Description

High-Precision Fiber Optic Delay Lines for Laboratory and OEM Applications

These optical delay lines are high‑performance fiber‑based devices designed to provide precisely controlled time delays for light signals over a wide wavelength range of 400–2000 nm. By combining high quality input and output fiber collimators with a carefully engineered free‑space propagation region, the delay lines enable exceptionally fine control of optical path length and therefore signal timing. The result is low insertion loss and sub‑picosecond resolution, making them ideal for modern high‑speed photonics, test and measurement, and coherent communication systems.

At the core of each delay line is an optical architecture that projects light from an input fiber into free space, controls the distance traveled in air, and efficiently couples the light back into an output fiber. The optical path length is varied either by changing the physical separation between the collimators or by reflecting the beam from a precisely positioned movable reflector. Because the speed of light in free space is well known and the mechanical motion is accurately controlled, the devices provide a direct and repeatable relationship between mechanical displacement and temporal delay, which can be calibrated in picoseconds for straightforward use in timing‑critical experiments and systems.

Broad Product Range Covering Manual, Motorized, and Miniature Designs

The delay line family includes several mechanical formats tailored to different integration needs and performance requirements. Lead screw‑based models, such as the ODL‑100 and ODL‑300, deliver stable, linear motion with excellent repeatability, and are available in manual or motorized configurations. For users who prefer direct micrometer adjustment, the ODL‑200 offers intuitive, fine‑resolution control suitable for benchtop experiments and quick optical path optimization. Reflector‑style designs, including manual and servo‑driven versions of the ODL‑600 and ODL‑650, extend the delay range while preserving low loss and robust alignment, supporting ranges from tens of picoseconds up to over 1200 picoseconds.

For applications where space is at a premium, the ODL‑700 miniature delay line provides up to approximately 13 picoseconds of delay in a footprint not much larger than a standard fiber patch connection. This compact design is particularly attractive for OEM integration in instruments such as portable interferometers, compact optical coherence tomography systems, and embedded fiber sensors, where mechanical stability, ease of mounting, and minimal added insertion loss are essential.

Fiber Options for Singlemode, Multimode, and Polarization Maintaining Operation

These optical delay lines are available with singlemode, multimode, or polarization maintaining (PM) fibers to match a broad variety of system architectures. For polarization‑sensitive applications, PM implementations typically use PANDA‑style fibers, offering excellent polarization extinction and stability. This is especially important for coherent detection, interferometric metrology, and polarization‑encoded communication schemes where any unwanted polarization rotation or fluctuation directly degrades signal quality and measurement accuracy.

The ability to build delay lines from alternative PM fiber structures or customer‑supplied fibers increases flexibility for specialized use cases, such as non‑standard operating wavelengths, custom numerical apertures, or fibers optimized for specific dispersion characteristics. This customizable fiber approach aligns the delay line’s behavior with the rest of the optical system, improving coupling efficiency, polarization alignment, and long‑term reliability in both laboratory and industrial environments.

Manual and Electrically Controlled Options with Sub‑Picosecond Resolution

Users can select between purely manual adjustment and advanced electrically controlled versions depending on their workflow and automation needs. Manual devices rely on precision lead screws or micrometers, delivering smooth mechanical motion and stable delay settings suitable for alignment tasks, static operating points, or occasional reconfiguration. The mechanical assemblies are engineered for low backlash and good thermal stability, ensuring that the set delay remains consistent over time and under typical laboratory conditions.

Electrically controlled delay lines incorporate servo motors with position encoders, enabling closed‑loop motion control with sub‑micron positioning accuracy. This translates into temporal resolution better than 0.003 picoseconds, more than sufficient for characterizing ultrafast pulses, compensating path length fluctuations, or conducting automated scan routines. 

