Acousto-optic Modulators

For small acoustic powers, the diffraction efficiency is proportional to the acoustic power; for higher powers, it saturates. For sufficiently high acoustic power, more than 50% of the optical power can be diffracted – in extreme cases, even more than 95% diffraction efficiency is achieved. High diffraction efficiencies are easier to achieve for short optical wavelengths.

The contrast ratio is defined as the ratio of maximum and minimum transmitted power. The latter may be limited by scattering. For the diffracted beam, the contrast ratio can be quite high (order of 1000), but the maximum transmission is then limited by the diffraction efficiency. A high maximum throughput is obtained for the non-diffracted (zero-order) beam, but in that case the contrast ratio is much lower.

The acoustic wave may be absorbed at the other end of the crystal (which is often cut at some angle to avoid standing-wave effects due to residual reflections). Such a traveling-wave geometry makes it possible to achieve a broad modulation bandwidth of many megahertz; it is ultimately limited by the single-pass propagation time of the acoustic wave through the region of the light beam. Other devices are resonant for the sound wave, exploiting the strong reflection of the acoustic wave at the other end of the crystal. The resonant enhancement can greatly increase the modulation strength (or decrease the required acoustic power), but reduces the modulation bandwidth.

Common materials for acousto-optic devices are tellurium dioxide (TeO₂), crystalline quartz, and fused silica; one also uses chalcogenide glasses (often flint glasses), indium phosphide and germanium – the latter two for infrared applications. For high frequency signal processing devices, materials like lithium niobate and gallium phosphide can be used. There are manifold criteria for the choice of the material, including the elasto-optic coefficients (there are actually different acousto-optic figure-of-merit values), the acoustic attenuation coefficient, the sound velocity, the transparency range, the optical damage threshold, and the required size.

Although most AOMs are bulk devices, there are also compact fiber-coupled versions (fiber-pigtailed AOMs). Light from the input fiber is first collimated, then sent through the modulator crystal and finally focused into the output fiber. The insertion loss is typically around 3 dB.

There are also integrated-optical devices containing one or more acousto-optic modulators on a chip. This is possible, e.g., with integrated optics on lithium niobate (LiNbO₃), as this material is piezoelectric, so that a surface-acoustic wave can be generated via metallic electrodes on the chip surface. Such devices can be used in many ways, e.g. as tunable optical filters or optical switches.

If an acousto-optic modulator is used as an amplitude modulator or an active Q-switch, the used electronic driver is usually a device operating with a fixed modulation frequency but a variable amplitude. The amplitude is often controlled with a analog input voltage or with a digital input signal (for on/off modulation).

The required RF drive power is substantial (sometimes several watts), and particularly for long optical wavelengths often not high enough to achieve a high diffraction efficiency.

Various aspects can be essential for the selection of an acousto-optic modulator for some application:

• The material should have a high transparency at the relevant wavelengths, and parasitic reflections should be minimized e.g. with anti-reflection coatings.
• In many cases, a high diffraction efficiency is important. For example, this matters when using the AOM as a Q switch in a high-gain laser, and even more so for cavity dumping. The required RF power influences both the electric power demands and cooling issues. It is lower for acousto-optic materials with high elasto-optic coefficients.
• Depending on the device design, the diffraction efficiency can be polarization dependent.
• For intracavity laser applications like Q switching and mode locking, and particularly for high-power applications, AOMs with low parasitic absorption are required, possibly also a high damage threshold for laser pulses. Large aperture are often required for high power levels. For applications concerning ultrashort pulses, chromatic dispersion and optical nonlinearities can be important.
• The input aperture size limited the usable beam radius. AOMs for large beams are more expensive (because more of the expensive crystal material is required), and tentatively they are slower (see below) and need more RF power.
• The switching time is critical for some applications (e.g. Q switching and particularly cavity dumping). It is limited by the finite velocity of sound in the acousto-optic medium. This implies that an AOM switching a laser beam with large diameter is necessarily slow. One may operate such a modulator with a focused laser beam of reduced diameter, but the diffraction efficiency may decrease due to the increased beam divergence.

Note that the diffraction efficiency depends nonlinearly on the acoustic drive power. For an effectively linear response, a suitable pre-distortion of the drive signal is required.

For acousto-optic frequency shifters and acousto-optic deflectors, other aspects can come into play. For example, a low velocity of sound is advantageous for achieving a wide range of beam angles.

Due to various trade-offs, quite different materials and operation parameters are used in different applications. For example, the materials with highest diffraction efficiencies are not those with the highest optical damage threshold. A large mode area can increase the power handling capability, but requires the use of a larger crystal or glass piece and a higher drive power, and also increases the switching time, which is limited by the acoustic transit time. For fast acousto-optic beam scanners, a large mode area is required for achieving a high pixel resolution, whereas a smaller mode area is required for a high scanning speed.

Acousto-optic modulators find many applications:

• They are used for Q switching of solid-state lasers. The AOM, called Q switch, then serves to block the laser resonator before the pulse is generated. In most cases, the zero-order (not diffracted) beam is used under lasing conditions, and the AOM is turned on when lasing should be prohibited. This requires that the caused diffraction losses (possibly for two passes per resonator round trip) are higher than the laser gain. For more details, see the article on acousto-optic Q switches.
• AOMs can also be used for cavity dumping of solid-state lasers, generating either nanosecond or ultrashort pulses. In the latter case, the speed of an AOM is sufficient only in the case of a relatively long laser resonator; an electro-optic modulator may otherwise be required.
• Active mode locking is often performed with an AOM for modulating the resonator losses at the round-trip frequency or a multiple thereof.
• An AOM can be used as a pulse picker for reducing the pulse repetition rate of a pulse train, e.g. in order to allow for subsequent amplification of pulses to high pulse energies.
• In laser printers and other devices, an AOM can be used for modulating the power of a laser beam. The modulation may be continuous or digital (on/off).
• In a noise eater device, the diffraction losses may be controlled with a feedback circuit such that the transmitted power has induced intensity noise.
• AOMs can be used as external modulators in certain laser communications systems.

Your question or comment:

Spam check:

  (Please enter the sum of thirteen and three in the form of digits!)

By submitting the information, you give your consent to the potential publication of your inputs on our website according to our rules. (If you later retract your consent, we will delete those inputs.) As your inputs are first reviewed by the author, they may be published with some delay.