The present disclosure relates generally to sensors, and more particularly, to sensors that include sensor elements such as resistors, heaters and/or other sensor elements.
Sensors are commonly used to sense various parameters in a wide variety of applications including, for example, medical applications, flight control applications, industrial process applications, combustion control applications, weather monitoring applications, as well as many other applications. Sensors often include sensor elements such as resistors, heaters and/or other sensor elements. In many cases, it is desirable for such sensor elements to have well-behaved characteristics, such as resistance and/or temperature coefficient characteristics.
The present disclosure relates generally to sensors, and more particularly, to sensors that include sensor elements such as resistors, heaters and/or other sensor elements. In some instances, a sensor element may include a first dielectric layer, a silicon layer on the first dielectric layer, and a metal-silicide layer integrally formed with the silicon layer such that the metal-silicide layer is separated from the first dielectric layer by the silicon layer. In some instances, the silicon layer may include a dopant. The type of metal-silicide, the thickness of the silicon and/or metal layer and the doping concentration of the silicon layer can all be selected to produce a desired resistance and/or temperature coefficient in the resulting sensor element. In some instances, a second dielectric layer may be situated on the metal-silicide layer and may include a dopant. The second dielectric layer may, in some cases, result from some of the silicon atoms and/or dopant diffusing through the metal-silicide layer and becoming oxidized. Regardless of how formed, the second dielectric layer may function as a low stress upper adhesion layer that supports further thin film deposition.
In some cases, the sensor may be a flow sensor that includes a heater element, an upstream sensing element situated upstream of the heater element, and a downstream sensing element situated downstream of the heater element. At least one of the heater element, the upstream sensing element and the downstream sensing element may include a first dielectric layer, a silicon layer on the first dielectric layer, a metal-silicide layer integrally formed with the silicon layer, and in some cases, a second dielectric layer situated on the metal-silicide layer. The silicon layer and/or the second dielectric layer may be doped with a dopant. In some cases, the upstream sensing element and the downstream sensing element may be included in a Wheatstone bridge.
An illustrative method for making a sensor element may include, for example, providing a first dielectric layer, providing a silicon layer on the first dielectric layer, doping the silicon layer with a concentration of a dopant, providing a metal layer on the silicon layer, and heating the silicon layer and the metal layer to integrally form a metal-silicide layer that consumes part of the silicon layer but leaves at least some of the silicon layer between the first dielectric layer and the metal-silicide layer. In some instances, the metal layer may include one or more of platinum (Pt), gold (Au), palladium (Pd), molybdenum (Mo), titanium (Ti), tungsten (W), hafnium (Hf), zirconium (Zr), chromium (Cr), Cobalt (Co), Copper (Cu), Nickel (Ni), Vanadium (V), Iron (Fe), Manganese (Mn) and Tantalum (Ta). Additionally, the silicon layer may include one or more of polysilicon, amorphous silicon, crystalline silicon or silicon-germanium (SiGe). The resultant sensing element may have a near linear positive or negative temperature coefficient of resistance (TCR), if desired.
The preceding summary is provided to facilitate an understanding of some of the features of the present disclosure, and is not intended to be a full description. A full appreciation of the disclosure can be gained by taking the entire specification, claims, drawings, and abstract as a whole.
The disclosure may be more completely understood in consideration of the following detailed description of various illustrative embodiments of the disclosure in connection with the accompanying drawings, in which:
The following description should be read with reference to the drawings wherein like reference numerals indicate like elements throughout the several views. The description and drawings show several embodiments which are meant to be illustrative of the present disclosure, and not limiting.
With reference to
In the illustrative embodiment of
In some instances, the first sensing element 114 and the second sensing element 116 may be thermally sensitive resistors that have a near (or substantially) linear positive or negative temperature coefficient of resistance, such that the resistance varies linearly with temperature. In some cases, the first and second sensing elements 114 and 116 may be thermistors. In some instances, the first sensing element 114, the second sensing element 116, and any additional sensing elements, may be arranged in a Wheatstone bridge configuration, but this is not required.
In the illustrative embodiment of
When a fluid flow is present in the fluid channel, and the heater element 112 is activated and heated to a temperature higher than the ambient temperature of the fluid in the fluid flow, the symmetrical temperature distribution may be disturbed and the amount of disturbance may be related to the flow rate of the fluid flow in the fluid channel. In this example, the flow rate of the fluid flow may cause the upstream sensing element 114 to sense a relatively cooler temperature than the downstream sensing element 116. In other words, the flow rate of the fluid flow may cause a temperature differential between the upstream sensing element 114 and the downstream sensing element 116 that is related to the flow rate of the fluid flow in the fluid channel. In some cases, the temperature differential between the upstream sensing element 114 and the downstream sensing element 116 may result in an output voltage differential between the upstream sensing element 114 and the downstream sensing element 116.
