
LBTEK's resonant electro-optic phase modulator (EOPM) is a device that achieves optical signal phase modulation based on the electro-optic effect and optical resonant cavity principle. This modulator selects lithium niobate with outstanding performance as the electro-optic crystal material. When an electric field is applied to the crystal, its refractive index changes, thereby generating a phase modulation effect on the optical signal passing through the crystal. The EOPM has a clear aperture of 3 mm and uses an SMA signal interface. Additionally, depending on the laser incidence direction, it offers flexible choices between horizontal and vertical polarization orientations, providing high adaptability for various application scenarios.

Installation of Resonant Electro-Optic Modulators
Product Model | Operating Wavelength | Resonant frequency | Damage threshold | Unit Price | Compare | Lead Time | ||
|---|---|---|---|---|---|---|---|---|
| EOPM-20M-C | 1000-1650 nm | 20 MHz | 2 W/mm2 | $3856.86 | 3 weeks | |||
| EOPM-20M-B | 800-1350 nm | 20 MHz | 2 W/mm2 | $3856.86 | 3 weeks | |||
| EOPM-20M-A | 450-800 nm | 20 MHz | 2 W/mm2 | $3856.86 | 3 weeks |
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LBTEK's Broadband Electro-Optic Phase Modulator (EOPM-BB) is a device that modulates the phase of optical signals based on the electro-optic effect principle. It features an extremely wide operating frequency range, functioning at any frequency from DC to 100 MHz. In terms of driving methods, this series has a half-wave voltage of 258V and supports two driving schemes: it can be used directly with an external high-voltage driver or through a combination of a "low-voltage signal source + power amplifier" to meet modulation requirements. The EOPM-BB has a clear aperture of 3 mm and uses an SMA signal interface. Additionally, depending on the laser incident direction, it offers flexible selection between horizontal and vertical polarization directions, providing high adaptability for various application scenarios.
Note: Power amplifiers can be directly purchased at the bottom of this product detail page.
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Installation of Broadband Electro-Optic Phase Modulators
Product Model | Operating Wavelength | Operating Frequency | Damage threshold | Unit Price | Compare | Lead Time | ||
|---|---|---|---|---|---|---|---|---|
| EOPM-BB-C | 1000-1650 nm | DC-100 MHz | 2 W/mm2 | $3268.53 | 3 weeks | |||
| EOPM-BB-B | 800-1350 nm | DC-100 MHz | 2 W/mm2 | $3268.53 | today | |||
| EOPM-BB-A | 450-800 nm | DC-100 MHz | 2 W/mm2 | $3268.53 | 3 weeks |

LBTEK's high-frequency resonant electro-optic phase modulators are based on the electro-optic effect and optical resonant cavity principles to achieve optical signal phase modulation. Utilizing the resonance principle, resonant electro-optic phase modulators can effectively reduce the half-wave voltage and increase the modulation depth. The resonant frequency of the EOPMR series high-frequency resonant electro-optic phase modulators is adjustable and can be tuned via the adjustment knob on the device. The signal interface type is SMA. The bottom of the device features M4 threaded holes for easy mounting onto posts. The polarization direction of the incident light must align with the label on the input end.
Note: Compatible drivers can be selected at the bottom of this product detail page.

EOM Installation Method
Product Model | Operating Wavelength | Resonant frequency | Damage threshold | Unit Price | Compare | Lead Time | ||
|---|---|---|---|---|---|---|---|---|
| EOMPR-14.75G-A New | 350-700 nm | 14.75 GHz@24 ℃ | 1 W/mm2@411 nm | Contact | Contact | |||
| EOMPR-12.2G-A New | 350-700 nm | 12.2 GHz@24 ℃ | 1 W/mm2@411 nm | Contact | Contact | |||
| EOMPR-8.96G-B New | 650-1100 nm | 8.96 GHz@24 ℃ | 3 W/mm2@780 nm | Contact | Contact | |||
| EOMPR-6.8G-B New | 650-1100 nm | 6.835 GHz@24 ℃ | 3 W/mm2@780 nm | Contact | Contact | |||
| EOMPR-5.3G-A New | 400-800 nm | 5.257 GHz@24 ℃ | 3 W/mm2@780 nm | Contact | Contact | |||
| EOMPR-4.6G-A New | 400-800 nm | 4.608 GHz@24 ℃ | 1 W/mm2@411 nm | Contact | Contact | |||
| EOMPR-3.07G-B New | 650-1100 nm | 3.07 GHz@24 ℃ | 3 W/mm2@780 nm | Contact | Contact | |||
| EOPMR-2.1G-A New | 350-700 nm | 2.105 GHz@24 ℃ | 1 W/mm2@411 nm | Contact | Contact |

The HF-EOMD high-frequency electro-optic modulator driver provided by LBTEK is primarily used for high-frequency EOMs and can drive the EOPMR series of electro-optic modulators. Depending on the compatible EOM, the signal source can generate frequency signals ranging from 1GHz to 15GHz, amplified to a maximum output of 35 dBm.

Back View of High-Frequency Electro-Optic Modulator Driver
Product Model | Center Frequency | Maximum Output Power | Unit Price | Compare | Lead Time | ||
|---|---|---|---|---|---|---|---|
| HF-EOMD-A New | 1-8 GHz | 35 dBm | Contact | Contact | |||
| HF-EOMD-B New | 8-14.7 GHz | 35 dBm | Contact | Contact |

LBTEK's RF Power Amplifier (RFPA) is a functional module designed to amplify low-amplitude radio frequency (RF) signals. It operates primarily within the 2 MHz to 500 MHz frequency band, providing power amplification even at frequencies as low as 2 MHz. Powered by a standard 9-15 V DC power supply, it can deliver a maximum output power of ≥1 W. This amplifier is suitable for driving traveling-wave electro-optic phase modulators.

Power Amplifier and Modulator Connection Diagram
Product Model | Amplify frequency band | Voltage Standing Wave Ratio (VSWR) | Unit Price | Compare | Lead Time | ||
|---|---|---|---|---|---|---|---|
| RFPA-2-500M New | 2MHz-500MHz | 1.1-1.4 | $241.87 | 3 weeks |