Patent Application
20250164428
The present disclosure relates to a gas sensor and a method for manufacturing a gas sensor.
In a conventional chemical sensor using a MEMS, a pair of electrodes is provided, and the distance between the electrodes is several micrometers even when the distance is the shortest. Although such a sensor exhibits sensitivity, its responsiveness is poor, and a long time is needed for concentration detection. Therefore, it was difficult to perform real-time measurement at intervals of several seconds to several tens of seconds. Meanwhile, as shown in Patent Literature 1, there has been reported a gas sensor which uses a nano-gap electrode having an inter-electrode distance of about several nm to 100 nm and which has improved responsiveness.
Although the sensor disclosed in Patent Literature 1 exhibited quick response when exposed to a gas to be detected, when the sensor was actually used, a long time was needed to recover its sensor characteristics. Also, since the mechanism of enhancing its responsiveness has not yet been elucidated, knowledge about a sensor configuration for obtaining quick response has been insufficient.
The present disclosure provides a gas sensor having enhanced responsiveness.
A gas sensor, which is a first aspect of the present disclosure, is characterized by comprising:
A gas sensor manufacturing method, which is a second aspect of the present disclosure, is a method for manufacturing the above-described gas sensor, wherein the sensitive membrane is formed by means of physical vapor deposition or chemical vapor deposition.
In the gas sensor manufacturing method, which is the second aspect of the present disclosure, heat treatment is performed for the sensitive membrane after being formed.
The technique according to the present disclosure can enhance responsiveness.
In the below, embodiments of the present disclosure will be listed and illustrated.
[1]A gas sensor of the present disclosure comprises:
In this configuration, since the division value obtained by dividing the voltage applied to the electrode portion by the inter-electrode volume is greater than 4.2×1016 V/m3 and not greater than 2.0×1025 V/m3, and the electrode area is equal to or greater than 2.5×10−15 m2, the response speed (rising and returning speeds) of the outputted electric signal can be increased.
[2] In the above-described gas sensor,
Since the gas sensor described in the above paragraph [2] has 4 or more electrode pairs and is configured such that the sum total of the electrode areas becomes equal to or greater than 2.5×10−15 m2, the sum total of the electrode areas becomes greater than that of the conventional technique. Thus, the response speed (rising and returning speeds) of the outputted electric signal can be increased.
[3] In the above-described gas sensor,
In the gas sensor described in the above paragraph [3], since the division value is not less than 6.0×1019 V/m3 and not greater than 2.0×1025 V/m3, the response speed (rising and returning speeds) of the outputted electric signal can be further increased.
[4] In the above-described gas sensor,
In the gas sensor described in the above paragraph [4], since a tunnel current effect is obtained, the response speed (rising and returning speeds) of the outputted electric signal can be further increased.
[5] In the above-described gas sensor,
In the gas sensor described in the above paragraph [5], since the resistance between the first electrodes and the second electrodes can be reduced, the response speed (rising and returning speeds) of the outputted electric signal can be further increased.
[6] In the above-described gas sensor, the sensitive membrane is a dense body.
In the gas sensor described in the above paragraph [6], since the sensitive membrane is densified, movement of electrons in depletion layers becomes easy, whereby the response speed (rising and returning speeds) of the outputted electric signal can be increased.
[7] In the above-described gas sensor, at least some particles which constitute the sensitive membrane are electrically coupled with one another.
In the gas sensor described in the above paragraph [7], since the particles which constitute the sensitive membrane are coupled with one another so as to enable electrical conduction, the contact resistance between the particles can be reduced. Accordingly, movement of electrons in depletion layers becomes easy.
[8]A method for manufacturing the above-described gas sensor in which the sensitive membrane is formed by means of physical vapor deposition or chemical vapor deposition.
In the gas sensor described in the above paragraph [8], since a homogeneous sensitive membrane can be formed, stable output of the electric signal becomes possible.
[9] In the above-described gas sensor manufacturing method, heat treatment is performed for the sensitive membrane after being formed.
In the gas sensor described in the above paragraph [9], since the particles which constitute the sensitive membrane are easily coupled with one another, the contact resistance between the particles can be reduced, whereby movement of electrons in depletion layers becomes easy.
