The disclosure of Japanese Patent Application No. 2010-217317 filed on Sep. 28, 2010 including the specification, drawings and abstract is incorporated herein by reference in its entirety.
The present invention relates to a semiconductor device. More particularly, it relates to a configuration of a resistance element included in a semiconductor device.
In the related art, a microcomputer and an oscillator have been separately manufactured. In recent years, inclusion of an oscillator in a chip of a microcomputer has achieved shrinkage of the layout area of a semiconductor device, reduction of the cost, and the like.
In order for a chip of a microcomputer to include an oscillator therein, the oscillation frequency of the oscillator is required to be stable even when the conditions such as voltage and temperature change. As one example, for a high-speed OCO (On Chip Oscillator) circuit included in a microcomputer, the oscillation frequency is required to be, for example, 40 MHz±1%.
The high-speed OCO circuit includes, for example, a resistance element for converting the current supplied from a constant current source into a voltage. The voltage determines the oscillation frequency. Therefore, when the resistance value of the resistance element varies according to the temperature, the oscillation frequency of the high-speed OCO circuit varies. For this reason, the temperature dependence of the resistance value of the resistance element is required to be reduced.
For example, Japanese Unexamined Patent Publication No. 2007-149965 (Patent Literature 1), and Japanese Unexamined Patent Publication No. 2006-216607 (Patent Literature 2) disclose a technology of inhibiting the temperature dependence of the resistance value by combining a resistance element having a positive temperature coefficient and a resistance element having a negative temperature coefficient. Patent Literature 1 discloses the following: the resistance value of a resistance element formed of nickel chromium has a positive temperature coefficient, and the resistance value of a resistance element formed of chromium silicon has a negative temperature coefficient. Patent Literature 2 discloses the following: the resistance value of a resistance element formed of N type polysilicon has a positive temperature coefficient, and the resistance value of a resistance element formed of P type polysilicon has a negative temperature coefficient.
[Patent Literature 1]
[Patent Literature 2]
Patent Literature 1 does not specifically disclose the temperature coefficient of the resistance value. Accordingly, Patent Literature 1 does not specifically disclose how much the temperature change rate of the resistance value of the resistance element including a nickel chromium resistance and a chromium silicon resistance is reduced.
On the other hand, Patent Literature 2 discloses that the change rate of the resistance value of the resistance element formed of N type polysilicon and P type polysilicon is −0.02% (within the temperature range of −45° C. to 125° C.). In the case of a circuit required to have a resistance element having a high-precision resistance value as with the high-speed OCO circuit, the temperature dependence of the resistance value is required to be as small as possible. Therefore, the resistance element formed of N type polysilicon and P type polysilicon may be inapplicable to such a circuit.
It is an object of the present invention to provide a semiconductor device having a resistance element whose resistance value shows a small temperature dependence.
A semiconductor device in accordance with one example of the present invention includes a semiconductor substrate, an insulation layer provided over the semiconductor substrate, a first resistance element provided over the insulation layer, and a second resistance element electrically coupled with the first resistance element. One of the first and second resistance elements is formed of titanium nitride. The other of the first and second resistance elements is formed of tantalum nitride.
In accordance with examples of the present invention, it is possible to provide a semiconductor device having a resistance element whose resistance value shows a small temperature dependence.
Below, embodiments of the present invention will be described in details by reference to the accompanying drawings. Incidentally, in the drawings, the same or similar parts are given the same reference numerals and signs, and a description thereon will not be repeated.
Referring to
The high-speed OCO circuit 100 includes a constant voltage circuit 101 including a constant current source. The constant voltage circuit 101 includes a depression type MOSFET Q1, a resistance element 110, and enhancement type MOSFETs Q2, Q3, and Q4. The MOSFETs Q1 and Q4 are N channel MOSFETs. The MOSFETs Q2 and Q3 are P channel MOSFETs. The high-speed OCO circuit 100 further includes enhancement type MOSFETs Q5 to Q7, a capacitor C1, a differential amplification circuit 102, a delay circuit 103, and a booster circuit 104.
