Description

ROF-PM-UV Low Vπ Lithium Niobate Phase Modulator

The ROF-PM-UV series is a high‑performance, low Vπ lithium niobate (LiNbO₃) phase modulator engineered for demanding optical fiber communication and sensing applications in the C‑band. Designed around a 1525–1565 nm operating wavelength range, this device provides precise and stable phase control for coherent optical systems, radio‑over‑fiber (ROF) links, and advanced research setups that require low drive voltage and excellent optical power handling. Its traveling‑wave electrode design enables high‑frequency operation while maintaining low insertion loss and high extinction integrity.

A key characteristic of the ROF-PM-UV phase modulator is its low half‑wave voltage. At low frequency (50 kHz), the typical Vπ is only 2.5 V, which significantly reduces the electrical drive requirements compared with standard LiNbO₃ phase modulators. Even at 10 GHz, the device maintains a typical Vπ of approximately 3.7 V, making it particularly attractive for high‑speed phase modulation, coherent detection schemes, and phase‑encoded modulation formats. This low‑voltage operation allows easier integration with conventional RF drivers, reduces overall system power consumption, and simplifies high‑speed circuit design in both laboratory and system‑level deployments.

The optical performance is optimized for low loss and high signal fidelity. Typical insertion loss is around 3.5 dB, while the optical return loss is better than −45 dB, ensuring minimal back‑reflections and stable operation in sensitive coherent and interferometric setups. Both input and output ports employ polarization‑maintaining (PM) PANDA fibers, helping to preserve the polarization state through the device and ensuring reliable phase modulation on the desired axis. Standard connector options include FC/PC and FC/APC, with other interface configurations available on request to match a wide variety of existing fiber‑optic infrastructures.

The ROF-PM-UV series offers a typical electro‑optic bandwidth of 10–12 GHz (−3 dB), making it suitable for high‑speed phase modulation in advanced optical communication systems and laboratory experiments. With a 50 Ω RF input impedance and SMA female electrical connector, it integrates smoothly with common test and measurement setups, vector network analyzers, arbitrary waveform generators, and RF driver amplifiers. The electrical design delivers an RF return loss better than −10 dB, contributing to cleaner modulation waveforms and reduced reflections in high‑frequency circuits.

High optical power endurance is another core strength of this modulator. The device is specified for input optical powers up to 20 dBm, enabling its use in systems where elevated launch powers are required to overcome fiber attenuation or to drive nonlinear processes at longer distances. This high damage threshold, paired with low half‑wave voltage, allows efficient implementation in applications such as Brillouin scattering mitigation, where controlled phase modulation reduces stimulated Brillouin scattering (SBS) in high‑power fiber links, particularly in long‑haul and specialty fiber systems.

Beyond classical communications, the ROF-PM-UV phase modulator is well suited for optical fiber sensing, laser coherent synthesis, and quantum optics experiments. In distributed and interferometric fiber‑optic sensors, stable and repeatable phase modulation is essential for improving resolution and sensitivity; the low Vπ and high bandwidth of this device support high‑frequency phase coding and multiplexing techniques. For coherent beam combining and laser phase locking, the modulator provides fine‑grained phase control with low drift, facilitating stable interferometric operation. In quantum communication and quantum key distribution (QKD) systems, its low‑noise phase modulation capability supports encoding of quantum states and implementation of phase‑encoded protocols.

The ROF-PM-UV is designed for robust operation across a broad range of environmental conditions. It supports operating temperatures from −10 °C to +60 °C and storage temperatures from −40 °C to +85 °C, with relative humidity from 5% to 90%. These specifications make it viable both for controlled laboratory environments and for integration into field‑deployed systems. With a maximum RF input power rating of 28 dBm and carefully engineered microwave structure, the device withstands demanding RF drive conditions needed for wideband modulation formats and multi‑tone or chirped modulation schemes.

The series supports flexible configuration through its ordering options, allowing users to select operating wavelength (centered near 1550 nm), RF bandwidth class (up to 10 GHz), fiber configuration (PM/PMF or hybrid PM/SMF), and connector facets such as FC/APC or FC/PC. 