A first embodiment in which the present disclosure is embodied will now be described with reference to
The gas sensor 10 includes a substrate 20, insulating layers 31 to 35, heating elements 40, an electrode portion 50, a sensitive membrane 60, a voltage application section 80 (see
The substrate 20 is composed of, for example, a silicon wafer. Although no particular limitation is imposed on the material of the substrate 20, the material is, for example, a semiconductor such as silicon. In the case where a ceramic substrate (e.g., a sapphire substrate, a zirconia substrate, an alumina substrate, or the like) is used for the substrate 20, formation of the insulating layers 31 to 34, which will be described later, can be omitted. No particular limitation is imposed on the planar shape of the substrate 20, and the planar shape of the substrate 20 may be, for example, rectangular or circular. No particular limitation is imposed on the size of the substrate 20, and the substrate 20 may be a rectangular substrate having a length of 0.1 mm to 10 mm measured along each side, or a circular substrate whose area is approximately the same as that of the rectangular substrate. No particular limitation is imposed on the thickness of the substrate 20, and the substrate 20 may have a thickness of, for example, 400 μm to 500 μm.
The substrate 20 may have a space portion 21 formed by removing a portion of the substrate 20. The space portion 21 is, for example, a cavity which penetrates the substrate 20 and is open to front and back surfaces thereof, a recess which is open to only one of the front and back surfaces of the substrate 20, or the like. Although no particular limitation is imposed on the shape of the opening 22 of the space portion 21, the sectional shape of the interior of the space portion 21, etc., in general, their shapes are simple shapes such as rectangular shape, circular shape, etc. No particular limitation is imposed on the size of the space portion 21. In the case where the space portion 21 is a cavity, the space portion 21 is preferably formed such that its opening at one of the front and back surfaces of the substrate 20 has a larger opening area as compared with its opening at the other of the front and back surfaces of the substrate 20. Although no particular limitation is imposed on their opening areas, the opening area of the larger opening is preferably set to 0.01 mm2 to 4 mm2, more preferably 0.25 mm2 to 2 mm2. In the case where the space portion 21 is a recess, its opening area may be set to the same range as the cavity.
The electrode portion 50, which will be described later, is insulated from the substrate 20 by the insulating layers 31 to 35 provided on the substrate 20. The insulating layers 31 to 35 may be formed on the entire surface of the substrate 20 or formed on only a portion of the substrate 20. The insulating layers 31, 33, and 35 are stacked on a surface (upper surface) of the substrate 20 on one side. The space portion 21 is provided in the substrate 20. In the case where the substrate 20 has the space portion 21, the insulating layers 31, 33, and 35 cover the opening 22 of the space portion 21 and are supported by the substrate 20. The insulating layers 31, 33, and 35 may be formed to cover the entire opening 22 or may be formed to cover a portion of the opening 22 if the insulating layers 31, 33, and 35 can be supported by the substrate 20. The insulating layers 32 and 34 are stacked on a surface (lower surface) of the substrate 20 on the other side. No particular limitation is imposed on the materials of the insulating layers 31 to 35 so long as they have sufficient insulating properties. Examples of the materials of the insulating layers 31 to 35 include silicon compounds such as SiO2, Si3N4, and SiOxNy (x and y are arbitrary values). No particular limitation is imposed on the shapes and thicknesses of the insulating layers 31 to 35. A monolayer insulating layer may be provided instead of the insulating layers 31, 33, and 35. By forming a silicon oxide film on the substrate 20, leak current between the electrodes of each electrode pair 70 can be prevented.
A plurality of heating elements 40 are provided in the gas sensor 10. The heating elements 40 are provided on the insulating layer 33 and are covered with the insulating layer 35. Lead portions (not shown) for supplying electric power from an external circuit are connected to the heating elements 40 via contact portions (not shown) for the heating elements (hereinafter referred to as “heating element contact portions”). Contact pads (not shown) are provided on the surfaces of the heating element contact portions. The heating elements 40 generate heat when a voltage is applied thereto. As a result, the temperature of the sensitive membrane 60 increases, whereby the sensitive membrane 60 is activated, and measurement of gas concentration becomes possible. No particular limitation is imposed on the positions where the heating elements 40 are disposed so long as they are located within the insulating layers 31, 33, and 35. In the case where the space portion 21 is formed in the substrate 20, the heating elements 40 are preferably disposed at positions corresponding to the space portion 21. By disposing the heating elements 40 at positions corresponding to the space portion 21, it is possible to suppress dissipation of heat from the heating elements 40 to the substrate 20. Also, since heat can be efficiently transferred to the sensitive membrane 60, the temperature of the sensitive membrane 60 can be controlled more accurately. Notably, the positions corresponding to the space portion 21 refer to a positional relation in which the heating elements 40 at least partially overlap with the space portion 21 in the thickness direction of the substrate 20, and it is more preferred that the entire heating elements 40 overlap with the space portion 21. The heating elements 40 have electrical conductivity, and no particular limitation is imposed on their material. For example, platinum, a platinum alloy, a nickel alloy, a chromium alloy, a nickel-chromium alloy, or the like may be used for the heating elements 40. Of these materials, platinum or a nickel-chromium alloy, which have large temperature coefficients of resistance and whose resistances and temperature coefficients of resistance are less likely to change in repeated use over a long period of time, are preferably used for the heating elements 40.
