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Fiber-coupled acousto-optic tunable filter| SIMTRUM Photonics Store

Fiber-coupled Acousto-optic Tunable Filter

SIMTRUM's fiber-coupled acousto-optic tunable filter (AOTF) is an optical device based on the acousto-optic effect that is used to select and adjust a specific wavelength of light. It changes the refractive index of light by transmitting sound waves into the acousto-optic crystal, thus achieving dynamic filtering of light. Adjusting the frequency of the sound wave can change the center wavelength of the filter to achieve the selection of different wavelengths of optical signals, AOTF has the characteristics of high flexibility, fast response and wide tuning range, and is widely used in spectroscopy, laser technology, optical communication and imaging systems.

In practice, we also need an RF driver to excite the ultrasonic waves in the crystal through the RF driver, so as to achieve modulation and selective filtering of light. The frequency and intensity of the RF signal control the wavelength selection and performance of the filter, so RF driving is the key to achieving efficient, tunable filtering.

Features

  • Easy integration with fiber optic systems
  • Suitable for the conditioning and filtering of optical signals in optical fiber networks

Applications

  • Spectral Analysis: AOTF is applicable in spectrophotometers for swiftly tuning the wavelength of the light source to measure and analyze various spectral components.
  • Multi-wavelength Imaging: AOTF enables rapid switching between different wavelengths of light in a multi-wavelength imaging system, facilitating the acquisition of images across different bands for applications such as environmental monitoring and medical imaging.
  • Communication System: In optical fiber communication, AOTF can be utilized for wavelength division multiplexing and demultiplexing to enhance system bandwidth and efficiency.

Mechanical Diagram (mm)


Product Specification

 Parameter OE-DK01-LF90-900/1100 OE-DK01-LF60-1500/1700 OE-DK01-LF70-800/1700 OE-DK01-LF100-1000/1300 OE-DK01-LF75-1300/1600
  Wavelength range (nm) 900-1100 1500-1700 800-1700 1000-1300 1300-1600
  Center frequency(MHz) 90 60 70 100 75
  Insertion loss(dB) <2.5 <3 <6 <2.5 <1.5
  Resolution(nm) ≤3 ≤5 ≤4 ≤4 ≤4
  Polarization extinction ratio(dB) >20
  Polarization-dependent losses(dB) <1 <1 0.5
  Fiber type HI1060 PM1550 corning 62.5/125mm 10/125 PM FUD3460 SMF28e
  Resistant to optical power(W) <1
  Drive power(W) <0.5
  Fiber optic connectors FC/APC
  Pigtail length(m) ≥1
  RF connectors SMA
  Input impedance(Ω) 50
  Operating temperature(℃) -20℃~55℃
  Storage temperature(℃) -40℃~70℃

 

 

 

The principle of action of AOTF (acousto-optic tunable filter) is based on the acousto-optic effect, the RF signal generated by the RF drive generates sound waves, these sound waves form an acousto-optic grating in the acousto-optic crystal, so as to modulate the intensity and frequency of the passing beam, by adjusting the frequency and intensity of the RF drive, the optical signal of different wavelengths can be selectively filtered to achieve selective transmission or suppression of the optical signal, and at the same time, the amplitude change of the RF signal affects the intensity of the sound wave, thereby changing the intensity of the optical signal and realizing dynamic light intensity control.

We offer matching RF drivers that can be modulated by both digital and analog signals.

 

  Parameter OE-DK01-SGY20/200-R1 OE-DK01-SGY75/220-R12 OE-DK01-SGY90/230-R13 unit
Control input interface specifications
  Input interface USB(The internal communication protocol is RS232)  
  Baud rate 9600 bps
Modulation input interface specifications
  Modulated signal Digital modulation (high level 3.3-5V; Low level 0-0.2V@1k Ω)Suspended as high V
  Input interface SMA  
Specifications of the RF output interface
  Output signal frequency 20-200 75-220 90-230 MHz
  Frequency stability 1 1 1 ppm
  Output signal power ≤2 ≤3 ≤5 W
  Minimum frequency step 1000 default Hz
  Power regulation range 10-100 %
  Output impedance 50 Ω
  Output interface SMA  
Specifications of the whole machine
  Maximum power consumption 15 20 20 W
  Operating voltage 24±1 Vdc
  Power connector Through-center capacitance (the core wire is positive, the solder lug is negative) +Vcc

 

 


AOTF takes advantage of the acousto-optic effect, which means that when sound waves travel through a medium, they have an effect on the light waves passing through the medium. This effect usually occurs in piezoelectric materials (such as lithium niobate, sodium titanate, etc.), where the sound wave changes the propagation path of the light wave through the ultrasonic lattice fluctuations generated by the electroacoustic conversion.

