CN103941577A - Atom gas cavity device with double reflectors and groove-shaped structure and manufacturing method thereof - Google Patents
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Abstract
本发明涉及具有双反射镜和凹槽形结构的原子气体腔器件及其制造方法。所述的原子气体腔器件由一层底部设有反射镜的具有凹槽的硅片和一层内部设有反射镜的玻璃片通过键合围成的腔体结构构成。所述的凹槽的横截面为倒梯形结构,由(100)型的单晶硅片通过硅各向异性湿法腐蚀形成,凹槽的侧壁为硅片的{111}晶面。玻璃片内部和硅片凹槽的底部各有一个反射镜,用于激光的多次反射。本发明所述的原子气体腔器件可用于原子钟和磁强计等系统中,激光在双反射镜间进行多次反射,从而增加激光与原子气体间的相互作用空间长度,使相干布局囚禁效应信号的信噪比增强,有利于提高系统的稳定度。
The invention relates to an atomic gas cavity device with a double mirror and a groove-shaped structure and a manufacturing method thereof. The atomic gas cavity device is composed of a cavity structure surrounded by a layer of silicon wafer with grooves provided at the bottom with a reflector and a layer of glass sheet with a reflector inside through bonding. The cross-section of the groove is an inverted trapezoidal structure, which is formed by (100) type single crystal silicon wafer through silicon anisotropic wet etching, and the side wall of the groove is the {111} crystal plane of the silicon wafer. There is a reflector inside the glass sheet and at the bottom of the groove of the silicon sheet, which are used for multiple reflections of the laser light. The atomic gas cavity device described in the present invention can be used in systems such as atomic clocks and magnetometers. Laser light is reflected multiple times between double mirrors, thereby increasing the interaction space length between laser light and atomic gas, and making the coherent layout trap effect signals The signal-to-noise ratio is enhanced, which is conducive to improving the stability of the system.
Description
技术领域 technical field
本发明属于微电子机械系统(MEMS)器件制作与封装技术领域,以及原子物理器件技术领域,具体涉及一种基于MEMS工艺的微型原子腔结构及其制造方法。 The invention belongs to the technical field of micro-electro-mechanical system (MEMS) device manufacturing and packaging, and the technical field of atomic physics devices, and specifically relates to a micro-atomic cavity structure based on MEMS technology and a manufacturing method thereof.
背景技术 Background technique
原子钟测量时间的精确度可以达到十亿分之一秒甚至更高,原子钟是目前最精准的人造钟,其相关研究具有重要的意义。CPT(Coherent Population Trapping,相干布局囚禁效应)原子钟是利用双色相干光与原子作用将原子制备成相干态,利用CPT信号作为微波鉴频信号而实现的原子钟频率源。由于具有易于微型化、低功耗和高频率稳定度等特点,CPT原子钟一经提出就受到各国研究机构的重视,并开展了深入的研究。 Atomic clocks can measure time with an accuracy of one billionth of a second or even higher. Atomic clocks are currently the most accurate artificial clocks, and their related research is of great significance. CPT (Coherent Population Trapping, coherent layout trapping effect) atomic clock is an atomic clock frequency source realized by using two-color coherent light to interact with atoms to prepare atoms into a coherent state, and using the CPT signal as a microwave frequency discrimination signal. Due to the characteristics of easy miniaturization, low power consumption and high frequency stability, the CPT atomic clock has been valued by research institutions in various countries since it was proposed, and in-depth research has been carried out.
CPT原子钟是一个复杂的系统,其核心部件就是原子气体腔。利用现在成熟的MEMS技术制作微型原子气体腔体,可以将被动型CPT原子钟尺寸缩小到芯片级。芯片级CPT原子钟能够大幅度减小原子钟体积与功耗,实现电池供电,并且可以批量、低成本生产,在军用、民用的各个领域具有巨大市场,因此成为原子钟的重要发展方向。 The CPT atomic clock is a complex system, and its core component is the atomic gas cavity. Using the now mature MEMS technology to make a miniature atomic gas cavity can reduce the size of the passive CPT atomic clock to the chip level. Chip-level CPT atomic clocks can greatly reduce the size and power consumption of atomic clocks, realize battery power supply, and can be produced in batches and at low cost. They have huge markets in various fields of military and civilian use, so they have become an important development direction for atomic clocks.