Optical Delay Lines with Sub-Picosecond Resolution

Specifications

Travel Range: 50 mm
Resolution: 635 um
Delay Range: 167 psec
Delay Resolution: 2 psec
Delay Range (standard): 167 ps
Delay Range (extended Manual Reflector Style): 330 ps or 600 ps
Delay Range (extended Reflector Style With Servo Motor): 330 ps, 600 ps or 1200 ps
Delay Range (miniature Style): up to 13 ps
Resolution (electrically Controlled Versions): submicron (<0.003 ps)
Wavelength Range: 400–2000 nm
Control Interface (electrically Controlled): RS-232 and TTL inputs
Fiber Types: singlemode, multimode, polarization maintaining (PANDA and others)

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Features

  • Ultra-Precise Optical Delay Control – Sub-picosecond temporal resolution (better than 0.003 ps with motorized versions) enables fine adjustment of optical path length for demanding timing‑critical experiments and systems.
  • Wide & Flat Spectral Operating Range (400–2000 nm) – Supports a broad wavelength span from visible to near‑IR, making the delay lines suitable for telecom bands (O, C, L), ultrafast lasers, broadband sources, and OCT systems without frequent re‑optimization.
  • Low Insertion Loss, High Signal Integrity – Precisely engineered fiber collimators and free‑space optics deliver low insertion loss and minimal back reflections for improved system dynamic range and stable measurements.
  • Expanded Delay Range up to >1200 ps – New extended‑range models provide optical delays from a few picoseconds up to over 1200 ps (e.g., 167 ps, 330 ps, 600 ps, 1200 ps options), covering short‑ and long‑range delay requirements in one product family.
  • Polarization Insensitive and PM Options – Available in standard singlemode, multimode, and polarization maintaining (PM) fibers (PANDA‑style and other structures on request), enabling use in polarization‑sensitive and polarization‑diverse systems.
  • Electrically Controlled & Manual Versions – Choose between fully motorized delay lines with servo motor, encoders, RS‑232/TTL control, or manual micrometer and lead‑screw models for simple, robust bench‑top operation.
  • High‑Resolution Motorized Servo Stages – Motorized ODL units (e.g., ODL‑300, ODL‑650) use precision servo motors with integrated encoders, providing repeatable, backlash‑compensated positioning and software‑addressable time delay in calibrated picosecond units.
  • Compact Miniature Delay Line Option – Miniature models (e.g., ODL‑700) offer up to ~13 ps delay in an extremely compact package, occupying only slightly more space than a standard fiber connector for easy integration into dense optical setups.
  • Robust Mechanical Design with Integrated Safety Stops – Home and end‑of‑travel sensors prevent over‑travel and mechanical damage, while precision rails and bearings ensure stable, low‑drift operation over time.
  • Flexible Fiber Interfaces & Connectivity – Supports common connector types and customer‑specified fibers; OZ Optics can build with user‑supplied fiber or alternative PM structures to match existing networks and experimental platforms.
  • Free‑Space Delay Architecture – Input/output fiber collimators project light into free space and recouple it back into fiber, enabling highly linear, repeatable delay control based on physical path length and compatible with a wide range of wavelengths and beam qualities.
  • Multiple Mechanical Styles for Different Use Cases – Available as reflector‑style delay lines, micrometer‑based stages, manual or motorized lead‑screw assemblies, and extended‑range configurations, so users can optimize for range, footprint, and adjustment method.
  • Ideal for High‑Speed Communications & PMD Compensation – Designed for use in coherent telecom systems and high‑bit‑rate test beds, offering precise delay and polarization management for PMD/dispersion emulation and compensation.
  • Optimized for Interferometry & Coherence Control – High stability and sub‑ps resolution make these ODLs well suited for interferometric sensors, optical coherence tomography (OCT), optical spectrum analyzers, and general coherence‑length tuning.
  • Computer & Lab‑Friendly Integration – RS‑232 control and simple TTL input signals allow straightforward integration into automated test systems, data acquisition setups, and research labs requiring programmable optical delay lines.
  • Application‑Proven in Research and Industry – Used worldwide in ultrafast optics labs, fiber‑optic sensing, coherent detection, and telecom development, providing a mature and reliable solution for precise optical delay management.

