F²R — Fiction to Reality XY Lab · AN-01
Step & repeat lithography
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Application note AN-01
Geometry from source CAD
MMXXVI
X 0.000000 mm   Y 0.000000 mm
Step <20 nm  Field —  State Idle
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XY Lab.

Mask projection lithography
on a printed stage

The new stageFig. 5 · Build

Same idea. Stiffer frame.

The second body keeps the one-piece print and gives the drive something solid to push against.

XY One proved that a printed flexure can move in nanometres. This body is what happened next: a cross-shaped base that bolts flat to a table, a closed frame around the slide holder, and printed rods running either side of each lead screw so the drive block cannot yaw as it travels.

It still comes off the bed in one piece. You still bolt on two motors, and it still moves.

Fig. 5 — The body printing, layer by layer, from the source CAD. Motors, screws and rods are hidden here: everything on screen during the reveal is a single print.

The mechanismDetail B · 26 mm

It bends instead of sliding.

The slide holder hangs on folded flexure beams and nothing else. Each drive block is tied to the frame by thin blades that bend, so it travels in a straight line along its own lead screw and resists every other direction. No friction to overcome, no backlash to unwind, nothing to shim into alignment by hand.

That is the trade the stage makes. Give up long travel, and precision stops being a machining problem. It becomes a printing problem — and printing is cheap.

Detail B — Blades cycling against their own datum outline. Only the blades bend; the base, the frame, the motor mounts and the lead screws are rigid. Deflection is exaggerated by roughly four thousand times.

On the benchFig. 6 · Setup

Four bolts to an optical table.

The base is a flat cross with a clearance hole at each arm, so the stage drops straight onto a standard breadboard on the 25 mm grid. Nothing is kinematic, nothing is bonded: bolt it down, and the frame borrows the table's mass.

Above it sits whatever writes. Here that is a mask and a projection lens pointed straight down at a post standing on the slide holder, which carries the sample clear of the frame. The beam never moves. The stage does all of the work.

Fig. 6 — The stage bolted to a 254 × 218 mm breadboard, with the sample post on the slide holder. Board and post follow the setup CAD; the stage itself is the source geometry.

Step and repeatFig. 7 · Live

The beam stays still. The wafer moves.

A 5 × 5 mm diced wafer sits on a post on the slide holder, lifted clear of the frame. The optics are fixed overhead. Each field is printed in a single shot through a mask, so the die is patterned a field at a time, and the shutter stays closed while the stage travels to the next one.

The mask carries one test cell — two bond pads, a supply rail, a single transistor with its gate finger, and a pair of meander test structures — imaged into a 900 µm field, the whole cell at once. Then the stage steps 900 µm, settles, and the shutter opens again. Nine fields in a 3 × 3 grid cover 2.7 × 2.7 mm of the die, inside the 3 mm envelope, and the whole thing repeats until the die is full.

Die5 × 5 mm diced
Written field900 × 900 µm
Fields per mount9 3 × 3
Step between fields900 µm
Field-to-field overlay210 nm stage limit

Fig. 7 — Live simulation of a step-and-repeat exposure. Stage travel is drawn one-to-one; die, fields and pattern are to scale. Feature size is set by the mask and the projection optics above, not by the stage — the stage decides only where each field lands.

Why it mattersThe argument

Lithography for the rest of us.

Patterning is how you turn a material into a device. Almost nobody gets to try.

Every microfluidic chip, every photonic waveguide, every MEMS sensor starts the same way: something has to put a pattern on a substrate with sub-micron placement. The optics for that are increasingly within reach — a UV source, a mask, a projection lens, a shutter. The stage under them has not been. A positioner good enough to place one field next to the next has cost more than most departments spend on a whole experiment, and that single line item is where a great many good ideas quietly stop.

This is the part we can fix. A stage that prints in one piece for about ₹1,500 turns the expensive half of a lithography tool into a consumable. A student can print two, break one, and keep going. A school can bolt one to a table beside the microscope it already owns. A lab in a place with no cleanroom can write real patterns on real substrates and find out whether the idea works before anyone writes a grant.

We are not claiming a fab on a bench. We are claiming that the positioning stage should stop being the reason you never tried.

