Electro-optic modulator

Phase modulation (PM) is a modulation pattern that encodes information as variations in the instantaneous phase of a carrier wave. The phase of a carrier signal is modulated to follow the changing voltage level (amplitude) of modulation signal. The peak amplitude and frequency of the carrier signal remain constant, but as the amplitude of the information signal changes, the phase of the carrier changes correspondingly. The analysis and the final result (modulated signal) are similar to those of frequency modulation. A very common application of EOMs is for creating sidebands in a monochromatic laser beam. To see how this works, first imagine that the strength of a laser beam with frequency \omega entering the EOM is given by :Ae^{i\omega t}. Now suppose we apply a sinusoidally varying potential voltage to the EOM with frequency \Omega and small amplitude \beta. This adds a time dependent phase to the above expression, :Ae^{i\omega t + i\beta\sin(\Omega t)}. Since \beta is small, we can use the Taylor expansion for the exponential :Ae^{i\omega t}\left( 1+i\beta\sin(\Omega t)\right) , to which we apply a simple identity for sine, :Ae^{i\omega t}\left( 1 + \frac{\beta}{2}\left(e^{i\Omega t} - e^{-i\Omega t}\right)\right) = A\left( e^{i\omega t}+\frac{\beta}{2}e^{i(\omega+\Omega) t}-\frac{\beta}{2}e^{i(\omega-\Omega) t}\right) . This expression we interpret to mean that we have the original carrier signal plus two small sidebands, one at \omega+\Omega and another at \omega-\Omega. Notice however that we only used the first term in the Taylor expansion – in truth there are an infinite number of sidebands. There is a useful identity involving Bessel functions called the Jacobi–Anger expansion which can be used to derive :Ae^{i\omega t + i\beta\sin(\Omega t)} = Ae^{i\omega t}\left( J_0(\beta) + \sum_{k=1}^\infty J_k(\beta)e^{ik\Omega t} + \sum_{k=1}^\infty (-1)^k J_k(\beta)e^{-ik\Omega t}\right) , which gives the amplitudes of all the sidebands. Notice that if one modulates the amplitude instead of the phase, one gets only the first set of sidebands, :\left( 1 + \beta\sin(\Omega t)\right) Ae^{i\omega t} = Ae^{i\omega t} + \frac{A\beta}{2i}\left( e^{i(\omega+\Omega) t} - e^{i(\omega-\Omega)t} \right) . ==Amplitude modulation==

A phase modulating EOM can also be used as an amplitude modulator by using a Mach–Zehnder interferometer. This alternative technique is often used in integrated optics where the requirements of phase stability is more easily achieved. The beam splitter divides the laser light into two paths, one of which has a phase modulator as described above. The beams are then recombined. Changing the electric field on the phase modulating path will then determine whether the two beams interfere constructively or destructively at the output, and thereby control the amplitude or intensity of the exiting light. This device is called a Mach–Zehnder modulator (MZM) and it is widely used as intensity modulator (IM) in fiber-optic communications. ==Polarization modulation==

Depending on the type and orientation of the nonlinear crystal, and on the direction of the applied electric field, the phase delay can depend on the polarization direction. A Pockels cell can thus be seen as a voltage-controlled waveplate, and it can be used for modulating the polarization state. For a linear input polarization (often oriented at 45° to the crystal axis), the output polarization will in general be elliptical, rather than simply a linear polarization state with a rotated direction. Polarization modulation in electro–optic crystals can also be used as a technique for time-resolved measurement of unknown electric fields. Compared to conventional techniques using conductive field probes and cabling for signal transport to read-out systems, electro–optical measurement is inherently noise resistant as signals are carried by fiber-optics, preventing distortion of the signal by electrical noise sources. The polarization change measured by such techniques is linearly dependent on the electric field applied to the crystal, hence providing absolute measurements of the field, without the need for numerical integration of voltage traces, as is the case for conductive probes sensitive to the time-derivative of the electric field. ==EOM technologies==

EOMs can be based on many operating principles and platforms. One can divide the EOMs in two categories – phase and amplitude modulation. In the following some prominent approaches in Silicon photonics are presented. Operating principles for phase modulation are the plasma dispersion effect, pockels effect, interband transitions, and carrier accumulation/depletion+Franz-Keldysh effect. For the amplitude modulation some operating principles are the Franz–Keldysh effect, quantum-confined Stark effect, and electrical gating. The plasma dispersion effect can be based on carrier injection, depletion, or accumulation. The most established Pockels type modulators are based on the lithium niobate on silicon platform. In recent years, other platforms were introduced, such as BTO on silicon, silicon polymer hybrid, silicon organic hybrids, plasmonics and thin-film lithium niobate. Interband transition rely on 2D materials and the carrier accumulation/depletion+Franz–Keldysh is based on a III-V platform. The Franz–Keldysh effect is used in electro-absorption modulators which are semiconductor devices. It describes a change in the absorption spectrum due to a shift in the band gap edge when an electric field is present. They are often built on a silicon–germanium platform. Modulators running on the quantum confined stark effect can rely on a III-V platform or on Ge-Si-Ge quantum wells. Electrical gating is built on a 2D material platform. ==See also==