In another illustrative embodiment, the mass flow and/or velocity of the fluid flow may be determined by providing a transient elevated temperature condition in the heater element 112, which in turn, may cause a transient elevated temperature condition (e.g., heat pulse) in the fluid flow. When there is a non-zero flow rate in the fluid flow, the upstream sensing element 114 may receive a transient response later than the downstream sensing element 116. The flow rate of the fluid flow can then be computed using the time lag between the upstream sensing element 114 and downstream sensing element 116, or between the time the heater element 112 is energized and when the corresponding elevated temperature condition (e.g., heat pulse) is sensed by one of the sensors, such as the downstream sensing element 116.
Performance of the flow sensing die 100 may be dependent on heat transferred to the sensing elements 114 and 116 through the fluid, and not through other heat conduction paths. In the illustrative embodiment shown, membrane 106 may substantially thermally isolate the heater element 112 and sensing elements 114 and 116 from the substrate 102. Without such thermal isolation, heat may be conducted to/from the flow sensor components from/to the substrate 102, which may reduce the sensitivity and/or performance of the sensing die 100. Material selection may provide an additional or alternative way to help thermally isolate the sensing elements 114 and 116, which may be used in flow sensors with or without thermally-isolating membranes. For example, low thermal conductivity materials may be used for the substrate 102, such as fused silica, fused quartz, and/or borosilicate glass. Additionally or alternatively, thermal isolation may be achieved on a substrate with low thermal conductivity thin films such as oxidized porous silicon, nitrides, aerogels, or any other suitable materials. These are just some examples.
In the illustrative embodiment of
In some illustrative embodiments, wire bond pads 122 may be disposed along multiple die edges, or at other locations on the sensing die 100, as desired. Wire bond pads 122 may be configured for communicating signals relative to the one or more flow sensing die elements, such as heater element 112 and/or sensing elements 114 and 116, and/or temperature sensing element 118. Wire bond pads may include or be formed primarily of gold, aluminum, copper, and/or any other suitable conductor material or material combination, as desired. Traces may be provided to electrically connect the wire bond pads 122 to appropriate flow sensor components. Although not shown, flow sensing die 100 may be combined with a top cap to form a fluid channel for receiving a fluid flow therethrough, if desired.
Other flow sensing die configurations are contemplated. For example, the flow sensing die may be configured as a microbridge or a Microbrick™ sensor assembly, but this is not required. Some illustrative methods and sensor configurations that are considered suitable for measuring the mass flow and/or velocity are disclosed in, for example, U.S. Pat. Nos. 4,478,076; 4,478,077; 4,501,144; 4,581,928; 4,651,564; 4,683,159; 5,050,429; 6,169,965; 6,223,593; 6,234,016; 6,502,459; 7,278,309; 7,513,149; and 7,647,842. It is contemplated that flow sensing die 100 may include any of these flow sensor configurations and methods, as desired. It should be recognized, however, that flow sensor 100 may be any suitable flow sensor, as desired. Also, and as indicated above, while a flow sensor 100 is used as an example, it is contemplated that the disclosure may be applied to other types of sensors including, for example, thermal conductivity sensors, self-heating sensors, chemical sensors, pressure sensors, and/or other types of sensors, as desired.
The heater elements 112, 212 and/or sensing elements 114, 116, 214, and 216 may each be configured to have a near linear (or substantially linear) temperature coefficient of resistance (TCR). The TCR value may be different for each of the heater elements 112, 212 and sensing elements 114, 116, 214 and 216. In some cases, the heating elements 112, 212 may have a near zero or negative TCR, and the sensing elements 114, 116, 214 and 216 may have a TCR value of at least about 1000 ppm/° C., at least about 2000 ppm/° C., in the range from about 2000 ppm/° C. to about 4000 ppm/° C., or any other suitable value, as desired.
In many cases, the heater elements 112, 212 and/or the sensing elements 114, 116, 214, and 216 may include at least one silicon layer and at least one metal-silicide layer. In some cases, the metal-silicide layer is integrally formed with the silicon layer. In some cases, the heater elements 112, 212 and/or the sensing elements 114, 116, 214, and 216 may each also include one or more dielectric layers. For example, in some cases, and as shown in the example of
In some instances, the first dielectric layer 236 may be any suitable dielectric material. Suitable dielectric materials may include, but are not limited to, silicon oxide, silicon nitride, silicon oxynitride, and the like. The silicon layer 242 may include, but is not limited to, polysilicon, amorphous silicon, crystalline silicon, silicon-germanium (SiGe), and the like. In some cases, the first dielectric layer 236 and the silicon layer 242 correspond to the insulating layer and silicon layer, respectively, of a silicon-on-insulator (SOI) wafer, but this is not required. In some cases, the silicon layer 242 may be doped to modulate the resistivity of the silicon layer 242. Exemplary dopants may include, but are not limited to phosphorous (P), boron (B), arsenic (As), antimony (Sb), gallium, aluminum, and/or the like.
