The present invention relates to a magnetic field measuring apparatus.
For example, PTL 1 (JP 2013-007720 A) and PTL 2 (JP 2012-183290 A) disclose an optical pumping magnetometer, as a magnetic field measuring apparatus, including a gas cell filled with an alkali metal gas inside by using such as a silicon substrate. Herein, for example, the above-described gas cell is made of glass in a conventional technique. However, a substrate is machined by using micro electro mechanical systems (MEMS) in a technique described in PTL 1, and a gas cell is formed in which a glass substrate, a substrate, and a glass substrate are laminated in this order. Further, a gas cell is formed by assembling multiple plate materials in a technique described in PTL 2.
PTL 1: JP 2013-007720 A
PTL 2: JP 2012-183290 A
For example, in a process for manufacturing a gas cell using an MEMS technique, a through hole is formed on a silicon substrate (Si substrate). After a first glass substrate is bonded on a lower surface of the Si substrate, for example, a second glass substrate is bonded on an upper surface of the Si substrate by introducing an alkali metal.
An example of a technique for introducing an alkali metal includes a technique in which a compound including the alkali metal is used since the alkali metal is unstable in the atmosphere. Specifically, in this technique, a micropipette and an inkjet coating apparatus are used by using a compound, as a solution, including an alkali metal, and the solution is dropped on a first glass substrate exposed at a bottom of a through hole. After the solution is dropped, the solution is dried, and then the through hole is sealed by a second glass substrate. Subsequently, by using such as photolysis and pyrolysis with respect to a compound existing in a dry state in a through hole, an alkali metal gas is produced from the compound and filled in the sealed through hole.
However, when an inventor of the present invention has considered the above-described technique for introducing an alkali metal, the inventor has found that there has been room for improvement to be described below. Specifically, the inventor has found that, in the above-described technique for introducing an alkali metal, for example, a dropped solution has creeped up on a side surface of a through hole due to surface tension, and also a phenomenon has occurred in which the solution spills over an outside of the through hole from a side surface thereof. In the case where this phenomenon occurs, the compound is precipitated from a side surface of the through hole to an outside if the solution is dried. Then, the through hole is sealed by the second glass substrate. However, as a result of that the compound is precipitated from a side surface of the through hole to an outside, the compound is inserted between the Si substrate and the second glass substrate in a sealing process.
Therefore, since the compound is inserted between the Si substrate and the second glass substrate, a bonding defect between the Si substrate and the second glass substrate occurs, and the bonding defect portion becomes a leak path. Accordingly, it becomes difficult to fully seal a gas in a gas cell, and a yield of the gas cell might be reduced. Specifically, in the above-described technique for introducing an alkali metal, there is a room for further improvement from a viewpoint of improving a manufacturing yield of a gas cell.
Herein, a case where an alkali metal gas is used is described as a specific representative example. However, the above-described improvement is widely possible in the case where, regardless of a gas type, a gas to be filled in a gas cell is introduced in a state in which the gas is a solution compound.
An object of the present invention is to provide a technique for improving a manufacturing yield of a gas cell included in a magnetic field measuring apparatus.
Other issues and new characteristics will be specified from descriptions described herein and attached drawings.
A magnetic field measuring apparatus according to an embodiment described herein includes a gas cell including a first cavity for filling a gas. The gas cell includes (a) a first sealing substrate, (b) a second sealing substrate, (c) a substrate member sandwiched between the first sealing substrate and the second sealing substrate, and (d) the first cavity penetrating the substrate member. The first cavity includes (e1) a first opening coming into contact with an upper surface of the first sealing substrate and (e2) a second opening coming into contact with a lower surface of the second sealing substrate. At this time, the first opening and the second opening are communicated each other, and accordingly the first cavity is formed. A plane size of the first opening is larger than a plane size of the second opening.
According to an embodiment described herein, a manufacturing yield of a gas cell included in a magnetic field measuring apparatus can be improved. In other words, according to the embodiment, reliability of the gas cell included in the magnetic field measuring apparatus can be improved.
If necessary for convenience in embodiments to be described below, the embodiments will be described by dividing into multiple sections or embodiments. However, unless especially specified, those are related to each other, and one embodiment is such as a variation, a detail, and a supplemental description in part or whole of another embodiment.
Further, in the embodiments described below, in the case where a number of elements (including a quantity, a value, an amount, and a range) are specified, it is not limited to a specific number, and it may be equal to, or greater, or less than the specific number, except for the case of being especially specified and being obviously limited to a specific number in principle.
