This invention relates to the field of integrated circuits. More particularly, this invention relates to forming resistors with a high temperature coefficient of resistance in integrated circuits.
In addition to transistors, other devices such as resistors, capacitors and diodes are formed during the manufacture of integrated circuits. These devices may be used to set voltage levels, pass or block signals, and form delay paths. In some cases these devices may be used to measure temperature.
The equation for the resistance of resistor material as a function of temperature is given by the equation
RTEMP=R0+C1ΔT+C2(ΔT)2
Where R0 is the resistance at a reference temperature such as room temperature, C1 is the linear temperature coefficient of resistance, C2 is the quadratic temperature coefficient of resistance, and ΔT is the difference between ambient temperature and the reference temperature.
Because the resistance of metals commonly used in integrated circuits such as copper and aluminum has low resistance, when a temperature sensing resistor is needed, a high resistance metal such as nickel or molybdenum is added to the integrated circuit process flow to form the temperature sensing resistor. Addition of a new metal to the manufacturing flow adds cost by requiring additional deposition and etching manufacturing steps.
When a device, such as a resistor, is embedded in an integrated circuit and used to measure temperature, it is desirable to have a large linear change in resistance with temperature, C1, with a low standard deviation and low lot-to-lot variation. It is also desirable for the material to have high resistivity so that less resistor area is needed to develop the required voltage drop.
The equation for resistance of resistor material as a function of temperature is given by the equation
RTEMP=R0+C1ΔT+C2(ΔT)2
Where R0=ρ*t/A is the resistance at a reference temperature such as room temperature, C1 is the linear temperature coefficient of resistance, C2 is the quadratic temperature coefficient of resistance, and ΔT is the difference between ambient temperature and the reference temperature. ρ is the resistivity of the material in μΩ-cm, t is the thickness of the resistor and A is the cross sectional area of the resistor.
As shown in TABLE 1, metals such as aluminum and copper have a large C1 but low ρ.
A high TCR resistor specification for deviation from nominal resistance may be +/−100 ppm/° C. for the linear temperature coefficient of resistance and +/−10 ppm/C for the quadratic temperature coefficient of resistance. This high TCR resistor tolerance may enable a temperature sensor accuracy of +/−0.01%/Δ° C.
Resistors that meet the requirements for an embedded resistor temperature sensor are illustrated in
In
Tungsten resistors with a variety of resistor structures may be formed simultaneously with the formation of tungsten contact plugs. Formation of examples of these tungsten resistor structures is illustrated in
In
In
In resistor structure 154, (
Resistor structure 152 is formed in a resistor trench between two polysilicon leads over isolation dielectric 22. Sidewall dielectric prevents the tungsten 136 from shorting to the polysilicon leads. The width and therefore the resistance of resistor 152 are largely independent of the exposure of the contact photo pattern and also upon the amount of contact over etch. The depth of resistor 152 depends upon how far down into the isolation dielectric the resistor trench is etched during contact over etch.
In
In
Resistor structure 148 is formed over active area to minimize resistor height variation due to contact over etch and is formed between polysilicon leads to minimize variation in width of the resistor due to contact pattern exposure and contact over etch.
Resistor structures 156 and 158 are similar to resistor structures 146 and 148 except that they are formed over an isolated p-well 34 instead of over an nwell. A resistor may be formed on a Schottky diode on n-type or on p-type semiconductor material as long as the Schottky diode may be reverse biased into high resistance preventing underlying semiconductor material from shorting the resistor.
A process for forming resistors in an integrated circuit simultaneously with forming tungsten contact plugs is described in
Referring now to
In
Pwell photoresist pattern 30 is removed and a transistor gate dielectric and a layer of polysilicon 42 are deposited on the integrated circuit wafer as shown in
Referring now to
In
In
Referring now to
Silicide layer 96 is then formed on the gates 60 and 62, source and drains 72 and 80, of the NMOS 142 and PMOS 144 transistors, on the polysilicon pairs 66 not covered silicide block dielectric layer 90, and on the lightly doped nwell 26 and isolated pwell 34 regions forming Schottky diodes where resistors 146, 148, 156, and 158 are to be formed. Because source and drain extension dopants and source and drain dopants are blocked from the wells, 26 and 34 where the resistors are to be formed, these regions remain lightly doped. Silicide forms a Schottky junction to these lightly doped regions. The Schottky diode may be reverse biased into a very high resistance state. Resistors 146, 148, 156, and 158 may be formed on reverse biased Schottky diodes without shorting to the underlying wells 26 and 34. Because the selectivity of contact etch to silicide is very high, the height of resistors formed on silicided active regions in wells 26 and 34 is well controlled.
Contact etch stop layers 100 and 101 and premetal dielectric (PMD) layer 108 are formed on the integrated circuit as shown in
The polysilicon leads in the polysilicon lead pairs are spaced closer together in
As shown in the top down view of the integrated circuit of in
The cross-section shown in
Intermetal dielectric layer 142 and first layer interconnect 144 are then formed on the integrated circuit. The interconnect 144 may be a metal such as aluminum alloy which is deposited and etched or may be a metal such as copper which is formed in dielectric trenches etched using a damascene process.
Resistor 152 is formed over isolation dielectric 22. Because of low selectivity of STI dielectric to contact etch, the height of resistor 152 depends upon how deep the resistor 152 trench penetrates into the STI dielectric 22 during contact over etch. The height and therefore resistance of the resistor 152 depends upon contact etch. First layer of interconnect geometries 164 and 166 form electrical contact to the heads of resistor 152. The interconnect geometries may overlap the resistor heads as on resistor 148 or may under lap the resistor heads as on resistor 152.
Resistor 154 is formed on a polysilicon platform 135. Silicide is blocked from forming on polysilicon platform 135. The polysilicon is high resistance. The depth of the resistor 154 trench is well controlled since the selectivity of polysilicon to the contact etch is very high. Because the height of the resistor 154 formed on the polysilicon platform 135 is significantly less than the height of the resistor 148 formed over nwell 26 and significantly less than the height of resistor 152 formed over STI dielectric 22, the resistance per unit length of resistor 158 is significantly higher than that of resistors 148 and 152. Because the resistance of resistor 158 is higher than that of resistors 148 and 152, a resistor 158 with equivalent resistance to resistors 148 and 152 may be formed in smaller area.
Resistors formed simultaneously with the formation of tungsten via plugs are illustrated in
As shown in
ILD layer 206 is formed on the integrated circuit over IMD layer 202 and over interconnect geometries 204, 210, and 212. A via photo resist pattern 208 is formed on the integrated circuit with openings to etch via 214 (
As shown in
One or both types of resistors 222 and 224 may be formed in a production integrated circuit. In addition a resistor with one resistor head contacted from above and the other resistor head contacted from below may be formed. The high TCR resistors described above are formed simultaneously with via plugs and without adding additional process steps or additional cost to the integrated circuit manufacturing flow.
Those skilled in the art to which this invention relates will appreciate that many other embodiments and variations are possible within the scope of the claimed invention.
Under 35 U.S.C. §§ 120, this continuation application claims priority to and benefits of U.S. patent application Ser. No. 13/586,672 (TI-69351), filed on Aug. 15, 2012, which also claims priority to U.S. Provisional Application No. 61/523,575, filed Aug. 15, 2011. The entirety of the above reference applications is herein incorporated by reference.
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Number | Date | Country | |
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20160071839 A1 | Mar 2016 | US |
Number | Date | Country | |
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61523575 | Aug 2011 | US |
Number | Date | Country | |
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Parent | 13586672 | Aug 2012 | US |
Child | 14864538 | US |