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Linewidth Enhancement Factor

Definition: a parameter quantifying the amplitude–phase coupling in a laser

Alternative term: Henry factor

Categories: laser devices and laser physicslaser devices and laser physics, physical foundationsphysical foundations

Units: (dimensionless)

Formula symbol: <$\alpha$>


Cite the article using its DOI: https://doi.org/10.61835/2c8

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Any free-running (not stabilized) single-frequency laser has a certain finite linewidth, which is essentially due to noise from spontaneous emission into the resonator modes. For simple cases, that fundamental limit for the linewidth was calculated by Schawlow and Townes even before the first laser was experimentally demonstrated. Whereas this limit was later shown to be closely approached by a number of solid-state lasers, significantly higher linewidth values were measured for semiconductor lasers (laser diodes) even when the influence of technical noise was very low. It was then later found by Charles H. Henry [1] that the increased linewidths result from a coupling between intensity and phase noise, caused by a dependence of the refractive index on the carrier density in the semiconductor. Henry introduced the linewidth enhancement factor <$\alpha$> (also called Henry factor or alpha factor) to quantify that amplitude–phase coupling mechanism; essentially, <$\alpha$> is a proportionality factor relating phase changes to changes of the gain:

$$\Delta \varphi = \frac{\alpha }{2} \cdot \Delta g$$

(The factor 1/2 serves to convert the change of power gain <$\Delta g$> to the change of amplitude gain.) Henry then found that the linewidth of the laser should be increased by the factor <$(1 + \alpha^2)$>, which turned out to be in reasonable agreement with experimental data.

Note that one may expect the linewidth enhancement factor to be the factor by which the linewidth is enhanced, but that factor is actually <$(1 + \alpha^2)$>.

Linewidth Enhancement Factor for Different Lasers

It is possible to calculate the <$\alpha$> factor of a semiconductor for a given carrier density from a band structure model, although this is not easy. For typical quantum wells, one often obtains values of the order to 2 to 5.

Quantum dot lasers are different from other semiconductor lasers (e.g. based on quantum wells) in terms of <$\alpha$> factor. Simple models suggest a very small <$\alpha$> factor, but different values are obtained experimentally – sometimes even negative values. This can be understood by taking into account the carriers not only of the quantum dots themselves, but also in the wetting layer. There are also various other subtle effects [6, 7].

Four-level solid-state lasers usually have a very small linewidth enhancement factor when operated near their gain maximum. Larger values are obtained when forcing operation at other wavelengths and for quasi-three-level laser gain media.

Additional Effects

Apart from increasing the laser linewidth in continuous-wave operation, a non-zero linewidth enhancement factor also causes a chirp when e.g. a laser is power modulated, or when an intense optical pulse passes an amplifier which it saturates.

Surprisingly, the amplitude–phase coupling related to the linewidth enhancement factor can under certain circumstances (with frequency-dependent loss) be used to reduce the linewidth even below the Schawlow–Townes limit [4, 5].

Measuring Linewidth Enhancement Factors

There are different methods for the measurement of the linewidth enhancement factor of a laser or a laser gain medium. Most common are those based on recording the optical spectrum of ASE for different excitation levels, on measuring amplitude and phase modulation caused by a modulated drive current, pump–probe measurements, and linewidth measurements.

More to Learn

Encyclopedia articles:


[1]C. H. Henry, “Theory of the linewidth of semiconductor lasers”, IEEE J. Quantum Electron. 18 (2), 259 (1982); https://doi.org/10.1109/JQE.1982.1071522
[2]C. H. Henry, “Theory of spontaneous emission noise in open resonators and its application to lasers and optical amplifiers”, J. Lightwave Technol. LT-4, 288 (1986)
[3]M. Osinski and J. Buus, “Linewidth broadening factor in semiconductor lasers – an overview”, IEEE J. Quantum Electron. 23 (1), 9 (1987); https://doi.org/10.1109/JQE.1987.1073204
[4]A. Yariv et al., “Self-quenching of fundamental phase and amplitude noise in semiconductor lasers with dispersive loss”, Opt. Lett. 15 (23), 1359 (1990); https://doi.org/10.1364/OL.15.001359
[5]Y. Shevy and H. Deng, “Frequency-stable and ultranarrow-linewidth semiconductor laser locked directly to an atom-cesium transition”, Opt. Lett. 23 (6), 472 (1998); https://doi.org/10.1364/OL.23.000472
[6]S. Melnik et al., “The linewidth enhancement factor <$\alpha$> of quantum dot semiconductor lasers”, Opt. Express 14 (7), 2950 (2006); https://doi.org/10.1364/OE.14.002950
[7]J. Molina Vázquez et al., “Linewidth enhancement factor of quantum-dot optical amplifiers”, IEEE J. Quantum Electron. 42 (10), 986 (2006); https://doi.org/10.1109/JQE.2006.881022
[8]T. Fordell and A. M. Lindberg, “Experiments on the linewidth-enhancement factor for a vertical-cavity surface-emitting laser”, IEEE J. Quantum Electron. 43 (1), 6 (2007); https://doi.org/10.1109/JQE.2006.884583
[9]R. P. Green et al., “Linewidth enhancement factor of terahertz quantum cascade lasers”, Appl. Phys. Lett. 92 (7), 071106 (2008); https://doi.org/10.1063/1.2883950
[10]S. Gerhard et al., “Frequency-dependent linewidth enhancement factor of quantum-dot lasers”, IEEE Photon. Technol. Lett. 20 (20), 1736 (2008); https://doi.org/10.1109/LPT.2008.2004675
[11]R. Pagano et al., “Above threshold estimation of alpha (Henry) parameter in stripe lasers using near- and far-field intensity measurements”, IEEE J. Quantum Electron. 47 (4), 439 (2011); https://doi.org/10.1109/JQE.2010.2091255
[12]A. Consoli et al., “Self-validating technique for the measurement of the linewidth enhancement factor in semiconductor lasers”, Opt. Express 20 (5), 4979 (2012); https://doi.org/10.1364/OE.20.004979
[13]B. Sinquin and M. Romanelli, “Determination of the linewidth enhancement factor of semiconductor lasers by complete optical field reconstruction”, Opt. Lett. 48 (4), 863 (2023); https://doi.org/10.1364/OL.483776

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Questions and Comments from Users


I would expect that the alpha factor to contribute only at low frequencies, with a cutoff frequency around the relaxation oscillation frequency. In such case, wouldn't the high frequency white noise level be the same as the ideal Schawlow–Townes limit?

The author's answer:

Yes, the linewidth enhancement factor is relevant only in frequency regions where the carrier density oscillates substantially.

For the linewidth, the low-frequency phase noise is relevant, so for that the factor fully counts, while very high-frequency noise is not affected.

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