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Summary: This in-depth article on acousto-optic modulators (AOMs) explains
An acousto-optic modulator (AOM) is a device which can be used for controlling the transmitted power of a laser beam with an electrical drive signal. It is based on the acousto-optic effect, i.e. the modification of the refractive index of some crystal or glass material by the oscillating mechanical strain of a sound wave (photoelastic effect).
Usually, an AOM is understood to be an intensity modulator; other acousto-optic devices are suitable for shifting the optical frequency (' acousto-optic frequency shifter) or the spatial direction (acousto-optic deflectors).
The key element of an AOM is a transparent crystal (or piece of glass) through which the light propagates. A piezoelectric transducer attached to the crystal obtains a strong oscillating electrical signal from an RF driver (often via an impedance matching device). The piezo transducer excites a sound wave with a frequency of the order of 100 MHz and with an acoustic wavelength which is typically between 10 μm and 100 μm and an acoustic power e.g. of the order of 1 W to 10 W. The intense sound wave generates a traveling strain wave in the material. Through the photo-elastic effect, that leads to a traveling refractive index grating, at which light can experience Bragg diffraction; therefore, AOMs are sometimes called Bragg cells.
Figure 1:
Schematic setup of a non-resonant acousto-optic modulator.A transducer generates a sound wave, at which a light beam is partially diffracted. The diffraction angle is exaggerated; it is normally only of the order of 1°.
For a very short interaction length in the modulator, one would operate in the Raman'Nath regime, where multiple diffraction orders are obtained. However, most AOMs operate in the Bragg regime, where there is a substantial diffraction efficiency for the first diffraction order and hardly any diffraction into other orders.
The optical frequency of the diffracted beam is increased or decreased by the frequency of the sound wave (depending on the propagation direction of the acoustic wave relative to the beam) and propagates in a slightly different direction. (The change in direction is smaller than shown in Figure 1 because the wavenumber of the sound wave is very small compared with that of the light beam.) The frequency and direction of the diffracted beam depend on the frequency of the sound wave, whereas the acoustic power is the control for the diffracted optical power. For most applications, the slight change of optical frequency is irrelevant.
The diffraction process may or may not be polarization-dependent, depending on the device designs (use of longitudinal or shear waves, isotropic or anisotropic material etc.). Further, the output polarization is the same as the input polarization for devices with an isotropic interaction, while for anisotropic modulators it is different, and these devices then work only for the correct input polarization. For AOMs, the use of longitudinal (compression) waves is most common, where the diffraction efficiency is strongly polarization-dependent. Polarization-independent operation can be obtained when using acoustic shear waves with the acoustic movement in the direction of the laser beam. As shear waves are typically slower, one then also obtains a larger Bragg angle, i.e., a better separation of the diffracted beam, which may be advantageous.
Typically, an AOM is placed in a small box, having two holes or optical windows on opposite sides for the laser beam going through, and a connector for the RF driver. Sometimes that box is placed on a rotating table for precise rotational adjustment.
The diffraction efficiency for a a given diffraction order (often the first order) is defined as the ratio of diffracted power to incident power.
The generated acoustic power is proportional to the RF drive power, which is proportional to the square of the RF amplitude. For small acoustic powers, the diffraction efficiency is proportional to the acoustic power; for higher powers, it saturates. (Obviously, it could not get larger than unity for sufficiently high drive power.) 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 ), 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 diffraction efficiency also depends on properties of the light beam. In particular, it may be deteriorated if the beam has a substantial beam divergence. For that, it should not be focused more strongly than necessary. Of course, the beam should also be well aligned, and its profile should not be clipped anywhere.
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 strongly 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 that 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.
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Various aspects can be essential for the selection of an acousto-optic modulator for some application:
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:
For light beams with extremely high peak power, the damage threshold and optical nonlinearities of solid-state media are a severely limiting factor. Therefore, it has been demonstrated that acouso-optic interactions can also be exploited in far more robust gases such as ambient air [7]. Here, an ultrasound wave in air with the following properties is required:
Other acousto-optic devices are based on the same kind of setup, but not used for power modulation, and therefore normally not called acousto-optic modulators:
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This module is a high-power RF driver, designed to drive a Q-Switch.
The driver has two digital modulation inputs: fixed and variable. These controls allow the customer to issue a pulse command of fixed pulse width, the duration determined by the driver's pulse width control, settable by the customer, or issue a variable pulse command, the duration determined by the input signal's pulse width.
The output power is controlled by the analog input, where the mode of operation is defined by ZZZ = A05 normal analog mode, or R05 analog switched to full RF mode or a triggered RF Ramp Down mode where ZZZ = FPS first pulse suppression mode or PPK pre-pulse kill mode. The choices of Frequency (XX), Output Power (YY), and Power Control (ZZZ) options are "Factory Set" when ordered.
This RF driver requires forced air cooling.
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