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Phase Modulators
Conoptics manufactures a range of laser accessories, including driver electronics, beam deflectors, and noise-reduction tools. As a pioneer in optics and laser accessories, Conoptics offers high-quality Phase Modulators designed for efficient laser modulation.
The standard modulators—models 350, 360, 370, 380, and 390—function as intensity modulators with a polarizer aligned to the crystal axis. Additionally, you can configure these modulators as polarization rotators, voltage variable wave plates, or Phase Modulators.
Furthermore, we construct all our modulators with the crystals aligned to activate the full cell as a phase modulator. However, in this setup, they cannot serve as intensity modulators, polarization rotators, or variable wave plates. Once configured as a phase modulator, you cannot reconfigure them for intensity modulation. Therefore, it is essential to choose the desired configuration carefully.
Conoptics’ Phase Modulator Products
Before the table:
The half wave voltage (Vπ) is the voltage required to induce a 180-degree phase shift in the optical signal passing through an electro-optic modulator. The wave voltage is a key parameter for both phase and amplitude modulators, as it determines the efficiency and drive requirements of the device. The applied voltage not only controls the phase shift but also shifts the resonance wavelength, directly affecting spectral modulation and bandwidth control. High voltage amplifiers are often required to achieve the necessary drive voltages for these modulators, and suitable electronic circuits can switch these voltages within a few nanoseconds, enabling ultrafast optical modulation. The modulation frequency is an important factor that impacts the operational bandwidth and determines the suitability of a modulator for specific high-speed applications.
| KD*P Series | Phase Sensitivity mrad/volt @ 500nm | V for ½ Wave Phase Modulator |
|---|---|---|
| 350-50-LA | 3.85 | 815 |
| 350-50 | 7 | 450 |
| 350-80 | 12 | 261 |
| 350-105 | 14.7 | 225 |
| 350-160 | 24 | 130 |
| 350-210 | 29 | 113 |
| ADP Series | Phase Sensitivity mrad/volt @ 500nm | V for ½ Wave Phase Modulator |
|---|---|---|
| 370-LA | 12 | 262 |
| 370 | 17 | 184 |
| 380 | 34 | 90 |
| 390 | 27 | 115 |
| LTA Series | Phase Sensitivity mrad/volt @ 830nm | V for ½ Wave Phase Modulator |
|---|---|---|
| 360-40 | 13 | 242 |
| 360-80 | 26 | 120 |
| 360-120 | 39 | 80 |
| 360-160 | 52 | 60 |
Related Laser Beam Products
Sensing and Imaging Applications
Electro optic modulators (EOMs) play a pivotal role in a wide array of sensing and imaging technologies, where precise control over a laser beam’s phase, frequency, or amplitude is essential. Leveraging the electro optic effect, these modulators enable high-speed, high-precision manipulation of optical signals, making them indispensable in advanced scientific and industrial applications.
One of the most prominent uses of electro optic modulators is in optical coherence tomography (OCT). In OCT systems, phase modulators are employed to modulate the phase of the laser beam, generating a reference signal that is crucial for reconstructing high-resolution, cross-sectional images of internal structures. The high modulation bandwidth and low insertion loss of these devices ensure that the optical power is efficiently utilized, resulting in sharper images and faster data acquisition.
In laser-induced fluorescence (LIF) spectroscopy, amplitude modulators are used to control the intensity of the laser beam. By introducing a modulation signal, these modulators help isolate the fluorescence response from background noise, enhancing the sensitivity and accuracy of molecular detection. The ability to achieve amplitude modulation with high electro optic coefficients and minimal power dissipation is particularly valuable in these sensitive measurements.
Microscopy techniques, such as stimulated emission depletion (STED) microscopy, also benefit from the use of phase modulators. Here, the phase of the laser beam is modulated to create a depletion signal, allowing for super-resolution imaging by selectively suppressing fluorescence in targeted regions. The high speed and precise phase shift capabilities of EOMs are critical for achieving the desired modulation depth and image clarity.
Beyond these examples, electro optic modulators are integral to a variety of other sensing and imaging systems, including optical fiber sensors, lidar, and optical communication networks. In these applications, the ability to modulate the optical frequency, amplitude, or phase of the input beam enables advanced data transmission, environmental monitoring, and real-time imaging.
Key features that make EOMs ideal for sensing and imaging include their high modulation bandwidth, which supports high-speed operation; low insertion loss, preserving optical power; and high electro optic coefficients, which ensure efficient modulation with lower voltage required. These attributes contribute to superior modulator performance, energy efficiency, and compatibility with a comprehensive range of laser systems and optical fibers.
However, there are also challenges to consider. Electro optic modulators can exhibit temperature dependence, which may affect the stability of the refractive index and, consequently, the modulation signal. Sensitivity to mechanical resonance frequencies can introduce unwanted amplitude modulation, potentially impacting measurement accuracy. Additionally, some modulator devices require such large voltages for operation that suitable electronic circuits and high voltage amplifiers are necessary, which can complicate system design.
Despite these challenges, the advantages of using electro optic modulators in sensing and imaging applications are clear. Their ability to deliver high speed, high precision, and reliable modulation of optical signals makes them a cornerstone technology in modern optical systems, from biomedical imaging to advanced data transmission and environmental sensing.
Model 102 Key Features:
| Height Adjustment Range: | 2.6 inches (6.6cm) | |
| Lowest Center Line | 4.15″, 10.5cm | |
| Highest Center Line | 6.75″, 17.2cm | |
| Height without Mounting Rings: | Fully Retracted Height | 2.30″, 5.8cm |
| Fully Extended Height | 4.90″, 12.4cm | |
| Weight | 3.33lbs. | |
| Height with Mounting Rings: (Center of Ring) | Fully Retracted Height | 3.90″, 9.9cm |
| Fully Extended Height | 6.50″, 16.5cm | |
| Weight | 3.95lbs. | |
| Dimensions: (Overall L x W x H) | Fully Retracted w/o Rings | 10″L x 3.6″W x 2.3″H |
| 25.4cm x9.1cm x 5.8cm | ||
| Fully Extended w/o Rings | 10″L x 3.6″W x4.9″H | |
| 25.4cm x9.1cm x12.4cm | ||
| Fully Retracted with Rings | 10″L x 3.6″W x 6.3″H | |
| 25.4cm x9.1cm x 16cm | ||
| Fully Extended with Rings | 10″L x 3.6″W x 8.9″H | |
| 25.4cm x9.1cm x 22.6cm | ||
| Alignment Tool Option: | Diameter is 5cm | Aperture 2mm |



