Self-mixing or back-injection laser interferometry is an interferometric technique in which a part of the light reflected by a vibrating target is reflected into the laser cavity, causing a modulation both in amplitude and in frequency of the emitted optical beam. In this way, the laser becomes sensitive to the distance traveled by the reflected beam thus becoming a distance, speed or vibration sensor. The advantage compared to a traditional measurement system is a lower cost thanks to the absence of collimation optics and external photodiodes.
Background After the development of the classic external interferometric configurations (Michelson and Mach-Zehnder interferometers) which consisted of lenses, beam splitter, mirrors, and corner cube, the possibility of creating a much simpler and more compact system was investigated. Starting in the 1980s, this new configuration known as retro-injection or self-mixing was explored and applications based on the retro-injection effect in commercial laser diodes appeared in the scientific literature.
In this type of interferometric configuration the fact is exploited that a small fraction of the light emitted by a laser, after having been reflected by a vibrating target, is re-injected into the laser cavity, where a sort of coherent radiation detection is realized: the power emitted by the laser is in fact modulated both in amplitude (AM) and in frequency (FM), generating a fringes interferometric signal. This signal is a periodic function of the phase Φ {\displaystyle \Phi } of the back-scattered field, according to the following relation:
Φ = 2 k s 0 = 2 2 π λ s 0 {\displaystyle \Phi =2ks_{0}=2{\frac {2\pi }{\lambda }}s_{0}}
where k {\displaystyle k} is the wave number and s 0 {\displaystyle s_{0}} is the physical distance between the laser source and the moving target. If a phase shift of an entire period is imposed, that is Δ Φ {\displaystyle \Delta \Phi } = 2 π {\displaystyle 2\pi } , we get Δ s {\displaystyle \Delta {\text{s}}} = λ 2 {\displaystyle {\tfrac {\lambda }{2}}} . So, if we can see an entire fringe on the oscilloscope screen, we can say that the phase shift due to the movement of the obstacle is 2 π {\displaystyle 2\pi } , that is λ {\displaystyle \lambda } / 2 {\displaystyle 2} . In this way, by counting the number of visible fringes, it is possible to calculate both the magnitude and the direction of the displacement with a resolution of λ {\displaystyle \lambda } / 2 {\displaystyle 2} . This was first demonstrated in 1978 by Silvano Donati. Compared to the classic interferometers that refer to Michelson one, this new type of interferometer is considerably simpler, since the laser beam already has all the information related to the signal that is no longer generated by the beating of two beams coming from optical path difference. Therefore, the reference optical path is no longer necessary for measurement and relies only on the interaction between the electric field that travels to the target and the electric field inside the laser cavity.
AM self-mixing laser interferometry
The trend of the amplitude modulated interferometric signal is shown, generated by a vibrating target (such as an audio speaker) powered through a sinusoidal voltage. For the properties of self-mixing laser interferometry, whenever the vibration of a vibrating target is such that its displacement is greater than or equal to λ 0 {\displaystyle \lambda _{0}} / 2 {\displaystyle 2} (where λ 0 {\displaystyle \lambda _{0}} is wavelength of employed laser), an interferometric fringe is created. However, with regard to amplitude modulation of the interferometric signal there are basically two consequences:
through the simple counting of the number of fringes generated, it is possible to retrieve the displacement of the target instruments that use only the amplitude modulation (AM) are not very sensitive The amplitude modulation (AM) of the emitted optical power is detected by the photodiode of monitor (PD) inside the laser package. In this particular interferometric technique the resolution of the displacement and vibration measurement is limited by a low signal-to-noise ratio or SNR, such that the system is only suitable for slow and wide measurements .
FM self-mixing laser interferometry
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