Harnessing electrostatics through temperature modulations to control ferroelectrics

Cameron A.M. Scott; Jorge \'I\~niguez-Gonz\'alez; Xabier Diaz de Cerio

arxiv: 2606.25850 · v1 · pith:WGFQKMONnew · submitted 2026-06-24 · ❄️ cond-mat.mtrl-sci · cond-mat.mes-hall

Harnessing electrostatics through temperature modulations to control ferroelectrics

Cameron A.M. Scott , Xabier Diaz de Cerio , Jorge \'I\~niguez-Gonz\'alez This is my paper

Pith reviewed 2026-06-25 20:11 UTC · model grok-4.3

classification ❄️ cond-mat.mtrl-sci cond-mat.mes-hall

keywords ferroelectricstemperature modulationdepolarizing fieldnon-electrical polingmultidomain statesLandau potentialsatomistic simulationspolar textures

0 comments

The pith

Temperature modulations harness the depolarizing field to achieve non-electrical poling in ferroelectrics.

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

The paper demonstrates that temperature modulations can serve as a method to dynamically control the ferroelectric state by using the depolarizing field for poling without electrical input. Using scale-independent Landau potentials and atomistic simulations, it shows how this approach works and extends to using temperature gradients with strain to create stable multidomain states. A reader would care if this opens new ways to manipulate ferroelectric materials in situations where electrical fields are difficult to apply or where alternative control is desired. The central idea is that temperature changes can be leveraged to influence polarization through electrostatic effects.

Core claim

Temperature modulations provide an alternative method for dynamically controlling the ferroelectric state. Temperature modulation can harness the depolarizing field to obtain non-electrical poling. Temperature gradients can be combined with strain to induce persistent polar textures such as multidomain states.

What carries the argument

Temperature modulation that harnesses the depolarizing field through scale-independent Landau potentials and predictive atomistic simulations.

Load-bearing premise

Scale-independent Landau potentials remain accurate under temperature modulations with strong depolarizing fields, and atomistic simulations capture the dynamics without additional adjustments.

What would settle it

Direct experimental observation of non-electrical poling or induced multidomain states in a ferroelectric sample subjected to controlled temperature modulations would confirm the claim; absence of such effects under the simulated conditions would challenge it.

Figures

Figures reproduced from arXiv: 2606.25850 by Cameron A.M. Scott, Jorge \'I\~niguez-Gonz\'alez, Xabier Diaz de Cerio.

**Figure 2.** Figure 2: FIG. 2. Phase diagram for temperature modulated ferro [PITH_FULL_IMAGE:figures/full_fig_p002_2.png] view at source ↗

**Figure 3.** Figure 3: FIG. 3. Polarization rotation under a sinusoidal temperature modulation using Langevin molecular dynamics with damping [PITH_FULL_IMAGE:figures/full_fig_p003_3.png] view at source ↗

**Figure 4.** Figure 4: FIG. 4. Rotation of dipoles under a sinusoidal temperature [PITH_FULL_IMAGE:figures/full_fig_p003_4.png] view at source ↗

**Figure 5.** Figure 5: FIG. 5. The combination of compressive strain and [PITH_FULL_IMAGE:figures/full_fig_p004_5.png] view at source ↗

read the original abstract

Temperature modulations provide an alternative method for dynamically controlling the ferroelectric state. In this paper, we use scale-independent Landau potentials and predictive atomistic simulations to explore how temperature modulation can harness the depolarizing field to obtain non-electrical poling. We further predict that temperature gradients can be combined with strain to induce persistent polar textures such as multidomain states.

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.

Desk Editor's Note private letter to a colleague

Temperature modulation to harness depolarizing fields for non-electrical poling is the new framing, but the Landau potential assumption under modulated temperature needs explicit checks.

read the letter

The main takeaway is that this paper proposes temperature modulations as a route to pole ferroelectrics by using the depolarizing field, without direct electrical input, and that temperature gradients plus strain can produce stable multidomain states. The novelty sits in applying that control strategy inside the usual Landau and atomistic framework.

The work does a reasonable job laying out why this matters for thin films where electrical poling is inconvenient. It sticks to scale-independent Landau potentials and predictive atomistic simulations, which keeps the approach grounded in existing tools rather than new fitting. The abstract also avoids obvious circularity by treating the temperature effect as an exploration rather than a retrofitted result.

The soft spot is the model validity under the claimed conditions. The central step assumes the Landau potentials stay accurate when temperature is modulated in the presence of strong depolarizing fields, yet nothing in the abstract shows a benchmark or test for that regime. If the full paper does not supply independent checks that the effective potential holds or that the atomistic runs match the Landau dynamics without adjustment, the predictions rest on an unverified step. That is the load-bearing part, not a side issue.

This is for condensed-matter modelers and device engineers who want alternatives to electrical poling. Someone already running ferroelectric simulations might pick up the temperature-gradient idea and test it themselves. It deserves peer review because the topic is practical and the methods are standard; referees can push on the validation without starting from scratch.