The source of the MOSFET Q1 is coupled to one end of the resistance element 110. The drain of the MOSFET Q1 and the drain of the MOSFET Q2, and the gate of the MOSFET Q2 and the gate of the MOSFET Q3 are mutually coupled. The drain of the MOSFET Q3 and the drain of the MOSFET Q4, and the gate of the MOSFET Q4 and the gate of the MOSFET Q1 are mutually coupled. The sources of the MOSFETs Q2 and Q3 are coupled to a source voltage Vcc. The other end of the resistance element 110 and the source of the MOSFET Q4 are coupled to the grounding voltage.
The constant voltage circuit 101 generates a given current flowing through the resistance element 110. From one end (node N) of the resistance element 110, there is outputted a constant voltage determined by the product of the current value and the resistance value (as one example, 5 kΩ) of the resistance element 110. The constant voltage is the reference voltage to be inputted to the negative input terminal of the differential amplification circuit 102.
The gate of the MOSFET Q5 is coupled to the gate of the MOSFET Q2 and the gate of the MOSFET Q3. The source of the MOSFET Q5 is coupled to the source voltage Vcc. The drain of the MOSFET Q5 is coupled to the source of the MOSFET Q6. The drain of the MOSFET Q6 is coupled to the drain of the MOSFET Q7. The source of the MOSFET Q7 is coupled to the grounding voltage.
The gate of the MOSFET Q6 and the gate of the MOSFET Q7 are coupled to the output terminal of the delay circuit 103. The drain of the MOSFET Q6 and the drain of the MOSFET Q7 are both coupled to one end (node N1) of the capacitor C1, and coupled to the positive input terminal of the differential amplification circuit 102.
The differential amplification circuit 102 compares the voltage generated by the constant voltage circuit 101 and the voltage of the capacitor C1. The capacitor C1 is charged or discharged according to the comparison result. By repetition of charging and discharging of the capacitor C1, a signal having a prescribed oscillation period is outputted via the delay circuit 103.
The booster circuit 104 includes an inverter IV1, enhancement type MOSFETs Q12 and Q13, and capacitors C2 and C3. The MOSFETs Q12 and Q13 are N channel MOSFETs.
A start signal CLK is inputted into the booster circuit 104. The booster circuit 104 boosts the voltage of the start signal CLK, and applies the boosted voltage to the gate of the MOSFET Q4 and the gate of the MOSFET Q1.
The start signal CLK is inputted to the inverter IV1 and the gate of the MOSFET Q12. The output terminal of the inverter IV1 is coupled to one end of the capacitor C2. The other end of the capacitor C2 is coupled to the drain of the MOSFET Q12, the drain of the MOSFET Q13, and the gate of the MOSFET Q13. The source of the MOSFET Q13 is coupled to one end (node N3) of the capacitor C3. The source of the MOSFET Q12 and the other end of the capacitor C3 are coupled to the grounding voltage.
The voltage outputted from the constant voltage circuit 101 is determined by the resistance value of the resistance element 110 and the current flowing through the resistance element 110. In accordance with the embodiment of this invention, it becomes possible to inhibit variation in resistance value of the resistance element 110 according to the temperature. Therefore, it is possible to stabilize the voltage outputted from the constant voltage circuit 101. Stabilization of the voltage outputted from the constant voltage circuit 101 can stabilize the oscillation frequency of the signal outputted from the high-speed OCO circuit (e.g., 40 MHz±1% or 40 MHz±0.2%). Namely, it is possible to stabilize the frequency of the oscillation circuit included in the chip of the microcomputer.
In order to prevent the resistance value from varying according to the temperature, in the related art, the resistance element 110 includes, for example, a combination of N type polysilicon and P type polysilicon. The resistance value of N type polysilicon has a positive temperature coefficient. In contrast, the resistance value of P type polysilicon has a negative temperature coefficient. Combination of both causes the positive temperature coefficient and the negative temperature coefficient to cancel each other. Therefore, it is possible to reduce the temperature coefficient of the resistance value.