Furthermore, in the embodiments described below, components thereof (including such as an element step) is not necessarily essential, except for the case of being especially specified and the case where it is considered to be obviously essential in principle.
Similarly, in the embodiments described below, when a shape and a positional relation of such as components are described, a substantially approximate or similar shape and relation are included, except for the case of being especially specified and the case where it is considered not to be approximate or similar in principle. This can be applicable to the above-described value and range.
Further, in every drawing for describing the embodiments, same members are denoted by the same reference signs in principle, and redundant descriptions thereof are omitted. Even a plan view may be hatched for clarification.
First, the optical system includes a semiconductor laser LD, an optical fiber OF1, a collimator lens LEN1, a polarizer PR, a wavelength plate WP, a condenser lens LEN2, an optical fiber OF2, and a photo detector PD.
The semiconductor laser LD functions as a light source which irradiates the gas cell GC with a light (pumping light) and emits a monochromatic laser light. For example, the semiconductor laser LD has a configuration in which an active layer is sandwiched by clad layers. In the semiconductor laser LD, inverted distribution is formed by injecting an electron and a hole into an active layer, and a laser light is emitted in which a phase is adjusted by using induced emission from a conduction band to a valence band.
The optical fiber OF1 functions as an optical path of a laser light emitted from the semiconductor laser LD. In this optical fiber OF1, for example, a core layer having a high reflective index is formed at a center portion, and a clad layer having a low reflective index is formed so as to surround the core layer. In the optical fiber OF1, a laser light is totally reflected on a boundary surface between the core layer and the clad layer. Therefore, the laser light efficiently passes through the core layer.
Next, the collimator lens LEN1 has a function to convert, into a parallel light, a laser light emitted from the semiconductor laser LD and passed through the optical fiber OF1. Subsequently, the polarizer PR and the wavelength plate WP convert, into a circular polarizing laser light, a parallel light emitted from the collimator lens LEN1. The circular polarizing laser light converted by the polarizer PR and the wavelength plate WP is emitted in the gas cell GC.
The condenser lens LEN2 condenses a laser light which has passed through the gas cell GC. The optical fiber OF2 forms a light path through which the laser light condensed by the condenser lens LEN2 passes. Further, the photo detector PD has a function to detect the laser light which has passed through the optical fiber OF2, and for example, and the photo detector PD includes a photodiode.
A magnetic system, for example, includes a coil COL which functions as a magnetic field production unit for producing a magnetic field. The coil COL can produce a static magnetic field and an alternating magnetic field. In
Next, the gas cell GC is filled with an alkali metal gas such as cesium, potassium, rubidium, and the gas cell GC is disposed so that a laser light is emitted from the semiconductor laser LD to the filled alkali metal gas through an optical system. A laser light entered into the gas cell GC is partially emitted from the gas cell GC, and the emitted laser light is entered into the photo detector PD by the optical system. Further, the gas cell GC is disposed so that a static magnetic field and an alternating magnetic field produced in the coil COL are applied.
In the case of disposing the semiconductor laser LD and the photo detector PD on an outer side of the coil COL through the optical fiber OF1 and the optical fiber OF2, a current and an electric wiring for driving the semiconductor laser LD and a current and an electric wiring from the photo detector PD prevent that a measurement error caused when uniformity of a magnetic field applied from the coil COL is deteriorated.
However, in the case where the above-described current and electric wiring are less effective, the semiconductor laser LD may be directly disposed on the collimator lens LEN1 without using the optical fiber OF1. Further, the photo detector PD may be directly disposed on the condenser lens LEN2 without using the optical fiber OF2, and the photo detector PD can be disposed so as to directly come into contact with the gas cell GC without using the condenser lens LEN2. In this case, the magnetic field measuring apparatus MMA according to the first embodiment can be downsized.
Furthermore, a light entered into the gas cell GC may be a circular polarizing light. Therefore, if the magnetic field measuring apparatus MMA can emit a circular polarizing light, any of components included in the optical system, such as the semiconductor laser LD, the collimator lens LEN1, the polarizer PR, the wavelength plate WP, the optical fiber OF1, and the optical fiber OF2, can be omitted, arrangement of the components can be switched, and a new component can be added.
Further, the magnetic field measuring apparatus MMA according to the first embodiment can use multiple gas cells GC arranged in an array. In this case, the semiconductor laser LD and the coil COL can be commonly used in the multiple gas cells GC. For example, laser lights emitted from the semiconductor laser LD can be distributed to each of the multiple gas cells GC, and a common magnetic field from the coil COL can be applied to the multiple gas cells GC.
