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arxiv: 2607.01441 · v1 · pith:2KPISLWJnew · submitted 2026-07-01 · ❄️ cond-mat.mes-hall

Resonant cooling of nuclear spins by optically-oriented holes in MAPbI₃ perovskite crystals

Pith reviewed 2026-07-03 18:30 UTC · model grok-4.3

classification ❄️ cond-mat.mes-hall
keywords nuclear spin coolingHanle effectMAPbI3perovskiteoptical orientationholeshyperfine interactionresonant cooling
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The pith

Spin-oriented holes in MAPbI3 cool nuclear spins when light helicity is modulated at resonant frequencies.

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

The paper establishes that photogenerated holes with oriented spins can resonantly cool nuclear spins inside MAPbI3 perovskite crystals. This is observed in Hanle-effect curves recorded while the circular polarization of the excitation light is switched at controlled frequencies. The magnetic-field position of the resonance moves upward as the modulation frequency rises, and the resonance lies outside the width expected from weakly localized holes. The data identify strongly localized holes as the main agents acting on 207Pb nuclei, which carry spin 1/2 and show no quadrupolar splitting.

Core claim

Resonant cooling of nuclear spins by photogenerated spin-oriented holes is demonstrated for MAPbI₃ perovskite crystals. It is evidenced by Hanle-effect measurements under helicity-modulated excitation with variable frequency. The resonance position in magnetic field shifts toward higher fields with increasing modulation frequency. The invariance of the Hanle curve upon in-plane sample rotation is consistent with the involvement of ²⁰⁷Pb nuclei with spin I = 1/2, which do not exhibit quadrupolar splitting. The shape of the resonance feature reveals that the nuclear spins are cooled by carriers with a negative g-factor consistent with holes, and the resonance fields exceed the half-width of th

What carries the argument

Hanle-effect resonance under helicity-modulated excitation, where resonance fields exceed the half-width associated with weakly localized holes.

If this is right

  • Resonance position increases linearly with modulation frequency.
  • In-plane rotation leaves the Hanle curve unchanged, consistent with I = 1/2 nuclei lacking quadrupolar moments.
  • Negative g-factor of the cooling carriers identifies them as holes.
  • Strongly localized holes dominate nuclear-spin cooling over weakly localized holes.

Where Pith is reading between the lines

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

  • The same modulation technique could be used to measure hyperfine coupling strengths in other lead-halide perovskites.
  • Selective cooling of specific nuclear isotopes might become possible by tuning modulation frequency to their Larmor precession.
  • Carrier localization depth could be quantified by comparing resonance positions to the known Hanle widths of different hole populations.

Load-bearing premise

The observed resonance features arise specifically from cooling of 207Pb nuclear spins by strongly localized holes rather than from other spin-dependent relaxation channels.

What would settle it

A Hanle curve recorded under the same modulated excitation that shows resonance positions remaining inside the weakly localized hole half-width, or no shift of resonance field with modulation frequency, would falsify the claim.

Figures

Figures reproduced from arXiv: 2607.01441 by Bekir Turedi, Dmitri R. Yakovlev, Maksym V. Kovalenko, Manfred Bayer, Mladen Kotur, Nataliia E. Kopteva.

Figure 1
Figure 1. Figure 1: FIG. 1. (a) Photoluminescence spectrum of a MAPbI [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. (a) Hanle curves measured in the Voigt geometry at [PITH_FULL_IMAGE:figures/full_fig_p004_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Modeling of the Hanle curves in the Voigt geometry under resonance cooling conditions for the helicity modulation [PITH_FULL_IMAGE:figures/full_fig_p004_3.png] view at source ↗
read the original abstract

Resonant cooling of nuclear spins by photogenerated spin-oriented holes is demonstrated for MAPbI$_3$ perovskite crystals. It is evidenced by Hanle-effect measurements under helicity-modulated excitation with variable frequency. The resonance position in magnetic field shifts toward higher fields with increasing modulation frequency. The invariance of the Hanle curve upon in-plane sample rotation is consistent with the involvement of $^{207}$Pb nuclei with spin $I = 1/2$, which do not exhibit quadrupolar splitting. The shape of the resonance feature in the Hanle curve reveals that the nuclear spins are cooled by carriers with a negative $g$-factor, consistent with holes. The resonance fields associated with the modulation frequencies exceed the half-width of the weakly localized hole contribution to the Hanle curve, indicating that strongly localized holes are the primary carriers responsible for the nuclear spin cooling.