 

1. Overview of working principle:

  • When the RF signal is loaded to the piezoelectric transducer, the piezoelectric transducer converts the electrical signal into an ultrasonic signal and transmits it to the acousto-optic medium because of the piezoelectric effect, and the ultrasonic signal forms a periodic acoustic wavefront (that is, acousto-optic wave) in the crystal.
  • This acoustic wavefront causes periodic changes in the refractive index of the acousto-optic medium, forming a refractive index grating, often called an ultrasonic grating, which produces diffraction effects on light waves passing through the crystal.
  • Depending on the relationship between the wavelength of the incident light and the frequency of the sound wave, the direction of propagation of the light wave in the crystal changes, selectively diffracting a certain wavelength of light.
  • By changing the frequency of the driving signal, the frequency of the sound wave can be adjusted, and thus the wavelength of the diffracted light wave. Therefore, AOTF can realize the function of quickly adjusting the filter wavelength.

 

2. Basic working process:

  • Light source: The beam is emitted from a laser or other light source.
  • AOTF crystal: The light beam passes through the acousto-optic crystal, during which the frequency of the sound wave determines the diffraction Angle of the light wave.
  • Tuning: By adjusting the frequency of the electrical signal, the wavelength of the sound wave changes, so as to achieve the selective diffraction of different wavelengths of light, to achieve the purpose of filtering.
  • Output beam: The diffracted beam is selected and output through the filter.

 

 


 

3.Calculation Formula:

The acousto-optical interaction can be described in terms of the Bragg diffraction condition. By adjusting the frequency of the RF signal, Λ can be altered, thereby enabling selective tuning of λ.

2Λsin(θ)=mλ

  • Λ represents the wavelength of the sound wave
  • θ denotes the angle between incident light and diffracted light
  • m signifies the diffraction order
  • λ refers to the wavelength of light 

 


Q: What is the input and output of AOTF fiber coupler head?

A: our AOTF both support free Space or fiber-coupled Input and output.

 

Q:Why use RF drivers?

A:Acoustic wave generation: AOTF works on the basis of the acousto-optic effect, in which sound waves produce periodic changes in the refractive index in the acousto-optic crystal. RF signals are converted into high-frequency sound waves that propagate through the crystal and form an acousto-optic front. RF drives are the primary means of generating these sound waves.

Wavelength adjustment: The frequency of the RF signal determines the frequency of the sound wave, which affects the refractive index period in the acousto-optic crystal. By adjusting the frequency of the RF signal, the wavelength of the light can be precisely controlled and selected.

Fast response: The RF driver enables fast adjustment of the AOTF for applications that require dynamic wavelength selection.

 

Q:Is it possible to use other types of drives?

A:Ultrasonic drive: In some special cases, low-frequency ultrasound can also be used for acousto-optic crystals, but this is usually not as efficient as RF signals. Ultrasound waves are less frequent, resulting in potentially larger devices, slower adjustment speeds, and higher material requirements.

Other wave methods: While RF driving is the most common and widely used method, theoretically, any acoustic wave generation method capable of producing periodic refractive index changes in an acousto-optic crystal can be used. However, these methods may not have the efficiency, precision, and speed of regulation of RF drives.

 

Q:What are the main factors affecting the wavelength selectivity of AOTF ?

A:

  1. Materials of acousto-optic crystals:

Acousto-optic effects:Different crystalline materials have different acousto-optic effects, which affect the modulation and selectivity of light. The acousto-optic coefficient of the material, such as the photoacoustic coupling coefficient, directly affects the performance of the filter.

Optical anisotropy: Some crystals are anisotropic and the propagation characteristics of light may differ in different directions, which can affect selectivity.

  1. Sound Frequency:Frequency vs. wavelength:The frequency of the sound wave determines the modulation range and filter width of the light wavelength in the acousto-optic crystal. The higher the frequency of the sound wave, the greater the range of wavelength choices that can be achieved.
  2. Sonic power:Power and efficiency: The power of the sound wave affects the intensity of the acousto-optic effect, which affects the selectivity and filtering accuracy of the AOTF. The right amount of power can improve the performance of a filter, but too much or too little power can lead to a decrease in performance.
  3. Beam incidence angle:Angle of incidence and selectivity: The angle of incidence of the beam affects the interaction between the sound wave and the light wave, which in turn affects the wavelength selectivity of the filter. Different angles of incidence change the diffraction conditions of the light, which affects the filtering effect.