Applications

  • Polarization Mode Dispersion (PMD) Compensation in High-Speed Optical Networks
    Used to finely adjust relative delays between polarization components in long-haul and metro DWDM systems, 40G/100G/400G coherent links, and ultra‑high bit‑rate testbeds, improving eye diagrams, Q‑factor, and BER performance.
  • Optical Coherence Tomography (OCT) and Time‑Domain Imaging Systems
    Provides precise reference‑arm path length control in time‑domain and swept‑source OCT, enabling depth scanning, coherence gating, axial resolution tuning, and calibration of medical and industrial OCT scanners.
  • Interferometric Sensors and Fiber-Optic Sensing
    Enables phase and path‑length matching in interferometric configurations such as Mach‑Zehnder, Michelson, Fabry–Pérot, Sagnac, and common‑path sensors used for strain, temperature, vibration, and acoustic sensing.
  • Coherent Optical Telecommunications and Coherent Detection Systems
    Aligns optical path lengths between signal and local oscillator in coherent receivers, supports polarization‑multiplexed QPSK/QAM formats, and optimizes DSP performance in advanced coherent transceivers and test setups.
  • Optical Spectrum Analyzers and Coherent Optical Spectrum Measurements
    Incorporated into scanning interferometer‑based spectrum analyzers and Fourier transform optical spectrum analyzers (FT‑OSA) to set the interferometer delay, spectral resolution, and free spectral range.
  • Optical Time‑Domain Reflectometry (OTDR) and Time‑Resolved Measurements
    Used to calibrate and offset reference paths in OTDR and time‑correlated single‑photon counting (TCSPC) systems, improving timing alignment and temporal resolution in backscatter and fluorescence measurements.
  • Pump–Probe, Ultrafast, and Femtosecond Laser Experiments
    Provides sub‑picosecond delay adjustment between pump and probe pulses in ultrafast spectroscopy, nonlinear optics, transient absorption, and carrier dynamics studies, enabling precise control of temporal overlap.
  • Optical Signal Processing and All‑Optical Logic
    Implements controlled path‑length differences for optical buffers, logic gates, clock recovery, temporal multiplexing/demultiplexing, and waveform shaping in research and prototype optical processing circuits.
  • Optical Coherence and Interferometer Alignment
    Used to match optical path lengths in white‑light and laser interferometers, enabling fringe contrast optimization, coherence length characterization, and calibration of metrology interferometers.
  • Time‑Division Multiplexing (TDM) and OTDM System Development
    Adds controlled delays between channels in high‑speed TDM/OTDM systems to manage channel spacing, skew compensation, bit‑walk‑off, and timing synchronization in optical bit‑interleaving experiments.
  • Calibration of Photonic Components and Test & Measurement Systems
    Serves as a tunable reference delay in characterization of modulators, detectors, switches, and integrated photonic circuits, enabling group delay, jitter, and timing skew measurements in lab and production testing.
  • Quantum Optics and Quantum Communication Experiments
    Aligns arrival times of single photons or entangled photon pairs at beam splitters in Hong‑Ou‑Mandel interference, time‑bin entanglement, and quantum key distribution (QKD) setups, optimizing visibility and coincidence rates.
  • Fiber Laser and Mode‑Locked Laser Optimization
    Used to adjust cavity length, synchronization between multiple cavities, and timing of reference pulses in mode‑locked fiber lasers, regenerative amplifiers, and frequency comb systems.
  • Coherent LIDAR, FMCW LIDAR, and Ranging Systems
    Balances or offsets optical paths in coherent and FMCW LIDAR, enabling calibration of range resolution, phase matching, and heterodyne detection performance.
  • Multipath Emulation and Channel Simulation
    Emulates controlled path delays in fiber‑based RF‑over‑fiber and microwave photonics testbeds to model multipath channels, delay spreads, and environmental variations.
  • Optical Synchronization of Distributed Systems
    Provides fine timing alignment between remote optical clocks, triggers, and reference signals in large‑scale experiments such as accelerators, telescopes, and synchronized laser facilities.
  • Polarization‑Maintaining (PM) System Alignment
    In PM configurations, used in conjunction with PM couplers, splitters, and interferometers to maintain and finely tune path length and state of polarization in coherent PM systems from 400–2000 nm.

