acousto-optic modulators (original) (raw)

Acronym: AOM

Definition: optical modulators based on the acousto-optic effect

Category: photonic devices

• optical modulators
  • acousto-optic modulators
    * acousto-optic deflectors
    * acousto-optic frequency shifters
    * acousto-optic Q-switches
    * acousto-optic tunable filters
  • electro-optic modulators
  • Pockels cells
  • electroabsorption modulators
  • liquid crystal modulators
  • intensity modulators
  • phase modulators

Related: Q-switchesoptical modulatorsacousto-optic Q-switchesacousto-optic deflectorsintensity modulatorspulse pickerselectro-optic modulatorsQ-switchingcavity dumpingactive mode locking

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Contents

What Are Acousto-optic Modulators?

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).

Operation Principle

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 in optical frequency is irrelevant.

Acousto-optic Modulation in Gases

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 acousto-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:

• The modulation frequency should be as high as possible to achieve a high enough deflection angle. Due to increasing ultrasound absorption in air for increasing frequency, the ultrasound frequency is limited to the order of 1 MHz — about two orders of magnitude less than is common with solid-state modulators. That results in a rather small deflection angle. Nevertheless, for very large beam diameters, where the beam divergence can be rather small, the deflection angle can be sufficient to fully separate the diffracted beam.
• The acoustic wave must be highly intense to achieve a high diffraction efficiency. With a very high-power driver, roughly 50% efficiency is achievable [7].

Details of AOMs

Diffraction Efficiency and Contrast Ratio

The diffraction efficiency for 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 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 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.

Polarization Dependence

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.

Traveling-wave and Resonant Designs

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.

Used Acousto-optic Materials

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.

Fiber-coupled and Integrated-optical AOMs

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.

Important Properties of Acousto-optic Modulators

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 apertures are often required for high power levels. For applications concerning ultrashort pulses, chromatic dispersion and optical nonlinearities can be important.
• The input aperture size limits the usable beam radius. AOMs for large beams are more expensive (because more of the expensive crystal material is required), and typically 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.

RF Drivers for AOMs

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 an 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.

See also the article on acousto-optic modulator drivers.

Applications of AOMs

Acousto-optic modulators find many applications:

• They are used for Q-switching of solid-state lasers. The AOM, here more specifically called an acousto-optic 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. 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 reduced intensity noise.
• AOMs can be used as external modulators in certain laser communications systems.

Other Acousto-optic Devices

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:

• Acousto-optic frequency shifters can be used for shifting the optical frequency, e.g. in optical frequency metrology.
• Acousto-optic deflectors are used for electrically controllable deflection of laser beams.
• Acousto-optic tunable filters are tunable bandpass filters, e.g. for wavelength tuning of lasers.

Frequently Asked Questions

This FAQ section was generated with AI based on the article content and has been reviewed by the article’s author (RP).

What is an acousto-optic modulator (AOM)?

An acousto-optic modulator (AOM) is a device that uses the acousto-optic effect to control the power of a laser beam.

How does an acousto-optic modulator work?

An RF driver sends an electrical signal to a piezoelectric transducer attached to a transparent crystal. The transducer generates a high-frequency sound wave, creating a traveling refractive index grating in the crystal. An incident laser beam diffracts off this grating, allowing its power to be controlled by the applied RF power.

What is the difference between the Bragg and Raman–Nath diffraction regimes?

Most AOMs operate in the Bragg regime, which occurs for a long interaction length and ensures that light is efficiently diffracted into a single order. Conversely, the Raman–Nath regime occurs for short interaction lengths and generates multiple diffraction orders.

What factors determine the diffraction efficiency of an AOM?

The diffraction efficiency depends primarily on the applied RF drive power, with higher power leading to higher efficiency up to a saturation point. It is also influenced by the optical wavelength and beam properties like divergence, which should be minimized for best performance.

What limits the switching time of an AOM?

The switching time is limited by the transit time of the sound wave across the laser beam's diameter. Consequently, modulators for larger beams are inherently slower. Focusing the beam can increase speed but may reduce efficiency due to increased beam divergence.

What are common materials for acousto-optic modulators?

Common materials include tellurium dioxide (TeO2), crystalline quartz, and fused silica. For infrared applications, materials like germanium are used, while lithium niobate is suitable for high-frequency or integrated-optical devices.

What are typical applications of acousto-optic modulators?

Is the optical frequency of light changed by an AOM?

Yes, the diffracted beam's optical frequency is shifted up or down by the frequency of the sound wave. For most intensity modulation applications, however, this slight frequency shift is irrelevant.

Suppliers

Sponsored content: The RP Photonics Buyer's Guide contains 39 suppliers for acousto-optic modulators. Among them:

⚙ hardware

GWU's assortment of acousto-optical components covers all kind of Q-switches, modulators, deflectors and frequency shifters for various applications. The acousto-optical modulators (AOM) can be configured in flexible design, free-space or fiber-coupled and can be equipped with suitable driving electronics.

⚙ hardware

SHIPS TODAY: These fiber-coupled acousto-optic modulators (AOM) are designed to offer an optimal solution for amplitude modulation of laser light in a single mode optical fiber. They are offered for wavelengths between 750 nm and 1750 nm with most models stock. These fiber AOMs are easy to use and allow direct control of the timing, intensity, and temporal shape of the laser output down to a few nanoseconds. A fiber-coupled AOM requires an RF driver. AeroDIODE offers a range of RF drivers configured for either digital input (TTL) or analog input configurations. Additionally, the AeroDIODE TOMBAK pulse picker synchronization tool is offered for complex synchronization applications such as pulse-picking a mode locked laser. NEW: a turn-key pulse picker solution is now also offered which combines the synchronization electronics with the high performances AOMs and associated drivers.

See also our tutorial on fiber-coupled modulators.

⚙ hardware

CSRayzer offers acousto-optic modulators with fast modulation speed, low insertion loss, high extinction ratio, low power consumption, good temperature stability and high performance reliability. The possible wavelength regions are from the visible to the infrared. They have an all-metal structure design, compact and sturdy hermetic packaging structure, and innovative packaging technology to ensure high reliability and temperature stability. CSRayzer provides free space or fiber-coupled versions in a wavelength range from 300 nm to 2000 nm, and frequency range from 35 MHz to 300 MHz. They are suitable e.g. for Q-switched fiber lasers, laser Doppler coherent applications, ultrafast laser frequency pulse pickers, and linear frequency adjustment.

⚙ hardware

New: Double-pass acousto-optic modulator, an all fiber-coupled, polarization-maintaining setup for tunable frequency shifting and laser light intensity modulation. The modular muticube™ system by Schäfter+Kirchhoff allows integration of various acousto-optical modulator setups, accommodating different laser wavelengths and RF frequency ranges. Complete fiber port clusters with integrated modulators can be built, and combined with monitor diodes, shutters, and beam splitters. More information.

⚙ hardware

Our acousto-optic modulators are optimized for low scatter and high laser damage threshold. Rise time, modulation rate, beam diameter, and power handling needs of the application need to be understood in order to identify the best acousto-optic modulator and RF driver solution.

We also offer fiber-coupled acousto-optic modulators.

Bibliography

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