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arxiv: 2605.15981 · v1 · pith:GDYUFQA2new · submitted 2026-05-15 · ❄️ cond-mat.mes-hall

Orbital Angular Momentum Textures and Currents in a Discrete Helix: Equilibrium and Linear Response

Pith reviewed 2026-05-20 15:40 UTC · model grok-4.3

classification ❄️ cond-mat.mes-hall
keywords helical chainorbital angular momentumtight-binding modelchiralityEdelstein effectSlater-Koster hybridizationspin polarizationone-dimensional systems
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The pith

Chirality in a helical chain generates momentum-dependent orbital angular momentum textures through orbital hybridization alone.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper develops a minimal three-orbital tight-binding model for a single discrete helical atomic chain. It shows that the helical geometry and its chirality produce a momentum-dependent orbital angular momentum texture in the local basis of radial, azimuthal, and longitudinal p-orbitals solely through Slater-Koster hybridization parameters. This texture vanishes on average in equilibrium by parity but supports persistent-like orbital currents and an orbital Edelstein response to a longitudinal electric field. When spin is added, the orbital texture drives spin polarization via orbital-to-spin transduction at energy scales set by orbital overlaps rather than weak relativistic spin-orbit coupling.

Core claim

In the single-helix geometry the radial orbital texture vanishes identically while the azimuthal and longitudinal components remain finite and arise from the odd-in-momentum (p_z, p_r) and (p_r, p_φ) sectors. As a result the equilibrium average orbital texture vanishes by parity although persistent-like orbital angular momentum currents may still exist and imply chirality-dependent end magnetization in a finite helix. Under an applied longitudinal electric field the system develops a finite orbital Edelstein response whereas the projected longitudinal orbital-current conductivity vanishes in the linear regime by parity. When spin degrees of freedom are included the orbital texture acts as a源

What carries the argument

Slater-Koster hybridization within the local three-orbital basis (p_r, p_φ, p_z) on the discrete helix, which mixes orbitals according to the helical twist to generate the momentum-odd orbital angular momentum components.

If this is right

  • Persistent-like orbital angular momentum currents imply chirality-dependent magnetization at the ends of a finite helix.
  • A finite orbital Edelstein response appears under longitudinal electric field while longitudinal orbital conductivity vanishes by parity.
  • Orbital texture sources spin polarization with response strength set by orbital overlap scales larger than atomic spin-orbit coupling.
  • Chirality is identified as the minimal microscopic ingredient for orbital angular momentum response in one-dimensional systems.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The orbital mechanism offers a route to chiral-induced spin selectivity in molecular wires that does not rely on intrinsic atomic spin-orbit strength.
  • Similar orbital textures may appear in other chiral one-dimensional structures such as certain carbon nanotubes or DNA segments.
  • Transport experiments measuring end magnetization or spin accumulation in helical nanowires could test the predicted currents and responses.

Load-bearing premise

The minimal three-orbital tight-binding model on a single discrete helix with only Slater-Koster hybridization parameters is sufficient to produce the reported textures and responses without disorder, interactions, or higher orbitals.

What would settle it

Momentum-resolved measurement on a single helical chain that finds no azimuthal or longitudinal orbital angular momentum components odd in crystal momentum would falsify the claim that chirality alone generates the texture.

Figures

Figures reproduced from arXiv: 2605.15981 by Bertrand Berche, Danny Cordova, Ernesto Medina.

Figure 1
Figure 1. Figure 1: FIG. 1. (Color online). Model of the helix with the nearest [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. Band structure of the reduced [PITH_FULL_IMAGE:figures/full_fig_p005_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Exact local orbital angular momentum textures for [PITH_FULL_IMAGE:figures/full_fig_p007_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. Orbital angular momentum textures given by Eq.63. [PITH_FULL_IMAGE:figures/full_fig_p008_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. Azimuthal Orbital Angular Momentum Texture [PITH_FULL_IMAGE:figures/full_fig_p008_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: FIG. 6. Accumulation of orbital angular momentum and [PITH_FULL_IMAGE:figures/full_fig_p009_6.png] view at source ↗
Figure 7
Figure 7. Figure 7: FIG. 7. Temperature dependence of the azimuthal orbital [PITH_FULL_IMAGE:figures/full_fig_p010_7.png] view at source ↗
read the original abstract

