The present disclosure relates to a semiconductor strain detection element having an impurity diffusion layer formed in a silicon substrate, and a MEMS actuator device including the same.
Micro sensing devices using technology of micro electro mechanical systems (MEMS) are being developed, and with advancement of MEMS technology, semiconductor strain detection elements used as an acceleration sensor, a pressure sensor, and a mechanical sensor are required to have an improved S/N ratio.
Patent Document 1: Japanese Laid-Open Patent Publication No. 6-102108
Patent Document 2: Japanese Laid-Open Patent Publication No. 2011-124344
In a semiconductor strain detection element such as a piezoelectric resistor element, for example, impurities are added to a P-type silicon substrate, to form an impurity diffusion layer that enables strain detection based on change in the resistance of the substrate surface.
In this semiconductor strain detection element, in order to enhance sensitivity of the impurity diffusion layer, a separated oxide film for suppressing an influence from another element therearound is required to be formed, and in order to protect the impurity diffusion layer that detects the resistance change, an insulation oxide film needs to be provided on the surface.
However, multiple trap levels exist in the interface between the semiconductor surface and the oxide film, and electric conduction carriers are trapped, to cause carrier fluctuation, which is observed as noise. Therefore, in the case of using a semiconductor strain detection element such as a piezoelectric resistor element for a MEMS actuator device, the S/N ratio is deteriorated, thus causing a problem that it is impossible to perform angle detection with high sensitivity.
The present disclosure has been made to solve the above problem, and an object of the present disclosure is to obtain a semiconductor strain detection element that is hardly influenced by noise from outside and thus has a high S/N ratio.
A semiconductor strain detection element according to one aspect of the present disclosure includes: a silicon substrate; and a first impurity diffusion layer having a conduction type different from the silicon substrate, the first impurity diffusion layer being formed inside under a surface of the silicon substrate, wherein an amount of strain in the silicon substrate is detected on the basis of change in a resistance of the first impurity diffusion layer.
The semiconductor strain detection element according to one aspect of the present disclosure can perform strain detection with a high S/N ratio without being influenced by noise from outside.
In the descriptions of embodiments and drawings, the same or corresponding parts are denoted by the same reference characters.
In the first embodiment of the present disclosure, the structure of a semiconductor strain detection element will be described with reference to
<Schematic Structure of Semiconductor Strain Detection Element>
In
By the plurality of semiconductor strain detection elements formed at the support portions 101, vibration strains in the longitudinal direction and the transverse direction of the MEMS actuator device 100 can be detected independently.
As shown in
In the present embodiment, as described later, a plurality of P-type impurity diffusion layers having different impurity ion densities are formed in the N-type silicon substrate 200, and these P-type impurity diffusion layers are collectively referred to as P-type impurity layer 103.
On the surface of the N-type silicon substrate 200, a thermal oxidization film 203 and an inter-layer insulation film 204 are formed, and contact halls are formed at some parts there. Via the openings of the contact halls, impurity layers 205 for ohmic contact formation are formed, and then metal wiring layers 206 for taking out electrodes are formed.
Finally, an insulation film 207 for protecting elements is formed in the uppermost layer.
The metal wiring layers 206 are formed at the left near side and the right far side in
<Process for Manufacturing Semiconductor Strain Detection Element>
With reference to
In the description of the process here, the case where the N-type silicon substrate 200 is used and the P-type impurity layer 103 is formed in the substrate using B+ (boron ion) as a dopant will be described. However, another P-type impurity may be used as a dopant.
Alternatively, using a P-type silicon substrate that is a different conduction type and using an N-type dopant such as P− (phosphorus ion), an N-type impurity layer may be formed in the P-type silicon substrate. Also in this case, the semiconductor strain detection element 105 that provides the same effect can be obtained.
Here, film thicknesses of constituent parts, manufacturing conditions, and the like described in the process for manufacturing the semiconductor strain detection element are merely an example, and are not limited to the film thickness, the manufacturing conditions, and the like described here. It is necessary to set appropriate conditions by performing examinations for each conduction type of substrates and each kind of impurity ions to be implanted.
(1) Formation of Thermal Oxidization Film
The N-type silicon substrate 200 shown in
In the thermal oxidization, heating was performed at about 1000° C. in an oxygen atmosphere. The thickness of the thermal oxidization film was about 0.3 μm.
(2) Formation of P-Type Impurity Layer
First, a resist pattern (not shown) is formed so as to be opened at a desired position on the N-type silicon substrate 200, using photomechanical process technology. It is preferable that the opening position is set so as to allow the P-type impurity layer 103 to be formed at a part where strain is most likely to occur, in the case of being mounted in the MEMS actuator device 100.