The electrode portion 50 (one or more electrode pairs 70) is provided on the surface of the insulating layer 35. One end of the first electrode 71 and one end of the second electrode 72 are disposed to face each other with a nano-gap formed therebetween. In the present first embodiment, the nano-gap means a gap of a distance of 100 nm or less between the one end of the first electrode 71 and the one end of the second electrode 72.
Each of the first electrode 71 and the second electrode 72 is formed of a single type of metal or a plurality of types of metals. Examples of the metal used to form the first electrode 71 and the second electrode 72 include gold (Au) and platinum (Pt). The first electrode 71 and the second electrode 72 have, for example, a two-layer structure including a lower layer electrode and an upper layer electrode. For example, the lower layer electrode is formed of titanium (Ti), and the upper layer electrode is formed of platinum (Pt).
Lead portions (not shown) for supplying electric power from the external circuit are connected to the first electrode 71 and the second electrode 72 via contact portions (not shown) for the electrodes (hereinafter referred to as “electrode contact portions”). Contact pads (not shown) are provided on the surfaces of the electrode contact portions.
The sensitive membrane 60 is provided on the upper surface of the first electrode 71, the upper surface of the second electrode 72, and the upper surface of the insulating layer 35. The sensitive membrane 60 is disposed between the first electrode 71 and the second electrode 72 of each electrode pair 70. The sensitive membrane 60 is preferably formed of a metal oxide. The sensitive membrane 60 is preferably formed of an oxide semiconductor. The oxide semiconductor is preferably an n-type semiconductor. Preferred examples of the n-type semiconductor include SnO2, ZnO, In2O3, Fe2O3, ITO (tin-doped indium), and WO3, whose resistances change easily.
The sensitive membrane 60 is preferably a dense body. The dense body is a body whose porosity is less than 10%. The surface of the sensitive membrane 60 is, for example, the surface of the dense body as shown in
At least some particles which constitute the sensitive membrane 60 are electrically coupled (bound) with one another. The expression “particles are electrically coupled with one another” is defined as a state in which at least a half of the surface area of a certain particle, excluding end portions, is in contact with the surfaces of other particles, and a path through which electrons having propagated through the certain particle propagate is formed in at least a half of the surface area of the particle. The particles electrically coupled with one another create a state in which electricity flows between the particles (a state in which electrical conduction is enabled). Since the particles which constitute the sensitive membrane 60 are electrically coupled with one another, the contact resistance between the particles can be reduced, whereby movement of electrons in depletion layers becomes easy.
The voltage application section 80 applies a voltage to the electrode portion 50 such that the voltage is applied between the first electrode 71 and the second electrode 72. The voltage application section 80 includes, for example, a voltage control circuit (a constant voltage circuit or the like) which performs an operation of applying a volage to the electrode portion 50 on the basis of electric power supplied from a power source, and a control section (CPU or the like) which controls the voltage control circuit.
The output section 90 outputs an electric signal representing the gas concentration detected by using the electrode portion 50. The output section 90 may include, for example, an amplifier which amplifies the electric signal, etc.
A gas detected by the gas sensor 10 is preferably flammable. The resistance of the gas sensor 10 can be changed by a flammable gas. Preferred examples of the flammable gas include ketones (e.g., acetone), alcohols (e.g., ethanol), carbon monoxide, nitrogen oxides (NO, N2O), aldehydes (e.g., acetaldehyde), sulfide gases (e.g., hydrogen sulfide), and VOC gases (e.g., toluene).
The gas sensor 10 is preferably of a resistance measurement type or of an impedance measurement type.