However, the temperature coefficient of polysilicon is generally about several thousand ppm. Further, the temperature coefficient of polysilicon is adjusted by the impurity concentration of polysilicon. For this reason, it is difficult to form a polysilicon resistance having a small temperature coefficient with stability.
Thus, it is considered that the resistance element 110 is formed of a metal material whose resistance value shows a small variation within the compensated temperature range of the semiconductor device. For example, by using titanium nitride (TiN) for the resistance element 110, it is possible to achieve a temperature coefficient (several hundred ppm) one order of magnitude smaller than the temperature coefficient of the polysilicon resistance.
However, when the precision of the oscillation frequency is required to be further enhanced, a resistance having a smaller temperature coefficient may be demanded. In accordance with the embodiment of the present invention, combination of a titanium nitride resistance and a tantalum nitride (TaN) resistance forms the resistance element 110.
The temperature coefficient of the resistance value of the titanium nitride resistance and the temperature coefficient of the resistance value of the tantalum nitride resistance (absolute values) are both about one order of magnitude smaller than the temperature coefficient of the resistance value of the polysilicon resistance. Therefore, it becomes possible to form a resistance element having a small temperature coefficient with stability.
The resistance value of the resistance element 111 is referred to as R1. The resistance value of the resistance element 112 is referred to as R2. The resistance value R of the resistance element 110 is expressed according to the following expression (1) (the sign “*” represents the product; the same applies to the following).
R=R1+R2=R1s(1+ΔR1)+R2s(1+ΔR2)=R1s+R2s+ΔR1*R1s+ΔR2*R2s (1)
where ΔR1 and ΔR2 are values having mutually opposite signs. For example, it is assumed that the resistance element 111 is a titanium nitride resistance, and that the resistance element 112 is a tantalum nitride resistance. In this case, ΔR1 is a positive value, and ΔR2 is a negative value. By appropriately setting the resistance values R1 and R2, it is possible to make ΔR1*R1s+ΔR2*R2s to be zero. R1s and R2s are temperature-independent components. When ΔR1*R1s+ΔR2*R2s=0, it is possible to obtain a temperature-independent resistance value R (=R1s+R2s).
The relationship between ΔR1 and ΔR2 is previously determined experimentally or by other methods. As a result, the relationship between R1s and R2s for obtaining ΔR1*R1s+ΔR2*R2s=0 is determined. The resistance value R is determined at the stage of, for example, circuit design. The resistance value R (design value), and the relationship between R1s and R2s determine the resistance values R1s and R2s. Accordingly, the values of the resistance values R1s and R2s are defined as resistance values R1 and R2, respectively. By appropriately setting respective widths, lengths, and thicknesses of the titanium nitride resistance and the tantalum nitride resistance, it is possible to obtain the resistance values.
Referring to
The tap layers Ma and Mb are covered with a surface-planarized second interlayer insulation film SO12. Over the second interlayer insulation film SO12, a metal resistance element layer Rm1 is provided. The metal resistance element layer Rm1 has a double-layer structure of a metal resistance film layer RM11 and an antioxidant film layer SN1. The metal resistance element layer Rm1 corresponds to the resistance element 111.
The metal resistance element layer Rm1 is covered with a surface-planarized third interlayer insulation film SO13. Over the third interlayer insulation film SO13, a metal resistance element layer Rm2 is provided. The metal resistance element layer Rm2 has a double-layer structure of a metal resistance film layer Rm12 and an antioxidant film layer SN2. The metal resistance element layer Rm2 corresponds to the resistance element 112.
The metal resistance element layer Rm2 is covered with a surface-planarized fourth interlayer insulation film SO14. The fourth interlayer insulation film SO14 is covered with a flat-surface passivation film SN12. The passivation film SN12 is covered with a flat-surface protective film PF.
