LDMOS Drift Resistance
Ohmic drift-region resistance of an LDMOS from effective resistivity and a rectangular current path.
Description
Ohmic drift-region resistance of an LDMOS from effective resistivity and a rectangular current path.
LDMOS Drift Resistance is a focused tool for the following task. Ohmic drift-region resistance of an LDMOS from effective resistivity and a rectangular current path. It reports Drift Ohms from the values you provide rather than inventing measurements, coefficients, or professional judgment that are not part of the input.
When to use LDMOS Drift Resistance
Use this semiconductor calculation for first-order device, material, fabrication, interconnect, packaging, or reliability estimates when every coefficient and unit convention is known.
- Resistivity Ohm Meters (Ω·m)
- Required number in Ω·m.
- Drift Length Meters (m)
- Required number in m.
- Path Width Meters (m)
- Required number in m.
- Path Thickness Meters (m)
- Required number in m.
The cited overview of Semiconductor device supplies background for the terminology and domain context used by this tool.1
How LDMOS Drift Resistance works
Ohmic drift-region resistance of an LDMOS from effective resistivity and a rectangular current path. Inputs are interpreted exactly in the displayed units and the calculation returns the following fields without presentation rounding.
- Drift Ohms (Ω)
- Returned number in Ω.
Limitations and assumptions
- Material composition, geometry, process history, temperature, electric field, bias, interfaces, parasitics, and fitted parameter ranges can invalidate a compact semiconductor model.
- Resistivity Ohm Meters must be at least 0.
- Drift Length Meters must be at least 0.
- Path Width Meters must be at least 0.
- Path Thickness Meters must be at least 0.
- Use finite inputs in the displayed units, preserve source measurements and assumptions, and independently verify consequential decisions.
Alternative or Complementary approaches
Compare the estimate with measured process data, current device documentation, and a higher-fidelity circuit, field, thermal, quantum, or TCAD model when the decision requires it.
References
-
Semiconductor device — Wikipedia contributors
Similar or alternative tools
- BJT Common-Emitter Current Gain Calculator
Convert the common-base current gain (alpha) to the common-emitter current gain (beta) via beta=alpha/(1-alpha) with alpha in (0,1) exclusive, dimensionless. Full double precision without premature rounding; handles near-1 cancellation by checking 1-alpha finite and non-zero and beta finite, reporting numeric_overflow for extreme alpha. Ideal transistor relation neglecting recombination and series resistance; invalid for alpha<=0 or >=1.
- Transfer Length Calculator
Convert specific contact resistivity and sheet resistance into the contact transfer length. Formula: Lt [µm] = 1e4 · sqrt(ρc [Ω·cm²] / Rsh [Ω/sq]). Inputs: ρc > 0 Ω·cm², Rsh > 0 Ω/sq. Output: Lt > 0 µm. Assumes uniform sheet resistance under the contact and the transmission-line model (long contact, negligible metal resistance).
- Diode Ideality Factor Calculator
Extract the diode ideality factor n from two forward-bias points on the exponential Shockley relation. Formula: n = (V2 - V1) / (Vt·ln(I2/I1)), where thermal voltage Vt = k·T/q (k=1.380649e-23 J/K, q=1.602176634e-19 C). Inputs: I1>0 mA, I2>0 mA and I1≠I2, V1 and V2 finite V, T>0 K (default 300 K). Output: n>0 (physical diode typically 1 ≤ n ≤ 2; n=1 ideal diffusion, n≈2 recombination/generation; n outside 1-2 indicates series resistance, high injection, or measurement error). Assumes forward exponential region, negligible series resistance, and constant temperature.