What is MOSFET Threshold Voltage?
The threshold voltage of a MOSFET is the minimum gate-to-source voltage (VGS) required to create a conducting channel between the drain and source terminals. Below this voltage, the MOSFET remains off, and above it, the device allows significant current flow.
In simpler terms, VTH is the voltage level at which an inversion layer forms at the semiconductor-oxide interface, enabling current conduction.
Types of Threshold Voltage
- Enhancement Mode MOSFETs: Require a positive gate voltage (for n-channel) greater than VTH to conduct.
- Depletion Mode MOSFETs: Have a built-in channel and can conduct at zero gate voltage; VTH is typically negative.
Physical Origin of Threshold Voltage
The threshold voltage arises from the need to invert the semiconductor surface beneath the gate oxide. Initially, the semiconductor surface is either p-type or n-type doped. When a gate voltage is applied, it modifies the surface potential, and when it reaches a critical value called the surface potential at threshold, an inversion layer forms.
Key Physical Phenomena:
- Flat-band voltage (VFB): The gate voltage where the energy bands of the semiconductor are flat, meaning no band bending.
- Oxide capacitance (Cox): The capacitance per unit area of the gate oxide layer.
- Bulk charge (QB): The charge required to invert the surface.
Mathematical Expression of Threshold Voltage
The general formula for the threshold voltage VTH is:
Where:
Symbol | Description | Units |
---|---|---|
VFB | Flat-band voltage | Volts (V) |
φF | Fermi potential (bulk potential) | Volts (V) |
q | Elementary charge | 1.602 × 10-19 C |
εs | Semiconductor permittivity | F/cm or F/m |
NA | Acceptor doping concentration | cm-3 |
Cox | Oxide capacitance per unit area | F/cm2 |
Explanation of Terms
- Flat-band Voltage (VFB): This voltage accounts for work function differences between the gate material and the semiconductor and any fixed oxide charges.
- Fermi Potential (φF): Defines the energy difference between intrinsic Fermi level and Fermi level in the doped semiconductor:
φF = (kT/q) × ln(NA / ni)
Where:
- k = Boltzmann constant = 1.38 × 10-23 J/K
- T = Absolute temperature in Kelvin
- ni = Intrinsic carrier concentration
Calculating Oxide Capacitance (Cox)
The oxide capacitance per unit area depends on the oxide thickness (tox) and oxide permittivity (εox):
Where:
- εox = ε0 × κ, with ε0 = permittivity of free space (8.854 × 10-14 F/cm) and κ = dielectric constant of SiO2 (≈ 3.9)
- tox = thickness of the oxide layer in cm
Example Calculation of MOSFET Threshold Voltage
Consider an n-channel MOSFET with the following parameters:
Oxide thickness, tox | 10 nm = 1×10-6 cm |
Acceptor concentration, NA | 1×1017 cm-3 |
Intrinsic carrier concentration, ni | 1.5×1010 cm-3 |
Temperature, T | 300 K |
Work function difference (gate-semiconductor), ΦMS | -0.95 V |
Fixed oxide charge, Qox | 0 |
Permittivity of Si, εs | 11.7 × ε0 = 11.7 × 8.854×10-14 F/cm |
Step 1: Calculate φF
φF = (kT/q) × ln(NA / ni) kT/q ≈ 0.0259 V at 300 K φF = 0.0259 × ln(1×1017 / 1.5×1010) = 0.0259 × ln(6.67×106) = 0.0259 × 15.72 ≈ 0.407 V
Step 2: Calculate oxide capacitance Cox
ε0 = 8.854 × 10-14 F/cm κ = 3.9 for SiO2 εox = κ × ε0 = 3.9 × 8.854×10-14 = 3.453 × 10-13 F/cm tox = 1 × 10-6 cm Cox = εox / tox = 3.453×10-13 / 1×10-6 = 3.453 × 10-7 F/cm²
Step 3: Calculate flat-band voltage VFB
VFB = ΦMS - (Qox / Cox) Given Qox = 0, so VFB = ΦMS = -0.95 V
Step 4: Calculate threshold voltage VTH
VTH = VFB + 2φF + ( sqrt(2 × q × εs × NA × 2φF) ) / Cox Calculate each term: εs = 11.7 × ε0 = 11.7 × 8.854×10-14 = 1.036×10-12 F/cm Calculate the numerator inside the sqrt: 2 × q × εs × NA × 2φF = 2 × 1.602×10-19 × 1.036×10-12 × 1×1017 × 2 × 0.407 = 2 × 1.602×10-19 × 1.036×10-12 × 1×1017 × 0.814 Calculate stepwise: 2 × 1.602×10-19 = 3.204×10-19 3.204×10-19 × 1.036×10-12 = 3.318×10-31 3.318×10-31 × 1×1017 = 3.318×10-14 3.318×10-14 × 0.814 = 2.7×10-14 sqrt(2.7×10-14) ≈ 5.2×10-7 C/cm² Divide by Cox: 5.2×10-7 / 3.453×10-7 = 1.51 V Therefore, VTH = -0.95 + 2(0.407) + 1.51 = -0.95 + 0.814 + 1.51 = 1.374 V
Analysis
The threshold voltage of approximately 1.37 V is typical for an n-channel MOSFET with the given parameters. This voltage must be exceeded by the gate-to-source voltage for the device to switch on effectively.
Note that the threshold voltage depends heavily on:
- Doping concentration (NA): Higher doping increases VTH because more charge is needed to invert the surface.
- Oxide thickness (tox): Thinner oxides increase Cox, reducing the voltage needed to induce charge, thus lowering VTH.
- Flat-band voltage (VFB): Influenced by gate material and oxide charges.
Frequently Asked Questions (FAQs)
1. Why is threshold voltage important in MOSFET operation?
The threshold voltage determines the gate voltage level at which the MOSFET starts to conduct significantly. It defines the switching point and affects the transistor's power consumption and speed.
2. Can threshold voltage vary with temperature?
Yes, VTH generally decreases with increasing temperature due to changes in semiconductor properties and carrier concentration.
3. What is the difference between threshold voltage and flat-band voltage?
Flat-band voltage (VFB) is the voltage at which there is no band bending in the semiconductor surface. Threshold voltage (VTH) is higher and includes the voltage needed to create an inversion layer and overcome bulk charge.
4. How does doping concentration affect VTH?
Increasing doping concentration increases the bulk charge that must be inverted, thereby increasing VTH.
5. What role does oxide thickness play in threshold voltage?
Thinner gate oxides increase gate capacitance (Cox), allowing the channel to form at lower gate voltages, thus reducing threshold voltage.
6. Can threshold voltage be controlled during fabrication?
Yes, by adjusting doping levels, oxide thickness, and gate material work function, manufacturers tailor the threshold voltage for desired device characteristics.
7. What is body effect on threshold voltage?
The threshold voltage increases if the source-to-body voltage is not zero, due to additional depletion charge. This is called the body effect and can be modeled as:
VTH = VTH0 + γ(√|2φF + VSB| - √|2φF|)
where γ is the body effect coefficient and VSB is the source-to-body voltage.
Conclusion
Understanding the MOSFET threshold voltage is essential for designing and analyzing electronic circuits that rely on MOS transistors. This parameter is rooted in semiconductor physics and controlled by material properties and fabrication parameters. By mastering the calculations and influences on VTH, engineers can optimize device performance for applications ranging from microprocessors to power electronics.