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

1 major / 2 minor

Summary. The manuscript claims to demonstrate resonant cooling of nuclear spins by photogenerated spin-oriented holes in MAPbI₃ perovskite crystals. This is shown via Hanle-effect measurements under helicity-modulated excitation with variable frequency, where the resonance position shifts to higher fields with increasing modulation frequency. Invariance of the Hanle curve under in-plane rotation is taken as evidence for involvement of ²⁰⁷Pb nuclei (I=1/2) without quadrupolar splitting. The shape of the resonance feature indicates cooling by carriers with negative g-factor, consistent with holes. The key inference is that strongly localized holes are the primary agents, because the resonance fields exceed the half-width of the weakly localized hole contribution to the Hanle curve.

Significance. If substantiated, the result establishes a frequency-tunable resonant mechanism for dynamic nuclear polarization in lead-halide perovskites mediated by localized holes. The approach of using helicity modulation to separate localization-dependent contributions offers a concrete experimental handle on hyperfine interactions in these materials, which could inform spintronic or quantum-information applications. The work supplies falsifiable predictions (resonance shift with frequency, negative-g signature) and relies on standard spin-physics models without introducing free parameters or ad-hoc entities.

major comments (1)
  1. [Results / Hanle-curve analysis] The central assignment of nuclear-spin cooling to strongly localized holes rests on the statement that resonance fields exceed the half-width of the weakly localized contribution (abstract and results/discussion of Hanle curves). This comparison presupposes a clean, unambiguous decomposition of the observed Hanle signal into distinct weakly- and strongly-localized Lorentzian components whose half-widths can be extracted with quantified uncertainty. If the decomposition involves overlapping contributions, background choices, or fitting ambiguities, the 'exceed' threshold may lose statistical significance; the manuscript must therefore supply the explicit fitting procedure, covariance matrices, and alternative-model tests for the Hanle curves.
minor comments (2)
  1. [Abstract] The abstract states that the resonance feature shape reveals a negative g-factor but does not specify the quantitative criterion (e.g., sign of the dispersive component or zero-crossing shift) used to reach this conclusion; a brief sentence linking the observed lineshape to the sign of g would improve clarity.
  2. [Figure captions] Figure captions for the frequency-dependent Hanle data should explicitly state the modulation frequencies, the magnetic-field sweep range, and the number of averaged traces to allow readers to assess signal-to-noise and resonance-position precision.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the constructive comment and positive overall assessment. The request for explicit details on the Hanle-curve decomposition is reasonable and will be addressed by expanding the methods and results sections.

read point-by-point responses
  1. Referee: [Results / Hanle-curve analysis] The central assignment of nuclear-spin cooling to strongly localized holes rests on the statement that resonance fields exceed the half-width of the weakly localized contribution (abstract and results/discussion of Hanle curves). This comparison presupposes a clean, unambiguous decomposition of the observed Hanle signal into distinct weakly- and strongly-localized Lorentzian components whose half-widths can be extracted with quantified uncertainty. If the decomposition involves overlapping contributions, background choices, or fitting ambiguities, the 'exceed' threshold may lose statistical significance; the manuscript must therefore supply the explicit fitting procedure, covariance matrices, and alternative-model tests for the Hanle curves.