Using the ion implantation device through the opening, as shown in
The formation of the first P-type impurity diffusion layer 201 and the second P-type impurity diffusion layer 202 was performed by doping B+, using a medium current ion implantation device. In the present embodiment, the first P-type impurity diffusion layer 201 was formed with an implantation amount of 3.5×1013 cm−2 and implantation energy of 80 keV, and the second P-type impurity diffusion layer 202 was formed with an implantation amount of 3.5×1013 cm−2 and implantation energy of 50 keV.
Regarding the B+ density distribution in the depth direction, description will be given later, using a calculated value and an actual measured value. In the impurity distribution in the depth direction in the case of forming the first and second P-type impurity diffusion layers 201, 202 using B+ in the N-type silicon substrate 200, in general, the greater the implantation energy is, the deeper the implantation can reach.
In the present embodiment, after implantation of the first P-type impurity diffusion layer 201, B+ is implanted with reduced implantation energy for the second P-type impurity diffusion layer 202. Therefore, as shown in
(3) Formation of Metal Wiring
On the thermal oxidization film 203 formed on the surface of the N-type silicon substrate 200, the inter-layer insulation film 204 is formed using plasma-enhanced CVD (PECVD) technology. By the inter-layer insulation film 204, and the thermal oxidization film 203 formed in the first step, the metal wiring layer 206 to be formed in an upper layer and the surface of the N-type silicon substrate 200 can be prevented from being short-circuited.
As shown in
In this step, the P-type impurity ion such as BF2 is implanted in the N-type silicon substrate 200 through the contact hall opening part, thereby establishing stable electric connection between the metal wiring layer 206 and the first and second P-type impurity diffusion layers 201, 202.
As shown in
Finally, the insulation film 207 for protecting elements is formed over the entire surface of the semiconductor strain detection element 105 as shown in
<Impurity Ion Density Distribution>
In the present embodiment, an evaluation sample was prepared by the same manufacturing process as in the present embodiment, in order to measure the distribution of the impurity ion density. That is, B+ was doped in the N-type silicon substrate 200 by a medium current ion implantation device, and the first P-type impurity diffusion layer 201 and the second P-type impurity diffusion layer 202 were formed as in the substrate shown in
The implantation condition was as follows. For the first P-type impurity diffusion layer 201, the implantation amount was 3.5×1013 cm−2 and the implantation energy was 80 keV, and for the second P-type impurity diffusion layer 202, the implantation amount was 3.5×1013 cm−2 and the implantation energy was 50 keV. In order to activate the impurities contained in the first and second P-type impurity diffusion layers 201, 202, heat treatment was performed at a maximum temperature of 980° C. for 270 minutes using a horizontal heat treatment furnace.
Regarding the sample prepared here,
In both figures, the vertical axis indicates B+ density (1/cm3), the horizontal axis indicates the diffusion depth (μm), and 0 μm in the diffusion depth indicates the surface of the N-type silicon substrate 200.
The one-dimensional simulation of the impurity distribution shown in
That is, as shown in
From the above, it can be said that the second P-type impurity diffusion layer 202 is formed on the first P-type impurity diffusion layer 201 and the entire P-type impurity layer 103 including the first and second P-type impurity diffusion layers 201, 202 is completely enclosed in the N-type silicon substrate 200.
<Effect of Semiconductor Strain Detection Element>
The semiconductor strain detection element 105 according to the present embodiment has a sectional structure shown in
In addition, the impurity ion density is high at a shallow part in the P-type impurity layer 103. Therefore, it is considered that the conduction path for carriers is pushed down by the impurity ions so as to be located closer to a center part in the P-type impurity layer 103. Thus, the distance from the interface between the N-type silicon substrate 200 and the oxide film, which is considered to be a noise source, to the conduction path for carriers, is increased, so that the noise influence decreases and the S/N ratio is improved.
It is noted that the effect obtained in the present embodiment can be obtained in the same manner also in the semiconductor strain detection element 105 configured to be a reverse conduction type by forming an N-type impurity layer in a P-type silicon substrate.
As the silicon substrate, a silicon substrate having an insulation layer in the substrate as in silicon on insulator (SOI) technology can also be used in the same manner, and the first impurity diffusion layer 201 can be formed inside the surface-side silicon substrate.
A semiconductor strain detection element 105 according to the second embodiment of the present disclosure is used in the MEMS actuator device 100 shown in
The present embodiment is different in the structure of the P-type impurity layer 103 formed in the N-type silicon substrate 200 shown in
First, as in the first embodiment, a resist pattern is formed so as to be opened at a desired position on the N-type silicon substrate 200, using photomechanical process technology. It is preferable that the opening is formed at a part where strain is most likely to occur, in the case of being mounted in the MEMS actuator device 100.