ROF PM UV Low Vpi 1550nm LiNbO3 Phase Modulator 10GHz

Specifications

Aperture Diameter: Not Specified
Peak Optical Power Density: Not Specified
Wavelength Range: 1525 – 1565 nm
Transmission: Not Specified
Extinction Ratio: Not Specified
Typical Wavelength: 1550 nm
Insertion Loss (typical): 3 dB
Insertion Loss (max): 3.5 dB
Optical Return Loss: ≥ 45 dB
Input Fiber Type: Panda PM
Output Fiber Type: Panda PM
Optical Fiber Interface: FC/PC, FC/APC or user specified
Operating Bandwidth (-3 DB): 10–12 GHz
RF Half-wave Voltage @ 50 KHz (min): 2.4 V
RF Half-wave Voltage @ 50 KHz (typ): 2.5 V
RF Half-wave Voltage @ 50 KHz (max): 2.6 V
RF Half-wave Voltage @ 10 GHz (typ): 3.4 V
RF Half-wave Voltage @ 10 GHz (max): 3.7 V
Electrical Return Loss S11 (min): 12 dB
Electrical Return Loss S11 (typ): 10 dB
RF Input Impedance: 50 Ω
Electrical Interface: SMA (f)
Maximum Input Optical Power: 20 dBm
Maximum Input RF Power: 28 dBm
Operating Temperature Range: -10 to +60 °C
Storage Temperature Range: -40 to +85 °C
Humidity Range: 5–90 % RH

Got questions about specs? Use the inquiry form to ask.

Document icon Download Data Sheet Download icon

Features

  • Ultra-Low Half-Wave Voltage (~2.5 V) – Low Vπ (2.4–2.6 V @ 50 kHz, ~3.4–3.7 V @ 10 GHz) minimizes RF drive power requirements, enabling efficient integration with compact, low‑power electronic drivers.
  • High Optical Power Handling – Engineered for high endurance to optical power (up to 20 dBm), suitable for demanding fiber‑optic links, coherent systems, and ROF (Radio-over-Fiber) deployments where high optical power is required.
  • Low Insertion Loss for Maximum Link Budget – Typical insertion loss of ~3–3.5 dB reduces system penalties and improves overall transmission performance in long‑haul and high‑capacity optical communication systems.
  • High Modulation Bandwidth up to 10–12 GHz – Wide electrical bandwidth (S21) supports high‑speed phase modulation for advanced modulation formats and next‑generation coherent communication systems.
  • Excellent Signal Integrity and Impedance Matching – 50 Ω RF input impedance with SMA(f) interface and electrical return loss S11 ≤ −10 dB ensures efficient RF power transfer and reduced reflections over the operating band.
  • Low Chirp, High Phase Linearity – Lithium niobate phase modulation design delivers low-chirp operation and linear phase response, ideal for advanced coherent modulation, phase shift keying, and phase-sensitive measurement systems.
  • Optimized for C-Band Operation (1525–1565 nm) – Designed for standard 1550 nm telecom window, fully compatible with EDFAs, WDM systems, and common C‑band photonic components.
  • PM Fiber Inputs and Outputs – Panda polarization-maintaining fibers on both input and output ports provide superior polarization stability for coherent detection, interferometry, and quantum communication experiments.
  • Flexible Optical Connector Options – Available with FC/PC or FC/APC connectors, as well as user-specified terminations, simplifying integration into existing fiber-optic testbeds and production systems.
  • Robust Environmental Performance – Wide operating temperature range from −10 °C to +60 °C and storage from −40 °C to +85 °C, with humidity tolerance 5–90% RH, supporting reliable performance in lab, field, and industrial environments.
  • High Optical Return Loss – Optical return loss better than −45 dB minimizes back‑reflections, protecting upstream lasers and improving stability in interferometric and coherent applications.
  • Ideal for Optical Fiber Sensing – High phase sensitivity and low Vπ make this modulator particularly suitable for distributed and interferometric fiber sensing systems, including phase-sensitive OTDR and interferometric sensors.
  • Coherent Communication and Laser Synthesis – Supports phase control and phase noise manipulation for coherent communications, laser coherent synthesis, optical frequency transfer, and optical phase-locked loop (OPLL) systems.
  • Precise Phase Delay and Phase Shifting – Designed for accurate and tunable phase delay, enabling use as a stable phase shifter in phased-array antenna systems, RF photonics links, and optical signal processing.
  • Quantum Communication Compatible – Polarization-maintaining design, low noise, and precisely controlled phase modulation make it suitable for quantum key distribution (QKD), entanglement-based experiments, and other quantum photonics systems.
  • Radio-over-Fiber (ROF) System Ready – Optimized performance in the 10 GHz range enables high‑fidelity RF signal transport over fiber, with reduced dispersion penalties and efficient sideband generation.
  • Effective SBS Mitigation in Fiber Links – Phase modulation capability is suitable for stimulated Brillouin scattering (SBS) suppression schemes, allowing higher launch powers in long fiber links and high-power distribution networks.
  • Integrated Lithium Niobate Platform – Based on mature LiNbO3 integrated modulator technology known for stability, repeatability, and proven reliability in telecom and photonic research environments.
  • Standard RF Interface for Easy Integration – SMA female RF port simplifies connection to common RF signal generators, AWGs, and drivers used in laboratories and production test setups.
  • Configurable Ordering Options – Multiple configurations available, including wavelength (1550 nm), bandwidth (10 GHz), fiber type (PM/PMF or PM/SMF), and connector facets (FC/APC, FC/PC, or custom), allowing optimization for specific system requirements.