Operation of Magnetic Field Measuring Apparatus
The magnetic field measuring apparatus MMA according to the first embodiment has a configuration as described above. An operation for measuring an external magnetic field (ΔB) existing in an external environment will be described below.
In
In this state, when a circular polarizing laser light enters into the gas cell GC, the circular polarizing laser light interacts with an alkali metal atom in the gas cell GC. Specifically, by a circular polarizing laser light, an electron of the alkali metal atom is excited between specific levels splitted by the Zeeman effect, and the excited electron is fallen to multiple ground levels splitted by the Zeeman effect at an equal probability. By repeating exciting and falling of the electron, in the multiple ground levels splitted by the Zeeman effect, electrons existing in the ground levels contributing to the excitation are reduced, and electrons existing in the ground levels not contributing to the excitation are increased. Consequently, electrons exist locally in the ground levels not contributing to the excitation (optical pumping). This means that electrons exist locally in a level having a specific spin state, and an alkali metal atom is spin-polarized. Thus, by using an optical pumping technique, alkali metal atoms in the gas cell GC can be spun in a specific direction.
Then, a synthesized magnetic field (B+ΔB) in which a static magnetic field and an external magnetic field are combined is applied to the gas cell GC. Polarized alkali metal atoms spin around the synthesized magnetic field by precession (Lamore precession). At this time, precession frequency in the precession is proportional to intensity of the applied synthesized magnetic field.
The magnetic field measuring apparatus MMA according to the first embodiment further applies an alternating magnetic field in addition to the static magnetic field (B) from the coil COL. When the frequency of an alternating magnetic field is gradually changed, and a frequency of the alternating magnetic field coincides with a precession frequency of the above-described precession, optical magnetic double resonance occurs, and an output light from the gas cell GC is modulated by the precession frequency (resonance frequency). The output light modulated by the precession frequency is detected by the photo detector PD via the condenser lens LEN2 and the optical fiber OF2. At this time, a modulation frequency of the output light is equal to the precession frequency. Therefore, the precession frequency can be known by detecting the modulation frequency of the output light by the photo detector PD. The precession frequency is proportional to a synthesized magnetic field (B+ΔB) via a proportional constant specific to an alkali metal atom. Therefore, in consideration that the proportional constant is already known, the applied static magnetic field (B) is also already known, and a precession frequency is known from a modulation frequency of an output light, it is found that an external magnetic field (ΔB) can be measured.
As described above, according to the magnetic field measuring apparatus MMA according to the first embodiment, when a precession frequency of a precession associated with spin polarization of an alkali metal atom sealed in the gas cell GC is indirectly measured by optical magnetic double resonance, it is found that an external magnetic field (ΔB) can be measured. Especially, in the magnetic field measuring apparatus MMA according to the first embodiment, the gas cell GC in which alkali metal gas (alkali metal atoms) are filled plays an important role as a sensor. Accordingly, it is found that enhancement of reliability of the gas cell GC is needed to improve measurement accuracy of the external magnetic field (ΔB). Especially, sealing of an alkali metal gas in the gas cell GC is important. If sealing in the gas cell GC is insufficient, an alkali metal gas is discharged from the leak path. In this case, a laser light entered into the gas cell GC and an alkali metal gas interacting with the laser light are reduced, and it has an adverse effect on measurement of the external magnetic field (ΔB).
The gas cell GC included in the magnetic field measuring apparatus MMA is focused in the first embodiment so as to reduce a sealing failure of an alkali metal gas in the gas cell GC. A technical idea for reducing the sealing failure according to the first embodiment will be described below.
Configuration of Gas Cell According to First Embodiment
Next,
Next,
As described above, in the sealing region SLR of the gas cell GC according to the first embodiment, the sealing substrate 1S is disposed on a lower surface of the substrate member SM, and also the sealing substrate 2S is disposed on an upper surface of the substrate member SM. Specifically, the sealing region SLR has a three layer structure including a glass, a substrate member, and a glass. At this time, for example, the sealing substrate 1S functions as a support member which supports the substrate member SM. On the other hand, the sealing substrate 2S functions as a lid member which covers the substrate member SM.
Next, as illustrated in
At least, an alkali metal gas, such as cesium, potassium, and rubidium are filled in the cavity CAV. However, in addition to the above-described alkali metal gas, a nitrogen gas, a rare gas, or a mixture gas thereof may be included in the cavity CAV.