Also in the present embodiment, the entire impurity layer including a plurality of layers formed in the N-type silicon substrate 200 is collectively referred to as P-type impurity layer 103.
<Process for Forming P-Type Impurity Layer>
First, as in the first embodiment, B+ is doped using a medium current ion implantation device, to form the first P-type impurity diffusion layer 201 and then the second P-type impurity diffusion layer 202.
The ion implantation condition is also the same as in the first embodiment. That is, the first P-type impurity diffusion layer 201 was formed with an implantation amount of 3.5×1013 cm−2 and implantation energy of 80 keV, and the second P-type impurity diffusion layer 202 was formed with an implantation amount of 3.5×1013 cm−2 and implantation energy of 50 keV.
Next, a third P-type impurity diffusion layer 300 is formed using B+ by the medium current ion implantation device.
The third P-type impurity diffusion layer 300 was formed with an implantation amount of 3.5×1013 cm−2 and implantation energy of 120 keV.
<Impurity Ion Density Distribution>
The impurity distribution in the depth direction in the N-type silicon substrate 200 in which the P-type impurity layer 103 was formed was measured. As in the first embodiment, as the depth from the substrate surface increased, the impurity ion density increased once, and the impurity ion density became the highest at a depth of about 0.2 μm. Then, as the depth further increased, the impurity ion density gradually decreased, and thereafter, the impurity ion density increased again from a position where the depth from the surface of the N-type silicon substrate 200 was about 0.35 μm.
From the above measurement result, it is considered that the first P-type impurity diffusion layer 201 was formed at an embedded position under the surface of the N-type silicon substrate 200. In addition, it is considered that, as a result of the subsequent formation of the second P-type impurity diffusion layer 202 in an overlapping manner at a shallow part near the surface in the first P-type impurity diffusion layer 201, a region having a high impurity ion density was formed at a position of 0.2 μm from the surface of the N-type silicon substrate 200. Further, in the present embodiment, it is considered that, as a result of the formation of the third P-type impurity diffusion layer 300 in an overlapping manner at a deep part of the first P-type impurity diffusion layer 201, a region having a high impurity ion density was formed at a depth of 0.35 μm from the surface of the N-type silicon substrate 200.
In the present embodiment, as shown in
<Effect of Semiconductor Strain Detection Element>
As shown in
Further, in the P-type impurity layer 103, the first P-type impurity diffusion layer 201 is sandwiched between the second and third P-type impurity diffusion layers 202, 300 having high impurity ion densities from the upper and lower sides. Thus, the conduction path for carriers is located closer to a center part in the impurity layer, and the distance from the interface between the N-type silicon substrate 200 and the oxide film, which is considered to be a noise source, to the conduction path for carriers, is very long. Therefore, the noise influence is small and the S/N ratio is improved.
It is noted that the effect in the present embodiment can be obtained in the same manner also in the semiconductor strain detection element configured to be a reverse conduction type by forming an N-type impurity layer in a P-type silicon substrate.
As the silicon substrate, a silicon substrate having an insulation layer in the substrate as in SOI technology can also be used in the same manner.
A semiconductor strain detection element 105 according to the third embodiment of the present disclosure is used in the MEMS actuator device 100 shown in
The present embodiment is different in the structure of the P-type impurity layer 103 formed in the N-type silicon substrate 200 shown in
First, as in the first and second embodiments, a resist pattern is formed so as to be opened at a desired position on the N-type silicon substrate 200, using photomechanical process technology, and the P-type impurity layer 103 is formed through the opening.
<Process for Forming P-Type Impurity Layer>
First, as in the second embodiment, B+ is doped using a medium current ion implantation device, to form the first P-type impurity diffusion layer 201, and then the second P-type impurity diffusion layer 202 and the third P-type impurity diffusion layer 300.
Parameters in each implantation step are the same as in the second embodiment. That is, the first P-type impurity diffusion layer 201 was formed with an implantation amount of 3.5×1013 cm−2 and implantation energy of 80 keV, the second P-type impurity diffusion layer 202 was formed with an implantation amount of 3.5×1013 cm−2 and implantation energy of 50 keV, and the third P-type impurity diffusion layer 300 was formed with an implantation amount of 3.5×1013 cm−2 and implantation energy of 120 keV.
At this stage, the first P-type impurity diffusion layer 201 is sandwiched between the second and third P-type impurity diffusion layers 202, 300 having high impurity ion densities from the upper and lower sides, and the P-type impurity layer 103 is formed at an embedded position under the surface of the N-type silicon substrate 200.
