Photonica

Threshold current

The drive current at which a semiconductor laser transitions from spontaneous to stimulated emission. Below threshold, the device emits as an LED; above threshold, output power scales nearly linearly with current.

The threshold current IthI_\text{th} marks the operating point at which optical gain in the laser cavity equals total cavity loss. Below threshold, photon density is set by spontaneous emission and the LIV curve exhibits weak superlinear dependence on current. Above threshold, stimulated emission dominates and output power scales nearly linearly with current.

Several extraction methods are in standard use and produce numerically different IthI_\text{th} values from the same LIV curve:

  • Two-segment linear fit. Independent linear fits to the LIV above and below threshold; the intersection is IthI_\text{th}. Most common method for clean LIV data.
  • Second-derivative peak. IthI_\text{th} taken at the maximum of d2P/dI2d^2 P / d I^2. Mathematically well-defined but sensitive to noise.
  • First-derivative inflection. IthI_\text{th} taken at the inflection point of lnP\ln P versus II.
  • Fixed power threshold. IthI_\text{th} taken at the current that produces a fixed reference output power. Simplest method; device-dependent.

The extraction method must be held constant across any dataset where IthI_\text{th} values are compared.

Typical values:

DeviceWavelengthIthI_\text{th}
Telecom DFB laser1310 / 1550 nm5–20 mA
9xx nm pump diode (high power)940–980 nm100 mA – 1 A
VCSEL850 nm0.5–5 mA
Quantum cascade laser4–10 μm100 mA – 2 A (pulsed)