Applications

  • Optical fiber sensing systems – High-sensitivity phase modulation for interferometric fiber sensors (FOGs, DAS, hydrophones, strain and temperature sensing) requiring low Vπ and low insertion loss.
  • Coherent optical fiber communication – Precise phase control in coherent transmitters and local oscillators for high-capacity DWDM, QPSK/QAM formats, and advanced coherent detection schemes.
  • Laser coherent beam combining – Phase stabilization and control in coherent laser arrays to increase output power and beam quality in industrial, medical, and defense laser systems.
  • Optical phase shifters and delay lines – Tunable phase shift in interferometers, optical phased arrays, and delay-line architectures for testing, metrology, and signal processing.
  • Microwave photonics and RF-over-Fiber (ROF) systems – Linear phase modulation for analog RF signal transport over fiber, antenna remoting, radar links, and broadband wireless fronthaul.
  • Low-chirp high-speed modulation – Generation of pure phase-modulated formats with minimal chirp for dispersion-managed fiber links and high spectral efficiency modulation.
  • Sideband generation and frequency combs – Creation of optical sidebands and phase-modulated spectra for frequency comb generation, wavelength conversion, and optical subcarrier multiplexing.
  • Stimulated Brillouin Scattering (SBS) mitigation – Phase dithering of high-power narrow-linewidth lasers to broaden linewidth and suppress SBS in long-haul and high-power fiber systems.
  • Quantum communication and quantum key distribution (QKD) – Stable phase modulation for encoding quantum states (phase and time-bin encoding) in fiber-based QKD and other quantum optics experiments.
  • Optical arbitrary waveform generation (OAWG) – High-speed phase control for synthesizing complex optical waveforms used in advanced communication formats and photonic signal processing.
  • Optical coherent detection and receiver testing – Local oscillator phase control, calibration, and test setups for coherent receivers and optical front-ends.
  • Metrology and precision timing – Phase control in ultra-stable laser systems, optical clocks, frequency transfer links, and fiber-delivered timing distribution.
  • Spectroscopy and lidar – Phase and frequency modulation for coherent Doppler lidar, FMCW lidar, and high-resolution spectroscopic techniques.
  • Optical signal processing and filtering – Implementation of phase-based optical filters, RF phase shifters, and photonic processors leveraging high-bandwidth phase modulation.
  • Research and development in integrated photonics – Versatile phase modulation element for labs developing new coherent modulation formats, photonic circuits, and advanced interferometric architectures.