In this case, an advantage to be described below is obtained. Specifically, when the magnetic field measuring apparatus according to the first embodiment measures an external magnetic field, an alkali metal gas (alkali metal atom) filled in the cavity CAV is spin-polarized so as to spin in the same direction by irradiation of a pumping light. However, when an alkali metal gas collides with an inner wall of the cavity CAV, spin polarization is disturbed. Therefore, it is preferable that an alkali metal gas does not collide with the inner wall of the cavity CAV. On this point, even if a nitrogen gas and a rare gas collide with an alkali metal gas, spin polarization of an alkali metal gas is not easily disturbed. Therefore, spin polarization of an alkali metal gas can be easily maintained by filling a nitrogen gas and a rare gas in the cavity CAV with an alkali metal gas. Specifically, there are two advantages of introducing a nitrogen gas and a rare gas. One advantage is that spin polarization of an alkali metal gas is not easily disturbed even if an nitrogen gas and a rare gas collide with the alkali metal gas. Another advantage is that spin polarization of an alkali metal gas can be easily maintained since a probability in which an alkali metal gas collides with an inner wall of the cavity CAV is reduced by introducing a nitrogen and a rare gas.
Further, it is effective that, for example, an inner wall of the cavity CAV is coated by paraffin. This is because, in the case where the inner wall of the cavity CAV is coated by paraffin, spin polarization is not easily disturbed even if an alkali metal gas collides with an inner wall of the cavity CAV. Therefore, from a viewpoint of maintaining spin polarization of an alkali metal gas filled in the cavity CAV, in other words, maintaining spin information of the alkali metal gas, it is preferable to apply a configuration in which a nitrogen gas and a rare gas are introduced in the cavity CAV with an alkali metal gas and a configuration in which an inner wall of the cavity CAV is coated by paraffin.
Further, a gas production material (compound) in a solid state and a liquid state which produces an alkali metal gas and a solid and a liquid of an excessive alkali metal might exist in the cavity CAV. However, since the gas production material in a solid state and a liquid state and a solid and a liquid of the excessive alkali metal are not necessarily exist, these materials are not illustrated in
Since it is concerned that the above-described gas production material and excessive alkali metal (solid and liquid) remaining in the cavity CAV become a shielding material which reduces light intensity of a laser light passing through the cavity CAV, from a viewpoint of preventing reduction in the light intensity of a laser light passing through the cavity CAV, preferably a small amount of the above-described gas production material and excessive alkali metal (solid and liquid) is remained, and further preferably the above-described gas production material and excessive alkali metal are not remained.
In the gas cell GC according to the first embodiment, a configuration is assumed in which a laser light is emitted to the cavity CAV from the sealing substrate 2S side to the sealing substrate 1S side illustrated in
Characteristics of Gas Cell According to First Embodiment
Next, a characteristic point of the gas cell GC according to the first embodiment will be described. The gas cell GC according to the first embodiment is characterized in that, for example, as illustrated in
The above-described characteristics of the gas cell GC can be expressed as described below. For example, in
In such a configuration, the characteristic configuration according to the first embodiment in which a plane size of the opening OP1 is larger than a plane size of the opening OP2, and the opening OP2 is included in the opening OP1 will be expressed as below.
Specifically, in
According to this characteristic point according to the first embodiment, for example, due to the configuration as illustrated in
However, according to the first embodiment, since the above-described characteristic points are included, a difference in level necessarily formed in a communicating portion between the opening OP1 and the opening OP2 prevents that the dropped solution creeps up on a side surface of the cavity CAV. Therefore, according to the first embodiment, it is prevented that the dropped solution creeps up on a side surface of the cavity CAV and also spills over on a front surface of the substrate member SM. In the case where a solution is dried, this means that it is prevented that a compound is precipitated on a front surface of the substrate member SM from a side surface of the cavity CAV. Then, as a result, according to the first embodiment, the cavity CAV provided on the substrate member SM is sealed by the sealing substrate 2S. In this case, it is prevented that a compound precipitates over a front surface of the substrate member SM from a side surface of the cavity CAV. Accordingly, according to the first embodiment, it is prevented that a compound is inserted between a front surface of the substrate member SM and the sealing substrate 2S. Therefore, in the gas cell GC according to the first embodiment, occurrence of a bonding defect caused by which a compound is inserted between a front surface of the substrate member SM and a lower surface of the sealing substrate 2S is prevented by providing the above-described characteristic points. Therefore, reliability with respect to hermetic sealing of the cavity CAV provided in the gas cell GC can be improved.
