical trap and Polarization Gradient Cooling (abbreviated as PGC) to obtain cold atomic groups with a temperature of about 15 μk.
S2:速度选择与态制备。S2: Speed selection and state preparation.
通过拉曼速度选择,原子团温度进一步降低至约1μk。态制备在磁不敏感的状态F=1,mF=0上。By Raman velocity selection, the cluster temperature is further reduced to about 1 μk. The state is prepared on the magnetically insensitive state F=1, m F =0.
S3:原子干涉。S3: Atom interference.
通过两束拉曼光对原子团施加π/2、π和π/2三束光脉冲,实现原子团的分束与合束,构建了一个原子干涉仪。Three beams of π/2, π and π/2 light pulses are applied to the atomic cluster by two beams of Raman light to realize beam splitting and beam combining of the atomic cluster, and an atomic interferometer is constructed.
S4:内态探测。S4: internal state detection.
在干涉完成后,将原子团自由下落一段时间,而后通过探测光配合回泵光、吹散光的作用,分别测得处于两基态超精细能级上的原子布居数,并最终得到跃迁概率以及重力加速度值。After the interference is completed, the atomic clusters fall freely for a period of time, and then through the action of the probe light combined with the pump light and the blown light, the population numbers of atoms in the two ground state hyperfine energy levels are respectively measured, and finally the transition probability and gravity are obtained. Acceleration value.
本发明提出了分离式倒金字塔的方案设计,只需要一根光纤引入真空腔1。本发明的优势在于:The present invention proposes a separate inverted pyramid scheme design, which only needs one optical fiber to be introduced into the vacuum cavity 1 . The advantages of the present invention are:
(1)系统整体体积小。与经典的六束光MOT相比,本发明只需要一束光进入真空腔1,激光模块省去了大量的光学器件,真空模块省略了水平方向MOT光的扩束筒2,从而缩小了真空模块和激光模块的体积。(1) The overall volume of the system is small. Compared with the classic six-beam MOT, the present invention only needs one beam of light to enter the vacuum cavity 1, the laser module saves a large number of optical devices, and the vacuum module omits the beam expander 2 of the MOT light in the horizontal direction, thus reducing the vacuum space. The volume of the module and the laser module.
(2)鲁棒性强。系统调试中只需要保证引入真空腔1的光纤功率稳定即可,易于实现。由于系统结构简单、调节变量少,在长时间工作时,出错概率低。(2) Strong robustness. During system debugging, it is only necessary to ensure that the power of the optical fiber introduced into the vacuum chamber 1 is stable, which is easy to implement. Due to the simple structure of the system and few adjustment variables, the error probability is low when working for a long time.
(3)调节灵活。与传统的金字塔方案相比,本发明将金字塔的四个面采用分立元件组合形成,每个面能够灵活、独立的调节,降低了加工和安装的精度要求的同时,提高了测量结果的稳定性。(3) Flexible adjustment. Compared with the traditional pyramid scheme, the present invention combines the four faces of the pyramid with discrete components, and each face can be adjusted flexibly and independently, reducing the accuracy requirements of processing and installation, and improving the stability of the measurement results .
(4)低成本。本发明与经典的六束光方案相比,节约了大量光学器件,从而降低了总体成本。(4) Low cost. Compared with the classical scheme of six beams of light, the present invention saves a lot of optical devices, thereby reducing the overall cost.
以上仅是本发明的优选实施方式,本发明的保护范围并不仅局限于上述实施例,凡属于本发明思路下的技术方案均属于本发明的保护范围。应当指出,对于本技术领域的普通技术人员来说,在不脱离本发明原理前提下的若干改进和润饰,应视为本发明的保护范围。The above are only preferred implementations of the present invention, and the protection scope of the present invention is not limited to the above-mentioned embodiments, and all technical solutions under the idea of the present invention belong to the protection scope of the present invention. It should be pointed out that for those skilled in the art, some improvements and modifications without departing from the principle of the present invention should be regarded as the protection scope of the present invention.
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