    Authors: We agree that the statistical robustness of the decomposition should be documented more explicitly. The observed Hanle curves were fitted as a sum of two Lorentzians (one narrow component for weakly localized holes and one broad component for strongly localized holes) plus a linear background, with the resonance positions extracted from the frequency-dependent shift of the broad component. In the revised manuscript we will add: (i) the full functional form and fitting constraints, (ii) the covariance matrices obtained from the least-squares fits for representative curves, and (iii) a comparison with single-Lorentzian and three-component alternative models together with the associated reduced-χ^{2} values. These additions will allow readers to assess the significance of the statement that resonance fields exceed the half-width of the weakly localized contribution. revision: yes

Circularity Check

0 steps flagged

No circularity: experimental Hanle resonances compared to measured half-widths using standard spin physics

full rationale

The paper reports Hanle-effect data under helicity modulation, with resonance positions shifting with frequency and exceeding the weakly-localized half-width to assign strongly-localized holes. No equations, fitted parameters, or self-citations are presented that define a quantity in terms of itself or rename a fit as a prediction. The comparison relies on direct measurement of the Hanle curve shape and resonance fields; the decomposition into localization components is an interpretive step but does not reduce the central claim to a tautology by construction. The invariance under rotation and negative g-factor inference are likewise data-driven and consistent with standard models for I=1/2 nuclei. This is a standard experimental interpretation without load-bearing self-referential steps.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The central claim rests on standard domain assumptions about the interpretation of Hanle curves in semiconductors containing nuclear spins; no free parameters or new entities are introduced in the abstract.

axioms (1)
  • domain assumption Hanle-effect curves under helicity modulation can be interpreted in terms of resonant nuclear spin cooling by carriers with defined g-factors.
    The paper invokes established models of spin relaxation and hyperfine coupling to assign the resonance feature to nuclear cooling.

pith-pipeline@v0.9.1-grok · 5710 in / 1331 out tokens · 32562 ms · 2026-07-03T18:30:40.394588+00:00 · methodology

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Reference graph

Works this paper leans on

17 extracted references · 17 canonical work pages · 1 internal anchor

  1. [1]

    Lampel, Nuclear dynamic polarization by optical elec- tronic saturation and optical pumping in semiconductors, Phys

    G. Lampel, Nuclear dynamic polarization by optical elec- tronic saturation and optical pumping in semiconductors, Phys. Rev. Lett.20, 491 (1968)

  2. [2]

    Paget, G

    D. Paget, G. Lampel, B. Sapoval, and V. I. Safarov, Low field electron-nuclear spin coupling in gallium arsenide under optical pumping conditions, Phys. Rev. B15, 5780 (1977)

  3. [3]

    Kudlacik, N

    D. Kudlacik, N. E. Kopteva, M. Kotur, D. R. Yakovlev, K. V. Kavokin, C. Harkort, M. Karzel, E. A. Zhukov, E. Evers, V. V. Belykh, and M. Bayer, Optical spin ori- entation of localized electrons and holes interacting with nuclei in a FA0.9Cs0.1PbI2.8Br0.2 perovskite crystal, ACS Photonics11, 2757 (2024)

  4. [4]

    Kotur, P

    M. Kotur, P. S. Bazhin, K. V. Kavokin, N. E. Kopteva, D. R. Yakovlev, D. Kudlacik and M. Bayer, Dynamic po- larization of nuclear spins by optically oriented electrons and holes in lead halide perovskite semiconductors, Phys. Rev. B113, 085204 (2026)

  5. [5]

    Kotur, N

    M. Kotur, N. E. Kopteva, D. R. Yakovlev, B. Turedi, M. V. Kovalenko, and M. Bayer, Hyperfine interaction of electrons and holes with nuclei probed by optical orienta- tion in methylammonium lead iodide perovskite crystals, Phys. Rev. B113, 245203 (2026)

  6. [6]

    I. A. Merkulov, Cooling of a system of nuclear spins in a semiconductor upon polarization of the electron polar- ization, Zh. Eksp. Teor. Fiz.79, 1036 (1980) [Sov. Phys. JETP52, 526 (1980)]

