FILTER PRODUCTS

to
to
to
to

EOM

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 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
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
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
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
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
Y-BRANCH 1X2 PHASE MODULATOR
EOspace Inc
Y-BRANCH 1X2 PHASE MODULATOR.

Specifications

Aperture Diameter: -- mm
Peak Optical Power Density: -- MW/cm^2
Wavelength Range: 400-700nm
Transmission: -- %
Extinction Ratio: Not Specified
Data Sheet
DUAL-PARALLEL MZM QPSK I/Q MODULATOR
EOspace Inc
LOW-VΠ VERSION: 25+GBAUD I/Q MODULATOR.

Specifications

Aperture Diameter: -- mm
Peak Optical Power Density: -- MW/cm^2
Wavelength Range: 400-700nm
Transmission: -- %
Extinction Ratio: Not Specified
Data Sheet
LOW-VΠ COMPACT X-CUT MODULATOR
EOspace Inc
1x1, 1x2, Low-Vπ compact X-cut modulator.

Specifications

Aperture Diameter: 5 mm
Peak Optical Power Density: -- MW/cm^2
Wavelength Range: 400-700nm
Transmission: -- %
Extinction Ratio: Not Specified
Data Sheet
Lithium Niobate Q-Switch Elements
Isowave
Deltronic Crystal’s Lithium Niobate, with its combination of excellent optical transmission and high electro-optic coefficient, is an ideal choice for Pockels Cell Q-Switching. Crystals are grown, oriented and cut to provide z-axis optical propagation. Q-Switch elements are polished, electroded and anti-reflection coated, ready ...

Specifications

Aperture Diameter: -- mm
Peak Optical Power Density: 300 MW/cm^2
Wavelength Range: 1064-1064nm
Transmission: -- %
Extinction Ratio: >= 10:1
Data Sheet
Q1025-TxxL-H AO Q-SWITCH
Isomet Corp
Q-switches are intracavity devices used to generate very high peak power, short duration laser pulses. These are typically loss modulators operating on the zero order beam. The goal of a Q-switch is to diffract as much power from the zero order as possible to increase the cavity loss and extinguish the laser output. When the RF drive ...

Specifications

Aperture Diameter: 1.0 mm
Peak Optical Power Density: 250 MW/cm^2
Wavelength Range: 1-1nm
Transmission: 85 %
Extinction Ratio: < 10:1
Data Sheet
Q1058C-SFxxL-H AO Q-SWITCH
Isomet Corp
Q-switches are intracavity devices used to generate very high peak power, short duration laser pulses. These are typically loss modulators operating on the zero order beam. The goal of a Q-switch is to diffract as much power from the zero order as possible to increase the cavity loss and extinguish the laser output. When the RF drive ...

Specifications

Aperture Diameter: 1.0-1.5 mm
Peak Optical Power Density: 300 MW/cm^2
Wavelength Range: 1-1nm
Transmission: 85 %
Extinction Ratio: < 10:1
Data Sheet
Q1072-SF24L AO Q-SWITCH
Isomet Corp
Q-switches are intracavity devices used to generate very high peak power, short duration laser pulses. These are typically loss modulators operating on the zero order beam. The goal of a Q-switch is to diffract as much power from the zero order as possible to increase the cavity loss and extinguish the laser output. When the RF drive ...

Specifications

Aperture Diameter: 1.5 mm
Peak Optical Power Density: 300 MW/cm^2
Wavelength Range: 1-1nm
Transmission: 80 %
Extinction Ratio: < 10:1
Data Sheet
Q-SWITCH 24MHZ, 4MM SHEAR, BARBED FITTINGS
Cascade Laser Corp
Q-SWITCH 24MHZ, 4MM SHEAR, BARBED FITTINGS

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
Custom Pockels Cells 

Specifications

Aperture Diameter: 19 mm
Peak Optical Power Density: 500 MW/cm^2
Wavelength Range: 240-1400nm
Transmission: >98% %
Extinction Ratio: >= 5000:1
...
Data Sheet
There are 26 different EOM from suppliers and manufacturers listed in this category. In just a few clicks you can compare different EOM with each other and get an accurate quote based on your needs and specifications. Please note that the prices of EOM vary significantly for different products based on various factors including technical parameters, features, brand name, etc. Please contact suppliers directly to inquire about the details and accurate pricing information for any product model. Simply navigate to the product page of interest and use the orange button to directly reach out to the respective supplier with one click.

Did You know?

The electro-optic effect is a result of the change in refractive index of a material when it is placed in DC or low-frequency electric field. Nonlinear optical materials with an incident static or low frequency electromagnetic wave will undergo modulation of refractive index and as such are often used as electro-optic modulators (EOM). In general, the modulation in refractive index in EOM may be induced on the amplitude, phase, frequency or polarization of the input beam. The most common EOM consists of a crystal whose refractive index depends on the strength of applied electric field. This implies if it is exposed to electric field, light will travel slower through it than in air. The phase of the light leaving the crystal can be controlled by changing the incident electric field as the phase delay is directly proportional to the time it takes for light to pass through the crystal.