The metal resistance film layer Rm11 is one of the titanium nitride resistance and the tantalum nitride resistance. The metal resistance film layer Rm12 is the other of the titanium nitride resistance and the tantalum nitride resistance. Namely, at a layer arranged above the layer of the tantalum nitride resistance, the titanium nitride resistance may be formed. Conversely, at a layer arranged above the layer of the titanium nitride resistance, the tantalum nitride resistance may be formed.
A contact plug CP1 couples the one end of the resistance element 111 and the tap layer Ma. A contact plug CP2 couples the other end of the resistance element 111 and the one end of the resistance element 112. A contact plug CP3 couples the other end of the resistance element 112 and the tap layer Mb. For the contact plugs CP1 to CP3, for example, tungsten (W) is used. The contact plug CP3 includes the contact plug CP1, and the contact plug CP2 coupled to the contact plug CP1.
The material for the contact plugs CP1 to CP3 is different from any of titanium nitride and tantalum nitride. Therefore, conceivably, the temperature characteristics of the resistance values of the contact plugs CP1 to CP3 may affect the temperature characteristics of the resistance value of the resistance element 110. When each of the contact plugs CP1 to CP3 is formed of tungsten as described above, the temperature coefficient of the resistance value of tungsten is about several thousand ppm (e.g., 3000 ppm). However, by increasing the proportion of contribution of the resistance value of the resistance element 110 to the overall resistance value of total of the resistance value of the resistance element 110, and the resistance values of the contact plugs CP1 to CP3, it is possible to reduce the variation in resistance value due to the temperature characteristics of the resistance values of the contact plugs CP1 to CP3.
In the case of a semiconductor device having a multilayer interconnection structure, the number of wiring layers is not limited to two so long as it is plural. Namely, the number of wiring layers arranged below the tap layers Ma and Mb shown in
Then, a description will be given to a method for manufacturing the semiconductor device in accordance with the first embodiment. Specifically, a description will be given to a manufacturing step of the resistance element 110 shown in
Then, over the first interlayer insulation film SO11, a wiring layer M is formed. The wiring layer M is a wiring layer arranged at the highest position of a plurality of wiring layers. The wiring layer M is deposited by a sputtering method. The wiring layer M has a lower layer M1, a wiring main body M2, and an upper layer M3. The lower layer M1 includes a TiN/Ti film. The wiring main body M2 includes a copper-added aluminum (Al—Cu) film. The upper layer M3 includes a TiN/Ti film. The film thickness of the wiring layer M is, for example, about several hundred nm to 1 μm.
Then, over the wiring layer M, an antireflective film SON11 is formed. The antireflective film SON11 is, for example, a plasma oxynitride film (P—SiON), and is formed by a CVD method.
For the antioxidant film layer SN1, for example, a plasma nitride (P—SiN) film is used. The plasma nitride film is formed by a CVD method.
Then, using a photolithographic technology and a dry etching treatment, patterning of the metal resistance element layer Rm1 is performed. By this step, the metal resistance element layer Rm1 is formed, and the metal resistance element layer Rm1 is electrically coupled with the tap layer Ma via the contact plug CP1.
Incidentally, the antioxidant film layer SN1 prevents the surface of the metal resistance film layer Rm11 from being exposed to an oxygen plasma atmosphere when resist removal is performed in the oxygen plasma atmosphere.
Over the tap layer Mb, the contact plug CP1 and the contact plug CP2 are coupled. As a result, the contact plug CP3 is formed.
Then, using a photolithographic technology and a dry etching treatment, patterning of the metal resistance element layer Rm2 is performed. By this step, the metal resistance element layer Rm2 is formed. For the antioxidant film layer SN2, a plasma nitride (P—SiN) film is used. The plasma nitride film is formed by a CVD method. The antioxidant film layer SN2 prevents the surface of the metal resistance film layer Rm12 from being exposed to an oxygen plasma atmosphere when resist removal is performed in the oxygen plasma atmosphere.
