Quantum Clarity LLC · HELIOS Project · March 2026

Electronic Bifurcation in NMC811 Battery Cathodes: A Hidden Phase Boundary Revealed by Quantum Simulation

At roughly 50% discharge, Ni-rich cathodes appear to operate near an electronic phase boundary. Ensemble VQE diagnostics map this boundary for the first time and reveal how cobalt, manganese, and aluminium each suppress it through mechanistically distinct pathways.
385 VQE Runs 4 Dopant Systems ~8 kcal/mol Basin Gap NVIDIA L40S · ganymede ~955× instability increase vs fully-lithiated baseline

⚡ The Problem

Ni-rich NMC811 cathodes deliver the highest energy density of any commercial lithium-ion chemistry — but they degrade faster than their lower-nickel counterparts, particularly near 50% state of charge. The root cause has remained poorly characterised at the electronic level.

What's known empirically

Voltage hysteresis, cracking, and oxygen loss all intensify around the mid-charge window. Cobalt and manganese additions help — but the mechanistic reason has not been directly demonstrated computationally.

What standard methods miss

DFT and classical force fields treat electronic structure as a single ground state. They cannot detect the co-existence of competing electronic configurations that this study directly reveals.

🔬 Our Approach: Ensemble VQE Landscape Diagnostics

Rather than computing a single ground state, our method runs many independent stochastic optimisations and analyses the resulting distribution of converged electronic solutions. The spread of those solutions — and whether they cluster into one basin or two — is the diagnostic signal.

🎲

Multi-seed ensemble

15–35 independent VQE runs per condition, each with a different random initialisation. Landscape topology emerges from the ensemble distribution.

📐

Symmetry-breaking probe

Controlled Jahn–Teller distortion (B3) breaks the local Ni–O octahedral symmetry, revealing latent electronic branches invisible at symmetric geometry.

📊

Basin detection

Energy scatter (σ), inter-basin gap, and basin count diagnose whether the landscape is single-valley or multi-valley — and by how much.

🔄

Substitution screening

Identical protocol repeated with Co, Mn, and Al substituted at the Ni bridging-oxygen site. Same probe, four mechanistically distinct responses.

💡 Key Discovery: Electronic Bifurcation at Mid-Charge

At the half-delithiated state (Li₁), the Ni-rich cluster undergoes a symmetry-hidden electronic bifurcation under a Jahn–Teller distortion probe. The energy landscape splits into two distinct basins — separated by ~8 kcal/mol — with zero overlap between the two populations of converged VQE solutions. The simulations use a Ni₂O₃Liₓ cluster model that captures the local electronic environment of the Ni–O octahedral site while remaining tractable for ensemble VQE calculations — not a full cathode lattice.

8.09
kcal/mol inter-basin gap (Ni Li₁ + B3)
3.75
kcal/mol σ — energy scatter at bifurcation
955×
instability ratio vs. fully-lithiated baseline
0
energy range overlap between two basins

The distortion does not create the instability — it reveals it. The JT probe acts as a symmetry-breaking detector that exposes a competing electronic configuration already present in the Ni²⁺/Ni³⁺ mixed-valence manifold. Without the probe, that branch is invisible to standard computation.

The Four-System Electronic Fingerprint

Substituting Co, Mn, and Al at the same site and applying the same probe produces four mechanistically distinct responses — a complete electronic fingerprint of the NMC chemistry family.

Ni
Bifurcation
d⁸/d⁷ · eg¹
Two competing basins appear. 8.09 kcal/mol gap. JT splits the partially-filled eg orbital.
Co
Suppresses
d⁷/d⁶ · low-spin
Second basin absent. eg degeneracy removed. σ drops 55% vs Ni. Gap = 0.
Mn
Stabilises
d³ · t₂g³ · JT-inactive
σ decreases under distortion (0.55× ratio). Resolves orbital ambiguity rather than splitting.
Al
Orbital depletion
d⁰ · no d-manifold
Single basin. No bifurcation channel exists. Roughens without splitting (2.38× ratio).
Dopant d-config B3/B0 σ ratio Basin behaviour under B3 Mechanism
Ni d⁸/d⁷ (eg¹) 2.22× Bifurcates — 2 basins, 8.09 kcal/mol gap JT splitting of eg¹
Co d⁷/d⁶ 1.43× Single basin, gap = 0 Orbital branch removal
Mn d³ (t₂g³) 0.55× Single basin — σ decreases Ambiguity resolution
Al d⁰ 2.38× Single basin, no bifurcation d⁰ orbital depletion
Transition-metal d-electron count axis
d⁰
Al
Orbital depletion
Mn
Ambiguity resolves
d⁷/d⁶
Co
Branch removed
d⁸/d⁷
Ni
Bifurcation ⚠
Increasing d-electron count and JT-activity →

🔵 Electronic Boundary Interpretation

The four-system substitution series suggests that the Ni configuration sits close to a transition between single-basin and bifurcated electronic regimes. Substituting Co, Mn, or Al moves the system back into a single-basin landscape — but through three distinct electronic mechanisms.

