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Electro-Optics

The LiNbO3 intensity modulator is widely used in high-speed optical communication system, laser sensing and ROF systems because of well electro-optic performance. The R-AM series based on MZ push-pull structure and X-cut design, has stable physical and chemical characteristics, which can be applied both in laboratory experiments and ...

Specifications

Aperture Diameter: - mm
Peak Optical Power Density: - MW/cm^2
Wavelength Range: 850-1550nm
Transmission: - %
Extinction Ratio: Not Specified
Data Sheet
Rof-AMBox Electro-optical intensity modulator is a highly integrated product owned by Rofea with independent intellectual property rights. The instrument integrates electro-optical intensity modulator, microwave amplifier and its driving circuit into one, which not only facilitates the use of users, but also greatly improves the ...

Specifications

Aperture Diameter: -- mm
Peak Optical Power Density: -- MW/cm^2
Wavelength Range: 1550-1550nm
Transmission: -- %
Extinction Ratio: Not Specified
Data Sheet
ROF-ModBox-SSB-1550 Suppression Carrier Single Sideband Modulation Unit is a highly integrated product of Rofea photoelectric with independent intellectual property rights. The product integrates Mach-Zehnder double parallel modulator, bias controller, RF driver And other necessary components into a unit, which doesn’t only ...

Specifications

Aperture Diameter: -- mm
Peak Optical Power Density: -- MW/cm^2
Wavelength Range: 1550-1550nm
Transmission: -- %
Extinction Ratio: Not Specified
Data Sheet
The LiNbO3 phase modulator is widely used in high-speed optical communication system, laser sensing and ROF systems because of well electro-optic effect. The R-PM series based on Ti-diffused and APE technology, has stable physical and chemical characteristics, which can meet requirement of the most applications in laboratory ...

Specifications

Aperture Diameter: -- mm
Peak Optical Power Density: -- MW/cm^2
Wavelength Range: 780-1550nm
Transmission: -- %
Extinction Ratio: Not Specified
Data Sheet
The PM1 Installation Stage and Pockels Cells Mounting Stand are essential components for the installation and mounting of Pockels Cells in optical systems. The PM1 Installation Stage is designed for the new PM1 series of Pockels Cells with a diameter of 25.4mm. On the other hand, the Pockels Cells Mounting Stand is specifically ...

Specifications

Adjust Angles, Tilts And Tip: ±3.5 °
Rotate Along The Z-ax: 180°
Adjusting Screw Threa: M6 × 0.25
Screw Sensitivity (: 0.5
Diameter: 25.4 mm
Data Sheet
The KTP (KTiOPO4) Pockels Cells are advanced optical devices designed for a wide range of applications. With high damage threshold, low piezoelectric resonance, and superior performance compared to other crystals, these Pockels Cells offer exceptional functionality. They operate at low frequency with a high duty ratio, making them ...

Specifications

Aperture Diameter: 5.5 mm
Peak Optical Power Density: -- MW/cm^2
Wavelength Range: 400-1000nm
Transmission: 98 %
Extinction Ratio: >= 500:1
...
Data Sheet
The DKDP (KD2PO4) Pockels Cells are high-performance optical devices with superior electro-optical coefficients and a high anti-light damage threshold. They feature a compact design for easy adjustment and offer high contrast and transmittance. With their good tolerance to the environment, these Pockels Cells are suitable for ...

Specifications

Aperture Diameter: -- mm
Peak Optical Power Density: -- MW/cm^2
Wavelength Range: 1064-1064nm
Transmission: -- %
Extinction Ratio: >= 1000:1, Not Specified
...
Data Sheet
The BBO (BaB2O4) Pockels Cell is an optical device that utilizes the electro-optical effect to control laser pulses. It offers exceptional performance with high damage threshold, low insertion loss, high extinction ratio, and ultra-low piezoelectric ringing effect. This Pockels Cell is designed to handle high laser power, maintain ...

Specifications

Aperture Diameter: 2.5 mm
Peak Optical Power Density: -- MW/cm^2
Wavelength Range: 355-1064nm
Transmission: -- %
Extinction Ratio: < 10:1
...
Data Sheet
The C-995 is a microprocessor-based control system that utilizes direct-digital-synthesis to deliver precise optical chopping rates from 4 Hz to 5000 Hz. Equipped with a large five-digit LED readout, the C-995 controller enables digital entry of the desired chopping rates from the front panel. Additionally, the C-995 is ...