In this embodiment, the metal resistance element layers Rm1 and Rm2 are formed further above the wiring layer M arranged at the highest position of a plurality of wiring layers via the insulation film. In order to achieve favorable coverage of the passivation film SN12 and the protective film PF, respective surfaces of the second interlayer insulation film SO12 and the third interlayer insulation film SO13 are planarized. Therefore, it is possible to equalize the thicknesses of the metal resistance film layer Rm11 and the metal resistance film layer Rm12 formed by a sputtering method. The thicknesses of the metal resistance film layer Rm11 and the metal resistance film layer Rm12 can be controlled with high precision. Accordingly, it is possible to enhance the precision of respective resistance values of the resistance elements 111 and 112.
Further, by disposing the metal resistance element layers Rm1 and Rm2 above the wiring layer M, it is possible to ease restrictions on the layout of the resistance elements 111 and 112. For example, in order to obtain a desirable resistance value, there may arise a necessity of elongating the resistance element. When the metal resistance element layers Rm1 and Rm2 are formed using the wiring layer M, or a wiring layer arranged below the wiring layer M, the chip area may increase due to elongation of the resistance element for obtaining a desirable resistance value. In accordance with this embodiment, it is possible to ease restrictions on the layout of the resistance elements 111 and 112. For this reason, it is possible to form the resistance element without increasing the chip area.
The tap layer Mc is, as with the tap layers Ma and Mb, the wiring layer M arranged at the highest position of a plurality of wiring layers. As shown in
The metal resistance element layers Rm1 and Rm2 are disposed at a position above the wiring layer M. Therefore, as shown in
As described up to this point, in accordance with the first embodiment, the semiconductor device includes a resistance element including a titanium nitride (TiN) resistance and a tantalum nitride (TaN) resistance coupled in series to each other. The titanium nitride resistance and the tantalum nitride resistance are small in temperature coefficient of the resistance value (several hundred ppm, as one example, 400 ppm). Further, the resistance value of the titanium nitride resistance has a positive temperature coefficient. On the other hand, the resistance value of the tantalum nitride resistance has a negative temperature coefficient. By combining the titanium nitride resistance and the tantalum nitride resistance, it is possible to provide a resistance element having a small temperature dependence, or substantially not having a temperature dependence.
In a second embodiment, a semiconductor device includes a resistance element including a titanium nitride resistance and a tantalum nitride resistance coupled in parallel to each other. In this respect, the second embodiment is different from the first embodiment. As with the first embodiment, this resistance element is included in a high-speed OCO circuit included in, for example, a microcomputer chip (see
Referring to
Incidentally, as indicated from the comparison between
The resistance value of the resistance element 111 is referred to as R1. The resistance value of the resistance element 112 is referred to as R2. The resistance value R of the resistance element 120 is expressed according to the following expression (2).
R=1/(1/R1+1/R2)=R1*R2/(R1+R2)={R1s(1+ΔR1)*R2s(1+ΔR2)}/{R1s(1+ΔR1)+R2s(1+ΔR2)}≈(R1s*R2s+ΔR1*R1s+ΔR2*R2s)/(R1s+R2s+ΔR1*R1s+ΔR2*R2s)=(1+ΔR1/R2s+ΔR2/R1s)/(1/R2s+1/R1s+ΔR1/R2s+ΔR2/R1s) (2),
where ΔR1 and ΔR2 are values having mutually opposite signs (e.g., ΔR1 is a positive value, and ΔR2 is a negative value). By setting the resistance values R1 and R2 at proper values, it is possible to satisfy the relationship of ΔR1/R2s+ΔR2/R1s=0. As a result, it is possible to obtain a temperature-independent resistance value R.
As described up to this point, in accordance with the second embodiment, the semiconductor device includes a resistance element including a titanium nitride resistance and a tantalum nitride resistance coupled in parallel to each other. As with the first embodiment, in accordance with the second embodiment, it is possible to reduce the temperature dependence, or to make substantially zero the temperature dependence also in the resistance element formed by parallel coupling.