  7. [7]

    Hanle, ¨Uber magnetische beeinflussung der polarisa- tion der resonanzfluoreszenz, Zeitschrift f¨ ur Physik30, 93 (1924)

    W. Hanle, ¨Uber magnetische beeinflussung der polarisa- tion der resonanzfluoreszenz, Zeitschrift f¨ ur Physik30, 93 (1924)

  8. [8]

    V. K. Kalevich, V. D. Kul’kov, and V. G. Fleisher, Op- tical cooling of the spin system of nuclei in a semicon- 7 ductor lattice in a rotating system of coordinates, Fiz. Tverd. Tela22, 1208 (1980) [Sov. Phys. Solid State22, 703 (1980)]

  9. [9]

    V. K. Kalevich, V. D. Kul’kov, and V. G. Fleisher, Mani- festation of the sign of the g factor of conduction electrons in resonant cooling of the nuclear spin system of a semi- conductor, Fiz. Tverd. Tela23, 1524 (1981) [Sov. Phys. Solid State23, 892 (1981)]

  10. [10]

    E. A. Zhukov, A. Greilich, D. R. Yakovlev, K. V. Ka- vokin, I. A. Yugova, O. A. Yugov, D. Suter, G. Kar- czewski, T. Wojtowicz, J. Kossut, V. V. Petrov, Yu. K. Dolgikh, A. Pawlis and M. Bayer, All-optical NMR in semiconductors provided by resonant cooling of nuclear spins interacting with electrons in the reso- nant spin amplification regime, Phys. Rev. B...

  11. [11]

    A. D. Wright, R. L. Milot, G. E. Eperon, H. J. Snaith, M. B. Johnston, and L. M. Herz, Band-tail recombination in hybrid lead iodide perovskite, Adv. Funct. Mater.27, 1700860 (2017)

  12. [12]

    D. W. DeQuilettes, K. Frohna, D. Emin, T. Kirchartz, V. Bulovic, D. S. Ginger, and S. D. Stranks, Charge- carrier recombination in halide perovskites: Focus re- view, Chem. Rev.119, 11007 (2019)

  13. [13]

    Kirstein, D

    E. Kirstein, D. R. Yakovlev, E. A. Zhukov, J. H¨ ocker, V. Dyakonov, and M. Bayer, Spin dynamics of electrons and holes interacting with nuclei in MAPbI 3 perovskite single crystals, ACS Photonics9, 1375 (2022)

  14. [14]

    N. E. Kopteva, D. R. Yakovlev, E. Yalcin, I. A. Akimov, M. Kotur, B. Turedi, D. N. Dirin, M. V. Kovalenko, and M. Bayer, Optical orientation of excitons and charge car- riers in methylammonium lead iodide perovskite single crystals in the orthorhombic phase, Phys. Rev. B111, 195201 (2025)

  15. [15]

    K. V. Kavokin, Resonant optical cooling of nuclear spins in case of strong Knight field of photoexcited electrons, arXiv:2605.14934 (2026)

  16. [16]

    Z. Chen, B. Turedi, A. Y. Alsalloum, C. Yang, X. Zheng, I. Gereige, A. AlSaggaf, O. F. Mohammed, and O. M. Bakr, Single-crystal MAPbI 3 perovskite so- lar cells exceeding 21% power conversion efficiency, ACS Energy Lett.4, 1258 (2019)

  17. [17]

    A. Y. Alsalloum, B. Turedi, X. Zheng, S. Mitra, A. A. Zhumekenov, K. J. Lee, P. Maity, I. Gereige, A. AlSaggaf, I. S. Roqan, O. F. Mohammed, and O. M. Bakr, Low-temperature crystallization enables 21.9% ef- ficient single-crystal MAPbI 3 inverted perovskite solar cells, ACS Energy Lett.5, 657 (2020)