目前,芯片级CPT原子钟的原子气体腔结构通常是中间为硅片两边为玻璃的三明治结构。先在单晶硅片上制作通孔,然后与Pyrex玻璃片键合形成半腔结构,待碱金属与缓冲气体充入后,再与另外一片Pyrex玻璃片键合形成密封结构。这种结构的碱金属原子气体腔结构的腔内光与原子作用光路长度受到硅片厚度及硅加工工艺的限制,通常为1mm~2mm,进一步增加厚度困难且昂贵,因此限制了光与原子相互作用光程,CPT信号的信噪比较低,影响了CPT原子钟的频率稳定度。 At present, the atomic gas cavity structure of the chip-level CPT atomic clock is usually a sandwich structure with a silicon wafer in the middle and glass on both sides. First make a through hole on the single crystal silicon wafer, and then bond it with a Pyrex glass sheet to form a half-cavity structure. After the alkali metal and buffer gas are filled, it is bonded with another piece of Pyrex glass sheet to form a sealed structure. The optical path length of the interaction between light and atoms in the alkali metal atom gas cavity structure of this structure is limited by the thickness of the silicon wafer and the silicon processing technology, usually 1 mm to 2 mm, and it is difficult and expensive to further increase the thickness, thus limiting the interaction between light and atoms. Due to the action optical path, the signal-to-noise ratio of the CPT signal is low, which affects the frequency stability of the CPT atomic clock.
发明内容 Contents of the invention
在现有研究基础上,为了进一步提高光与原子相互作用的光程,增大CPT信号信噪比、增加频率稳定度,本发明提供一种具有双反射镜和凹槽形结构的原子气体腔器件及其制造方法。 On the basis of existing research, in order to further improve the optical path of the interaction between light and atoms, increase the signal-to-noise ratio of the CPT signal, and increase the frequency stability, the present invention provides an atomic gas cavity with double mirrors and a groove-shaped structure Devices and methods of making them.
具有双反射镜和凹槽形结构的原子气体腔器件包括硅片和玻璃片,所述硅片的一侧面设有凹槽,凹槽内底部设有下反射镜;所述玻璃片的一侧面设有上反射镜;硅片和玻璃片通过键合形成原子气体腔器件,玻璃片上的上反射镜对应位于硅片的凹槽内,且与下反射镜对应。 The atomic gas chamber device with double reflection mirrors and groove-shaped structure comprises a silicon wafer and a glass wafer, one side of the silicon wafer is provided with a groove, and the inner bottom of the groove is provided with a lower reflector; one side of the glass wafer is An upper reflection mirror is provided; the silicon wafer and the glass wafer are bonded to form an atomic gas cavity device, and the upper reflection mirror on the glass wafer is correspondingly located in the groove of the silicon wafer and corresponds to the lower reflection mirror.
所述凹槽的横截面为倒梯形,凹槽为湿法腐蚀形成,硅片的类型为(100)型硅片,且腐蚀形成的凹槽的侧壁和玻璃片的夹角为54.7度。 The cross section of the groove is an inverted trapezoid, the groove is formed by wet etching, the type of silicon wafer is (100) type silicon wafer, and the angle between the side wall of the groove formed by etching and the glass sheet is 54.7 degrees.
所述凹槽的宽度W为倒梯形的横截面的底面宽度,且为硅片厚度H的两倍以上。 The width W of the groove is the width of the bottom surface of the inverted trapezoidal cross section, and is more than twice the thickness H of the silicon wafer.
