Link to Harold

Harold can model the detailed physics of (multi) quantum well structures such as laser diodes or electro-absorption modulators (EAM), but is restricted to simple device structures based on a single uniform cavity.

In contrast PICWave can model complex devices including DFB and tuneable lasers, laser + modulator devices, and all manner of integrated circuits. However it does not have the ability to compute gain/refractive index spectra from a detailed description of the quantum well structure – rather it starts with a set of “material functions” describing e.g. the gain versus carrier density dependence (for lasers/SOAs), or refractive index versus reverse bias voltage (for EAMs).

Harold allows you to do a detailed material simulation (laser or EAM) and import the results into PICWave. This gives you the best of both worlds – a detailed quantum mechanical model of the electronic structure, and a flexible device model. It also has the benefit of allowing the device model to run at high speed since the material functions generated by Harold can be evaluated very quickly. 

PICWave allows you to import detailed material gain models from Harold or other sources. The following information can be generated by Harold and imported into PICWave:

• Epilayer structure
• Gain versus wavelength, carrier density, temperature
• Spontaneous emission spectra vs. carrier density, temperature
• Spontaneous lifetime (including spontaneous emission, Auger) vs. carrier density, temperature
• Two-level carrier model to reproduce carrier capture/escape/transport time
• Carrier mobility and doping levels
• Refractive index and free-carrier absorption vs. carrier density and temperature
• Diffusion coefficient, bandgap and other material parameters

Once they have been exported into PICWave, the gain curves for the hetero-structure need to be fitted in order to be used by the time domain model. This is done in PICWave using a Wide-Band Gain Fitting, which allows you to maintain the accuracy of the fitted curves over a very wide range of wavelength. You can see here in comparison the fitted gain curves obtained with a parabolic fitting, for which the fitting is only valid near the gain peak. 

Please see here for a comparison of the active component (laser diode, SOA, modulators etc.) modelling capabilities of PICWave, Harold, Harold XY and Harold QCSE.