The metal-silicide layer 248 may be formed by first depositing a metal layer on the silicon layer 242, followed by sintering to produce a metal-silicide layer 248 in a process referred to as silicidation, as will be described in greater detail below. The metal layer, and thus the metal-silicide layer 248, may be formed using one or more metals including, but not limited to, platinum (Pt), gold (Au) palladium (Pd), molybdenum (Mo), titanium (Ti), tungsten (W), hafnium (Hf), zirconium (Zr), chromium (Cr), cobalt (Co), copper (Cu), nickel (Ni), vanadium (V), iron (Fe), manganese (Mn), and/or tantalum (Ta). These are just examples.
In some cases, the second dielectric layer 254 may be formed over the metal-silicide layer 248. The second dielectric layer 254 may be formed from any suitable dielectric material. Suitable dielectric materials may include, but are not limited to silicon oxide, silicon nitride, silicon oxynitride, and the like. In some cases, the second dielectric layer 254 may be deposited, grown, or otherwise formed over the metal-silicide layer 248. This may include using one or more deposition techniques such as sputtering, plasma vapor deposition, and chemical vapor deposition, to name a few. In some instances, the second dielectric layer 254 may be produced during the silicidation process, where some of the silicon atoms and/or dopant atoms in the silicon layer 242 diffuse through the metal-silicide layer 248 and becoming oxidized, thereby forming the second dielectric layer 254. Regardless of how formed, the second dielectric layer 254 may function as a low stress upper adhesion layer that supports further thin film deposition.
The TCR of each of the heater and/or sensing elements 112, 212, 114, 116, 214 and 216 may be controlled, at least in part, by controlling the thickness of the silicon layer 242 and/or the metal-silicide layer 248 that is used to form the heater or sensing elements 112, 212, 114, 116, 214, and 216. Additionally, the concentration of dopant in the silicon layer 242 may also be used, in part, to control the TCR of the heater and/or sensing elements 112, 212, 114, 116, 214, and 126. In some cases, the concentration of dopant in the silicon layer 242 may range from 1012 cm−3 and 1021 cm−3. Other variables contributing to the TCR may include the initial silicon layer 242 thickness and the initial metal layer thickness (e.g. the thickness of the metal layer used to form the metal-silicide layer 248).
During the silicidation process used to form the metal-silicide layer 248, all the metal initially deposited onto the silicon layer 242 may be consumed to form the metal-silicide layer 248 and hence, the metal-silicide layer thickness tms will be determined, at least in part, by the initial metal thickness tmo,
t
ms=κmtm. (1)
Additionally, to help ensure that at least part of the silicon layer 242 remains underneath the silicide film (e.g. to promote adhesion after silicidation), the initial silicon layer thickness may be
t
Si
o>κmsκmtmo+κoxtox. (2)
Where toSi is the initial silicon layer thickness, tms and tox are the final metal-silicide and oxide layer thicknesses, respectively, κms is the thickness ratio of the metal silicide layer formed to the amount of silicon layer consumed, and κox is the thickness ratio of the oxide layer (e.g., second dielectric layer 254) to the amount of the silicon layer consumed. Thus, the remaining silicon layer thickness tSi may be expressed as:
t
Si
=t
Si
o−κmstms−κoxtox. (3)
The sheet resistance of the composite film, including the metal-silicide layer 248 and the under lying silicon layer 242, may contribute to the overall TCR of the heater and/or sensing elements. For example, the sheet resistance can be derived based on the property of the two conductive films using equation (4), which is presented below:
Where the ρms and ρSi are the resistivities of the metal-silicide layer 248 and the remaining silicon layer 242, respectively. From equation (4), the temperature coefficient of the resistance (TCR) of the heating and/or sensing element 112, 212, 114, 116, 214, and/or 216 may be derived using equation (5), which is presented below:
Where TCRms TCRSi are the temperature coefficients of resistance for the metal-silicide layer 248 and the remaining silicon layer 242, respectively.
In some instances, the thickness tms may range from about 500 angstroms to about 1 micron, and the remaining silicon layer 242 thickness tSi may range from about 100 angstroms to about 1 micron, but these are just examples. The TCR of the heating and/or sensing elements may be at least 1000 ppm/° C., at least about 2000 ppm/° C., in the range from about 2000 ppm/° C. to about 4000 ppm/° C., or any other suitable value, as desired.