具有双反射镜和凹槽形结构的原子气体腔器件的具体制备操作步骤如下: The specific preparation steps of the atomic gas cavity device with double mirrors and groove-shaped structure are as follows:
1).在硅片上制作凹槽 1). Make grooves on the silicon wafer
选择(100)型的硅片,利用二氧化硅作为掩膜层进行各向异性湿法腐蚀,在硅片的一侧面上形成一百个以上横截面为倒梯形的凹槽; Select a (100) type silicon wafer, use silicon dioxide as a mask layer to perform anisotropic wet etching, and form more than one hundred grooves with an inverted trapezoidal cross section on one side of the silicon wafer;
2).在玻璃上制作反射镜 2). Make a reflector on the glass
采用蒸发工艺或溅射工艺,利用硬掩模或剥离技术,在玻璃片的一侧面上制作一百个以上的金属膜反射镜,即上反射镜;在硅片上的每个凹槽的底部制作一百个以上的金属膜反射镜,即下反射镜; Using evaporation process or sputtering process, using hard mask or lift-off technology, make more than one hundred metal film mirrors on one side of the glass sheet, that is, the upper mirror; at the bottom of each groove on the silicon wafer Make more than one hundred metal film mirrors, that is, lower mirrors;
3).硅-玻璃键合 3). Silicon-glass bonding
进行硅-玻璃键合,同时通入碱金属蒸汽和缓冲气体,使硅片和玻璃片密封形成原子气体腔器件; Silicon-glass bonding is carried out, and alkali metal vapor and buffer gas are introduced at the same time, so that the silicon wafer and the glass wafer are sealed to form an atomic gas cavity device;
4).划片 4). Scribing
以硅片上的凹槽为单元,将整个硅片进行划分,形成一百个以上单个的原子气体腔器件。 Divide the entire silicon wafer with the groove on the silicon wafer as a unit to form more than one hundred single atomic gas cavity devices.
所述碱金属蒸汽为铷蒸汽或铯蒸汽,所述的缓冲气体为85%的氮气、10%的氢气和5%的二氧化碳的混合气体。 The alkali metal vapor is rubidium vapor or cesium vapor, and the buffer gas is a mixed gas of 85% nitrogen, 10% hydrogen and 5% carbon dioxide.
本发明的有益技术效果体现在以下方面: Beneficial technical effect of the present invention is embodied in the following aspects:
1.本发明的原子气体腔器件使得激光与碱金属原子之间作用光程主要由凹槽的底部宽度决定,因此可以不局限于硅片厚度,通过改变原子腔体尺寸设计易于增加激光与原子气体间的相互作用空间长度,使相干布局囚禁效应信号的信噪比增强,有利于提高系统的稳定度; 1. The atomic gas cavity device of the present invention makes the optical path between the laser and the alkali metal atoms mainly determined by the width of the bottom of the groove, so it is not limited to the thickness of the silicon wafer, and it is easy to increase the laser and the atomic cavity by changing the size of the atomic cavity. The length of the interaction space between gases enhances the signal-to-noise ratio of the coherent layout trapping effect signal, which is conducive to improving the stability of the system;
2.本发明的原子气体腔器件的制造技术主要基于硅的各向异性湿法腐蚀工艺和硅-玻璃阳极键合等成熟MEMS工艺,因此成本低,易于实现; 2. The manufacturing technology of the atomic gas chamber device of the present invention is mainly based on mature MEMS processes such as silicon anisotropic wet etching process and silicon-glass anode bonding, so the cost is low and easy to implement;
3.基于MEMS批量加工的特点,在同一批次的流片中,可以完成不同尺寸的原子气体腔的制造。 3. Based on the characteristics of batch processing of MEMS, in the same batch of tape-out, the manufacture of atomic gas cavities of different sizes can be completed.
附图说明 Description of drawings
图1为本发明结构横剖图。 Fig. 1 is a cross-sectional view of the structure of the present invention.
图2为本发明原子气体腔器件的关键尺寸标识图。 Fig. 2 is a key dimension identification diagram of the atomic gas cavity device of the present invention.