In a third embodiment, a titanium nitride resistance and a tantalum nitride resistance are stacked. In this respect, the third embodiment is different from the first embodiment. As with the first embodiment, this resistance element is included in a high-speed OCO circuit included in a microcomputer chip (see
The length of the resistance element 111 and the length of the resistance element 112 are both L. The width of the resistance element 111 is W1. In contrast, the width of the resistance element 112 is W2. W1<W2. As with the first and second embodiments, the resistance element 111 is one of the titanium nitride resistance and the tantalum nitride resistance. The resistance element 112 is the other of the titanium nitride resistance and the tantalum nitride resistance.
The metal resistance element layer Rm3 is covered with the third interlayer insulation film SO13. The semiconductor device in accordance with the third embodiment does not have a fourth interlayer insulation film SO14. In this respect, the semiconductor device in accordance with the third embodiment is different from the semiconductor device in accordance with the first embodiment (see
The configuration of other portions of the semiconductor device shown in
The metal resistance film layer Rm11 is one of the titanium nitride resistance and the tantalum nitride resistance. The metal resistance film layer Rm12 is the other of the titanium nitride resistance and the tantalum nitride resistance. Namely, the titanium nitride resistance may be formed above the tantalum nitride resistance. Conversely, the tantalum nitride resistance may be formed above the titanium nitride resistance.
The methods for manufacturing the metal resistance element layer Rm3 have no particular restriction. However, for example, the method described below can be employed. First, over the planarized surface of the second interlayer insulation film SO12, a TiN film (metal resistance film layer Rm11) is formed by a sputtering method. Then, using a photolithographic technology and a dry etching treatment, patterning of the metal resistance film layer Rm11 is performed.
Subsequently, by a sputtering method, a TaN film (metal resistance film layer Rm12) is formed. Using a photolithographic technology and a dry etching treatment, patterning of the metal resistance element layer Rm2 is performed so that the TaN film and the TiN film are stacked one over another. The TaN film may be stacked over the TiN film by a lift-off method. Namely, patterning of a photoresist is performed using a photolithographic technology so that an opening of the photoresist (space pattern) is formed at a portion thereof overlapping the TiN film. Then, the TaN film is deposited by sputtering. Finally, the photoresist is removed. As a result, it is possible to stack the TaN film having a length L and a width W2 over the TiN film.
Subsequently, the antioxidant film layer SN1 (P—SiN film) is formed by a CVD method. Using a photolithographic technology and a dry etching treatment, patterning of the antioxidant film layer SN1 is performed. Specifically, patterning of the antioxidant film layer SN1 is performed so that the length of the antioxidant film layer SN1 is L, and so that the width of the antioxidant film layer SN1 is W1.
The equivalent circuit of the resistance element 120 shown in
The resistance value of the resistance element 111 is referred to as R1. The resistance value of the resistance element 112 is referred to as R2. The resistance value R of the resistance element 110 can be expressed as 1/{(1/R1)+(1/R2)}=R1*R2/(R1+R2) as described above. When R1=R1s(1+ΔR1), and R2=R2s(1+ΔR2), the resistance value R can be expressed according to the following expression (3).
The term of ΔR1*ΔR2 included in the numerator of the fraction is omitted. Further, the denominator is Taylor-expanded, resulting in transposition to the numerator. As a result, the above (3) is transformed as follows.
By setting the second term inside the parentheses on the right-hand side of the above (4) to zero, it is possible to eliminate the temperature dependence of the resistance value R. Namely, the conditions such that R2*ΔR1+R1*ΔR2=0 becomes necessary.