Specifically, an essence of the technical idea according to the first embodiment is to form a difference in level functioning as a stopper for blocking that a solution creeps up on a side surface of the cavity CAV by surface tension. As an embodiment for embodying the configuration, in the first embodiment, the cavity CAV is formed by the openings OP1 and OP2 which communicate each other and have a different plane size. According to the configuration, in the first embodiment, a difference in level which functions as a stopper is provided on a side surface of the cavity CAV. The difference in level formed on a side surface of the cavity CAV blocks that a solution creeps up due to surface tension.
Manufacturing Method for Gas Cell According to First Embodiment
The gas cell GC according to the first embodiment is configured as described above, and a manufacturing method therefor will be described below with reference to drawings.
First, as illustrated in
Next, as illustrated in
An example of the both side etching technique includes a wet etching using such as potassium hydroxide (KOH) solution. In the wet etching, etching can be performed from the both sides of a front surface and a back surface of the substrate member SM at the same time. The openings OP1 and OP2 can be formed on the substrate member SM by performing the wet etching once.
In a process in which the openings OP1 and OP2 are formed on the substrate member SM, the openings are not necessarily formed by the above-described wet etching using the mask films MSK1 and MSK2. For example, the substrate member SM can be machined directly by such as a laser light and a drill. In this case, formation of the mask films MSK1 and MSK2 can be omitted.
Further, as illustrated in
Next, as illustrated in
Next, as illustrated in
In the first embodiment, as illustrated in
The gas production material GPM in a liquid state may include, for example, a compound which produces a gas other than an alkali metal such as a nitrogen gas like barium azide (BaN6) and other materials such as liquid paraffin, in addition to a compound including an alkali metal.
Next, as illustrated in
In the first embodiment, as illustrated in
Next, as illustrated in
At this time, a process for sealing the cavity CAV provided on the substrate member SM by the sealing substrate 2S may be performed in an atmosphere such as a nitrogen gas and a rare gas so that the nitrogen gas and the rare gas are sealed in the cavity CAV. The nitrogen gas and the rare gas include a function to prevent disturbance of the spin polarization of an alkali metal gas.
In the first embodiment, as described above, since a difference in level is formed on a communication portion between the openings OP1 and OP2, it is prevented that the dropped gas production material GPM in a liquid state creeps up on a side surface of the cavity CAV and also spills over on a front surface of the substrate member SM. Further, in a process for drying the gas production material GPM, it is prevented that the gas production material GPM adheres on a front surface of the substrate member SM.
As this result, according to the first embodiment, a bonding defect between the substrate member SM and the sealing substrate 2S can be prevented which is caused when a compound is inserted between the substrate member SM and the sealing substrate 2S. Accordingly, in the first embodiment, a manufacturing yield of a gas cell can be improved.
After the cavity CAV is sealed, an alkali metal gas and a nitrogen gas are produced from the gas production material GPM by causing a photodecomposition reaction and a thermal decomposition reaction with respect to the gas production material GPM existing on an upper surface of the sealing substrate 1S in the cavity CAV. Accordingly, an alkali metal gas and a nitrogen gas are filled in the cavity CAV.
As described above, a gas cell in the magnetic field measuring apparatus according to the first embodiment can be manufactured. In the first embodiment, a single gas cell is described as an example. However, multiple gas cells may be formed on a wafer, and a single gas cell may be cut as needed.
In the first embodiment, an example in which the openings OP1 and 0P2 are formed on the substrate member SM has been described. In a second embodiment, an example will be described in which a first substrate member and a second substrate member, which is different from the first substrate member, are provided, and an opening OP1 is formed on the first substrate member, and an opening OP2 is formed on the second substrate member. A gas cell GC according to the second embodiment has almost the same configuration as the gas cell GC according to the first embodiment.
Configuration of Gas Cell According to Second Embodiment
As illustrated in
Next,
In the second embodiment as described above, for example, due to a configuration as illustrated in
Accordingly, also in the second embodiment, it is prevented that a compound is precipitated on a front surface of the substrate member SM from a side surface of the cavity CAV. Consequently, also in the second embodiment, it is prevented that a compound is inserted between a front surface of the substrate member SM and the sealing substrate 2S. Therefore, in the gas cell GC according to the second embodiment, occurrence of a bonding defect can be prevented which is caused by which a compound is inserted between a front surface of the substrate member SM and a lower surface of the sealing substrate 2S. Therefore, reliability with respect to hermetic sealing of the cavity CAV provided in the gas cell GC can be improved.
Especially, in the second embodiment, the opening OP1 and the opening OP2 are formed on a separate substrate member. Specifically, in the second embodiment, as illustrated in
Manufacturing Method for Gas Cell According to Second Embodiment
The gas cell GC according to the second embodiment is configured as described above, and a manufacturing method therefor will be described below with reference to drawings.