图3为激光在本发明的原子气体腔器件中的光路示意图。 Fig. 3 is a schematic diagram of the optical path of the laser in the atomic gas cavity device of the present invention.
图4为激光在传统原子气体腔中的光路示意图。 Fig. 4 is a schematic diagram of the optical path of a laser in a conventional atomic gas cavity.
上图中:硅片1、玻璃片2、原子气体腔3、上反射镜4、下反射镜5、H为硅片的厚度,W为凹槽底部宽度,α为凹槽的侧壁和玻璃片之间的夹角。 In the figure above: silicon wafer 1, glass wafer 2, atomic gas cavity 3, upper mirror 4, lower mirror 5, H is the thickness of the silicon wafer, W is the width of the bottom of the groove, α is the side wall of the groove and the glass angle between slices.
具体实施方式 Detailed ways
下面结合附图,通过实施例对本发明作进一步地说明。 The present invention will be further described through the embodiments below in conjunction with the accompanying drawings.
实施例1Example 1
参见图1和图2,具有双反射镜和凹槽形结构的原子气体腔器件包括硅片1和玻璃片2。硅片1的一侧面设有凹槽,凹槽的横截面为倒梯形,凹槽内底部设有下反射镜5;玻璃片2的一侧面设有上反射镜4;硅片1和玻璃片2通过键合形成原子气体腔3器件,玻璃片2上的上反射镜4对应位于硅片1的凹槽内,且与下反射镜5对应。 Referring to FIG. 1 and FIG. 2 , an atomic gas cavity device with double mirrors and a groove-shaped structure includes a silicon wafer 1 and a glass wafer 2 . One side of the silicon chip 1 is provided with a groove, the cross section of the groove is an inverted trapezoid, and the inner bottom of the groove is provided with a lower reflector 5; one side of the glass sheet 2 is provided with an upper reflector 4; the silicon chip 1 and the glass sheet 2 The atomic gas cavity is formed by bonding 3 The device, the upper mirror 4 on the glass sheet 2 is correspondingly located in the groove of the silicon wafer 1, and corresponds to the lower mirror 5.
如图3所示,激光在原子气体腔3器件中的光程主要由凹槽底部的宽度W决定,通过调节W的大小即可改变光程。参见图4,在传统的原子气体腔器件中,激光直接从顶端射入,底端射出,光程由硅片的厚度H决定。 As shown in Figure 3, the optical path of the laser in the atomic gas cavity 3 device is mainly determined by the width W of the bottom of the groove, and the optical path can be changed by adjusting the size of W. Referring to Figure 4, in a traditional atomic gas cavity device, the laser is directly injected from the top and emitted from the bottom, and the optical path is determined by the thickness H of the silicon wafer.
具有双反射镜和凹槽形结构的原子气体腔器件的具体制备操作步骤如下: The specific preparation steps of the atomic gas cavity device with double mirrors and groove-shaped structure are as follows:
1.选取厚度为0.5~1mm的N(100)型的硅片1,利用二氧化硅做掩模,利用氢氧化钾溶液进行各向异性湿法腐蚀工艺,在硅片1上形成二百个横截面为倒梯形的凹槽,凹槽的侧壁即为{111}晶面,凹槽的底部宽度为3mm。氢氧化钾腐蚀的温度为60℃; 1. Select an N(100) type silicon wafer 1 with a thickness of 0.5-1 mm, use silicon dioxide as a mask, and use potassium hydroxide solution to perform anisotropic wet etching process to form two hundred silicon wafers on the silicon wafer 1. The cross section is an inverted trapezoidal groove, the side wall of the groove is the {111} crystal plane, and the width of the bottom of the groove is 3mm. The corrosion temperature of potassium hydroxide is 60°C;
2.采用蒸发工艺,利用剥离技术,在玻璃片2的一侧面上制作二百个金属膜反射镜,即上反射镜4;在硅片1的每个凹槽的底部制作二百个金属膜反射镜,即下反射镜5; 2. Using the evaporation process and the stripping technique, make two hundred metal film mirrors on one side of the glass sheet 2, that is, the upper mirror 4; make two hundred metal film mirrors at the bottom of each groove of the silicon chip 1 Reflector, i.e. lower reflector 5;
3.进行硅-玻璃键合,同时通入铷蒸汽和缓冲气体,使硅片1和玻璃片2密封形成原子气体腔器件;缓冲气体为85%的氮气、10%的氢气和5%的二氧化碳组成的混合气体。阳极键合的工艺条件为:温度400℃,电压600V; 3. Carry out silicon-glass bonding, and pass rubidium vapor and buffer gas at the same time, so that silicon wafer 1 and glass wafer 2 are sealed to form an atomic gas cavity device; the buffer gas is 85% nitrogen, 10% hydrogen and 5% carbon dioxide Composed of gas mixtures. The process conditions of anodic bonding are: temperature 400°C, voltage 600V;
4.划片 4. Dicing
以硅片1上的凹槽为单元,将整个硅片1进行划分,形成二百个单个的原子气体腔3器件。 Taking the grooves on the silicon wafer 1 as a unit, the entire silicon wafer 1 is divided to form two hundred individual atomic gas cavity 3 devices.