An electrical index in the electrode portion 50 of the gas sensor 10 will be described. A division value obtained by dividing, by an inter-electrode volume, the voltage V applied to the electrode portion 50 by the voltage application section 80 is defined as an electrical index (hereinafter referred to simply as an index) X in the electrode portion 50. The inter-electrode volume B is the product of an inter-electrode distance D and an electrode area S. Namely, the index X is represented by the following Expression (1).
For example, in the case where the electrode pair 70 shown in
In the case where the electrode portion 50 is composed of a single electrode pair 70, the inter-electrode distance D is the distance (shortest distance) in the first direction between the first electrode 71 and the second electrode 72 constituting that electrode pair 70. Meanwhile, in the case where the electrode portion 50 is composed of a single electrode pair 70, the inter-electrode distance D is the smallest one of the distances (shortest distances) in the first direction between the first electrodes 71 and the second electrodes 72 in all the electrode pairs 70.
In the case where the electrode portion 50 is composed of a single electrode pair 70, the electrode area S is the electrode area of one electrode (for example, the first electrode 71) of that electrode pair 70. Meanwhile, in the case where the electrode portion 50 is composed of a plurality of electrode pairs 70, the electrode area S is the sum total of the electrode areas of electrodes on one side (for example, the first electrodes 71) of all the electrode pairs 70.
A specific method for obtaining the electrode area in each electrode portion 50 will be described. First, one first electrode 71 is selected (in the case where the electrode portion 50 includes a single electrode pair 70, the first electrode 71 of that electrode pair 70 is selected), and a cut surface is set. For example, the first electrode 71 of the electrode pair 70 for which the above-described inter-electrode distance D was determined is selected. For example, a plane which orthogonally intersects a plate face of the substrate 20 and passes through a position which is offset from a first end (an end portion on the second electrode 72 side) of the selected first electrode 71 toward a second end (an end portion located on the side opposite the second electrode 72) by a distance (preferably, 25 nm) which falls within the range of 10 nm to 100 nm is defined as a cut surface of the electrode portion 50. In the example of
One example of a method for measuring the electrode area appearing in the cut surface will be described. In the cut surface of the first electrode 71, the width W of the first electrode 71 is defined by the length of the shortest overlap between the cut surface and a straight line which intersects the side surfaces of the first electrode 71 and is parallel to the plate face of the substrate 20. Here, the side surfaces are surfaces located on the left and right sides of the cut surface and each including a portion having an inclination of 450 or less in relation to a straight line orthogonally intersecting the plate face of the substrate 20 (also referred to as an orthogonal line) and a portion located below that portion. In the case where the left and right sides of the cut surface are curved, each side surface is a portion where a tangent line to a curved portion has an inclination of 45° or less in relation to the orthogonal line. Also, in the cut surface of the first electrode 71, the height H of the first electrode 71 is defined by the length of the shortest overlap between the cut surface and an orthogonal line intersecting the upper surface of the first electrode 71. The product of the width W and the height H of the first electrode 71 is defined as the electrode area appearing in the cut surface of the first electrode 71. Here, the upper surface refers to a surface portion which is located at a center of the cut surface in the left and right direction and is other than the side surfaces.
For example, in the cut surface of the first electrode 71 as shown in
Notably, the electrode area S may be obtained by selecting a predetermined number of first electrodes 71 (for example, 100 first electrodes 71) from the plurality of first electrodes 71, calculating the average of cross sectional areas of the selected first electrodes 71, and multiplying the obtained average by the number of the first electrodes 71 contained in the electrode portion 50.
The index in the electrode portion 50 (the index X represented by Expression (1)) is greater than 4.2×1016 V/m3 and not greater than 2.0×1025 V/m3, preferably not less than 6.0×1019 V/m3 and not greater than 2.0×1025 V/m3, more preferably not less than 6.0×1020 V/m3 and not greater than 2.0×1025 V/m3. By virtue of such a configuration, the response speed (rising and returning speeds) of the electric signal outputted by the output section 90 can be increased.
The above-described electrode area S is not less than 2.5×10−15 m2 and not greater than 2.1×10−11 m2, preferably not less than 2.1×10−14 m2 and not greater than 2.1×10−12 m2. Notably, in the case where the electrode portion 50 is composed of a single electrode pair 70, the electrode area S is the electrode area of the first electrode 71 of that electrode pair 70, and, in the case where the electrode portion 50 is composed of a plurality of electrode pairs 70, the electrode area S is the sum total of the electrode areas of the first electrodes 71 of all the electrode pairs 70. By virtue of such a configuration, the response speed (rising and returning speeds) of the electric signal outputted by the output section 90 can be increased.