What this is not

  • Not a resolution claim. The smallest feature you can write is set by the wavelength and the optics overhead, not by the stage.
  • Not a cleanroom. No filtered air, no temperature control, no vibration isolation beyond the table you bolt it to.
  • Overlay between fields is bounded by the stage's repeatable increment, currently 210 nm, and by whatever the frame drifts through a long write.
  • The exposure shown here is a simulation built from the stage's measured numbers. Patterned substrates from this setup are the next thing we publish.
Measured performanceFig. 1 · Live

Moves in Nanometers

Under optical tracking the stage resolves individual increments below 20 nanometres — roughly one four-thousandth the width of a human hair — against a measurement noise floor of 0.6 nanometres. The smallest increment it repeats dependably, move after move, is 210 nanometres. Both numbers belong to a machine built for the price of a good pair of shoes.

Resolved incrementbelow 20 nm
Repeatable increment210 nm (per 25 microsteps)
Noise floor0.6 nm
Build cost₹1,500 ($15.6)
ConstructionOne monolithic print

Fig. 1 — Live simulation of the slide holder seeking random targets inside its travel envelope. The holder moves on both axes; each drive block and its hardware travel only along their own lead screw, and the blades bend to take up the difference. Frame, base and motors are rigid. Displacement against the datum outline is magnified roughly 4,000×.

Optical trackingFigs. 3–4 · Measured

Measured, not modelled.

Every number on this page came off the bench. A marker on the slide holder, filmed at 20 frames per second and tracked frame by frame against a calibrated scale. Two runs from that work are below.

Staircase plot of nine commanded moves at 25 microsteps each, with a step-size histogram and linearity residuals.
Fig. 3 — Coarse commands, 25 microsteps each. Nine moves average 210 nm with a coefficient of variation of 0.13 and no retrograde motion; the fit gives 214.4 nm per command, worst residual 52 nm over 2.33 µm of travel. Driven one microstep at a time the same stage averages 6.8 nm, but the scatter is larger than the mean and a quarter of commands run backwards. That contrast is why 210 nm is the number we stand behind.
Tracking run showing driven and parasitic axes, staircase detail, step-size distribution, measurement noise floor and cross-axis coupling.
Fig. 4 — Single-microstep commands on the Y axis. The half-second plateau means resolve individual increments well below 20 nm. Across a quiet stretch the measurement noise floor sits at 0.57 nm on Y and 1.36 nm on X, against a camera pixel of 57.3 nm, so the tracker is reading far finer than one pixel. Cross-axis coupling runs at 9.2 per cent.

Notes

  • Sub-20 nm individual increments optically resolved, against a 0.6 nm measurement noise floor.
  • Minimum reliably repeatable increment is currently 210 nm, at 25 microsteps per command.
  • Single-microstep commands resolve below 20 nm but do not yet repeat: 15 per cent land dead, and a quarter reverse.
  • All figures are from video tracking. Independent interferometric validation is the next step.
Where it sitsPublished datasheets

Not the finest. The cheapest by three orders of magnitude.

A piezo stage will out-resolve us by a factor of fifty. A bearing stage will out-travel us by a factor of four. Neither of them comes off a print bed for the price of lunch, and that is the whole argument.

StageTravelFine motionPrice
F2R-XY-01XY · printed flexure + stepper 3 × 3 mm <20 nmresolved; 210 nm repeatable (per 25 microsteps) ₹1,500≈ $15.60
Thorlabs NFL5DP20X only · steel flexure + 20 µm piezo 5 mm20 µm piezo 20 nmopen loop; 10 nm on the −S ≈ $945+ driver
Newport 9062-XY-NP-MXY · gothic-arch bearings, Picomotor on Y, micrometer on X 12.7 mm <30 nmmin. incremental motion, Picomotor axis On request
Newport NPXY100XY · piezo + flexure 100 µm 0.2 nmopen loop ≈ £3,854+ amplifier
Newport NPXY200SGXY · piezo + flexure + strain gauge 200 µm160 µm closed 4 nmclosed loop; 0.4 nm open ≈ £6,577+ amplifier
Figures from manufacturer datasheets, checked August 2026. Not a like-for-like comparison: the piezo stages resolve far finer than we do, but only across a hundred microns, and every stage listed here needs a controller or amplifier that is priced separately. Prices are indicative list, before tax and shipping.
Bill of materialsEx works, 2026
₹1,500≈ $15.6
in materials

The XY stage costs about ₹1,500 to build. That is $15.60 in materials.

