Custom Optical Scanning
& Autofocus Systems
Engineered for Your Application

OFH designs and builds custom voice-coil driven optical systems: closed-loop autofocusing heads for laser processing, resonant mirror scanners for OCT, and 2D beam deflectors for imaging and metrology. Complete integrated systems or individual subsystems.

Completed Systems

We've Built These. We Can Build Yours.

Two distinct systems, one for precision laser processing, one for OCT beam scanning.
Both built on the same core expertise: voice-coil actuation, leaf-spring suspension, and custom opto-mechanical integration.

closed-loop-autofocusing-optical-head
Laser Processing

Closed-Loop Autofocusing Optical Head

Complete opto mechanical system for sub-micron focal tracking on moving, non-planar surfaces. Integrated custom voice-coil actuator, leaf-spring suspension, off-axis AF sensor with dual-element segmented photodiode, beam-shaping optics, and digital PID servo — in a single cleanroom-ready block, built around a 0.61 NA writing lens.

±2.5 µm
Focus accuracy
±2.5 mm
Tracking range
1.2 kHz
Servo bandwidth
single-mirror-dual-axis-scanner
OCT / Biomedical Imaging

Resonant Mirror Actuator for OCT Beam Scanning

Custom voice-coil driven mirror actuator for an OCT portable system, delivering sinusoidal beam deflection at a tunable resonant frequency. Designed for optical path modulation with a partial mirror in the reference arm. Beryllium-copper leaf springs with adjustable working length for frequency tuning. Built and qualified by OFH before delivery.

380 Hz
Resonant frequency
±20 µm
Mirror stroke (amplitude)
4 mm
Mirror clear aperture
±30 Hz
Frequency tuning range
What We Build

Complete Systems or Any Subsystem in Isolation

Every engagement is scoped to what you need. Some clients come to us for an integrated system. Others need
a single subsystem — a specific actuator, a custom suspension, or a 2D scanner — to plug into their existing platform.

Complete System

Integrated Autofocusing Optical Head

The complete closed-loop head, built to your wavelength, NA, bandwidth and envelope.

Focus tracking rangeconfigurable, e.g. ±2.5 mm
Focus accuracy (closed loop)configurable, e.g. ±2.5 µm
Servo bandwidthconfigurable, e.g. 0–1.2 kHz
Writing wavelengthconfigurable, e.g. 1550 nm
Complete System

Resonant Mirror Scanner for OCT

Resonant voice-coil mirror scanner, with the resonant frequency set to your system at assembly.

Resonant frequencyconfigurable, e.g. 380 Hz
Mirror strokeconfigurable, e.g. ±20 µm
Frequency tuningvia spring working length
Mirror apertureconfigurable to your beam
Subsystem

Voice-Coil Actuator (VCM)

Single-axis electromagnetic drive for fast, precise linear or angular positioning of rather heavy moving objects. Used wherever you need high-bandwidth force control without stiction, backlash, or wear. Can be configured for resonant or non-resonant operation depending on application.

Drive forceconfigurable, e.g. 7.2 N
Moved massconfigurable to your range, e.g. 50 g
Stroke / deflectionconfigurable to your range
Frequency rangeconfigurable, e.g. 0–1.2 kHz
Operation moderesonant or non-resonant
Subsystem

Leaf-Spring Flexure Suspension

Parallelogram beryllium-copper leaf-spring suspension for frictionless, repeatable linear guidance. No lubrication, no wear, no stiction. Own suspension frequency spectrum is set by spring mechanical design — tunable at assembly for prototype flexibility.

Materialberyllium copper leaf springs
Main resonant frequencyconfigurable, e.g. 14–380 Hz
Spectrum of own harmonicsconfigurable by spring shape, e.g. ≤ 4 resonances in 0 – 1kHz range
Dampingconfigurable, e.g. −18 to −22 dB
Movement planarityconfigurable, e.g. <15 arcmin
Subsystem

Autofocus Sensor & Servo Controller

Off-axis focus error detection using a segmented photodiode (quadrant or dual-element), generating sum and differential signals for S-curve based focus error discrimination. Paired with a digital PID servo controller driving the VCM.

Sensor typequadrant or dual-element photodiode
AF sensitivityconfigurable, e.g. 22 mV/µm
Control bandwidthconfigurable, e.g. 0–1.2 kHz
Operating modessearch · track · auto-recovery
Subsystem

2D Angular Beam Scanner

Dual-axis mirror scanner for 2D beam deflection over a target field. OFH has designed and modeled 2D VCM scanners for OCT systems with scan fields up to 16 × 12 mm. Can be paired with F-theta or telecentric scan lenses for flat-field imaging.

Beam deflection angleup to 60⁰ for all azimuth angles
Deflecting mirror clear aperture diameterconfigurable, e.g. Ø18 mm
Scan lens compatibilityF-theta, telecentric, custom
Deflecting mirror angular position sensing2D
Technology

How These Systems Work

If you're evaluating whether OFH can solve your problem, these are the underlying technologies we work in.

