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Simple algorithm for evaluating SU(2) non-abelian geometric phase in the vicinity of molecular conical intersection of odd electron number

Chenchen Song

Oct 30, 2026arXiv:2611.00434v1
physics.chem-ph
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Scorecard· 16/16
5.0/10 impact

Elegant, correct-looking geometric algorithm and symmetry theorems for a niche problem, but without independent numerical validation or any real-molecule application.

Abstract

Molecular conical intersection of odd-electron number are known to give arise to non-abelian geometric phases. In this work, we present a simple algorithm for evaluating the SU(2) geometric phases given a trajectory represented as a discrete set of coordinates in the 5-dimensional branching space. Motivated by the special property that such conical intersection behaves as abelian ones in 3-dimensional subspace, we take two steps to establish the algorithm. We first prove that it is possible to construct an augmented trajectory consisting of spherical triangles that has the same geometric phases as the original trajectory. We then prove that the geometric phase contribution from each spherical triangle can be evaluated from its properties using Stokes' theorem in a way that closely resembles abelian conical intersections. The total geometric phases are thus evaluated by path-ordered products of contributions from each spherical triangle. Based on the augmented trajectory, we further show that the geometric phases of the upper and lower states will switch under inversion transformation of the trajectory. This relation is further generalized to show that the Wilson loop, defined as the trace of the geometric phases, will switch between the two states under any 5-dimensional improper isometric transformation. Example calculations of geometric phases for trajectories generated on 5-dimensional polytopes are also presented and discussed.

AI Impact Assessments

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Core Contribution

The paper gives a closed-form, integration-free algorithm for computing the SU(2) non-abelian geometric phase (holonomy) along a discretized closed trajectory in the 5-dimensional branching space of a T²=−1 conical intersection, i.e. an odd-electron molecule with Kramers degeneracy. The key idea is that the Yang-monopole-like connection is abelian when restricted to any 3D S² subspace. The author inserts the north pole as an extra vertex and decomposes the S⁴-projected trajectory into a chain of spherical triangles. Each triangle contributes exp(−D̂σ/2) for the upper state or exp(−B̂σ/2) for the lower state. The area σ comes from the spherical SAS formula. The Berry connection factors D̂ and B̂ come from quaternion expressions of the longitudes. The total phase is a path-ordered product. The method needs no numerical integration of the connection and no explicit gauge transformations.

A second result relates the upper and lower state phases. Φ⁺ of a trajectory equals Φ⁻ of its inversion image on the opposite chart. The Wilson loop (the trace) is invariant under proper SO(5) transformations and swaps between states under improper ones. Trajectories with improper symmetry therefore have W⁺=W⁻. The examples are 5-simplex and 5-demicube trajectories. On the simplex, Wilson loop values split cleanly by permutation parity. On the demicube, the examples show path dependence and non-commutativity.

Methodological Rigor

The derivation is logically clean and builds on the author's earlier Yang-monopole paper. The abelianization on S² and the use of Stokes' theorem within charts, with a bridging segment λ to handle the chart transition, are carefully argued. The augmentation step relies on the pole-directed arcs contributing identity, which follows from A_θ=0. The parity result on the simplex is a nontrivial internal consistency check that the symmetry theorems predict correctly.

Weaknesses:

  • There is no independent numerical validation, such as comparing against direct path-ordered integration of the connection or against adiabatic propagation of a 4×4 Hamiltonian. The paper relies on analytic consistency alone.
  • No real molecular system is tested. The author admits that g and h vectors with spin-orbit coupling are not routinely available.
  • The straight-line interpolation in R⁵ is an assumption, and sensitivity to it is deferred.
  • Degenerate cases (antipodal points, poles, ϕ=0 or π) are handled via supplementary material.
  • There is no discussion of numerical stability or conditioning near the singular point or near the poles.
  • The method assumes the loop is in the vicinity of a single point-like intersection with fixed branching vectors, whereas real seams are curved.
  • Potential Impact

    The immediate audience is small: theorists working on geometric phases in molecular conical intersections with spin-orbit coupling, plus synthetic gauge field and Yang monopole communities (cold-atom work by Spielman et al.). The algorithm applies to any Hamiltonian of the form of Eq. 6, so it could serve holonomic quantum computing and the study of non-abelian Wilczek–Zee phases in quantum control. The paper suggests uses such as separating geometric forces from dynamical effects in non-adiabatic dynamics and designing molecular qubits. These are speculative at this stage. The Wilson loop symmetry relations (Eq. 55–56) are elegant and could guide interpretation, but they are of limited practical use without real-system data.

    Timeliness & Relevance

    Interest in non-abelian gauge structures, Yang monopoles and topological classification of non-adiabaticity in chemistry is rising. Spin-orbit-coupled non-adiabatic dynamics are a growing area, but the field is still bottlenecked by the lack of electronic structure tools for T²=−1 branching spaces. The paper addresses a computational gap that practitioners will only face once those tools mature, so adoption may lag.

    Strengths

  • The algorithm is simple, parallelizable and geometrically transparent, and it is explicitly tied to a prior rigorous framework.
  • The symmetry/Wilson loop theorems give genuine structural insight, including a parity criterion.
  • Python code and coordinates are supplied in the supplementary material.
  • The paper is organized so that readers can use the algorithm without the fiber bundle machinery.
  • Limitations

  • It is a purely theoretical and geometric work with no validation against an independent method and no physical application. The "simple algorithm" claim is not benchmarked against standard numerical holonomy computation, which is already straightforward (a product of small-step SU(2) matrices).
  • The advantage is mostly conceptual and exactness-related rather than demonstrated.
  • The prerequisites for practical use remain unmet, and the physical consequences, such as observable effects on dynamics, are not shown.
  • Heavy dependence on the author's own previous paper and notation. The text is dense with quaternion conventions, and some typographical issues exist (e.g., section references).
  • The audience is niche.
  • Other Observations

    The reproducibility is good for the algorithm since formulas are explicit. The examples are artificial, so the results are not surprising: they confirm theorems. The novelty is moderate, being a clever decomposition rather than a new paradigm. The impact will likely be modest, with citations from topological/gauge-theoretic chemical physics and perhaps synthetic gauge field work.

    Rating:5/ 10
    Significance 4.5Rigor 6Novelty 6Clarity 6

    Generated Nov 3, 2026

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