First, as illustrated in
Next, as illustrated in
Next, as illustrated in
Next, as illustrated in
In the second embodiment as described above, the substrate member SM1 and the substrate member SM2 are separately prepared, the opening OP1 is formed so as to penetrate the substrate member SM1, and the opening OP2 is formed so as to penetrate the substrate member SM2. Therefore, in a manufacturing method for the gas cell GC according to the second embodiment, in a relatively easy process, the opening OP1 is formed on the substrate member SM1, and also the opening OP2 is formed on the substrate member SM2.
In terms of this point, in the above-described first embodiment, it has been necessary to form the openings OP1 and OP2 having different widths from a both sides of one substrate member SM, and a complicated manufacturing process has been needed. On the other hand, in the second embodiment, although the substrate member SM1 and the substrate member SM2, which are separately disposed, are needed to be prepared, a process to form a single opening OP1 on the substrate member SM1 and a process to form a single opening OP2 on the substrate member SM2 are relatively simple in comparison with the process according to the first embodiment. Consequently, a difficulty level in a manufacturing process for the gas cell GC according to the second embodiment is lower than that of a manufacturing process for the gas cell according to the first embodiment. Accordingly, a manufacturing yield can be improved. Specifically, in terms of improving the manufacturing yield of the gas cell GC, the manufacturing process for the gas cell GC according to the second embodiment is superior to the manufacturing process for the gas cell GC according to the first embodiment.
Next, as illustrated in
For example, as illustrated in
Next, as illustrated in
In the second embodiment, as illustrated in
Next, the gas production material GPM in a liquid state is dried by heating the gas production material GPM in a liquid state. Accordingly, the gas production material GPM in a solid state is precipitated on an upper surface of the sealing substrate 1S in the opening OP1.
Next, as illustrated in
In the second embodiment, as described above, since a difference in level is formed on a communication portion between the openings OP1 and OP2, it is prevented that the dropped gas production material GPM in a liquid state creeps up on a side surface of the cavity CAV and also spills over on a front surface of the substrate member SM2. Further, in a process for drying the gas production material GPM, it is prevented that the gas production material GPM adheres on a front surface of the substrate member SM2.
As this result, according to the second embodiment, a bonding defect between the substrate member SM2 and the sealing substrate 2S can be prevented which is caused when a compound is inserted between the substrate member SM2 and the sealing substrate 2S. Accordingly, a manufacturing yield of a gas cell can be improved.
After the cavity CAV is sealed, an alkali metal gas and a nitrogen gas are produced from the gas production material GPM by causing a photodecomposition reaction and a thermal decomposition reaction with respect to the gas production material GPM existing on an upper surface of the sealing substrate 1S in the cavity CAV. Accordingly, an alkali metal gas and a nitrogen gas are filled in the cavity CAV. As described above, a gas cell of the magnetic field measuring apparatus according to the second embodiment can be manufactured.
In the third embodiment, an example will be described in which, in openings OP1 and OP2 forming a cavity CAV of a gas cell GC, a depth of the opening OP1 having a larger plane size is equal to or less than 1 mm. A gas cell GC according to the third embodiment has almost the same configuration as the gas cell GC according to the first embodiment.
Configuration of Gas Cell According to Third Embodiment
Next,
Characteristics of Gas Cell According to Third Embodiment
The gas cell GC according to the third embodiment is configured as described above, and a manufacturing method therefor will be described below with reference to drawings.
First, as illustrated in
Next, as illustrated in
Next, after the patterned mask film MSK5 is removed, a patterned mask film MSK6 is formed on a front surface of the substrate member SM in which the opening OP1 is formed by using a photolithography technique and an etching technique. The mask film MSK6 is patterned so as to expose a region for forming the opening OP2 of which width is narrower than a width of the opening OP1. The mask film MSK6 is, for example, formed of a silicon oxide film.
Then, as illustrated in
In the third embodiment, as illustrated in
Next, as illustrated in
Next, for example, a gas production material GPM including a solution of a compound including an alkali metal such as cesium azide (CsN3) is dropped on an upper surface of the sealing substrate 1S in the opening OP1. A micropipette and a dispenser can be used to drop the gas production material GPM in a liquid state. At this time, as illustrated in
Thus, in the third embodiment, since the gas production material GPM is soaked in the small gap GP, it is prevented that the dropped gas production material GPM creeps up on a side surface of the opening OP2. Therefore, according to the third embodiment, it is prevented that the dropped gas production material GPM in a liquid state creeps up on a side surface of the openings OP2 and also spills over on a front surface of the substrate member SM.
