Joint project UM6P · EHU · from Fadila El Kouihen's thesis to neutron and synchrotron beam time

The 12 cathodes, as structures to be determined

Fadila El Kouihen's thesis made cobalt-low NCA and cobalt-free NMA cathodes, doped them in four design lines and coated one for solid-state cells. It refined their cells on laboratory Cu Kα data and read their Li/Ni mixing from an intensity ratio, I(003)/I(104). Every argument it builds is about where the nickel goes. This page shows what each probe can see in these cathodes, what every material will be measured with, and which structural question each measurement answers.

12materials2with a refined Li/Ni mixing, today10open structural questions5probes≈ 25shifts in the first round

Who can be told apart, layer by layer

A powder pattern measures a site's total scattering. X-rays weigh each atom by its electrons, Z; neutrons by its coherent scattering length, b, which is negative for lithium and manganese. Two occupants of a site can be separated only by a probe in which they differ, and a valence by none: that needs the absorption edge.

What each probe sees, computed

The NMA reference, LiNi0.8Mn0.15Al0.05O2 in R3̄m. For each question, two models that differ by that question alone; the structure factors of both from diff-ref-struct's core; the change of the powder pattern measured.

Share of the scattering power, Σnf² for X-rays and Σnb² for neutrons. Nickel dominates both; in neutrons oxygen carries 42 % and manganese scatters with the opposite sign. Natural Li, Mn and Co absorb: μR ≈ in an 8 mm can, correctable.
Cu Kα, 2θ ≤ 90°D2B neutrons, 1.594 ÅID22 X-rays, 0.354 Å
Rdiff = Σ|IB − IA| / ΣIA over reflections grouped by d, log scale. The factor at the right compares D2B with Cu Kα when neutrons see more, the better X-ray probe with D2B when X-rays do; "alike" when the three are within 30 %. Rdiff measures contrast, not precision: where both probes see a parameter, refining them together removes what either leaves correlated.

The materials: what is known, what each will get

The twelve materials as the thesis designed them: the cobalt line from NCA to the cobalt-free NMA, and the branches that dope or coat NCA and NMA. Colour by what the thesis determined, or by how many probes are planned. The squares under each value are the planned determinations. Select a material for what was refined, what does not close, and what each measurement will determine for it.

D2BID22operandoEXAFSPDF
Co reduction (§II.6.1)Fe/Sb co-doping (§II.6.2, II.6.5)Mg, Y, La substitution (§II.6.3)Sc, Na single-site (§II.6.4)LiNbO₃ coating, solid state (Ch. IV)

Cells with a bold frame are the key set K9, measured with high-resolution neutrons. "n/a": the thesis gives no value for that material in that mode. Ni²⁺ is computed from the nominal formula with the usual valences; the Fe/Sb–NMA formula as printed has 1.10 metals and gives 0.55.

Ten questions, five probes

● the probe that answers the question; ○ one that does not answer it alone but fixes a quantity the answer needs (a composition, a lattice, a valence). "Home" is the work before beam time: the lithium balance, surface species, XPS and Mössbauer, lab XRD with an internal standard.

How to read the circles

In the refinement sense: a ○ probe does not answer the question by itself, but measures something the answering probe's refinement needs, a fixed value that cuts down what the answer can be. In Rietveld terms it supplies a constraint or a restraint.

  • F01Where the nickel is. D2B is ●: it refines Ni and Mn on both layers, and only neutrons tell Ni from Mn. ID22 is ○: it fixes the cell and the peak shape, and with resonant data at the Ni K edge gives an independent check. Home is ○: the ICP composition and charge balance bound how much Ni can be on the Li layer.
  • F02How much lithium. D2B and home are both ●: neutrons refine the Li occupancy of the bulk, the titration and washed ICP separate the surface lithium. Without the second, a Li deficit in the bulk and Li₂CO₃ on the surface look the same.
  • F03The metal layer and the Ni valence. D2B is ● for the Mn/Co/Ni occupancies; EXAFS is ● for the Ni²⁺ fraction, which charge balance predicts and the Ni K edge measures.
  • F05Fe and Sb. EXAFS is ●: Sb K and Fe K give valence and local site. Home (Mössbauer) and the joint refinement are ○: they close the formula that the valences must fit.

So the circle is a supporting measurement: it does not see the answer, it removes the alternatives.

Bayesian probability refinement · BPR

Each technique narrows what the structure can be

Read the grid as probabilities. No single technique determines these cathodes, but each one rules out part of what they could be, and together they leave little room. The spirit enters twice: it decides which experiments to ask for, and later how their results are analysed together.

Before the beam · design

Choose the combination, not the instrument

Every structural parameter has a probe that sees it (●) and others that remove what it trades off against (○). For the mixing both diffraction probes see it, so the design is the joint refinement; for the identity of the metal only neutrons see it; for the valence only the edge. The next step after the contrast computed above is the expected width of each answer for each combination, from the same structure factors with realistic counts.

After the beam · analysis

One model, every measurement

One structural model of each material, and every measurement a term in its probability: the ID22 and D2B patterns as two likelihoods sharing the cell and the metal layer; ICP, titration and XANES as priors on the composition, the surface lithium and the Ni valence, with their uncertainties. The result is a distribution: how much Ni sits on the Li layer, how much of it is Mn, how sure the combined data are.

ParameterSeen by (likelihood)Narrowed by (prior, constraint)What the combination removes
Ni on the Li layerD2B, ID22ICP; charge balance; Ni K edge (Ni²⁺)the correlation of mixing with displacement parameters, absorption and preferred orientation
Ni or Mn on the Li layerD2BID22 resonant at the Ni K edge; ICP Mna metal on the Li layer of unknown identity
Li contentD2Bwashed ICP; titration of LiOH and Li₂CO₃surface lithium counted as bulk
Ni²⁺ fractionNi K XANESrefined Li-layer Ni; charge balancea valence inferred from a formula
Dopant site (Y, La, Mg, Sc, Na)ID22 (Y, La), D2B (Mg, Sc)Y K, La K, Sc K EXAFS; second-phase fractionsa site read from a cell shift
Fe, Sb valence and the formulaFe K, Sb K XANESMössbauer; ICP; joint refinementa formula with 1.10 metals and an asserted Sb⁵⁺

diff-ref-struct already shows the path of a refinement in configuration space (its Explore module); the Bayesian layer, posterior distributions over the same parameters, is the extension this project would use first on real data.

From the samples to the beam, 2027

Separate proposals that cite each other and the garnet proposals of the companion project. Shift counts are estimates, to be checked with each instrument's contact. A shift is 8 h.

P0 · at homeLithium balance, surface species, XPS, Mössbauer, lab XRD with SiNov 2026 – Feb 2027
ILL · 15 Feb 2027P1 D2B, the key set K9 and two cycled electrodes (≈ 6 shifts)two-thirds of proposers from member countries
ESRF · 1 Mar 2027P2 ID22, all twelve (≈ 4) · P3 operando ID31/ID15A (≈ 6) · P4 BM23 (≈ 9)Sc K on BM08 / BM20 · BM25 SpLine as the Spanish route
BeamILL cycle 202 (23 Mar – 24 May) or later; ESRF Aug 2027 – Feb 2028joint refinements in diff-ref-struct
P5 · Sep 2027The coated cathode in the solid-state cell: PDF, Nb Kwith the garnet strand of the joint project