Specifications

Chopping Rates: 4 to 5000 Hz
Frequency Resolution: 0.001 Hz
Data Sheet
Q-Switch 24MHz | Shear or Compression Acoustic Modes
Cascade Laser Corp
This is a 24 MHz Q-Switch cell featuring Shear or Compression (Longitudinal) Acoustic Modes

Specifications

Aperture Diameter: 3 mm
Peak Optical Power Density: 1000 MW/cm^2
Wavelength Range: 1047-1064nm
Transmission: 99.6 %
Extinction Ratio: Not Specified
Data Sheet
Q-Switch Cell 24MHz, 3mm Aperture, Shear Acoustic Mode
Cascade Laser Corp
This is a 24MHz Q-Switch Cell with a 3mm Aperture featuring Shear Acoustic Mode

Specifications

Aperture Diameter: 3 mm
Peak Optical Power Density: 1000 MW/cm^2
Wavelength Range: 1047-1064nm
Transmission: 99.6 %
Extinction Ratio: Not Specified
...
Data Sheet
Q-Switch 27MHz 4mm Shear 6mm | RA Push Fittings | Metric Mount
Cascade Laser Corp
This is a 27MHz Q-Switch featuring RA Push Fittings and a Metric Mount

Specifications

Aperture Diameter: 4 mm
Peak Optical Power Density: 1000 MW/cm^2
Wavelength Range: 1047-1064nm
Transmission: 99.6 %
Extinction Ratio: Not Specified
...
Data Sheet
Phase modulator is a modulation device developed based on electro-optic effect and high frequency resonator theory, which can phase modulate polarized light. It is often used in precision optics systems such as laser interference, optical frequency combs, laser frequency stabilization, atomic cooling, and quantum state ...

Specifications

Aperture Diameter: 2 mm
Peak Optical Power Density: 1 MW/cm^2
Wavelength Range: 355-780nm
Transmission: 97 %
Extinction Ratio: Not Specified
...
Data Sheet
Pockels cell is a modulator about polarized light designed based on the Pockels effect. It is a key component in the laser cavity Q-switching, pulse selection and regenerative amplification system, and one of the best choices for intensity, phase and frequency modulation in laser processing and detection equipment.Moduoptik modified ...

Specifications

Aperture Diameter: 4 mm
Peak Optical Power Density: 1 MW/cm^2
Wavelength Range: 515-1064nm
Transmission: 99 %
Extinction Ratio: >= 1000:1
...
Data Sheet
Generation of a two-step high-voltage pulse with nanosecond rising edges. First step duration of the output high- voltage pulse is determined by trigger pulse duration. Second step amplitude of the output HV pulse is equal to the double voltage of first step. Driver can be used for ultrafast optical beam modulation and deflection, ...
Data Sheet
Generation of high-voltage quasi-rectangular pulses with nanosecond rising and falling edges. HV output duration is determined by trigger pulse duration. Driver can be used for ultrafast optical beam modulation and deflection, control of laser regenerative amplifiers and pulse pickers. Models: PCD-041 – HV pulse duration is ...
Data Sheet
DKDP Pockels CellsDKDP electro-optic Q-switches (Q-switch, Pockels Cells) are widely used in large-caliber, high-power, narrow-pulse (<1 Ons) laser systems due to their unique physical properties and excellent optical quality.The DKDP crystal is a uniaxial crystal with excellent optical quality with an extinction ratio of ...

Specifications

Aperture Diameter: 50 mm
Peak Optical Power Density: 700 MW/cm^2
Wavelength Range: 300-1100nm
Transmission: 97 %
Extinction Ratio: >= 1000:1
Data Sheet
QBD-series consists of several Pockels cell driver circuit boards that differ with output voltage range (up to 6.0kV bipolar) and operating scheme. QBD-series is specially designed to control Pockels cells by applying a fast switching high voltage. The modules require +24VDC power supply and pulse generator to set an operating ...
Data Sheet
QBU-series is specially designed to control Pockels cells by applying a fast switching high voltage. The modules require +24 V DC power supply and pulse generator to set an operating frequency and pulse width. An output voltage level can be programmed in working range by user either manually (through onboard configuration ...
Data Sheet
LITHIUM NIOBATE Q-SWITCHES 7100-2
Alfalight
The G&H electro-optic Q-switch employs the highest optical quality lithium niobate available. The electro-optic effect of lithium niobate makes it extremely useful for Pockels cell Q-switching of several laser types including Nd:YAG, Nd:YALO, Nd:YLF and Er:YLF. Lithium niobate Q-switches are used in both military and commercial ...

Specifications

Aperture Diameter: 25 mm
Peak Optical Power Density: 200 MW/cm^2
Wavelength Range: 633-633nm
Transmission: -- %
Extinction Ratio: >= 10:1
Data Sheet
LS-101 Pockel Cell Based Stabilizer
Brockton Electro-Optics Corp
For those in need in UV stabilization down to 325nm we have been selling our LS-101 model as a semi-custom system. Based on the CRi LS-100 model, the LS-101 is a Pockel cell based stabilizer which is available by special order. Please contact us for details. For those operating in the UV by using a doubled or tripled fundamental beam ...