Referee Report

1 major / 0 minor

Summary. The manuscript claims that temperature modulations can be used to dynamically control ferroelectric states by harnessing the depolarizing field for non-electrical poling, based on scale-independent Landau potentials combined with predictive atomistic simulations. It further predicts that temperature gradients, when combined with strain, can induce persistent polar textures such as multidomain states.

Significance. If the central predictions are substantiated, the work would provide a non-electrical route to poling and domain engineering in ferroelectrics, which could be relevant for low-power device concepts. The explicit combination of continuum Landau modeling with atomistic simulations is a methodological strength that allows direct comparison of effective potentials and dynamics.

major comments (1)

The central claims rest on the assumption that scale-independent Landau potentials remain accurate and unmodified when temperature is modulated in the presence of strong depolarizing fields. No explicit validation, benchmark against atomistic results, or demonstration that the effective potential is unchanged (or that atomistic simulations reproduce the Landau dynamics without parameter adjustment) is provided for this regime. This assumption is load-bearing for both the non-electrical poling prediction and the multidomain texture claim.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their careful reading and constructive feedback. The single major comment is addressed point-by-point below. We agree that additional explicit validation would strengthen the central claims.

read point-by-point responses

Referee: The central claims rest on the assumption that scale-independent Landau potentials remain accurate and unmodified when temperature is modulated in the presence of strong depolarizing fields. No explicit validation, benchmark against atomistic results, or demonstration that the effective potential is unchanged (or that atomistic simulations reproduce the Landau dynamics without parameter adjustment) is provided for this regime. This assumption is load-bearing for both the non-electrical poling prediction and the multidomain texture claim.

Authors: We appreciate the referee highlighting this point. The scale-independent Landau potentials are constructed by design to remain valid across length scales without explicit size dependence, and the atomistic simulations are performed in a predictive mode without parameter fitting to the continuum model. However, we acknowledge that the manuscript does not contain a direct side-by-side benchmark of the effective potential or dynamical trajectories under simultaneous temperature modulation and strong depolarizing fields. To address this, we will add a new supplementary section that compares the polarization evolution obtained from the Landau model and from the atomistic simulations for a representative thin-film geometry under the relevant temperature-modulation protocol. This comparison will be performed without any adjustment of the atomistic parameters. We therefore accept the need for this addition. revision: yes

Circularity Check

0 steps flagged

No significant circularity detected

full rationale

The abstract and available text describe application of scale-independent Landau potentials and atomistic simulations to temperature-modulated ferroelectric control. No derivation equations, parameter fits, or self-citations are quoted that reduce any claimed prediction to its own inputs by construction. The methods are presented as external tools used for exploration rather than self-defined or fitted to the target outcomes, leaving the chain self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Abstract-only review prevents identification of specific free parameters, axioms, or invented entities; standard Landau theory is invoked but details are absent.

pith-pipeline@v0.9.1-grok · 5594 in / 972 out tokens · 24117 ms · 2026-06-25T20:11:59.808818+00:00 · methodology

discussion (0)

Reference graph

Works this paper leans on

14 extracted references

[1]

F. M. Chiabrera, S. Yun, Y. Li, R. T. Dahm, H. Zhang, C. K. Kirchert, D. V. Christensen, F. Trier, T. S. Jes- 5 persen, and N. Pryds, Freestanding perovskite oxide films: Synthesis, challenges, and properties, Annalen der Physik534, 2200084 (2022)

2022
[2]

S. S. Hong, M. Gu, M. Verma, V. Harbola, B. Y. Wang, D. Lu, A. Vailionis, Y. Hikita, R. Pentcheva, J. M. Rondinelli,et al., Extreme tensile strain states in la0. 7ca0. 3mno3 membranes, Science368, 71 (2020)

2020
[3]

Strukov and A

B. Strukov and A. Davtian, Study of dielectric, elas- tic and pyroelectric properties of tgs crystals placed in nonequilibrium conditions, Ferroelectrics63, 77 (1985)

1985
[4]

Choudhury, L

N. Choudhury, L. Walizer, S. Lisenkov, and L. Bellaiche, Geometric frustration in compositionally modulated fer- roelectrics, Nature470, 513 (2011)

2011
[5]

J. V. Mantese, N. W. Schubring, A. L. Micheli, and A. B. Catalan, Ferroelectric thin films with polarization gradi- ents normal to the growth surface, Applied physics letters 67, 721 (1995)

1995
[6]

J. V. Mantese and S. P. Alpay,Graded ferroelectrics, transpacitors and transponents(Springer, 2005)

2005
[7]

X. Xu, T. Wang, P. Chen, C. Zhou, J. Ma, D. Wei, H. Wang, B. Niu, X. Fang, D. Wu,et al., Femtosec- ond laser writing of lithium niobate ferroelectric nan- odomains, Nature609, 496 (2022)

2022
[8]

J. D. Jackson,Classical electrodynamics(John Wiley & Sons, 2012)

2012
[9]

Pulzone, N

M. Pulzone, N. S. Fedorova, H. Aramberri, and J. ´I˜ niguez-Gonz´ alez, Machine learning landau free-energy potentials for third-principles simulations, Physical Re- view B112, 224113 (2025)

2025
[10]