Voice-Coil Actuator

Electromagnetic Linear & Angular Drive

A voice-coil actuator (VCM) generates force by passing current through a coil in a static magnetic field produced by high effective NdFeB and SmCo magnets. Special dampers provide the flatter-free movement. No gears, no screws, no contact — just smooth, bidirectional force proportional to current. This makes VCMs ideal for high-frequency, high-precision motion where friction or backlash would introduce error. OFH designs both the magnetic circuit and the coil geometry for your force, stroke, and bandwidth target.

Leaf-Spring Suspension

Flexure-Based Frictionless Guidance

A parallelogram leaf-spring suspension guides the moving part of an actuator with zero friction and zero wear. The resonant frequency is determined by spring stiffness and moving mass — OFH models and tunes this to match your operating frequency. Beryllium-copper springs offer the best fatigue life and stiffness-to-mass ratio for optical actuator applications. Spring working length is tunable at assembly for prototype flexibility.

Segmented Photodiode AF

Quadrant & Dual-Element Focus Error Detection

Autofocus systems use a segmented photodiode — quadrant (four-quadrant) or dual-element — to detect the focus error signal. An off-axis probe beam is reflected from the target surface; its position on the detector shifts with defocus, generating an S-curve error signal. The sum signal (A+B) gives intensity; the differential signal (A−B) gives focus error. OFH designs both the optics and the signal processing electronics.

F-Theta & Scan Lenses

Flat-Field Beam Scanning Optics

A galvo or VCM scanner deflects a beam angularly, but without a scan lens, the focused spot traces a curved arc — not a flat field. F-theta lenses convert angular deflection to linear scan position, providing a flat image field and constant spot velocity. For OCT and confocal applications, telecentric scan lenses (like the Thorlabs LSM series) maintain constant beam angle at the sample. OFH models the full scan system in Zemax, including scan lens, field curvature, and spot size across the field.

Closed-Loop Servo

Digital PID Control for Optical Actuators

A closed-loop servo reads the position or focus error from a sensor, computes a correction via a PID (proportional-integral-derivative) controller, and drives the VCM coil current to minimize error. The digital PID controller provides the easy adaptability of servo system to your specific tracking system. The servo bandwidth — how fast the loop can respond — is limited by the actuator’s mechanical resonances. OFH designs the full control loop: sensor, signal conditioning, digital PID implementation, and VCM driver, matched to your required tracking accuracy and surface dynamics.

Design Decision

Resonant vs. Non-Resonant Actuator Operation

One of the first questions in any OCT scanner or mirror actuator design. Both approaches are feasible. The
right choice depends on your power budget, frequency stability requirements, and system complexity tolerance.

Resonant Operation
~10× lower power consumption — the mechanical resonance does the work
Frequency stability defined by spring-mass mechanics, not electronics — inherently immune to driver drift
Electro-mechanical feedback possible: oscillation frequency self-defined by mechanical response
Requires precise resonant frequency tuning at assembly (±12–15 Hz achievable)
Needs mirror position sensor for closed-loop amplitude control
Less flexible if your target frequency changes
Non-Resonant Operation
Simpler design with relaxed manufacturing tolerances
No fine resonance tuning required at assembly
Frequency can be set and changed electronically
Operating frequency and drift fully defined by electronic driver stability
Amplitude less stable — working point is on the slope of the mechanical frequency response
Significantly higher power consumption
Applications

Where OFH Optical Scanning Systems Are Used

If your application requires a focused beam to track, scan, or write on a surface — at speed,
at sub-micron accuracy, or in a compact form factor — this is the class of system OFH builds.

OCT Lateral Scanning

2D scanners that sweep the beam laterally across tissue to build the B-scan. OFH has modeled 2D scan systems for fingerprint-scale fields and can build the actuators and drive electronics to match.

Laser Marking & Engraving

Closed-loop autofocus heads that maintain focus on curved, tilted, or mechanically imperfect surfaces without stopping the scan — sub-micron tracking accuracy at 1.2 kHz servo bandwidth.

Sub-Surface & Volumetric Laser Writing

High-NA writing heads with active Z-focus control for writing patterns inside a volume — holographic data storage, 3D microstructure fabrication, two-photon polymerization.

Semiconductor Inspection & Metrology

Non-contact surface height mapping and defect detection across large-area substrates. Active focus maintenance for confocal and structured-light systems scanning wafers and panels.

Confocal & Scanning Microscopy

High-bandwidth focus and beam-steering actuators for confocal, two-photon, and light-sheet microscopy. OFH models the full optical train — scanner, scan lens, objective — in Zemax.

Laser Material Processing

Focus-controlled write heads for annealing, scribing, trimming, and surface modification on non-flat substrates. Microelectronic component trimming and tuning with sub-micron focal control.

OCT Reference Arm Modulation

Precise optical path length modulation in time-domain and swept-source OCT systems. Resonant or non-resonant operation — OFH can model and build both, and advise which is appropriate for your system.