Next, by a high current ion implantation device, ion implantation using BF2 is performed on lateral surfaces of the P-type impurity layer 103, with an implantation amount of 1.0×1015 cm−2 and implantation energy of 140 keV, to form a fourth P-type high-density impurity diffusion layer 400.
Here, in the ion implantation by the high current ion implantation device, BF2 has been used as the implantation source. However, another P-type impurity ion can also be used in the same manner by adjusting the implantation amount and the implantation energy.
<Impurity Ion Density Distribution>
As in the second embodiment, the P-type impurity layer 103 formed in the N-type silicon substrate 200 has a structure in which the first P-type impurity diffusion layer 201 is sandwiched between the second and third P-type impurity diffusion layers 202, 300 from the upper and lower sides, and regions having high impurity ion densities are formed at depths of about 0.2 μm and about 0.35 μm from the surface of the N-type silicon substrate 200.
Further, in the present embodiment, as shown in the sectional structure in
<Effect of Semiconductor Strain Detection Element>
As shown in
Further, in the P-type impurity layer 103, the first P-type impurity diffusion layer 201 is sandwiched between the second and third P-type impurity diffusion layers 202, 300 having high impurity ion densities from the upper and lower sides, and sandwiched between the fourth P-type high-density impurity diffusion layers 400 from both lateral ends. Thus, the conduction path for carriers is located closer to a center part in the impurity layer, and the distance from the interface between the N-type silicon substrate 200 and the oxide film, which is considered to be a noise source, to the conduction path for carriers, is very long. Therefore, the noise influence is small and the S/N ratio is improved.
In addition, the fourth P-type high-density impurity diffusion layer 400 functions as a gettering layer for capturing contamination impurities in the N-type silicon substrate 200. Thus, noise in the output of the semiconductor strain detection element 105 is further reduced and the S/N ratio is improved.
It is noted that the effect in the present embodiment can be obtained in the same manner also in the semiconductor strain detection element configured to be a reverse conduction type by forming an N-type impurity layer in a P-type silicon substrate.
As the silicon substrate, a silicon substrate having an insulation layer in the substrate as in SOI technology can also be used in the same manner.
In the present embodiment, the P-type impurity layer 103 is formed such that the periphery is surrounded by the second and third P-type impurity diffusion layers 202, 300 and the fourth P-type high-density impurity diffusion layer 400 having high impurity ion densities. Conversely, a P-type impurity layer having a higher impurity ion density that the periphery may be formed near the center of the P-type impurity layer 103, and a P-type impurity layer having a lower impurity ion density may be formed around the periphery. Even in this case, the semiconductor strain detection element 105 having a high S/N ratio can be obtained.
Although the disclosure is described above in terms of various exemplary embodiments and implementations, it should be understood that the various features, aspects and functionality described in one or more of the individual embodiments are not limited in their applicability to the particular embodiment with which they are described, but instead can be applied, alone or in various combinations to one or more of the embodiments of the disclosure.
It is therefore understood that numerous modifications which have not been exemplified can be devised without departing from the scope of the present disclosure. For example, at least one of the constituent components may be modified, added, or eliminated. At least one of the constituent components mentioned in at least one of the preferred embodiments may be selected and combined with the constituent components mentioned in another preferred embodiment.
Number | Date | Country | Kind |
---|---|---|---|
JP2019-100926 | May 2019 | JP | national |
Number | Name | Date | Kind |
---|---|---|---|
5291788 | Oohata | Mar 1994 | A |
5643803 | Fukada et al. | Jul 1997 | A |
20060207339 | Sumigawa | Sep 2006 | A1 |
20070228500 | Shimazu | Oct 2007 | A1 |
20130228022 | Brown | Sep 2013 | A1 |
20150276517 | Ashida | Oct 2015 | A1 |
Number | Date | Country |
---|---|---|
6-102108 | Apr 1994 | JP |
6-204408 | Jul 1994 | JP |
7-131035 | May 1995 | JP |
8-18070 | Jan 1996 | JP |
2010025698 | Feb 2010 | JP |
2011-124344 | Jun 2011 | JP |
Entry |
---|
Communication dated Dec. 8, 2020, from the Japanese Patent Office in Application No. 2019-100926. |
Office Action dated Jan. 18, 2022 in German Application No. 10 2020 205 274.3. |
Communication dated Aug. 4, 2020, from the Japanese Patent Office in application No. 2019-100926. |
Number | Date | Country | |
---|---|---|---|
20200378848 A1 | Dec 2020 | US |