ТеО2 Blanks for Acousto-Optical Deflectors

Elent A offers ТеО2 blanks for Acousto-Optical Deflectors (AOD) – ТеО2 crystals cut, oriented, polished and in case of customer request coated.

  • 2,5 mm (110) х 15 mm (1-10) х 9 mm (001)
  • 2,5 mm (110) х 13 mm (1-10) х 19 mm (001)
  • 4,5 mm (110) x 5 mm (1-10) x 30 mm (001)
  • 5 mm (110) х 15,5 mm (1-10) х 8 mm (001)
  • 5 mm (110) х 22 mm (1-10) х 8 mm (001)
  • 6 mm (110) х 23 mm (1-10) х 14 mm (001)
  • 6,5 mm (110) x 8 mm (1-10) x 31 mm (001)
  • 8 mm (110) x 8 mm (1-10) x 20 mm (001)
  • 8 mm (110) x 13,5 mm (1-10) x 31 mm (001)
  • 8 mm (110) x 22,5 mm (1-10) x 36 mm (001)
  • 13 mm (110) x 19 mm (1-10) x 38 mm (001)
ТеО<sub>2</sub> Blanks for Acousto-Optical Deflectors 3

The most commonly used geometry shown in Fig. a is more preferable for the visible region, whereas the geometry displayed in Fig. b is more suitable for the infrared region. Polarization of the incident light is shown in the figures.

ТеО<sub>2</sub> Blanks for Acousto-Optical Deflectors 1

Under angle β beam is normally fall on incoming edge and corresponds to the angle of Bragg interaction with acoustical column. One of the methods to select angle γ – outgoing diffracted beam is parallel to the incoming.

We also offer for our customer pair of blanks (manufactured from one piece or manufacture identical two pieces with all characteristics high repeatability) for 2D deflectors.

But we are not limited by standard sizes, we also can offer ТеО2 crystals produced according to your specific requirements.

For your information please find below some technical information that probably can be useful for you. Also in case of you may need any additional information please don’t hesitate contact us.

AOD primary goal was laser beam deflection to realize a large number of resolvable spots so that it may be used to replace mechanical scanners such as the rotating polygons.
In recent years most of the effort was directed toward Bragg cells for optical signal processing applications.
But finally nowadays AODs have many advantages over electro-mechanical devices, such as fast response time, high precision, and stability of a raster obtained.

AODs provide a simple solid state scanner which eliminates the inherent drawbacks of mechanical scanners due to moving parts such as facet errors and the requirement of realignment because of bearing wear.

Acousto-optic deflectors find many applications based on continuous laser beam deflection (one axle (1D) as well as 2 axis (2D)) and vector (random) scanning.
The most interesting, demanded and important applications are:

  • scanners;
  • aser tweezers;
  • RGB systems for laser projectors;
  • laser scanning microscopy and profilometry;
  • measurements of surfaces of specimens over some predefined grid of points.

Main deflector principles
As a rule, light diffraction on the wave of slow shear acoustic mode in crystallographic surface (110) is used in paratellurite to provide most efficiency of acousto-optical interaction.
Typical construction acousto-optic cell made on the basis of paratellurite is shown on picture. The phase velocity of the sound wave is normal to the plane of transducer and directed at the angle α with respect to crystallographic direction [110]. The sound energy flow vector does not coincide with the corresponding wave vector, due to high acoustic anisotropy present in the paratellurite crystals. Angle of sound energy drift A is quiet big and can reach 70 degrees that should be taken into consideration for cell geometrical sizes calculations.

ТеО<sub>2</sub> Blanks for Acousto-Optical Deflectors 2

In AOD, the most important performance parameters are resolution and speed.
Resolution, or the maximum number of resolvable spots, is defined as the ratio of the range of deflection angle divided by the angular spread of the diffracted beam, i.e.,

where where is the width of the incident beam and  ξ  is the a factor (near unity) that depends on the incident beam’s amplitude distribution.
For a non-truncated Gaussian beam ξ =4/π.

Where is the acoustic-transit time across the optical aperture. Notice that the acoustic-transit time also represents the (random) access time and is a measure of the speed of the deflector. Equation shows that the resolution is equal to time (aperture) bandwidth product. This is the basic trade of f relation between resolution and speed (or bandwidth) of AODs. In the design of AODs, the primary goal is to obtain the highest diffraction efficiency for the specified bandwidth and resolution (or time aperture)

Reference list:

  1. Xu J and Stroud R 1992 Acousto-Optic Devices (New York:Wiley)
  3. Goutzoulis A and Pape D 1994 Design and Fabrication of Acousto-Optic Devices (New York: Dekker)