 

Q:What is the difference between AOM EOM and AOTF?

A:

  Characteristic AOM (Acousto-Optic Modulator) AOTF (Acousto-Optic Tunable Filter)
  Function Light intensity, frequency, and phase modulation Wavelength selection and tuning
  Working principle Modulating the light beam through the diffraction grating formed by sound waves Selecting specific wavelengths of light through the diffraction grating formed by sound waves
  Application Laser modulation, frequency shifting,
optical switching, pulse modulation
Spectral analysis, multi-wavelength imaging,
wavelength selection in optical communication
  Structural Complexity Relatively simple More complex, more precise design

Acousto-Optic Device

Product Type Wavelength Choice Aperture Frequency Driver 
  Acousto-optic deflector (AODF) 266, 355, 364 , 405, 488, 515, 532, 561, 813, 1064, 1083nm 1 to 26mm 70-230Mhz Yes
  Acousto-optic frequency shifters (AOFS) 633, 1064nm 1 and 3mm 20-115Mhz Yes
  Acousto-optic modulators (AOM) Free space  266, 343,355,532,800,1045,1064, 9600,10600nm and 450-900nm 0.5 to  8mm 40-200Mhz Yes
  Acousto-optic modulators (AOM) Fiber  780,1030,1064,1550nm and 910-940nm lost <3dB 40-300Mhz Yes
  Acousto-optic tunable filter (AOTF)  640-1100n,400-700nm, 400-1000m 2 and 2.5mm / Yes
  PHASE MODULATORS 280, 355, 370, 420, 461, 532, 650,780,935, 960 nm 2 and 3mm 1Ghz - 25Mhz Yes
  Acousto-optic Q-switch (AOQS) 1064, 1342, 1532, 1550, 10600nm 1 to 11mm 20 - 80Mhz /
  Pockels Cells 515, 532, 800, 1030, 1064nm 3 to 10mm / /

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Compare Model Drawings & Specs Availability Reference Price
(USD)
OE-DK01-LF90-900/1100
Wavelength range:900-1100nm,Center frequency:90MHz,Insertion loss:<2.5dB,Resolution:≤3nm
4-6week $5005.41
OE-DK01-LF60-1500/1700
Wavelength range:1500-1700nm,Center frequency:60MHz,Insertion loss:<3dB,Resolution:≤5nm
4-6week $5005.41
OE-DK01-LF70-800/1700
Wavelength range:800-1700nm,Center frequency:70MHz,Insertion loss:<6dB,Resolution:≤4nm@1550nm
4-6week $6006.49
OE-DK01-LF100-1000/1300
Wavelength range:1000-1300nm,Center frequency:100MHz,Insertion loss:<2.5dB,Resolution:≤4nm
4-6week $5005.41
OE-DK01-LF75-1300/1600
Wavelength range:1300-1600nm,Center frequency:75MHz,Insertion loss:<1.5dB,Resolution:≤4nm
4-6week $5005.41

OE-DK01-SGY90/230-R13 - Parameter

OE-DK01-SGY75/220-R12 - Parameter

OE-DK01-SGY20/200-R1 - Parameter

OE-DK01-LF75-1300/1600 - Parameter

OE-DK01-LF100-1000/1300 - Parameter

OE-DK01-LF70-800/1700 - Parameter

OE-DK01-LF60-1500/1700 - Parameter

OE-DK01-LF90-900/1100 - Parameter

OE-DK01-SGY90/230-R13 - Download

OE-DK01-SGY75/220-R12 - Download

OE-DK01-SGY20/200-R1 - Download

OE-DK01-LF75-1300/1600 - Download

OE-DK01-LF100-1000/1300 - Download

OE-DK01-LF70-800/1700 - Download

OE-DK01-LF60-1500/1700 - Download

OE-DK01-LF90-900/1100 - Download

Accessories

Compare Model Drawings & Specs Availability Reference Price
(USD)
OE-DK01-SGY20/200-R1
Baudrate: 9600 bps,Modulation signal: digital modulation (high 3.3-5V; Low level 0-0.2V@1KΩ),Input interface: SMA,Output signal frequency: 20-200 MHz,Output signal power: ≤2W
4-6week $2002.16
OE-DK01-SGY75/220-R12
Baudrate: 9600 bps,Modulation signal: digital modulation (high 3.3-5V; Low level 0-0.2V@1KΩ),Input interface: SMA
4-6week $2002.16
OE-DK01-SGY90/230-R13
Baudrate: 9600 bps,Modulation signal: digital modulation (high 3.3-5V; Low level 0-0.2V@1KΩ),Input interface: SMA
4-6week $2002.16