Holographic Data Storage

Precision optical pickup actuators for next-generation holographic and archival optical storage media — a domain where OFH has deep historical experience from the data storage era.

Adaptive Optics & Interferometry

Fast tip/tilt and piston correction elements for wavefront correction systems. Phase modulation via controlled mirror displacement in interferometric measurement setups.

How It Works

You Define the Requirements. We Engineer to Them.

These are the inputs you bring to OFH. We size, model, and build the system around your numbers, not a fixed catalog.

Operating Frequency

Resonant or non-resonant. Set by your scan rate, surface dynamics, or OCT A-scan frequency.

10 Hz – 2+ kHz

Wavelength

Writing and/or sensing wavelength. 850 nm typical for OCT; 1550 nm for telecom-band laser processing.

400 nm – 1600 nm

Scan Field / Stroke

Mirror stroke or linear travel, driven by your surface runout, scan field size, or OCT depth range.

±20 µm to ±5 mm+

Focus Accuracy

Determined by your spot size requirement, depth-of-focus budget, and surface non-planarity.

Sub-µm to tens of µm

Form Factor

Footprint, beam height, mass, mounting interface — designed to fit your optical bench or OEM housing.

Your envelope

Environment

Material selection, sealing, and power constraints matched to your operating environment and duty cycle.

Lab · Cleanroom · Portable
Related Systems

Other Systems We've Designed and Built

Linear Mirror Scanner from Optics for Hire

Linear Scanning Mirror

A vibrating mirror that modulates optical path length for OCT and interferometry. Resonance tunable from 200 to 500 Hz, 5–8 mm aperture, sub-10 arc-second deflection accuracy, in a 16-gram package.

single-mirror-dual-axis-scanner

Dual Axis Scanning Mirror

Two-axis deflection from a single mirror in a 33.5 × 20 mm cylinder. ±15° scan angle, 5.5 mm clear aperture, open or closed loop, proven past two million cycles in laser wobble welding and OCT.

Reducing speckle noise in 3D mapping

3D Depth Mapping

A pattern projector and an astigmatic lens turn projected spots into ellipses whose shape encodes distance. No intensity or phase measurement, so it resists multi-path interference and changing ambient light.

FAQ

Custom Optical Scanning & Autofocus Systems FAQ

Can OFH build a complete system, or just the subsystem I need?

Both. Some clients come to us for a fully integrated system — like a closed-loop autofocusing optical head with the actuator, suspension, AF sensor, beam-shaping optics, and digital servo in a single block. Others need a single subsystem — a voice-coil actuator, a leaf-spring flexure suspension, an autofocus sensor with servo controller, or a 2D angular beam scanner — engineered to plug into their existing platform.

Resonant operation offers roughly 10× lower power consumption and frequency stability defined by the spring-mass mechanics rather than electronics, but it requires precise frequency tuning at assembly and a mirror position sensor for amplitude control. Non-resonant operation is simpler to build and lets you set and change the frequency electronically, at the cost of higher power consumption and stability that depends on the drive electronics. OFH has built both and can advise based on your power budget and frequency stability requirements.

Our completed systems include a closed-loop autofocusing optical head with ±2.5 µm focus accuracy over a ±2.5 mm tracking range at 1.2 kHz servo bandwidth, and a resonant mirror actuator for a portable OCT system delivering ±20 µm mirror stroke at 380 Hz with a ±30 Hz frequency tuning range.

You define the requirements and we engineer to them: operating frequency from 10 Hz to 2+ kHz, wavelengths from 400 nm to 1600 nm, strokes from ±20 µm to ±5 mm and beyond, focus accuracy from sub-micron to tens of microns, plus your form factor, mounting interface, and operating environment — lab, cleanroom, or portable.

OCT beam scanning and reference-arm modulation, laser marking and engraving on curved or tilted surfaces, sub-surface and volumetric laser writing, semiconductor inspection and metrology, confocal and scanning microscopy, laser material processing, holographic data storage, and adaptive optics.

Yes. Zemax modeling of the full scan system — scanner, scan lens, field curvature, and spot size across the field — is included, and we review feasibility at no charge before you commit to a project.

A voice-coil actuator produces smooth, bidirectional force proportional to current, with no gears, screws, or contact — meaning no stiction, backlash, or wear. Combined with a beryllium-copper leaf-spring suspension, it delivers frictionless, repeatable motion that is ideal for high-frequency, high-precision optical positioning.

Customer Feedback

University ClientCustom ophthalmology research optics
"I have a background in optics, but lens design has always been a mystery to me. Your explanations helped me to decipher it. I am grateful for your expertise. It is a blessing for me to work with you and OFH."
Grow Light StartupCustom illumination optics design
"We really enjoy working with you guys and your professionalism is admirable. We shall also revert back once we have the commercialization process sorted."
Industrial Distance Measurement CompanyCustom lens for precision measurement product
"Your team is moving so fast, I feel like a turtle. Every time we ask something, our question is promptly answered and your team often brings up aspects that we haven't considered."