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arxiv: 2607.00668 · v1 · pith:S6SW55X2new · submitted 2026-07-01 · ❄️ cond-mat.mes-hall · cond-mat.mtrl-sci· physics.chem-ph· quant-ph

Spinterface-like mechanism of the chirality-induced spin selectivity in donor chiral-bridge acceptor complexes

Subhajit Sarkar , Oliver L. A. Monti , Yonatan Dubi This is my paper

Pith reviewed 2026-07-02 07:21 UTC · model grok-4.3

classification ❄️ cond-mat.mes-hall cond-mat.mtrl-sciphysics.chem-phquant-ph
keywords chirality-induced spin selectivityspinterface mechanismdonor-chiral bridge-acceptorLindblad modelspin polarizationtime-resolved EPRsolenoidal fieldcharge transfer
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The pith

A current-induced solenoidal field from charge transfer through a chiral bridge, interacting with the residual donor electron, produces the observed spin selectivity in isolated molecular complexes.

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

The paper introduces an intramolecular mechanism in donor-chiral bridge-acceptor complexes where the photoexcited electron traversing the bridge exchanges with the donor electron, treated as a localized moment. This exchange generates an effective magnetic field at the interface that breaks spin degeneracy and enables selective transport. The model combines this field with donor thermalization and bridge spin mixing to yield substantial polarization on experimental timescales. A reader would care because the account unifies CISS observations in molecules lacking metal contacts with the same physics used for device interfaces.

Core claim

In the two-electron Lindblad model, the charge-transfer electron exchanges with the residual donor electron acting as a localized magnetic moment; the resulting through-bridge current produces an effective solenoidal field at the donor-bridge interface that breaks spin degeneracy and directional symmetry, enabling spin-selective transport without intrinsic spin-orbit coupling on the bridge. The interplay of this field, donor thermalization breaking time-reversal symmetry, and bridge spin mixing produces tens-of-percent polarization matching reported signatures in triads and DNA hairpins.

What carries the argument

Two-electron Lindblad model with current-induced solenoidal field generated by exchange between the charge-transfer electron and the residual donor electron treated as a localized magnetic moment.

If this is right

  • Spin polarization reaches tens of percent under realistic temperatures and charge-transfer times.
  • Polarization strength varies explicitly with solenoidal coupling, temperature, and spin-mixing rates.
  • The same internal mechanism reproduces CISS signatures seen in both molecular triads and DNA hairpins.
  • Spin selectivity occurs without requiring strong intrinsic spin-orbit coupling on the chiral bridge.

Where Pith is reading between the lines

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

  • Varying donor-bridge distance or temperature in time-resolved EPR could map the predicted dependence on field strength and thermalization.
  • The account suggests that CISS-like filtering may appear in other photoexcited chiral systems that support an internal localized moment.
  • If the mechanism holds, removing the donor electron should eliminate the polarization while leaving bridge chirality unchanged.

Load-bearing premise

The residual donor electron functions as a localized magnetic moment that couples to the through-bridge current to create an effective solenoidal field at the interface.

What would settle it

Absence of spin polarization when the donor electron is removed or when charge transfer is blocked while keeping the chiral bridge intact.

Figures

Figures reproduced from arXiv: 2607.00668 by Oliver L. A. Monti, Subhajit Sarkar, Yonatan Dubi.

Figure 1
Figure 1. Figure 1: Schematic depiction for the Donor-chiral-bridge-acceptor (D–χB–A) system within the Hubbard picture. Photoexcitation of the donor (D) injects an elec￾tron into the chiral bridge χB (with N = 4), which propagates toward the acceptor-sink (A) with hopping amplitude thop and can recombine back to D. Injection and recombination are described by the Lindblad operators Linj and Lrec, while local spin mixing at t… view at source ↗
Figure 2
Figure 2. Figure 2: (a) Schematic of D–χB–A complex in terms of its singlet-triplet state manifold. The bare singlet-triplet gap in the donor is governed by the exchange coupling JD. The same exchange coupling in the donor-bridge manifold is distance-dependent, with Jj being smaller for transfer to a more distant bridge site. (b) Thermalization mechanism at the interface. The current-induced field produces a Zeeman splitting … view at source ↗
Figure 3
Figure 3. Figure 3: Spin–polarization vs. effective strength of the solenoid field at different temperatures: Plot of the steady-state spin–polarization P versus the solenoidal-coupling magnitude α0 on a log scale at a fixed mixing rate γm = 0.014thop; curves correspond to four temperatures (see legend) [PITH_FULL_IMAGE:figures/full_fig_p013_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: Effect of spin mixing on the CISS-polarization: Plot on a log −linear of CISS-polarization P in % with the relative mixing strength γm/thop in the first bridge site for three different effective strengths of the solenoid coupling strength α0, top, middle, and bottom panels, respectively, for four different temperatures. 16 [PITH_FULL_IMAGE:figures/full_fig_p016_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: Temperature dependence of CISS-polarization for different effective strengths of the solenoid fields: Plot of the steady-state CISS polarization P(γ ∗ m) with temperature T for four different solenoidal-coupling magnitudes α0 (see legend) on a linear scale. balance asymmetry controlling this bias is progressively reduced, so the cycle generates a smaller net imbalance between the triplet projections per pa… view at source ↗
Figure 6
Figure 6. Figure 6: TOC Graphic 30 [PITH_FULL_IMAGE:figures/full_fig_p030_6.png] view at source ↗
read the original abstract