实施例2Example 2
本实施例的原子气体腔的结构如图1所示,具体实施方案如下: The structure of the atomic gas chamber of the present embodiment is as shown in Figure 1, and the specific implementation is as follows:
1.选取厚度为0.5~1mm的P(100)型的硅片1,利用氮化硅做掩模,通过TMAH溶液进行各向异性湿法腐蚀,在硅片1上形成横截面为倒梯形的一百五十个凹槽,凹槽的侧壁即为{111}晶面,通孔的横向宽度为5mm。TMAH溶液腐蚀的温度为80℃; 1. Select a P(100) silicon wafer 1 with a thickness of 0.5-1 mm, use silicon nitride as a mask, and perform anisotropic wet etching through TMAH solution to form an inverted trapezoidal cross section on the silicon wafer 1. One hundred and fifty grooves, the side walls of the grooves are {111} crystal planes, and the lateral width of the through holes is 5mm. The corrosion temperature of TMAH solution is 80°C;
2.采用溅射工艺,利用硬掩模技术,分别在玻璃片2的一侧面上制作一百五十个金属膜反射镜,即上反射镜4;在硅片1的每个凹槽的底部制作一百五十个金属膜反射镜,即下反射镜5; 2. Using the sputtering process and hard mask technology, one hundred and fifty metal film mirrors, namely the upper mirror 4, are fabricated on one side of the glass sheet 2; at the bottom of each groove of the silicon wafer 1 Make one hundred and fifty metal film reflectors, that is, the lower reflector 5;
3.进行硅-玻璃键合,同时通入铯蒸汽和缓冲气体,使硅片1和玻璃片2形成密封的原子气体腔器件;缓冲气体为85%的氮气、10%的氢气和5%的二氧化碳组成的混合气体,阳极键合的工艺条件为:温度400℃,电压600V; 3. Carry out silicon-glass bonding, and feed cesium vapor and buffer gas at the same time, so that silicon wafer 1 and glass wafer 2 form a sealed atomic gas chamber device; the buffer gas is 85% nitrogen, 10% hydrogen and 5% hydrogen Mixed gas composed of carbon dioxide, the process conditions of anodic bonding are: temperature 400°C, voltage 600V;
4.划片,以硅片1上的凹槽为单元,将整个硅片1进行划分,形成一百五十个单个的原子气体腔3器件。 4. Scribing, using the grooves on the silicon wafer 1 as a unit, divide the entire silicon wafer 1 to form one hundred and fifty individual atomic gas cavity 3 devices.
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| CN106707202B (en) * | 2017-01-11 | 2019-05-21 | 上海理工大学 | High spatial resolution detector for magnetic field and method |
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| CN111316031B (en) * | 2017-12-15 | 2022-04-26 | 德州仪器公司 | Method for generating gas in cavity of sealed gas chamber |
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Application publication date: 20140723 |