Joint project UM6P · EHU · from Zakaria Kharbouch's thesis to neutron and synchrotron beam time

The 38 garnets, as structures to be determined

Zakaria Kharbouch's thesis made 38 Ga-stabilised LLZO garnets in two families and refined two quantities per garnet, the lattice parameter and the phase fractions, on laboratory Cu Kα data. Every argument it builds on them is about lithium and about which site each dopant takes. This page shows what each probe can see in these garnets, what every one of the 38 compositions will be measured with, and which structural question each measurement answers.

38compositions2quantities refined each, today11open structural questions5probes≈ 29shifts in the first round

Who can be told apart, site by site

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 does not follow Z and is negative for lithium and hydrogen. Two occupants of a site can be separated only by a probe in which they differ.

What each probe sees, computed

The Ga–Ta reference, Li6.3Ga0.2La3Zr1.9Ta0.1O12 in I4̄3d, built from the neutron structure of cubic LLZO. 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. In X-rays La and Zr are 89 % of the pattern; in neutrons oxygen is more than half and lithium eight times more visible. Natural Li absorbs: μR ≈ in an 8 mm can, correctable.
Cu Kα, 2θ ≤ 100° (the thesis)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. Rdiff measures contrast, not precision: the synchrotron's counts and resolution make its small differences measurable, which is why X-ray and neutron data are refined jointly. X-rays without anomalous terms, since a powder adds F(hkl) and F(h̄k̄l̄).

The matrix: what is known, what each garnet will get

The 38 compositions of the thesis, each family branching from its co-doped reference into three La-site series. Colour by what the thesis determined, or by how many probes are planned. The squares under each value are the planned determinations. Select a cell for what was refined, what does not close, and what each measurement will determine for that composition.

D2BD20ID22EXAFSPDF
Family A · Chapter III · Ta5+ on the Zr site · Rietveld with all phases

Ga–M–Ta

Li6.3+(3−n)xGa0.2La3−xMxZr1.9Ta0.1O12
Family B · Chapter IV · Sc3+ on the Zr site · lattice parameter only

Ga–M–Sc

Li6.5+(3−n)xGa0.2La3−xMxZr1.9Sc0.1O12

The thesis gives phase fractions and Li₂ZrO₃ only for the Ta family; Sc cells show "n/a" in those modes. Cells with a bold frame are the key set K12, re-made fresh for the high-resolution neutron work. Nominal vacancies are 7 − Li from the weighing formula, M on the La site.

Eleven 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 site occupancy). "Home" is the work before beam time: fresh samples under argon, ICP-OES, TGA–MS, 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.

  • G02How much lithium, and where. D2B and D20 are ●: they refine the Li occupancies of 12a, 12b and 48e. Home (ICP-OES) is ○: it gives the total Li per formula unit, which the neutron refinement then distributes over the sites. Without it, the total Li and the displacement parameters trade off against each other.
  • G01The Ga site and the acentric distortion. D2B is ●. ID22 is ○: in the joint refinement it fixes the lattice parameter, the peak shape and the heavy atoms, so the neutron data are left to determine only Li, Ga and O.
  • G04Where Y sits. EXAFS is ●, the only direct view of Y's coordination. ID22 is ○: it measures the La-site occupancy, which, with the ICP total of Y, says how much Y is not on La. An indirect bound, not a site assignment.
  • G03Al from the crucibles. Home (ICP for Al) is ●. D2B is ○: once the Al content is known, the neutrons say which site it shares with Ga.

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 garnets, but each one rules out part of what they could be, and together they leave little room. That is the spirit of the project, in two moments: it decides which experiments to ask for, and later it decides 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 (○). A proposal is good when, for each question, the two are both in the plan. The contrast computed above is the first step: the pattern change says which probe sees a parameter. The next step is the expected width of the answer for each combination of probes, from the same structure factors with realistic counts, so that the shifts go where they narrow the answer most.

After the beam · analysis

One model, every measurement

One structural model of each composition, and every measurement a term in its probability: the ID22 and D2B patterns as two likelihoods sharing the lattice and the heavy atoms; ICP-OES and TGA as priors on the composition and the protons, with their own uncertainties, not as hard constraints; EXAFS coordination numbers as a prior on the Y site fraction. The result is not one set of numbers with esd's but a distribution: how much Li sits on 12a, 12b and 48e, and how sure the combined data are of it.

ParameterSeen by (likelihood)Narrowed by (prior, constraint)What the combination removes
Li per site, 12a 12b 48eD2B, D20ICP total Li; TGA protons; charge balancethe trade-off of Li occupancy against displacement parameters; H mistaken for Li
Ga on 12a, acentric O1/O2D2BID22 lattice, profile and heavy atoms; ICP GaGa and the distortion fitted against an uncertain cell and peak shape
Al on 12aICPD2B site scatteringan Al content with no site, or a site with no Al content
Y on La or on ZrEXAFS (Y K edge)ID22 La-site occupancy; ICP Y; resonant diffractiona site fraction inferred from a lattice parameter alone
Ba, Rb in the garnetD2B (Ba), ID22 (Rb)ID22 BaZrO₃ fraction; ICP; Rb K EXAFSa solubility read from a second phase instead of the garnet
Phase fractions, powder and pelletID22D2B (Li₂ZrO₃ contrast); ICP Zr/Lafractions that do not close the mass balance

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: no facility takes one combined X-ray and neutron proposal for materials. Shift counts are estimates, to be checked with each instrument's contact. A shift is 8 h.

P0 · at homeK12 fresh under argon; ICP-OES, TGA–MS, lab XRD with SiNov 2026 – Feb 2027
ILL · 15 Feb 2027P1 D2B, the key set (≈ 8 shifts) · P3 D20, the matrix and the ramps (≈ 6)two-thirds of proposers from member countries
ESRF · 1 Mar 2027P2 ID22, all 38 and the pellets (≈ 6) · P4 BM23, Y Rb Ga Zr edges (≈ 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 2027PDF (ID15A, D4c); the synthesis watched in situsecond round, on P1–P2 results