Frequently Asked Questions

What is the ROF-PM-UV low Vπ phase modulator and what are its key features?
The ROF-PM-UV is a low half‑wave voltage (low Vπ) lithium niobate (LN) phase modulator designed for 1550 nm optical systems. It offers a typical half‑wave voltage of about 2.5 V at low frequency and 3.7 V at 10 GHz, low insertion loss (~3–3.5 dB), high modulation bandwidth (10–12 GHz), and high optical power handling (up to +20 dBm input). The device uses Panda polarization‑maintaining (PM) fiber on both input and output and supports FC/PC or FC/APC connectors. These characteristics make it suitable for high‑speed optical coherent communication, RF‑over‑fiber links, optical fiber sensing, and quantum communication experiments.
What are the typical applications of the ROF-PM-UV 1550 nm low Vπ phase modulator?
The ROF-PM-UV series is used wherever precise, high‑speed phase control of a 1550 nm optical carrier is required. Main applications include: (1) Optical fiber communication and coherent transmission systems, where it performs stable phase shifting with low drive voltages; (2) RF‑over‑fiber (ROF) systems and microwave photonics, for generating and transporting high‑frequency RF signals over fiber; (3) Optical fiber sensing and interferometric sensors, where accurate phase modulation improves sensitivity and dynamic range; (4) Phase delay (phase shifter) functions in coherent beamforming and optical phased arrays; (5) Quantum communication and quantum optics experiments, such as phase encoding in QKD and interferometric state preparation; and (6) Suppression of stimulated Brillouin scattering (SBS) by applying phase modulation to broaden the optical spectrum.
What are the main optical and electrical specifications of the ROF-PM-UV modulator?
Key specifications for the ROF-PM-UV low Vπ phase modulator are: Optical: operating wavelength 1525–1565 nm (optimized around 1550 nm), insertion loss 3–3.5 dB (typ.), optical return loss ≤ –45 dB, Panda PM fiber pigtails on input and output, FC/PC or FC/APC connectors (or user‑specified). Electrical: –3 dB bandwidth S21 typically 10–12 GHz, RF half‑wave voltage Vπ ≈ 2.4–2.6 V at 50 kHz and ≈ 3.4–3.7 V at 10 GHz (per electrode), electrical return loss S11 ≤ –10 to –12 dB, 50 Ω RF input impedance, SMA (female) RF connector. These parameters are in line with comparable 10 GHz class LiNbO₃ phase modulators used in telecom‑band photonics.
How do I properly operate and drive the ROF-PM-UV low Vπ phase modulator?
To operate the ROF-PM-UV correctly, use a narrow‑line 1550 nm laser coupled into the input Panda PM fiber, aligning polarization with the slow axis (usually marked by a key or stress rod line). Connect the RF drive to the SMA female port, using a 50 Ω matched coaxial line and driver/amplifier. To achieve a π phase shift, the required drive voltage is approximately the specified Vπ (≈ 2.5 V at low frequency and ≈ 3.7 V at 10 GHz). For linear phase modulation, use a smaller drive amplitude (e.g., Vπ/2) and ensure the RF signal stays within the maximum RF power rating (+28 dBm). Keep the device within its operating temperature range of –10 to +60 °C and avoid sharp bends or stress on the PM fibers. If used for SBS suppression or RF‑over‑fiber, continuous‑wave or broadband RF signals can be applied, provided both optical and RF power limits are respected.
What are the maximum ratings (optical power, RF power, and environment) for the ROF-PM-UV?
The ROF-PM-UV phase modulator is specified for: maximum input optical power of +20 dBm (100 mW) to avoid photorefractive damage and heating, maximum RF input power of +28 dBm, operating temperature from –10 °C to +60 °C, storage temperature from –40 °C to +85 °C, and relative humidity between 5% and 90% (non‑condensing). For long‑term reliability, it is generally recommended to operate below absolute maximum limits, especially in continuous‑wave high‑power applications, and to ensure proper thermal management and clean, dry environmental conditions similar to those used for other LiNbO₃ telecom‑band modulators.
What fiber types and connector options are available for the ROF-PM-UV modulator?
The standard ROF-PM-UV configuration uses Panda polarization‑maintaining (PM) fiber on both input and output ports (PM/PMF). According to the ordering information, other options may include mixed PM/SMF configurations depending on the suffix chosen (e.g., PS for PM/SM). Connector options are FC/PC (FP) and FC/APC (FA) as standard; a custom interface (SP) can be requested. When ordering, you specify: modulator type (PM‑‑phase modulator, UV‑‑low Vπ), operation wavelength code (15 for 1550 nm band), bandwidth code (10G for 10 GHz), fiber configuration (PS or PP), and connector type (FA, FP, or SP). Using FC/APC is common in coherent and high‑stability phase applications due to reduced back‑reflection compared to FC/PC.
How does the low Vπ of the ROF-PM-UV benefit my optical fiber communication or RF-over-fiber system?
A low Vπ (≈ 2.5 V at low frequency and ≈ 3.7 V at 10 GHz) means the ROF-PM-UV requires significantly lower drive voltage to achieve a π phase shift compared to conventional LiNbO₃ modulators with higher Vπ. In practical terms, this allows the use of lower‑power RF amplifiers, reduces system power consumption, and eases impedance‑matching and high‑frequency design constraints. For coherent communication and RF‑over‑fiber links, lower Vπ improves modulation efficiency, enables higher modulation indices at the same RF power, and can enhance signal‑to‑noise ratio. It also simplifies integrating the modulator with broadband arbitrary waveform generators and drivers commonly used in advanced modulation formats and microwave photonics experiments.

Got more questions? Use the inquiry form to ask the supplier directly.

Similar Products

Request Quote