In less time than it takes to fill in a quotation form for a commercial stage, you could be doing real positioning work on an F²R.

Writing patterns. Scanning samples under a microscope. Aligning optics. Building instruments nobody has thought of yet.

The hard part of nanopositioning was never the physics. The hard part was affording it.

QuestionsAsk us more

The things people ask.

How can a 3D print position to 20 nanometres?

Because nothing slides. The stage moves by bending 0.5 mm blades of plastic, and a blade under load deflects by an amount set by its geometry, not by its surface finish. Layer lines and printer tolerance would wreck a sliding bearing; they barely matter to a flexure. Precision moves from the machine shop into the CAD file, and CAD is free.

What is the difference between resolved and repeatable?

Resolved means we can see the stage make a move that small: individual increments below 20 nm show up cleanly above a 0.6 nm measurement noise floor. Repeatable means you can ask for that increment and get it every time. Today that number is 210 nm. The gap between the two is honest work still to be done, and it is why both numbers are on this page.

So what resolution can it write?

That is the wrong question to ask the stage. Feature size comes from the wavelength, the numerical aperture and the resist. The stage decides where a feature lands, not how small it is. Ours will place one field next to the next to within its repeatable increment, currently 210 nm, which is what sets overlay across a step-and-repeat job. Feature size is the mask's problem; placement is ours.

What would I need on top of the stage to actually write?

A source, a mask carrying your pattern, a lens to project it onto the substrate, a shutter, a coated substrate, and controls that can sequence them together. None of that is in the ₹1,500. What the ₹1,500 buys you is the part that used to cost more than all of it put together.

How far does it travel?

About 3 mm on each axis. That is the trade a flexure makes: the blades have a finite elastic range, and pushing past it costs you linearity long before it costs you the part. A 5 mm die needs two mountings to cover; if you need centimetres in one go, you want a bearing stage.

How was it measured?

Video tracking. A marker on the slide holder, filmed at 20 fps and tracked frame by frame against a calibrated scale, with sub-pixel centroid fitting. Independent interferometric validation is the next step, and until that is done every figure here should be read as tracker-derived.

What do I need to build one?

A printer that can hold a 0.5 mm wall cleanly, two small stepper motors with drivers, a microcontroller, and the screws, rods and lead screws in the bill of materials. Print, bolt on the motors, flash the firmware. There is no assembly step in between, because there is nothing to assemble.

Can I buy one instead of printing it?

Yes. We build XY Lab to order with its stepper drivers and your choice of Arduino Nano or ESP32, for ₹2,500 including shipping within India — order one here. Pilot builds, lab sets and collaborations go to the same inbox, and a human answers.

Something not answered here? Send it over — this list grows from real questions.

Get oneTwo ways

Build it, or buy it built.

The stage is open source. The repository is where the project lives, and it fills out as each part of the build is cleaned up and documented. Clone it, print it, drive it past where we stopped — and tell us what breaks. No printer, or no time? We will print, assemble and check one for you.

Option A · Open source Assemble XY Lab Free files and the parts list. About ₹1,500 in parts and a printer that holds a clean 0.5 mm wall. Get the files ↗
Option B · Pre-assembled Buy one built Printed, motors fitted, drivers and an Arduino Nano or ESP32 in the box. ₹2,500, shipping within India included. Buy · ₹2,500 →

github.com/atharvdubey22ug-glitch/XY-Stage-files — and if you write something with one, we very much want to see it.

Distribution for realityReplies from a human

Contact us

Collaborations, pre-orders, questions about the characterisation, or an application we haven't thought of. A human reads every message, and answers quickly.

atharvdubey.nj@gmail.com
+91 81092 85020
github.com/atharvdubey22ug-glitch/XY-Stage-files

Supported by an equity-free grant from , the Frugal Founder’s Fund.

F²R fiction to reality
F²R instrumentation
atharvdubey.nj@gmail.com · Tel. +91 81092 85020
F2R-XY-01 / AN-01

© 2026 F²R — Fiction to Reality. Application note AN-01 · Step-and-repeat lithography / F2R-XY-01. Stage figures obtained by video-tracking characterisation and may vary between builds. The exposure sequence on this page is a simulation driven by those figures.

F2R-XY-01 · XY Lab · Loading geometry