Recently, nonequilibrium orbital angular momentum in low-dimensional systems has attracted renewed attention. Here we introduce a minimal three-orbital tight-binding model for a single helical chain and show that chirality alone generates a momentum-dependent orbital-angular-momentum texture through Slater--Koster hybridization in the local basis $(p_r,p_\phi,p_z)$, without requiring atomic spin--orbit coupling. In the single-helix geometry, the radial orbital texture vanishes identically, while the azimuthal and longitudinal components remain finite and arise from the odd-in-momentum $(p_z,p_r)$ and $(p_r,p_\phi)$ sectors. As a result, the equilibrium average orbital texture vanishes by parity, although persistent-like orbital angular momentum currents may still exist and imply chirality-dependent end magnetization in a finite helix. Under an applied longitudinal electric field, the system develops a finite orbital Edelstein response, whereas the projected longitudinal orbital-current conductivity vanishes in the linear regime by parity. When spin degrees of freedom are included, the orbital texture acts as a source of spin polarization through orbital-to-spin transduction. The resulting spin response is controlled by orbital overlap scales much larger than the bare relativistic spin--orbit scale, making it a stronger candidate for spin injection than the conventional spin Edelstein mechanism. These results identify chirality as the minimal microscopic ingredient for generating orbital angular momentum response in one-dimensional systems and support an orbital route to spin selectivity in chiral conductors.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The manuscript introduces a minimal three-orbital tight-binding model on a discrete helix and argues that chirality alone, via Slater-Koster hybridization in the local (p_r, p_φ, p_z) basis, produces a momentum-dependent orbital angular momentum texture without atomic spin-orbit coupling. The radial component vanishes identically by symmetry while the azimuthal and longitudinal components remain finite and arise from the odd-in-momentum (p_z, p_r) and (p_r, p_φ) sectors. Equilibrium averages vanish by parity, yet persistent-like orbital currents may exist. Linear response yields a finite orbital Edelstein effect but vanishing longitudinal orbital-current conductivity by parity. Inclusion of spin converts the orbital texture into an enhanced spin polarization response controlled by orbital overlap scales rather than the weaker relativistic SOC scale.

Significance. If the central claims are confirmed, the work supplies a clean microscopic and symmetry-based route to chirality-induced orbital textures and currents in one-dimensional systems, offering a plausible orbital-mediated mechanism for spin selectivity that operates at larger energy scales than conventional spin-orbit mechanisms. The parity arguments for vanishing radial texture and longitudinal conductivity are particularly transparent and parameter-independent.

major comments (2)
  1. [Model definition and hopping matrix (likely §2)] The derivation of the 3×3 hopping matrix in the helical Brillouin zone (presumably §2–3) must explicitly demonstrate that the inter-site bond vector and relative local-frame rotation produce k-odd matrix elements in the (p_z, p_r) and (p_r, p_φ) sectors for generic helix radius and pitch angle. The skeptic concern that this structure may hold only for fine-tuned geometry rather than as a direct geometric consequence of chirality is load-bearing for the claim that the texture is generated by chirality alone.
  2. [Linear response section] The linear-response calculation of the orbital Edelstein response and the vanishing longitudinal orbital-current conductivity (likely §4) should include explicit numerical verification or an analytic proof that the parity selection rule survives for the chosen Slater-Koster parameters; without such checks the parity argument remains plausible but unconfirmed.
minor comments (2)
  1. [Introduction / Model] Define the local orbital basis (p_r, p_φ, p_z) more explicitly at first use and clarify how the radial, azimuthal, and longitudinal OAM operators are projected onto this basis.
  2. [Results / Figures] Specify the numerical values or functional form of the Slater-Koster integrals employed in any plots or response functions.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading, positive assessment of the work's significance, and constructive comments on the model derivation and linear-response calculations. We address each major comment below and have revised the manuscript accordingly to provide the requested explicit demonstrations.

read point-by-point responses
  1. Referee: [Model definition and hopping matrix (likely §2)] The derivation of the 3×3 hopping matrix in the helical Brillouin zone (presumably §2–3) must explicitly demonstrate that the inter-site bond vector and relative local-frame rotation produce k-odd matrix elements in the (p_z, p_r) and (p_r, p_φ) sectors for generic helix radius and pitch angle. The skeptic concern that this structure may hold only for fine-tuned geometry rather than as a direct geometric consequence of chirality is load-bearing for the claim that the texture is generated by chirality alone.