The shortest inter-electrode distance among all the electrode pairs 70 in the electrode portion 50 is preferably not less than 5 nm and not greater than 100 nm. By virtue of such a configuration, a tunnel current effect is obtained between the electrodes, whereby the response speed (rising and returning speeds) of the electric signal outputted by the output section 90 can be further increased.
The total of the widths W of the first electrodes 71 of all the electrode pairs 70 in the electrode portion 50 (in the case where the electrode portion 50 includes a single electrode pair 70, the width W of the single first electrode 71) is preferably equal to or greater than 20 nm. By virtue of such a configuration, it is possible to reduce the resistance to electron movement, thereby increasing the response speed (rising and returning speeds) of the outputted electric signal.
A method for manufacturing the gas sensor 10 in which the present disclosure is embodied will be described with reference to
The method for manufacturing the gas sensor 10 includes a step of forming the electrode portion 50 on the substrate 20 by a lift-off method and a step of forming the sensitive membrane 60 in a gap portion of the electrode portion 50.
First, insulating layers 31, 33, and 35 and heating elements 40 are formed on a cleaned substrate 20 (silicon wafer). The cleaned substrate 20 is placed in a heat treatment furnace, and a silicon oxide film (see
No particular limitation is imposed on the method for forming the heating elements 40. For example, a component which becomes the heating element 40 is caused to adhere to and deposit on the surface of the insulating layer 33, and then, unnecessary portions are removed by various types of etching methods, which are similar to the method described as an example in the description of the method for forming the space portion 21. Subsequently, as shown in
Subsequently, as shown in
Subsequently, as shown in
In the case where, as shown in
Subsequently, as shown in
Heat treatment may be performed for the sensitive membrane 60 after being formed. As a result, particles contained in the sensitive membrane 60 are bonded together, whereby the sensitive membrane 60 becomes dense. The heat treatment is performed by using the heater (heating element 40) provided in the gas sensor, and the temperature is changed by supplying electricity to the heater. As a result, the particles constituting the sensitive membrane 60 are easily bonded together, whereby the contact resistance between the particles can be reduced, and movement of electrons in depletion layers becomes easy.
The following description relates to an example of the effect of the present configuration.
In the gas sensor 10 of the first embodiment, when the product of the inter-electrode distance D in the first direction between the first electrode 71 and the second electrode 72 and the electrode area S of the first electrode 71 in a cut surface orthogonal to the first direction is defined as an inter-electrode volume B, the division value (index X) obtained by dividing, by the inter-electrode volume B, the voltage applied to the electrode portion 50 by the voltage application section 80 is greater than 4.2×1016 V/m3 and not greater than 2.0×1025 V/m3. The electrode area S is equal to or greater than 2.5×10−15 m2. In this configuration, since the division value obtained by dividing the voltage applied to the electrode portion 50 by the inter-electrode volume B is greater than 4.2×1016 V/m3 and not greater than 2.0×1025 V/m3, and the electrode area S is equal to or greater than 2.5×10−15 m2, the response speed (rising and returning speeds) of an outputted electric signal can be increased.
Since the gas sensor 10 of the first embodiment includes 4 or more electrode pairs 70 and is configured such the electrode area S, which is the sum total of the respective electrode areas, becomes equal to or greater than 2.5×10−15 m2, the electrode area S becomes greater than that of the conventional technique. Thus, the response speed (rising and returning speeds) of the outputted electric signal can be increased.
In the gas sensor 10 of the first embodiment, since the division value is not less than 6.0×1019 V/m3 and not greater than 2.0×1025 V/m3, the response speed (rising and returning speeds) of the outputted electric signal can be further increased.
In the gas sensor 10 of the first embodiment, the inter-electrode distance which is the smallest among all the electrode pairs 70 in the electrode portion 50 is 5 nm to 100 nm. By virtue of this, a tunnel current effect is obtained between the electrodes, whereby the response speed (rising and returning speeds) of the outputted electric signal can be further increased.
In the gas sensor 10 of the first embodiment, the total of the widths of the first electrodes 71 of all the electrode pairs 70 in the electrode portion 50 is equal to or greater than 20 nm. By virtue of this, the resistance between the first electrodes and the second electrodes can be reduced, whereby the response speed (rising and returning speeds) of the outputted electric signal can be further increased.