J. C. Wojde l, P. Hermet, M. P. Ljungberg, P. Ghosez, and J. ´I˜ niguez, First-principles model potentials for lattice- dynamical studies: general methodology and example of application to ferroic perovskite oxides, Journal of Physics: Condensed Matter25, 305401 (2013)

2013
[11]

Bratkovsky and A

A. Bratkovsky and A. Levanyuk, Formation and rapid evolution of domain structure at phase transitions in slightly inhomogeneous ferroelectrics and ferroelastics, Physical Review B66, 184109 (2002)

2002
[12]

D. G. Schlom, L.-Q. Chen, C.-B. Eom, K. M. Rabe, S. K. Streiffer, and J.-M. Triscone, Strain tuning of ferroelec- tric thin films, Annu. Rev. Mater. Res.37, 589 (2007)

2007
[13]

Mart´ ınez, S

E. Mart´ ınez, S. Garc´ ıa, E. Marin, O. Vasallo, G. Pena- Rodriguez, A. Calder´ on, and J. Siqueiros, Dielectric and thermal properties of x pbtio3-(1- x) srtio3 polycrystals, Journal of materials Science39, 1233 (2004)

2004
[14]

Tsukada, A

S. Tsukada, A. Kanagawa, and K. Ohwada, Temperature-gradient investigation of phase transi- tions in ferroelectrics using cooling and heating stage, Japanese Journal of Applied Physics62, 106501 (2023)

2023

[1] [1]

F. M. Chiabrera, S. Yun, Y. Li, R. T. Dahm, H. Zhang, C. K. Kirchert, D. V. Christensen, F. Trier, T. S. Jes- 5 persen, and N. Pryds, Freestanding perovskite oxide films: Synthesis, challenges, and properties, Annalen der Physik534, 2200084 (2022)

2022

[2] [2]

S. S. Hong, M. Gu, M. Verma, V. Harbola, B. Y. Wang, D. Lu, A. Vailionis, Y. Hikita, R. Pentcheva, J. M. Rondinelli,et al., Extreme tensile strain states in la0. 7ca0. 3mno3 membranes, Science368, 71 (2020)

2020

[3] [3]

Strukov and A

B. Strukov and A. Davtian, Study of dielectric, elas- tic and pyroelectric properties of tgs crystals placed in nonequilibrium conditions, Ferroelectrics63, 77 (1985)

1985

[4] [4]

Choudhury, L

N. Choudhury, L. Walizer, S. Lisenkov, and L. Bellaiche, Geometric frustration in compositionally modulated fer- roelectrics, Nature470, 513 (2011)

2011

[5] [5]

J. V. Mantese, N. W. Schubring, A. L. Micheli, and A. B. Catalan, Ferroelectric thin films with polarization gradi- ents normal to the growth surface, Applied physics letters 67, 721 (1995)

1995

[6] [6]

J. V. Mantese and S. P. Alpay,Graded ferroelectrics, transpacitors and transponents(Springer, 2005)

2005

[7] [7]

X. Xu, T. Wang, P. Chen, C. Zhou, J. Ma, D. Wei, H. Wang, B. Niu, X. Fang, D. Wu,et al., Femtosec- ond laser writing of lithium niobate ferroelectric nan- odomains, Nature609, 496 (2022)

2022

[8] [8]

J. D. Jackson,Classical electrodynamics(John Wiley & Sons, 2012)

2012

[9] [9]

Pulzone, N

M. Pulzone, N. S. Fedorova, H. Aramberri, and J. ´I˜ niguez-Gonz´ alez, Machine learning landau free-energy potentials for third-principles simulations, Physical Re- view B112, 224113 (2025)

2025

[10] [10]

J. C. Wojde l, P. Hermet, M. P. Ljungberg, P. Ghosez, and J. ´I˜ niguez, First-principles model potentials for lattice- dynamical studies: general methodology and example of application to ferroic perovskite oxides, Journal of Physics: Condensed Matter25, 305401 (2013)

2013

[11] [11]

Bratkovsky and A

A. Bratkovsky and A. Levanyuk, Formation and rapid evolution of domain structure at phase transitions in slightly inhomogeneous ferroelectrics and ferroelastics, Physical Review B66, 184109 (2002)

2002

[12] [12]

D. G. Schlom, L.-Q. Chen, C.-B. Eom, K. M. Rabe, S. K. Streiffer, and J.-M. Triscone, Strain tuning of ferroelec- tric thin films, Annu. Rev. Mater. Res.37, 589 (2007)

2007

[13] [13]

Mart´ ınez, S

E. Mart´ ınez, S. Garc´ ıa, E. Marin, O. Vasallo, G. Pena- Rodriguez, A. Calder´ on, and J. Siqueiros, Dielectric and thermal properties of x pbtio3-(1- x) srtio3 polycrystals, Journal of materials Science39, 1233 (2004)

2004

[14] [14]

Tsukada, A

S. Tsukada, A. Kanagawa, and K. Ohwada, Temperature-gradient investigation of phase transi- tions in ferroelectrics using cooling and heating stage, Japanese Journal of Applied Physics62, 106501 (2023)

2023