The chirality-induced spin selectivity (CISS) effect has been invoked to explain recent reports of differences in the time-resolved EPR signals between chiral and achiral molecules. However, the microscopic origin of these differences and their connection to CISS remains contested, particularly since these systems lack a metal interface. Here we introduce an intramolecular spinterface-like mechanism that naturally arises within donor-chiral bridge-acceptor (D--$\chi$B--A) complexes and quantitatively reproduces experimentally reported observed spin polarization in time-resolved EPR studies. In our two-electron Lindblad model, the photoexcited charge-transfer electron traversing the chiral bridge exchanges with the residual donor electron, which acts as a localized magnetic moment analogous to an induced magnetic moment on an electrode surface. The resulting through-bridge charge current produces an effective solenoidal field at the donor--bridge interface, breaking spin degeneracy and directional symmetry, thus enabling spin-selective transport without invoking intrinsic spin-orbit coupling on the bridge. We show that the interplay between this current-induced field, donor thermalization (which breaks time-reversal symmetry), and bridge spin mixing yields tens-of-percent polarization over realistic experimental conditions and charge-transfer time scales, matching reported CISS signatures in triads and DNA hairpins. By explicitly resolving the dependence on solenoidal coupling strength, temperature, and spin-mixing rates, the model identifies the regime in which internal spinterfaces can generate robust CISS-like spin filtering. These findings demonstrate that CISS-like signals in isolated D--$\chi$B--A complexes are fully compatible with a spinterface mechanism, providing a unified conceptual framework for interpreting both device-based and molecule-internal CISS platforms.

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

3 major / 1 minor

Summary. The manuscript proposes an intramolecular spinterface-like mechanism for chirality-induced spin selectivity (CISS) in donor-chiral bridge-acceptor (D-χB-A) complexes. A two-electron Lindblad master equation models exchange between the photoexcited charge-transfer electron and the residual donor electron (treated as a localized magnetic moment), generating an effective solenoidal field at the donor-bridge interface. Combined with donor thermalization (breaking time-reversal symmetry) and bridge spin mixing, this produces tens-of-percent spin polarization over realistic charge-transfer timescales, matching reported EPR signatures in triads and DNA hairpins. The model explicitly tracks dependence on solenoidal coupling strength, temperature, and spin-mixing rates.

Significance. If the central mechanism holds with independently fixed parameters, the work would supply a unified conceptual framework for CISS-like signals in isolated molecular systems lacking metal interfaces, bridging device-based and molecule-internal observations. The explicit resolution of parameter dependence is a strength, allowing identification of relevant regimes without invoking strong intrinsic spin-orbit coupling.

major comments (3)
  1. [Abstract (model description)] The effective solenoidal field at the donor-bridge interface is introduced phenomenologically in the two-electron Lindblad model without derivation from the underlying Coulomb or current-density operators in the D-χB-A Hamiltonian. This is load-bearing for the central claim, as the reported polarization levels depend directly on the (unspecified) coupling strength; if this strength is not fixed by molecular parameters, the match to experimental CISS signatures reduces to a fit rather than a prediction.
  2. [Abstract (two-electron Lindblad model)] The residual donor electron is posited to act as a localized magnetic moment analogous to an induced moment on an electrode surface, enabling the spinterface-like mechanism. This axiom is introduced without microscopic justification from the isolated D-χB-A Hamiltonian and is load-bearing for the analogy; its validity determines whether the current-induced field can arise internally.
  3. [Abstract (parameter dependence)] Donor thermalization and bridge spin-mixing rates are listed among the free parameters whose interplay yields the polarization. While the model resolves their dependence, the absence of independent constraints on these rates (from molecular structure or separate experiments) means the tens-of-percent polarization is not yet shown to be robustly predicted rather than tuned.
minor comments (1)
  1. [Abstract] The abstract refers to 'time-resolved EPR studies' and 'reported CISS signatures' but does not cite specific experimental papers or datasets against which the Lindblad results are compared; adding these references would strengthen the quantitative matching claim.