When the resistance elements 111 and 112 are equal in resistance length, and the resistance elements 111 and 112 are different in width as shown in
The sheet resistance value of the resistance element 111 is referred to as ρ1; the resistance length of the resistance element 111 is referred as L1; and the width of the resistance element 111 is referred to as W1. The sheet resistance value of the resistance element 112 is referred to as ρ2; the resistance length of the resistance element 112 is referred to as L2; and the width of the resistance element 112 is referred to as W2. The resistance value R1 of the resistance element 111 is expressed as R1=ρ1*(L1/W1), and the resistance value R2 of the resistance element 112 is expressed as R2=ρ2*(L2/W2). Therefore, R2*ΔR1+R1*ΔR2=0 can be replaced with the following (5).
Herein, L1=L2. Therefore, the above (5) can be transformed as follows.
Therefore, by setting the ratio of W1 and W2 so as to satisfy the relationship shown in the above (6), it is possible to eliminate the temperature dependence of the resistance value R.
Further, as shown in
In this case, the conditions (R2*ΔR1+R1*ΔR2=0) for eliminating the temperature dependence of the resistance value R are determined in the following manner.
First, the sheet resistance ρ is expressed as ρ=σ/t, where σ denotes the volume resistance, and t denotes the film thickness. The above (5) can be transformed as follows.
where σ1 denotes the volume resistance of the resistance element 111, t1 denotes the film thickness of the resistance element 111, σ2 denotes the volume resistance of the resistance element 112, and t2 denotes the film thickness of the resistance element 112,
L1=L2, and W1=W2. Therefore, the above (7) can be transformed as follows.
By selecting the film thicknesses t1 and t2 so as to satisfy the relationship expressed by the above (8), it is possible to obtain a resistance value R having no temperature dependence.
As described up to this point, in accordance with the third embodiment, the titanium nitride resistance and the tantalum nitride resistance are stacked one over another. This eliminates the necessity of the contact plug for mutual coupling between the titanium nitride resistance and the tantalum nitride resistance, or the contact plug for coupling each of the titanium nitride resistance and the tantalum nitride resistance to the wiring layer M (tap layer Mc shown in
As described above, the temperature coefficient of the resistance value of the contact plug may be larger than the temperature coefficient (absolute value) of each resistance value of the titanium nitride resistance and the tantalum nitride resistance. In accordance with the third embodiment, it is possible to provide a resistance element more reduced in temperature dependence than the resistance element in accordance with the first or second embodiment, or a resistance element substantially not having a temperature dependence.
Further, in accordance with the third embodiment, the fourth interlayer insulation film SO14 can be omitted from the configuration in accordance with the first embodiment. Therefore, in accordance with the third embodiment, it is possible to reduce the manufacturing cost of the semiconductor device as compared with the first embodiment.
A semiconductor device in accordance with a fourth embodiment includes a plurality of the resistance elements in accordance with any of the first to third embodiments, and thereby enables adjustment of the resistance value.
The resistance circuit 150 can be used in place of, for example, the resistance element 110 in the constant voltage circuit 101 shown in
Each of the resistance elements 151 to 155 is selected when the corresponding MOSFET is turned off. Whereas, it is rendered in a non-selected state when the corresponding MOSFET is turned on. The MOSFETs Tr1 to TR5 are each independently turned on or off. Therefore, it is possible to control the resistance value between the node Na and the node Nb. Further, conceivably, the temperature dependence (temperature coefficient) of the resistance value varies between the resistance elements 151 to 155. Use of this enables the fine adjustment of the temperature dependence of the resistance value between the node Na and the node Nb.
Incidentally, in
Further, the resistance elements in accordance with the embodiments are not limited to those for use in an OCO circuit. The present invention is applicable to a semiconductor device including a circuit required to be minimized in variation of the resistance value according to the temperature.
The embodiments herein disclosed should be considered illustrative but not limiting in all aspects. The scope of the present invention is defined not by the description of the embodiments but the appended claims, and intended to embrace all changes that come within the meaning and range of equivalency of the claims.
The present invention is in particular advantageously applicable to semiconductor devices having resistance elements.
Number | Date | Country | Kind |
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2010-217317 | Sep 2010 | JP | national |