Then, the gas production material GPM in a liquid state is dried by heating the gas production material GPM in a liquid state. Accordingly, the gas production material GPM in a solid state is precipitated in the small gap GP by the opening OP1.
Next, as illustrated in
In the third embodiment, mainly the gas production material GPM is soaked in the small gap GP by capillary phenomenon, and therefore it is prevented that the dropped gas production material GPM in a liquid state creeps up on a side surface of the cavity CAV and also spills over on a front surface of the substrate member SM. Further, in a process for drying the gas production material GPM, it is prevented that the gas production material GPM adheres on a front surface of the substrate member SM.
As this result, according to the third embodiment, a bonding defect between the substrate member SM and the sealing substrate 2S can be prevented which is caused when a compound is inserted between the substrate member SM and the sealing substrate 2S. Accordingly, a manufacturing yield of a gas cell can be improved.
After the cavity CAV is sealed, an alkali metal gas and a nitrogen gas are produced from the gas production material GPM by causing a photodecomposition reaction and a thermal decomposition reaction with respect to the gas production material GPM existing locally in the gap GP. Accordingly, an alkali metal gas and a nitrogen gas are filled in the cavity CAV. In the case where an alkali metal gas is produced from the gas production material GPM by a photodecomposition reaction, a light used in the photodecomposition reaction is emitted from a lower surface (back surface) side of the sealing substrate 1S.
As described above, a gas cell of the magnetic field measuring apparatus according to the second embodiment can be manufactured. Especially, in the third embodiment, as illustrated in
Variation
Next, a variation of the third embodiment will be described.
In the gas cell GC according to the variation, the groove CU (recessed portion) is formed on an upper surface of the sealing substrate 1S, and the opening OP1 is formed from the groove CU. At this time, a depth of the groove CU formed on the sealing substrate 1S is equal to or less than 1 mm.
In the variation, as with the third embodiment, since a gas production material GPM is soaked in a small gap GP, it is prevented that the dropped gas production material GPM creeps up on a side surface of the opening OP2. As this result, according to the variation, it is prevented that the dropped gas production material GPM in a liquid state creeps up on a side surface of the openings OP2 and also spills over on a front surface of the substrate member SM. Further, in the variation, as with the third embodiment, since the gas production material GPM in a solid state can exist locally in the gap GP by the groove CU (opening OP1), it is prevented that a laser light passing through the cavity CAV is reflected or absorbed.
In the variation, the groove CU is formed on the sealing substrate 1S, and the opening OP2 is formed on the substrate member SM. Thus, a process for etching both sides by forming mask films on both sides of the substrate member SM as in the first embodiment and a process for forming the openings OP1 and OP2 on the substrate member SM by using a photolithography technique and an etching technique twice as in the third embodiment are not needed. Specifically, a manufacturing process for the substrate member SM according to the variation can be simplified in comparison with the processes in the first embodiment and the third embodiment. Further, in the variation, the opening OP2 is formed on the substrate member SM, and the opening OP1 is formed on the sealing substrate 1S. Therefore, machining can be easily adjusted in comparison with the case where the openings OP1 and OP2 are formed on the same substrate member SM.
In the first to third embodiments, an example has been described in which one cavity CAV has been formed in one gas cell GC. However, in a fourth embodiment, an example will be described in which cavities CAV1 and CAV2 are formed in one gas cell GC.
For example, in a configuration example in which one cavity CAV is formed in one gas cell GC, in the case where a gas production material GPM in a solid state is remained in the cavity CAV, the gas production material GPM in a solid state might disturb a laser light passing through the cavity CAV. In the fourth embodiment, cavities CAV1 and CAV2 are provided in one gas cell GC. The cavity CAV1 in which the gas production material GPM in a solid state is remained and the cavity CAV2 through which a laser light passes are separately disposed. The gas cell GC according to the fourth embodiment including the above configuration will be described below with reference to drawings.
Configuration of Gas Cell According to Fourth Embodiment
In the fourth embodiment, the cavity CAV2 includes the openings OP3 and OP4, but are not limited to, and the cavity CAV2 may include a single opening. Specifically, in the fourth embodiment, at least, the cavity CAV1 includes the openings OP1 and OP2, and the cavity CAV2 can have an arbitrary shape.
