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Research method

Transmission Electron Microscopy (TEM)

Transmission electron microscopy forms an image (and often a diffraction pattern) from electrons that have passed through a thin specimen. Diameters, lattice fringes, selected-area diffraction and cryo-TEM pitch measurements report local size and order at the nanometre scale. In this library TEM is used to size silver and platinum particles, to check polymer vesicles after a SAXS run, to measure amyloid fibril helical pitch, and to watch pyrite cubes grow from clusters — each time on a small counted set of objects, not on the whole flask.

Materials chemists reach for TEM when the question is how big, how crystalline, or how the morphology evolved. It answers 'what does this thin region look like at nanometre resolution?' Its main limitation is sampling: tens of particles, a dried grid, or a reconstructed catalyst after electrochemistry need not represent the working ensemble, and TEM length scales are not SEM length scales.

Studies

24

Findings

6

7 supporting · 0 challenging · 0 qualifying citations

Open tensions

2

Currently

What we know

  1. TEM of a glycerol/PVP silver synthesis, counting ~50 particles, tracks a solvent knob that UV-vis only sees as SPR. Up to ~60% glycerol, particles stay ultra-small (<10 nm) with a stable 410–450 nm plasmon; above ~70–80% glycerol, SPR and size rise, spanning about 10–160 nm (extremes 1.8 nm and 159 nm). High glycerol viscosity also complicates DLS, so TEM is doing work that a single hydrodynamic diameter cannot.
  2. Stirring time is another TEM-readable size knob. Glutathione-capped Ag at 60 °C grows TEM diameters 3.20, 4.83 and 6.19 nm at 36, 48 and 72 h as fcc metal forms and SPR appears at 344–354 nm. Blackberry-leaf Ag is much larger by TEM (50–120 nm) with SPR at 449 nm — same metal, different length scale, both still images of dried particles.
  3. On a fuel-cell catalyst, TEM size splits into two populations whose electrochemistry is not equal. Heat treatment of 1.8 nm sputtered Pt on PEG/Vulcan carbon yields a bimodal 2.5 ± 0.8 nm and 6.7 ± 1.8 nm distribution; the larger particles dominate ORR activity. TEM here is the size histogram that rotating-disk voltammetry then ranks.
  4. After a ~2 mL in situ SAXS PISA run, TEM is the morphology check, not the nucleation clock. Micelles nucleate at 9–10 min by SAXS; worms appear near PHPMA DP 134 after 28–29 min; vesicles reach Dv = 227 ± 16 nm. HPMA conversion exceeds 99% within 80 min (GPC Mn 51 200 g mol⁻¹, Đ = 1.25). The SAXS clock is faster than the lab ¹H NMR rate jump.
  5. Cryo-TEM pitch can distinguish two amyloid polymorphs that mixed nucleation might have been expected to scramble. Aβ40 fibrils have a helical half-pitch of 162 nm versus 31 nm for Aβ42; first fibrils are Aβ42 (<13% Aβ40). Cross-seeding is weak versus self-seeding. Atomic mixed-oligomer structures are not solved.

Largest unresolved question

TEM and SEM are not interchangeable length scales. The glycerol silver paper uses TEM (~50 particles) for ultra-small (<10 nm) objects and SEM for larger particles as glycerol exceeds ~70–80% and sizes reach tens to 159 nm. Quoting 'electron microscopy showed 10 nm particles' without which microscope and which glycerol fraction mixes those regimes.

Procedure

How it works

The main stages of the method. Specific protocols and analysis choices vary between studies.

  1. Prepare a thin specimen

    Electrons only transmit through a thin region — a nanoparticle drop-cast on a grid, a microtomed slice, or a cryo film. Drying, staining, and which patch the operator photographs are already a sample, not a view of the whole flask.

  2. Pass electrons through the sample

    A high-energy beam is focused through the specimen in vacuum. Contrast comes from how much the local thickness, density, and diffraction scatter or absorb those electrons.

  3. Form an image or a diffraction pattern

    The transmitted electrons can be imaged (bright field, lattice fringes) or selected-area diffracted. Cryo-TEM can also measure helical pitch on a frozen hydrated object. Each mode reports local size and order at the nanometre scale.

  4. Count a small set of objects

    Diameters, cube edges, or vesicle walls are measured on tens to hundreds of particles. That distribution is what the grid held and what was photographed; DLS or a bulk assay can disagree without either being 'wrong.'

  5. Do not treat the micrograph as the working ensemble

    TEM answers what this thin region looks like at nanometre resolution. A crystalline nanocube on the grid need not be the electrocatalyst after cycling, a TEM diameter is not by itself the activity-determining size, and TEM length scales are not SEM length scales.

Common misconceptions

  • A TEM image is the whole sample.

    Glycerol Ag sizes rest on ~50 particles; DLS at high glycerol is compromised by viscosity. GSH-capped Ag still grows more polydisperse with time. A grid selects what dried and what the operator photographed.

  • If TEM shows a crystalline nanocube, that crystal is the electrocatalyst.

    NiFeS₂ porous cubes are pre-catalysts: after CVs the active material is amorphous S-doped metal (oxy)hydroxide. η₁₀ < 260 mV is measured on the reconstructed film, and a GCE η₁₀ is not a device metric.

  • Particle diameter from TEM is the quantity that determines activity.

    Bimodal Pt (2.5 and 6.7 nm) is both visible by TEM; ORR is dominated by the larger 6.7 ± 1.8 nm set. Size is necessary characterisation, not a substitute for a kinetic ranking.

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