As shown in
In some instances, the silicon layer 304 may then be doped with a suitable dopant, such as phosphorous (P), arsenic (As), boron (B), antimony (Sb), and/or the like. In some cases, the concentration of dopant in the silicon layer 242 may range from 1012 cm−3 and 1021 cm−3. Next, a masking layer 308 may be provided on select portions or regions of the silicon layer 304. This may be followed by etching the exposed regions of the silicon layer 304. Any number of suitable etching techniques may be used. The masking layer 308 may then be removed, and a metal layer 312 may be deposited onto the surface of the dielectric layer 302 and remaining silicon layer 304. The metal layer 312, and thus the resulting metal-silicide layer 316, may be formed using one or more metals including, but not limited to, platinum (Pt), gold (Au) palladium (Pd), molybdenum (Mo), titanium (Ti), tungsten (W), hafnium (Hf), zirconium (Zr), chromium (Cr), cobalt (Co), copper (Cu), nickel (Ni), vanadium (V), iron (Fe), manganese (Mn), and/or tantalum (Ta). These are just examples.
The assembly may then be sintered for an appropriate amount of time at a suitable temperature to convert the metal layer 312 and the underlying silicon layer 304 to an integral metal-silicide layer (e.g. through silicidation). As discussed previously, substantially all the metal layer 312 that is deposited onto the silicon layer 304 may be consumed to form the metal-silicide layer 316, as shown in
A second dielectric layer 318 may be formed from any suitable dielectric material. Suitable dielectric materials may include, but are not limited to silicon oxide, silicon nitride, silicon oxynitride, and the like. In some cases, the second dielectric layer 318 may be deposited, grown, or otherwise formed over the metal-silicide layer 316. This may include using one or more deposition techniques such as sputtering, plasma vapor deposition, and chemical vapor deposition, to name a few. In some instances, the second dielectric layer 318 may be produced during the silicidation process, where some of the silicon atoms and/or dopant atoms in the silicon layer 304 diffuse through the metal-silicide layer 316 and becoming oxidized, thereby forming the second dielectric layer 318. Regardless of how formed, the second dielectric layer 318 may function as a low stress upper adhesion layer that supports further thin film deposition.
In some cases, a nitride layer or cap 320 may be deposited over the remaining metal-silicide layer 316, the exposed first dielectric layer 302, and the second dielectric layer 318. The nitride layer or cap 320 may be deposited via sputtering or via chemical or plasma vapor deposition. Additionally, in some cases, the substrate 300 may be back-side etched to define a void (e.g. void 110 of
A silicon wafer was initially cleaned by a megasonic cleaning process. Next, the silicon wafer was oxidized under the conditions set forth in Table 1 below.
The thickness of the silicon oxide layer was determined to be about 9700 Å.
Next, polysilicon was deposited onto the silicon oxide layer. The polysilicon was deposited at an initial thickness of 3000 Å at a temperature of 620° C. The actual thickness of the resulting polysilicon layer was measured at 3120 Å.
Deposition of the polysilicon layer was followed by the introduction of a dopant. In this example, POCl3 was introduced into the gaseous environment resulting in phosphorous as the dopant. The conditions for introduction of the dopant are set forth below in Table 2.
The measured sheet resistance of the resulting polysilicon layer was 19.9±0.3 Ω/sq.
Next, the polysilicon layer was patterned using a photo masking technique followed by plasma etching. The wafer was then cleaned.
Platinum was then deposited onto the surface of the wafer including the polysilicon layer at an initial thickness of 500 Å. The sheet resistance of the polysilicon layer including the platinum metal layer was measured and found to be 4.05±0.3 Ω/sq.
Silicidation of the platinum and polysilicon layers to form a platinum-silicide layer was carried out by sintering the wafer at 450° C. in a nitrogen environment for about 16 minutes and then in an ambient air environment for about 10 minutes. The remaining platinum metal was stripped from the wafer using Aqua Regia.
A SEM image of a resultant sensor element is shown in
The resultant thickness of the platinum-silicide layer was determined to be approximately 109.0 nm, which agreed with the theoretical prediction for the thickness of this layer. The thickness of the remaining polysilicon layer was determined to about 233.3 nm. The TCR of the sensor element was measured and found to be 2000 ppm/° C.
Having thus described several illustrative embodiments of the present disclosure, those of skill in the art will readily appreciate that yet other embodiments may be made and used within the scope of the claims hereto attached. Numerous advantages of the disclosure covered by this document have been set forth in the foregoing description. It will be understood, however, that this disclosure is, in many respect, only illustrative. Changes may be made in details, particularly in matters of shape, size, and arrangement of parts without exceeding the scope of the disclosure. The disclosure's scope is, of course, defined in the language in which the appended claims are expressed.