Proof of format

A complete LabForge recipe — redacted sample

The actual working document the engine ships — every field, every section, the real structure. The exact setpoint values are redacted here, the way a directory hides an unlisted number: you can see there is a complete spec — mechanism, full process, equipment, expected result, QC acceptance, failure modes, the engine's own revision log — but the numbers are what you buy. Your Single Recipe unlocks the sharp spec, calculated for your chamber. One worked example (an evaporation route); sputter and reactive-sputter recipes are produced to the same depth.

LabForge recipe report · client & job ID redacted

✓ FEASIBLE PHYSICS: ESTABLISHED (L1) CONFIDENCE: HIGH PROFILE: GENERAL MATERIALS
🔒 Values redacted

Every field below is real and complete — the exact setpoint values are obscured, like an unlisted number. The sharp recipe, calculated for your chamber, ships with a Single Recipe — $599.

Develop an amorphous-carbon Zernike-type phase plate to correct aberration-induced phase-contrast loss in a TEM electron column.

The complete deliverable — nothing summarized

A LabForge recipe is a full, run-ready specification. This one contains all of the following, and so will yours:

recipe contents
route selection    the candidate process + why it was chosen
mechanism         the governing equation + every derived value
process spec      every step, every setpoint — pressures, rates,
                  powers, temperatures, times, tolerances
equipment         the exact tools the route requires
expected result   what the finished film does, quantified
QC acceptance     measurable pass/fail criteria
failure modes     where the process will drift, and the guard
revision log      the engine's own self-corrections, shown
stated limits     what the route does NOT do — plainly

Amorphous-carbon Zernike thin-film phase plate, back-focal-plane placement

The unscattered central beam passes through a FIB-milled center hole; scattered beams traverse the carbon film and acquire a π/2 phase shift, restoring low-spatial-frequency phase contrast.

mechanism & derived values
mechanism          Δφ = σ(E) · V0 · t
target phase       π/2   (1.5708 rad)

σ (200 kV)         0.00729 rad/(V·nm)
σ (300 kV)         0.00653 rad/(V·nm)
V0 (a-C)           7.8 ± 0.6 V   (mean inner potential)

t (π/2)            30.9 nm @ 300 kV · 27.6 nm @ 200 kV
working band       27–31 nm across 200–300 kV
calibration       V0·t confirmed per run by EELS log-ratio

The engine caught and corrected its own first draft

Before this recipe shipped, the engine ran its own numbers back through the physics — and flagged three corrections:

  1. Re-anchored the relativistic interaction constant σ — a one-voltage-step ladder error worth 10–15% drift in the phase calculation.
  2. Corrected the π/2 target thickness from 15 nm to 30.9 / 27.6 nm — which then reproduced the canonical published value (~31 nm carbon at 300 kV; Danev & Nagayama, Ultramicroscopy 88, 2001) exactly.
  3. Replaced a post-FIB O₂-plasma clean with a vacuum bake — the plasma step would have etched the ~30 nm carbon film it was meant to clean.
Why this matters

The engine self-corrected — and its corrected answer landed on a value published in the literature 25 years ago, without being told. That is the difference between derived physics and looked-up numbers.

Six steps — substrate prep to QC, every setpoint

Substrate preparation

Freshly cleaved mica carrier; the film is later floated onto a molybdenum grid. Plasma-clean the bare grid only — never the finished film (step 5).

carrier          mica, ASTM V2 grade, freshly cleaved
grid             molybdenum, 300 mesh
solvent clean    acetone / IPA, ultrasonic, 5 min
plasma (grid)    Ar/O₂, 20 W, 2 min — bare grid only
base pressure    8 × 10⁻⁷ Torr

Carbon film — e-beam evaporation

The load-bearing step. Recalibrate the QCM tooling factor against EELS log-ratio on a witness sample before the run — mean inner potential and film density co-vary, so the tooling factor is confirmed, not assumed.

target thickness  30.9 nm @ 300 kV · 27.6 nm @ 200 kV
thickness band    27–31 nm (voltage-dependent)
deposition rate   0.03 nm/s
chamber pressure  5 × 10⁻⁷ Torr
source            pyrolytic graphite, 99.999%
throw distance    300 mm
substrate motion  static (no rotation)
substrate temp    293 K
QCM density       2.0 g/cm³ (recalibrate tooling vs EELS)

Float-off & grid transfer

Release the carbon film from the mica onto a clean water surface and transfer it to the Mo grid. Handle wet-to-dry to avoid tearing the ~30 nm membrane.

FIB center-hole milling

Mill the central aperture that passes the unscattered beam. Milling time scales with the corrected (thicker) film.

ion source       Ga⁺ @ 30 kV
beam current     10 pA
hole diameter    0.7 µm ± 0.05
milling time     ~16 s (est., scales with thickness)

Contamination control — vacuum bake

No plasma on the finished film — O₂ would etch the amorphous carbon and drift the phase shift out of tolerance. Bake for contamination control, then operate the plate heated in-column.

vacuum bake      373–473 K · 30–60 min
plasma on film   none — O₂ etches a-C
in-column op.    heated holder, ~473–573 K
storage          high-vacuum desiccator, < 1 × 10⁻³ Torr

Characterization & QC

The measurements that confirm the plate meets spec before it goes into the column.

phase shift      accept 1.5708 rad ± 10%
thickness unif.  ± 2 nm
film thickness   EELS log-ratio map (calibrates V0·t)
phase verify     Thon-ring diffractogram — graphene / catalase
hole diameter    SEM/TEM, 0.7 µm ± 0.05

The exact tool set this route needs

equipment
deposition        e-beam PVD system with QCM rate monitor
film transfer     float-off station
aperture          FIB-SEM dual beam (Ga⁺)
metrology / QC    TEM (EELS + diffractogram capability)
pre-clean         plasma cleaner — pre-deposition, bare grid only

What the finished plate does

Installed at the back focal plane, the plate passes the unscattered central beam through the FIB hole untouched, while the scattered beams pick up a π/2 (1.5708 rad) phase shift traversing the carbon film. The result is restored low-spatial-frequency phase contrast — the weak-phase detail an aberrated, defocused column otherwise loses — at the ± 10% phase tolerance set in QC.

Where this process drifts — and the guard

O₂ plasma on the finished film

Etches the ~30 nm carbon, thins it by multiple nm, and drifts the phase shift out of the ± 10% window. Guard: plasma only on the bare grid (step 1); vacuum bake — not plasma — for the finished film (step 5).

Contamination & charging drift in-column

Beam-induced carbon build-up and charging shift the phase over a session. Guard: operate the plate heated (~473–573 K) and store under high vacuum between uses.

QCM tooling-factor error

Assumed density mis-reads deposited thickness, and V0·t misses π/2. Guard: recalibrate the tooling factor against an EELS log-ratio witness sample before the run (step 2).

Stated limitation of this route

What this route does not do

This plate compensates the contrast-transfer consequence of aberrations and defocus. It does not null the Cs/Cc coefficients themselves — that requires a multipole corrector or an adaptive-field device. Every LabForge recipe states its limits this plainly.

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