Specifications

Long Term Stability: 0.03 %
Aperture: 2 mm
Data Sheet
LS-PRO Laser Intensity Stabilizer
Brockton Electro-Optics Corp
With a 2MHz noise reduction bandwidth, this hybrid stabilizer uses a Liquid Crystal (LC) cell and Pockels cell feedback elements. This allows us to provide a high frequency noise reduction without the HIGH VOLTAGE drive requirements of typical Pockels cell stabilizers.

Specifications

Long Term Stability: 0.03 %
Aperture: 2 mm
Wavelength Range: 400-700 nm
Transmittance @ 633nm: 80%
Data Sheet
LPC Laser Power Controller
Brockton Electro-Optics Corp
The Laser Power Controller (LPC) offers automated regulation and control of laser beam power. The LPC works with virtually any CW or mode-locked laser. The LPC can be controlled digitally using an RS-232 or optional GPIB interface, or via an analog input jack. An on-board microprocessor provides a 4-digit display of actual output ...

Specifications

Long Term Stability: 0.03 %
Aperture: 4 mm
Wavelength Range: 400-1700 nm
Data Sheet
KD*P (Potassium Dideuterium Phosphate) is the most widely used material for electro-optical applications due to its excellent E-O properties.  An electro-optic material such as KD*P can alter the polarization state of light passing through it, when an applied voltage induces birefringence change in the crystal. When used in ...

Specifications

Aperture Diameter: 3-30 mm
Peak Optical Power Density: 1000 MW/cm^2
Wavelength Range: 400-1200nm
Transmission: 98 %
Extinction Ratio: >= 1000:1
...
Data Sheet
RTP (Rubidium Titanyl Phosphate - RbTiOPO4) is a very desirable crystal material for electro­optic modulators and Q-switches. Due to its natural birefringence, It always works in pairs which are carefully matched to compensate the birefringence. The laser light propagates either in X-axis or Y-axis, and is polarized along the ...

Specifications

Aperture Diameter: 2-8 mm
Peak Optical Power Density: 600 MW/cm^2
Wavelength Range: 500-3000nm
Transmission: 98.5 %
Extinction Ratio: >= 100:1
...
Data Sheet

Frequently Asked Questions

Electro-optics is a field that combines optics and electronics to create devices and systems for applications in imaging, sensing, and communications. These systems often involve the use of materials such as semiconductors, crystals, and polymers to manipulate light and create optical signals.

Electro-optics systems can be used for a wide range of applications, including laser communication, thermal imaging, optical spectroscopy, and more. They can provide high-resolution imaging, fast data transfer, and high sensitivity sensing.

Electro-optic devices include modulators, detectors, and sensors. Modulators are used to modulate the intensity or phase of light, while detectors are used to detect light signals. Sensors can be used to measure various physical parameters, such as temperature or pressure, by detecting changes in the properties of light.

Choosing the right electro-optics system for your application depends on several factors, such as the required performance specifications, cost, and ease of integration. At Findlight.net, you can explore a wide range of electro-optics systems and devices, and consult with the experts of different suppliers to find the right solution for your specific needs.

Electro-optics refers to the manipulation of light using electrical fields, while optoelectronics involves the use of electronic devices to generate, detect, or control light. Electro-optics is often used to create optoelectronic devices, such as modulators and detectors.

One of the main challenges in developing electro-optics technology is reducing loss and noise in the signal path, as well as increasing the signal-to-noise ratio. Another challenge is integrating different types of materials, such as semiconductors and polymers, into a single device or system.

The future of electro-optics technology is expected to involve further integration with other fields, such as photonics and nanotechnology. This will enable the development of more compact and efficient systems, with higher data transfer rates and greater sensing capabilities.

At Findlight.net, we offer a wide range of resources and information on electro-optics technology, including product guides, technical articles, and expert advice. You can also browse our selection of electro-optics systems and devices to find the right solution for your needs.

At Findlight.net, you can find a wide range of electro-optics systems, including modulators, detectors, sensors, and more. We offer products from leading manufacturers, with options for custom solutions and expert consultation.

Electro-optics is a rapidly advancing field that combines optics and electronics to create devices and systems for a wide range of applications. These systems are used in imaging, sensing, and communications, and often involve the use of materials such as semiconductors, crystals, and polymers. Electro-optics systems can provide high-resolution imaging, fast data transfer, and high sensitivity sensing.

Did You know?

Electro-optics technology combines the principles of optics and electronics to create devices and systems for applications in imaging, sensing, and communications. The technology involves the use of materials such as semiconductors, crystals, and polymers to manipulate light and create optical signals. Electro-optic devices include modulators, detectors, and sensors, and can be used for applications such as laser communication, thermal imaging, and optical spectroscopy. These systems often require precision design and engineering, and can provide high-resolution imaging, fast data transfer, and high sensitivity sensing. As the field of electro-optics continues to advance, new materials and devices are being developed with even greater performance capabilities. At Findlight.net, you can explore the latest electro-optics technology and devices to find the right system for your specific needs.