In the gas sensor 10 of the first embodiment, the sensitive membrane 60 is a dense body. Therefore, movement of electrons in depletion layers becomes easy, and the response speed (rising and returning speeds) of the outputted electric signal can be increased.
In the gas sensor 10 of the first embodiment, at least some particles which constitute the sensitive membrane 60 are electrically coupled with one another. Since the particles which constitute the sensitive membrane 60 are coupled with one another so as to enable electrical conduction, the contact resistance between the particles can be reduced, and, thus, movement of electrons in depletion layers becomes easy.
In the method for manufacturing the gas sensor 10 of the first embodiment, the sensitive membrane 60 is formed by means of physical vapor deposition or chemical vapor deposition. Therefore, the sensitive membrane 60 can be homogeneously formed, and, thus, stable output of an electric signal becomes possible.
In the method for manufacturing the gas sensor 10 of the first embodiment, heat treatment is performed for the sensitive membrane 60 after being formed. As a result, the particles which constitute the sensitive membrane 60 are easily coupled with one another, and the contact resistance between the particles can be reduced. Therefore, movement of electrons in depletion layers becomes easy.
The present disclosure will now be described further specifically by means of examples.
Gas sensors of Experimental Examples 1 to 6 and Comparative Examples 1 and 2 shown in Table 1 were manufactured by the steps which will be described below. Experimental Examples 1 to 6 correspond to examples.
A silicon substrate (hereinafter also referred to simply as a substrate) of 3 mm×5 mm was used for the gas sensors of Experimental Examples 1 to 6 and Comparative Examples 1 and 2. An insulating layer was formed on the front and back surfaces of the substrate. The insulating layer is composed of a first insulating layer formed of silicon oxide (SiO2) and a second insulating layer stacked on the surface of the first insulating layer and formed of silicon nitride (Si3N4).
A space portion was formed in the substrate in such a manner that the space portion is open to the surface on the side where the insulating layer was formed. The area of the opening of the space portion was 1 mm2. Heating elements are formed in the insulating layer at positions corresponding to the space portion. Heating element lead portions (not shown) for supplying electric power are connected to the heating elements. The heating element lead portions have contact portions for connection to an external circuit. The heating elements and the heating element lead portions have a two-layer structure composed of a Pt layer and a Ti layer.
One pair or plural pairs of electrodes are formed on the surface of the insulating layer at positions corresponding to the heating elements. A sensitive membrane is formed on the surface of the insulating layer at a position corresponding to the heating elements. The sensitive membrane is formed on the surface of the insulating layer in such a manner that the sensitive membrane comes into contact with the upper surfaces of the electrodes. Electrode lead portions are connected to the electrodes. The electrode lead portions have electrode contact portions for connection to the external circuit.
Each of the electrodes of Experimental Examples 1 to 6 has a lower layer electrode formed on the surface of the insulating layer and an upper layer electrode formed on the upper surface of the lower layer electrode. The lower layer electrode is formed of Ti. The upper layer electrode is formed of Pt. The thickness of the lower layer electrode is 3 nm. The thickness of the upper layer electrode is 10 nm.
Each of the electrodes of Comparative Examples 1 and 2 has a lower layer electrode formed on the surface of the insulating layer and an upper layer electrode formed on the upper surface of the lower layer electrode. The lower layer electrode is formed of Ti. The upper layer electrode is formed of Pt. The thickness of the lower layer electrode is 20 nm. The thickness of the upper layer electrode is 40 nm.
A silicon substrate having a thickness of 400 μm was immersed in a cleaning solution and cleaning was performed.
The cleaned silicon substrate was placed in a heat treatment furnace, and a silicon oxide film having a thickness of 100 nm, which would become an insulating layer (first insulating layer), was formed on the entire surface of the substrate by means of thermal oxidation treatment.