This is consistent with the idea that Ni-rich cathodes operate near an electronic bifurcation boundary where small perturbations — from strain, thermal fluctuations, or Li ordering — can alter the topology of the electronic landscape.

The results are consistent with Ni-rich cathodes operating near an electronic phase boundary. Only the Ni configuration produces a two-basin topology. All dopant substitutions remain single-basin under the same distortion — but through four mechanistically distinct pathways. The pipeline classifies mechanism, not just stability outcome.

⚡ Why This Matters

The electronic bifurcation at mid-charge is a candidate mechanism for several empirically observed failure modes in high-nickel cathodes that have not previously had a direct electronic-structure explanation.

Voltage hysteresis

Path dependence in charge/discharge curves is consistent with the system toggling between two competing electronic basins.

Rate sensitivity

A bifurcation threshold crossed by thermal or mechanical fluctuations would create strong sensitivity to cycling rate and temperature.

Crack formation

Electronic bifurcation under local strain is consistent with particle cracking concentrated at mid-charge — the known failure window.

Why Co and Mn help

This is the first direct computational demonstration that Co and Mn suppress the instability through different electronic mechanisms — not a single stabilisation pathway.

The distortion threshold insight: The amplitude ladder experiment shows the Ni landscape first stabilises under small distortions before bifurcating at larger ones. This establishes a critical threshold — the instability is not inevitable, it is triggered. Small perturbations in real cells (strain, Li ordering, thermal fluctuations) near this threshold could push the system across the boundary.

🧪 Computational Screening

The four confirmed systems define a mechanism-class framework that converts the pipeline from an empirical screen into an electronically-informed one. Candidate dopants can be assigned a predicted class before simulation based on d-electron count and ligand-field logic.

Mechanism classes

Class A (eg-active): Likely to bifurcate — Ni³⁺-like d⁷, Cu²⁺-like d⁹.

Class B (branch-removing): Suppresses bifurcation — Co confirmed, Rh/Ir analogues predicted.

Class C (ambiguity-resolving): Stabilises — Mn confirmed, Cr³⁺ predicted.

Class D (d-depleted): Single-basin roughening — Al confirmed, Mg²⁺, Ti⁴⁺ predicted.

Design rule

Prefer dopants that remove the Ni eg¹ branch (Class B), resolve ambiguity without creating new branches (Class C), or deplete the local d-manifold (Class D).

Avoid dopants that introduce new symmetry-sensitive partially-occupied eg states (Class A).

Next validation targets: Cr³⁺ (Class C predicted) and Mg²⁺/Ti⁴⁺ (Class D predicted).

This framework enables rapid computational pre-screening of dopants and coatings before experimental synthesis. Because each candidate requires only ~3–4 GPU hours, the approach can evaluate dozens of potential modifications in days rather than months of laboratory iteration.

~3–4 GPU hrs / candidate · single L40S
Dopant Predicted class Predicted response Status
Ni (d⁷)Class ABifurcates✅ Confirmed
Co (d⁷/d⁶)Class BSuppresses✅ Confirmed
Mn (d³)Class CStabilises✅ Confirmed
Al (d⁰)Class DSingle-basin roughening✅ Confirmed
Cr³⁺ (d³)Class CMn-like stabilisation🔬 Predicted
Mg²⁺ (no d)Class DAl-like roughening🔬 Predicted
Ti⁴⁺ (d⁰)Class DAl-like or mixed🔬 Predicted
Cu²⁺ (d⁹)Class APotentially Ni-like⚠️ Caution

🌐 Broader Vision

This work is part of the Quantum Clarity electronic-structure platform — applying GPU-accelerated ensemble VQE to problems where electronic topology determines material behaviour. The same methodology that revealed the NMC bifurcation is directly applicable across energy and catalytic materials.

Battery cathodes

NMC, NCA, and LNMO families. Screen dopants and coatings for mid-charge bifurcation suppression before synthesis.

Solid-state interfaces

Stack pressure in solid-state cells maps directly onto the B3 distortion amplitude — the same probe, a new physical context.

Transition-metal catalysis

JT-active sites appear across CO₂ reduction, water oxidation, and C–H activation. The bifurcation diagnostic applies wherever eg degeneracy is at play.

Electronic topology mapping

Beyond stability ranking — mechanism classification. The platform detects which electronic phase boundary a system operates near, not just whether it is stable.

📊 Campaign Metrics

System
Ni₂O₃Liₓ cluster (x=0,1,2)
Active space
(10e,10o) · 20 qubits
Ansatz
UCCSD depth 6 · ~3100 Pauli terms
Total VQE runs
385 (383 valid · 99.5%)
Dopant systems
Ni · Co · Mn · Al
Seeds per condition
15–35 independent
Hardware
NVIDIA L40S · ganymede
Total GPU time
~38 hours

Connect & Collaborate

Results are in preparation for submission to ACS Energy Letters / Journal of Power Sources. Dataset publication pending. Interested in screening your dopant candidates or coatings?

Coming soon: Zenodo dataset · Cr³⁺ and Mg²⁺ validation runs · NCA extension