In the fourth embodiment, the gas production material GPM in a solid state exists in the cavity CAV1, and the gas production material GPM does not exist in the cavity CAV2. Specifically, the gas production material GPM which produces an alkali metal gas exists on an upper surface of the sealing substrate 1S in the cavity CAV1, and the gas production material GPM does not exist on an upper surface of the sealing substrate 1S in the cavity CAV2. However, a space in the cavity CAV1 and a space of the cavity CAV2 are connected through the communication path CNU, and therefore, an alkali metal gas produced by the gas production material GPM existing in the cavity CAV1 exists also in the cavity CAV2 through the communication path CNU. Specifically, in the gas cell GC according to the fourth embodiment, an alkali metal gas is filled in both of the cavities CAV1 and CAV2.
In the fourth embodiment, a laser light used for measuring a magnetic field passes through the cavity CAV2. Accordingly, since the gas production material GPM in a solid state does not exist in the cavity CAV2, it is prevented that a laser light is reflected and absorbed by the gas production material GPM in a solid state when the laser light passes through the cavity CAV2 of the gas cell GC.
Specifically, a basic concept of the fourth embodiment is that the cavity CAV1 in which the gas production material GPM is disposed and the cavity CAV2 through which a laser light used for measuring a magnetic field passes are separately disposed, and the cavity CAV2 as well as the cavity CAV1 can be filled with an alkali metal gas by spacially communicating the cavities CAV1 and CAV2. Accordingly, even if the gas production material GPM is not disposed in the cavity CAV2, an alkali metal gas can be filled in the cavity CAV2, and an adverse effect by the gas production material GPM in a solid state can be removed by causing a laser light to pass through the cavity CAV2. Consequently, in a magnetic field measuring apparatus using the gas cell GC according to the fourth embodiment, performance including magnetic field measurement accuracy can be improved.
Characteristics of Gas Cell According to Fourth Embodiment
The gas cell GC according to the fourth embodiment is configured as described above, and a manufacturing method therefor will be described below with reference to drawings.
First, as illustrated in
Next, as illustrated in
Next, after the patterned mask film MSK7 is removed, a patterned mask film MSK8 is formed on a front surface of the substrate member SM, in which the groove CU1 is formed, by using a photolithography technique and an etching technique, and also a patterned mask film MSK9 is formed on a back surface of the substrate member SM. The mask film MSK8 and the mask film MSK9 are, for example, formed of a silicon oxide film.
Next, as illustrated in
Then, the substrate member SM and the sealing substrate 1S are bonded. For example, in the case where a Si substrate is used as the substrate member SM, and a borosilicate glass substrate is used as the sealing substrate 1S, the substrate member SM and the sealing substrate 1S can be bonded by anode bonding.
Next, for example, a gas production material GPM including a solution of a compound including an alkali metal such as cesium azide (CsN3) is dropped on an upper surface of the sealing substrate 1S in the opening OP1. A micropipette and a dispenser can be used to drop the gas production material GPM in a liquid state. Since the openings OP1 and OP3 are separated each other, the gas production material GPM in a liquid state which is dropped on an upper surface of the sealing substrate 1S in the opening OP1 does not flow on an upper surface of the sealing substrate 1S in the opening OP3.
In the fourth embodiment, as illustrated in
Next, the gas production material GPM in a liquid state is dried by heating the gas production material GPM in a liquid state. Accordingly, the gas production material GPM in a solid state is precipitated on an upper surface of the sealing substrate 1S in the opening OP1.
Next, as illustrated in
After the cavities CAV1 and CAV2 are sealed, an alkali metal gas and a nitrogen gas are produced from the gas production material GPM by causing a photodecomposition reaction and a thermal decomposition reaction with respect to the gas production material GPM existing on an upper surface of the sealing substrate 1S in the cavity CAV1. Accordingly, an alkali metal gas and a nitrogen gas are filled in the cavity CAV1. Further, the produced alkali metal gas and nitrogen gas are filled also in the cavity CAV2 through the communication path CNU.
As described above, a gas cell in the magnetic field measuring apparatus according to the fourth embodiment can be manufactured. In the fourth embodiment, the cavities CAV1 and CAV2 are formed in a stage before hermetically sealing, but it is not limited thereto. For example, the communication path CNU can be formed by evaporating a part of the substrate member SM by irradiating a region for forming a communication path with a high energy laser light after the cavities CAV1 and CAV2 are hermetically sealed.
The invention by the present inventor has been specifically described above based on the embodiments. However, the present invention is not limited to the embodiments, and can be changed variously without departing from the gist of the invention.
Filing Document | Filing Date | Country | Kind |
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PCT/JP2013/071533 | 8/8/2013 | WO | 00 |