A silicon nitride film was formed on the first insulating layer of the substrate by means of plasma CVD in which SiH4 and NH3 were used as source gases. A silicon nitride film having a thickness of 400 nm was formed on the surface (upper surface) of the substrate on one side and used as an insulating layer (lower insulating layer). A silicon nitride film having a thickness of 200 nm was formed on the surface (lower surface) of the substrate on the other side and used as an insulating layer (lower insulating layer). After that, heating elements were formed on the surface of the second insulating layer by using a DC sputtering device. Specifically, a Ti layer having a thickness of 25 nm was formed on the surface of the second insulating layer, and a Pt layer having a thickness of 250 nm was further formed on the surface of this Ti layer, whereby the heating elements were formed. Next, patterning of resist was performed by means of photolithography, and the pattern of the heating elements was formed by means of etching. After that, a silicon nitride film having a thickness of 400 nm, which would become the upper insulating layer of the second insulating layer, was formed in the same manner as in the case of the lower insulating layer. In this manner, the second insulating layer and the heating elements disposed in the second insulating layer were formed.
The insulating layers were etched by means of dry etching so as to remove portions corresponding to the heating element contact portions, thereby exposing portions (portions of the heating elements) which would become the heating element contact portions. After that, by using a DC sputtering device, a Ti layer having a thickness of 20 nm was formed, and a Pt layer having a thickness of 40 nm was then formed. After sputtering, patterning of resist was performed by means of photolithography, whereby the heating element contact portions were formed.
By using a DC sputtering device, a Cr layer having a thickness of 50 nm was formed on the substrate, and an Au layer having a thickness of 1 μm was formed on its surface. After that, patterning of resist was performed by means of photolithography, and, by means of etching, respective contact pads were formed on the surfaces of the electrode contact portions and the heating element contact portions.
The substrate was immersed into a TMAH (tetramethylammonium hydroxide) solution, and anisotropic etching of silicon was performed so as to form a space portion at a position corresponding to the heating elements. The space portion was formed such that an opening was formed in the surface on which the insulating layers were formed.
Tin oxide (SnO2) was used as nanoparticles of a metal oxide provided at nanogap portions of the nanogap electrodes. A membrane was formed by using an RF sputtering device in which a tin oxide target for sputtering was used. The substrate was heated to 280° C., and tin oxide was sputtered, while sputtering to regions other than a region where a sensitive membrane was to be formed was prevented by a mask, whereby a sensitive membrane was formed. At that time, a membrane having a thickness of 20 nm or 200 nm was formed.
Notably, a bonding treatment (heat treatment) may be further performed so as to produce a more dense sensitive membrane. The heat treatment at that time was performed by using the heater (the heating elements 40) provided in the gas sensor. Specifically, by applying electricity to the heater, the temperature was elevated, and, in clean air, the gas sensor was heated at 300° C. to 600° C. for 10 minutes to 5 hours. Notably, it is sufficient that oxygen coexists so as to prevent reduction of tin oxide, and, therefore, the atmosphere may be a simulated gas produced from a gas cylinder or the like.
Table 1 shows the results of evaluation performed for the manufactured gas sensors by using a gas sensor evaluation device 100 shown in
Notably, the inter-electrode distance (shortest inter-electrode distance) was measured through planar observation performed, by using an SEM (scanning electron microscope), in a state in which the electrode portion was formed. In Experimental Examples 1 to 6, the width and the height of the first electrode in its cut surface were averaged values (averaged first electrode height and width) of 100 electrode pairs randomly selected from the 580 electrode pairs. The cut surface was mirror-polished and was observed under an SEM (scanning electron microscope) for measurement.
Acetone was used as a gas to be detected. Measurement was performed by using purified air as a base gas and using acetone supplied from a 2000 ppm/N2 balance cylinder (product of TAKACHIHO CHEMICAL INDUSTRIAL CO., LTD.) Acetone was mixed with purified air by using the mass flow controllers 102 and 103 such that the concentration of acetone became a predetermined concentration (here 4, 10, or 100 ppm). The measurement flow rate was 200 sccm. The measurement atmosphere was controlled by using the heater (heating elements) disposed in each gas sensor. Specifically, electric power supplied to the heater was controlled such that the temperature of the gas sensor became 250° C. The heater temperature was controlled by using the previously calculated correlation between the heater temperature and the heater resistance; i.e., by supplying electric power to the heater in accordance with the heater resistance.
As to rising time and returning time, T90 represents a time needed to reach 90% of an initial value (a value at the time when sensitivity saturates), which is considered as 100%. Similarly, T50 represents a time needed to reach 50% of the initial value (a value at the time when sensitivity saturates), which is considered as 100%. In Experimental Example 4, the rising responsiveness (T90 response speed) at the time of exhibition of sensitivity was 5 seconds or less, and the output returned to the original value within 15 seconds in a recovery period. A conceivable reason of this is that the inter-electrode electric field strength is high.