Simulated Author's Rebuttal

3 responses · 0 unresolved

We thank the referee for the careful reading and constructive comments. We address each major comment below with clarifications and planned revisions where appropriate.

read point-by-point responses

  1. Referee: [Abstract (model description)] The effective solenoidal field at the donor-bridge interface is introduced phenomenologically in the two-electron Lindblad model without derivation from the underlying Coulomb or current-density operators in the D-χB-A Hamiltonian. This is load-bearing for the central claim, as the reported polarization levels depend directly on the (unspecified) coupling strength; if this strength is not fixed by molecular parameters, the match to experimental CISS signatures reduces to a fit rather than a prediction.

    Authors: We acknowledge that the solenoidal field enters the model as an effective coupling. This is motivated by the expectation that through-bridge charge current generates a local magnetic field at the donor interface, consistent with the Biot-Savart relation applied to molecular length scales. In the revised manuscript we will add an appendix estimating the coupling magnitude from representative molecular current densities, bridge geometry, and charge velocities, showing that the values used lie within the physically plausible range. This will clarify that the reported polarization levels are achievable for realistic parameters rather than arbitrary fits. revision: partial

  2. Referee: [Abstract (two-electron Lindblad model)] The residual donor electron is posited to act as a localized magnetic moment analogous to an induced moment on an electrode surface, enabling the spinterface-like mechanism. This axiom is introduced without microscopic justification from the isolated D-χB-A Hamiltonian and is load-bearing for the analogy; its validity determines whether the current-induced field can arise internally.

    Authors: The residual donor electron is modeled as a localized spin-1/2 because, following photoinduced charge transfer in D-χB-A complexes, the donor moiety carries an unpaired electron whose spin degree of freedom is spatially localized on the donor. This description is standard for charge-transfer states. In the revision we will insert a short derivation showing how the effective exchange interaction between the transferred electron and the donor spin emerges from the two-electron Hamiltonian of the isolated D-χB-A system, thereby grounding the analogy more firmly. revision: yes

  3. Referee: [Abstract (parameter dependence)] Donor thermalization and bridge spin-mixing rates are listed among the free parameters whose interplay yields the polarization. While the model resolves their dependence, the absence of independent constraints on these rates (from molecular structure or separate experiments) means the tens-of-percent polarization is not yet shown to be robustly predicted rather than tuned.

    Authors: The rates were chosen to lie within ranges reported in the experimental literature on molecular triads and DNA hairpins (thermalization from EPR relaxation data; spin mixing from hyperfine and residual spin-orbit effects). The revised manuscript will cite these independent experimental constraints explicitly and will demonstrate that the polarization remains in the tens-of-percent range across the experimentally reported intervals, thereby showing robustness rather than fine tuning. revision: partial

Circularity Check

0 steps flagged

No significant circularity; model parameters are explicit and result is not reduced to input by construction

full rationale

The abstract and description present a two-electron Lindblad model that introduces an effective solenoidal field phenomenologically at the donor-bridge interface. The central result is that polarization of tens of percent arises from the interplay of this field, donor thermalization, and bridge spin mixing for realistic values of the (explicitly resolved) coupling strength, temperature, and mixing rates. No self-citations, self-definitional steps, or equations are quoted that would make the polarization output equivalent to a fitted input or prior author result by construction. The model identifies regimes of parameter space rather than claiming a parameter-free first-principles derivation, satisfying the criteria for a self-contained (non-circular) analysis.

Axiom & Free-Parameter Ledger

3 free parameters · 2 axioms · 2 invented entities

The central claim rests on the applicability of the two-electron Lindblad framework, the electrode-surface analogy for the donor electron, and several tunable parameters (solenoidal coupling, spin-mixing rates, temperature) whose values are chosen to reproduce experimental polarization magnitudes.

free parameters (3)
  • solenoidal coupling strength
    The model explicitly resolves dependence on this quantity to produce the reported polarization levels.
  • bridge spin-mixing rates
    Tunable parameter controlling spin scrambling on the chiral bridge.
  • donor thermalization rate
    Controls time-reversal symmetry breaking and is set to realistic experimental conditions.
axioms (2)
  • domain assumption Two-electron Lindblad master equation accurately captures the open-system dynamics of the photoexcited D-χB-A complex
    Invoked as the modeling framework throughout the abstract.
  • ad hoc to paper The residual donor electron behaves as a localized magnetic moment analogous to an electrode surface
    Central analogy enabling the solenoidal-field construction without intrinsic bridge SOC.
invented entities (2)
  • effective solenoidal field at the donor-bridge interface no independent evidence
    purpose: Breaks spin degeneracy and directional symmetry to enable spin-selective transport
    Generated by the through-bridge charge current in the model
  • intramolecular spinterface-like mechanism no independent evidence
    purpose: Explains CISS-like spin filtering in isolated complexes without metal interface or intrinsic SOC
    New conceptual construct introduced to unify device and molecular observations

pith-pipeline@v0.9.1-grok · 5850 in / 1689 out tokens · 36576 ms · 2026-07-02T07:21:02.297106+00:00 · methodology

discussion (0)

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