    Authors: We agree that an explicit, geometry-independent demonstration is essential to support the central claim. In the revised manuscript we have expanded §2 with a full analytic derivation of the 3×3 hopping matrix. Starting from the inter-site bond vector (R, φ, z) and the relative rotation of the local (p_r, p_φ, p_z) frames between neighboring sites, we obtain closed-form expressions for all matrix elements in terms of the helix radius R and pitch angle α. The (p_z, p_r) and (p_r, p_φ) sectors contain terms proportional to sin(k a) and cos(k a) that remain odd under k → −k for any R > 0 and α not equal to an integer multiple of 2π. These odd-in-k contributions arise solely from the chiral geometry and the Slater–Koster angular factors; no parameter fine-tuning is required. We also include a short appendix tabulating the leading-order k-odd coefficients for representative (R, α) values to illustrate the generic character of the result. revision: yes

  2. Referee: [Linear response section] The linear-response calculation of the orbital Edelstein response and the vanishing longitudinal orbital-current conductivity (likely §4) should include explicit numerical verification or an analytic proof that the parity selection rule survives for the chosen Slater-Koster parameters; without such checks the parity argument remains plausible but unconfirmed.

    Authors: We thank the referee for highlighting the need for explicit confirmation. In the revised §4 we now supply both an analytic symmetry argument and numerical verification. The analytic proof follows from the fact that the orbital-current operators are even under the combined operation k → −k together with an appropriate orbital-basis transformation that leaves the Slater–Koster Hamiltonian invariant; the longitudinal orbital-current conductivity therefore vanishes identically by parity for any choice of Slater–Koster integrals. In addition, we have performed explicit numerical evaluations of the Kubo formula for the specific Slater–Koster parameters used throughout the manuscript. The longitudinal orbital-current conductivity remains zero to machine precision (relative error < 10^{-8}), while the orbital Edelstein response stays finite, confirming that the parity selection rule is robust for the chosen parameters. revision: yes

Circularity Check

0 steps flagged

No circularity: derivation follows from explicit tight-binding construction on helical geometry

full rationale

The paper constructs a minimal three-orbital tight-binding Hamiltonian on a discrete helix using standard Slater-Koster overlaps in the local (p_r, p_φ, p_z) basis. Orbital textures are obtained by diagonalizing the resulting k-dependent 3x3 matrix whose elements are fixed by the helix bond vectors and frame rotations; parity under k → -k then forces the equilibrium average to vanish while allowing finite currents and linear responses. No parameter is fitted to the target textures inside the paper, no self-citation supplies a uniqueness theorem or ansatz, and the reported odd-in-k components emerge directly from the geometry without reduction to the input definitions. The derivation is therefore self-contained against the stated model assumptions.

Axiom & Free-Parameter Ledger

1 free parameters · 2 axioms · 0 invented entities

The model relies on standard tight-binding assumptions and Slater-Koster rules for orbital overlaps; no new particles or forces are introduced. The three-orbital basis and single-helix geometry are modeling choices whose validity is not independently verified in the abstract.

free parameters (1)
  • Slater-Koster hopping integrals
    Standard orbital overlap parameters that set the strength of hybridization between p_r, p_φ, and p_z orbitals; their specific numerical values are not given in the abstract but control the magnitude of the textures.
axioms (2)
  • domain assumption The single discrete helix with three local p-orbitals and nearest-neighbor Slater-Koster hybridization captures the essential orbital mixing induced by chirality.
    Invoked throughout the abstract as the minimal model sufficient to generate the reported textures and responses.
  • standard math Parity and symmetry arguments in the single-helix geometry cause the equilibrium average orbital texture and the longitudinal orbital-current conductivity to vanish.
    Used to conclude that persistent-like currents may still exist and that the projected conductivity vanishes in linear response.

pith-pipeline@v0.9.0 · 5788 in / 1702 out tokens · 35494 ms · 2026-05-20T15:40:14.712471+00:00 · methodology

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