In Experimental Example 4, since the voltage applied to the electrode portion is 2.5 V, the electric field strength becomes 6.0×1020 V/m3. Meanwhile, in the case of Comparative Examples 1 and 2, in which the inter-electrode distance is 20 μm, the rising responsiveness (T90 response speed) was 30 seconds, which is relatively quick, but the output did not return to a value corresponding the base resistance (Va) within the measurement time; i.e., T50 was 300 seconds or longer, which shows that the recovery properties are very poor. A conceivable reason of this is that, in Comparative Examples 1 and 2, the electric field strength is low unlike Experimental Examples 1 to 6. In Comparative Examples 1 and 2, since the height of the first electrode is 60 nm and the width of the first electrode is 50 μm, the electric field strength becomes 4.2×1016 V/m3. The thickness of the SnO2 layer was 200 nm.
In Experimental Examples 2 and 5, the voltage applied to the electrode portion was 0.25 V, and in Experimental Examples 3 and 6, the voltage applied to the electrode portion was 0.025 V. As shown in Table 1, when the applied voltage is lowered to 0.025 V, the returning responsiveness (returning of the output) becomes slightly bad. Namely, this test revealed that it is preferred that the electric field strength is 6.0×1018 V/m3 or higher.
The dependency of current on gas concentration measured in Experimental Examples 1 to 6 shows that the concentration of oxygen vacancies of tin oxide changes with gas. Namely, a conceivable reason of this is that, when the gas sensor is exposed to the gas to be detected and the oxygen partial pressure becomes low, which is shown as a change from
The present invention is not limited to the embodiment described by the above description with reference to the drawings, and, for example, embodiments which will be described below are contained in the technical scope of the present invention. Also, various features of the above-described embodiments and the embodiments which will be described below may be combined in any manner so long as a conflict does not occur.
In the above-described first embodiment, as the method for measuring the area of the cut surface of the first electrode 71, a method for measuring the width W and the height H of the cut surface has been shown as an example. However, other methods may be used. For example, the area of the cut surface may be measured by using an analysis software program or the like.
In the above-described first embodiment, the inter-electrode distance of an electrode pair whose inter-electrode distance (shortest distance) is the smallest among the plurality of electrode pairs is employed as the inter-electrode distance D. However, the average of the inter-electrode distances (shortest distances) of all of the plurality of electrode pairs or the average of inter-electrode distances (shortest distances) of a predetermined number of electrode pairs selected from the plurality of electrode pairs may be used.
In the above-described first embodiment, the plane which passes through a certain position which is offset from the first end (an end portion on the second electrode 72 side) of the first electrode 71 by a certain distance which falls within the range of 10 nm to 100 nm is defined as a cut surface, and the conditions of the index X and the electrode area are defined for that cut surface. However, there may be employed a configuration which satisfies the conditions of the above-described index X and the above-described electrode area in any of cut surfaces which pass through positions which are offset from the first end by distances of 10 nm to 100 nm.
In the above-described first embodiment, the electrode area S is obtained by calculating the average value of the sectional areas of a predetermined number (for example, 100) of first electrodes 71 among the plurality of first electrodes 71, and multiplying the average value by the number of the first electrodes 71. However, the electrode area S may be obtained by adding together the sectional areas of the all the first electrodes 71, without calculating the average value.
In the above-described first embodiment, gold (Au), platinum (Pt), and titanium (Ti) are shown as examples of the materials of the first electrode 71 and the second electrode 72. However, the materials may be elements which are high in catalytic activity such as palladium (Pd), ruthenium (Ru), rhodium (Rh), and iridium (Ir).
In the above-described first embodiment, the heating elements 40 and the electrode portion 50 are formed on the insulating layer 33 and the insulating layer 35, respectively. However, they may be formed on an insulating film such as a silicon oxide (SiO2) film or an alumina (Al2O3) film.
Notably, the embodiments disclosed this time should be considered to be illustrative and not to be restrictive in all aspects. The scope of the present invention is not limited to the embodiments disclosed this time, and it is intended that the present invention encompasses all modifications within the range shown by the claims and the range of equivalents of the claims.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2022-073680 | Apr 2022 | JP | national |
| Filing Document | Filing Date | Country | Kind |
|---|---|---|---|
| PCT/JP2023/013804 | 4/3/2023 | WO |
