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Research method

X-ray Photoelectron Spectroscopy (XPS)

X-ray photoelectron spectroscopy measures binding energies of core electrons ejected from the near-surface of a solid (typically the top few nanometres). Peak positions report oxidation state and liganding (S 2p of thiolate versus unbound thiol; Ni⁰ versus Ni–N single-atom signatures; Ni³⁺/Ni²⁺ ratios), and survey scans give atomic percentages. In this library XPS is used to argue what the surface is — a SAM, a carbon-coated Ni particle, a reconstructed LDH, a pyrolysis-free Fe site — not to measure a faradaic efficiency by itself.

Electrochemists reach for XPS when bulk diffraction cannot tell whether the working skin is metal, oxide, single atoms, or leftover ligand. It answers 'what oxidation states and heteroatoms sit in the photoelectron escape depth?' Its main limitation is that a surface ratio is not a catalytic cycle, Ti-supported films can confound O/C, and the absence of a Ni–N peak is an argument against one structural hypothesis, not a complete operando mechanism.

Studies

17

Findings

5

6 supporting · 0 challenging · 0 qualifying citations

Open tensions

2

Currently

What we know

  1. XPS can prove chemisorption of a thiol sugar on gold and still not give a binding constant. On ~15 nm citrate AuNPs and sputtered Au films, S 2p at 162 eV marks Au–S; C–O (286.5 eV) rises about six-fold on films after 1-β-D-thio-glucose. Nanoparticles retain ~30% unbound thiol and lower thioglucose density, hence weaker maltose-binding-protein uptake; SIMS peaks at 358 and 375 u mark TG–pocket complexes. No calibrated Kd is reported.
  2. XPS plus STEM can decide nanoparticle versus single-atom nickel for CO₂-to-CO electrolysis. Carbon-coated Ni on N-doped carbon (loading ~3.6–4.0 wt%) shows Ni⁰ and no Ni–N single-atom peak; HAADF-STEM sees 10–100 nm particles. CO faradaic efficiency reaches ~94% at −0.7 V vs RHE, with 22.7 mA cm⁻² at −1.1 V. Long-term MEA stacks and C2+ products are not claimed.
  3. Valence ratios from XPS/XAS can be the design handle for OER. NaBH₄ reduction of NiFe LDH raises Ni³⁺/Ni²⁺ from 0.39 to 1.32 and Fe²⁺/Fe³⁺ from 0.40 to 1.49, with oxygen vacancies near Fe by EXAFS. O₂ faradaic efficiency is 95.9% (7.48×10⁻⁵ mol O₂ at 50 mA for 10 min). A full electrolyzer lifetime and a complete microkinetic OER cycle are not provided.
  4. XPS also reports how much metal is actually on a molecular or pyrolysed catalyst. A pyrolysis-free Fe–PIPhen on Vulcan XC-72 has 0.748 at% Fe, onset ~0.85 V, average n = 3.94 at 1600 rpm, and H₂O₂ yield 1.6–3.1% (k₁/k₂ = 30–50). A Co–N–C material identified as isolated Co²⁺ in a CoN₄C₈-1-2O₂ motif (XPS with XANES/EXAFS/STEM) gives 97% azo yield and TOF 35.9 h⁻¹ — still without in-operando proof of the hydrogenation cycle.
  5. On photoelectrodes, XPS sits beside XRD/SEM/UV-vis rather than replacing them. AACVD BiOCl/Br/I films are phase-pure tetragonal matlockite; untreated BiOCl (p-type) and BiOI (n-type) are unstable for PEC, while BiOBr reaches ca. 0.38 mA cm⁻² at 1 V vs Ag/AgCl without a sacrificial donor. XPS does not by itself explain why Cl and I films fail stability.

Largest unresolved question

XPS is a surface vote; XRD/STEM decide how that vote relates to the bulk. The Ni CO₂ paper uses missing Ni–N XPS intensity plus 10–100 nm STEM particles to reject a single-atom picture; the Co–N–C paper uses XPS with EXAFS to assert isolated CoN₄. Same spectroscopy, opposite structural conclusions, because the materials differ — you cannot treat 'XPS showed the metal state' as portable.

Procedure

How it works

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

  1. Eject core electrons from the near-surface

    Soft X-rays illuminate the solid in vacuum; photoelectrons escape from typically the top few nanometres. Anything deeper than the escape depth is invisible, which is why XPS is a surface method rather than a bulk assay.

  2. Convert kinetic energy to binding energy

    The spectrometer measures kinetic energy; binding energy follows once the photon energy and a charge-reference are set. Charging, adventitious carbon, and the reference choice can shift apparent peak positions.

  3. Assign oxidation state and liganding

    Peak positions and shapes are fitted to species — thiolate versus unbound thiol, Ni⁰ versus Ni–N, Ni³⁺/Ni²⁺. Overlapping envelopes and shake-up structure make those fits model-dependent, not unique fingerprints.

  4. Report atomic percentages from survey scans

    Survey intensities are turned into atomic percent of the analysed surface. That composition is not a count of catalytic sites, and a support such as Ti can confound O/C so that a film is not a copy of the colloid.

  5. Read the skin, not the catalytic cycle

    XPS answers which oxidation states and heteroatoms sit in the photoelectron escape depth. Absence of a Ni–N peak is an argument against one site hypothesis, not a claim that nitrogen is absent from the support, and a surface ratio is not a faradaic efficiency or an operando mechanism.

Common misconceptions

  • If XPS shows Ni⁰ and no Ni–N peak, the catalyst cannot have any nitrogen and must be single-phase metal.

    The CO₂-to-CO paper argues metallic Ni nanoparticles (3.6–4.0 wt%) on an N-doped carbon support whose coating plus N suppress HER. Absence of a Ni–N single-atom signature is a site assignment, not a claim that nitrogen is absent from the support.

  • An XPS atomic percent of Fe is the active-site density that produces the RRDE electron number.

    Fe–PIPhen reports 0.748 at% Fe and n = 3.94 with 1.6–3.1% H₂O₂. Loading is low and part of the polymer is microcrystalline; there are no PEMFC data. XPS percent is composition of the analysed surface, not a count of catalytic turnovers.

  • S 2p at 162 eV on gold nanoparticles means every thiol is bound and the SAM is identical to a flat-gold film.

    NPs retain ~30% unbound thiol and lower thioglucose density than sputtered films, where C–O intensity rises ~6-fold. Ti-supported NP films also confound O/C, so film XPS is not a copy of the colloid surface.

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