Frequently Asked Questions

What is an OZ Optics fiber optic delay line and how does it work?
An OZ Optics fiber optic delay line (ODL) is a precision device that introduces a controlled time delay to an optical signal traveling in fiber. It uses an input and output fiber collimator to launch light into free space and recapture it after a defined path length. The optical delay is adjusted by changing the free‑space distance—either by mechanically varying the separation between collimators (lead screw, micrometer) or by moving a reflector with a manual or motorized stage. Because the delay is proportional to the optical path length in air, very fine motion (sub‑micron) translates into sub‑picosecond timing resolution, which is ideal for coherent communications, interferometry, OCT systems, and PMD compensation.
What delay range and resolution do OZ Optics optical delay lines provide?
OZ Optics optical delay lines are available in multiple models and ranges, from miniature units with up to about 13 ps of delay (ODL‑700) to extended reflector‑style delay lines offering 167 ps, 330 ps, 600 ps, and up to over 1200 ps of adjustable delay (e.g., ODL‑600 and ODL‑650). Motorized versions using servo motors and encoders achieve sub‑micron mechanical resolution, corresponding to sub‑picosecond temporal resolution (
Which fiber types and wavelength ranges are supported by these optical delay lines?
OZ Optics ODLs support a broad wavelength range from approximately 400 nm to 2000 nm, covering VIS, NIR, and telecom bands (O, C, L, etc.). They can be configured with singlemode, multimode, or polarization maintaining (PM) fibers. By default, polarization maintaining versions typically use PANDA‑style PM fiber, which offers high extinction ratio and stable polarization, but OZ Optics can also build with alternative PM fiber structures on request. In addition, they are willing to use customer‑supplied specialty fibers when needed for specific wavelengths or dispersion characteristics, similar to custom delay lines offered by other specialized photonics vendors.
What is the difference between manual and electrically controlled (motorized) OZ Optics delay lines?
Manual OZ Optics delay lines use mechanical actuators such as micrometers or lead screws (e.g., ODL‑100, ODL‑200, ODL‑300, ODL‑600 manual versions) to change the optical path length. The user adjusts them by hand and can lock the position once the desired delay is reached; they are ideal for fixed or infrequently adjusted setups. Electrically controlled versions (e.g., ODL‑650 and motorized ODL‑300/600 variants) integrate a servo motor with position encoders, offering computer control via RS‑232 and simple TTL inputs. These motorized ODLs allow automated scanning, repeatable positioning, sub‑picosecond step sizes, and include home and end‑of‑travel sensors to prevent damage, making them suitable for dynamic experiments and remote operation in high‑speed optical testing.
Are OZ Optics delay lines polarization sensitive or suitable for polarization maintaining applications?
The standard OZ Optics optical delay line design is polarization insensitive in its basic singlemode configuration over the 400–2000 nm operating range, making it suitable for most intensity‑based measurements. For polarization‑critical applications—such as coherent telecommunications, interferometric sensors, and polarization mode dispersion (PMD) compensation—OZ Optics offers dedicated polarization maintaining (PM) versions built primarily with PANDA‑type PM fiber. These PM ODLs preserve the input polarization state with high stability, comparable to other high‑end PM fiber delay lines on the market, and can be further customized with alternative PM fibers or user‑supplied fibers if required by the system design.
What are typical applications for OZ Optics fiber optic delay lines?
OZ Optics ODLs are used wherever precise optical timing control is required. Key applications include PMD compensation in high‑speed optical communication networks, arm length control in fiber‑based interferometric sensors, path matching in coherent telecommunications systems, optical coherence tomography (OCT) reference arm delay adjustment, and tunable delay in spectrum analysis and time‑resolved optical measurements. Their low insertion loss, wide wavelength range, polarization maintaining options, and sub‑picosecond resolution make them well suited for both R&D laboratories and OEM integration, similar to delay solutions offered by other leading photonics manufacturers.
How do I control and integrate an OZ Optics motorized optical delay line into my setup?
Motorized OZ Optics delay lines are designed for straightforward integration into optical testbeds and automated measurement systems. The servo‑motor drive with encoder feedback can be controlled via an RS‑232 interface, allowing direct connection to a PC, test instrument, or embedded controller using standard serial commands. Many users drive these units from LabVIEW, Python, or MATLAB by issuing simple position or delay setpoints in picoseconds. For basic setups, TTL inputs can be used for manual stepping or triggering. Built‑in home and limit sensors simplify initialization, ensure safe motion, and allow repeatable return to known delay positions, which is critical for long‑term stability and automated scanning routines.

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