Ellipticity effects on diffusive magnon spin and heat transport in easy-plane ferromagnets
Pith reviewed 2026-05-20 03:46 UTC · model grok-4.3
The pith
Ellipticity of magnons leads to enhanced heat transport and axis-dependent spin transport in easy-plane ferromagnets.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The central discovery is that magnon ellipticity, induced by perpendicular magnetic anisotropy in easy-plane ferromagnets, alters the diffusive transport properties. Using a perturbative solution of the Boltzmann equation, the spin conductivity is shown to increase for easy-axis and decrease for hard-axis configurations, while the thermal conductivity increases in both cases for 3D and 2D systems.
What carries the argument
The magnon dispersion relation obtained from the Landau-Lifshitz-Gilbert equation with anisotropy, which determines the elliptical character and is inserted into the expressions for transport coefficients.
Load-bearing premise
The Boltzmann transport equation is solved assuming small deviations from equilibrium and using a single isotropic relaxation time for all magnons.
What would settle it
Direct measurement of the magnon thermal conductivity in an easy-plane ferromagnet sample before and after inducing a perpendicular anisotropy, to check for the predicted increase.
Figures
read the original abstract
When a magnetic material hosts spin-wave excitations, or magnons, the local magnetization can rotate in circular or elliptical orbits, the latter arising naturally in the presence of magnetic anisotropies transverse to the equilibrium magnetization. This article investigates the diffusive transport of elliptical magnons in easy-plane ferromagnets. Our analysis starts with the derivation of the magnon dispersion relation and magnon spin from the Landau-Lifshitz-Gilbert equation with a perpendicular magnetic anisotropy. Then, using the Boltzmann transport equation in the relaxation time approximation and perturbation analysis, the magnon-spin and magnon thermal conductivities are obtained, quantifying the magnon transport in the insulator. Our calculations demonstrate that, in both three- and two-dimensional systems, the effects of ellipticity on magnon transport coefficients result in an enhancement or a decrease, depending on whether magnets with a easy or hard perpendicular-to-plane axis are considered, respectively. On the other hand, our results predict an enhancement of the magnon heat transport for both easy- and hard-axis magnetic systems. Our study supports previous works on magnon ellipticity and makes a step towards clarifying its effect on magnon transport properties.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript investigates ellipticity effects on diffusive magnon spin and heat transport in easy-plane ferromagnets. Starting from the LLG equation with perpendicular anisotropy, the authors derive the magnon dispersion relation and magnon spin for elliptical orbits. They then employ the Boltzmann transport equation in the relaxation time approximation with perturbation analysis to obtain expressions for the magnon spin and thermal conductivities in 2D and 3D systems. The key findings are that ellipticity causes enhancement or decrease in spin transport coefficients depending on easy or hard perpendicular axis, respectively, while heat transport is enhanced for both types of systems.
Significance. Should the central results prove robust, this study offers valuable insights into how magnon ellipticity influences transport properties, building on prior research in magnonics. The explicit calculations for both spin and heat conductivities in different dimensions provide a basis for understanding anisotropic effects in magnetic insulators, with potential applications in spin caloritronics.
major comments (1)
- [Boltzmann transport section] The derivation of transport coefficients relies on the relaxation-time approximation with a single, isotropic and wavevector-independent relaxation time. As the elliptical magnon modes arise from the anisotropy, this is likely to make the scattering rates (and thus tau) momentum-dependent, particularly for magnon-phonon or magnon-magnon scattering. This could change the quantitative corrections and possibly the qualitative enhancement/decrease behavior for the spin conductivity. The paper should either justify the constant-tau choice or provide an estimate of the error introduced by this approximation.
minor comments (1)
- [Abstract] The abstract mentions 'easy or hard perpendicular-to-plane axis' but the title specifies 'easy-plane ferromagnets'; a brief clarification on the distinction between easy-plane and the perpendicular anisotropy would help.
Simulated Author's Rebuttal
We thank the referee for the careful reading of our manuscript and the constructive comments provided. We have addressed the major comment in detail below and made revisions to the manuscript to incorporate the referee's suggestions.
read point-by-point responses
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Referee: The derivation of transport coefficients relies on the relaxation-time approximation with a single, isotropic and wavevector-independent relaxation time. As the elliptical magnon modes arise from the anisotropy, this is likely to make the scattering rates (and thus tau) momentum-dependent, particularly for magnon-phonon or magnon-magnon scattering. This could change the quantitative corrections and possibly the qualitative enhancement/decrease behavior for the spin conductivity. The paper should either justify the constant-tau choice or provide an estimate of the error introduced by this approximation.
Authors: We agree that the assumption of a constant, wavevector-independent relaxation time is an approximation that warrants further discussion, particularly given the anisotropy introduced by ellipticity. In the original manuscript, this choice was made to focus on the intrinsic effects of the elliptical magnon orbits on the transport coefficients through modifications to the dispersion, velocity, and spin density. This is a standard approach in the literature on magnon transport in anisotropic systems to separate band effects from scattering details. To address the referee's concern, we will revise the manuscript to include a dedicated paragraph in the Boltzmann transport section. There, we will justify the constant-τ approximation by arguing that the ellipticity primarily affects the magnon group velocities and the spin carried by each mode, leading to the reported enhancement or reduction in conductivities. For scattering processes like magnon-phonon interactions, while momentum dependence exists, the qualitative behavior for small anisotropy parameters (as considered in our perturbation analysis) remains dominated by the changes in the density of states and velocities rather than scattering anisotropy. We note that a full microscopic treatment of k-dependent τ would require specifying the dominant scattering mechanism and is left for future studies. However, we believe the trends we report are robust under this approximation. revision: yes
Circularity Check
Derivation self-contained; no reduction to inputs by construction
full rationale
The paper derives the magnon dispersion and spin polarization from the LLG equation including perpendicular anisotropy, yielding elliptical orbits that modify group velocity and density of states. It then inserts these into the Boltzmann transport equation solved in the relaxation-time approximation under a perturbative expansion around local equilibrium, using an explicitly stated single isotropic relaxation time. The resulting spin and thermal conductivities are computed integrals over the modified dispersion; the reported enhancement or suppression due to ellipticity therefore follows directly from the altered velocities and DOS rather than from any fitted parameter or self-referential definition. No load-bearing self-citations, uniqueness theorems imported from prior author work, or ansatzes smuggled via citation are present in the provided text. The constant-tau assumption is a standard modeling choice whose validity is a separate question of approximation quality, not a circularity in the derivation chain itself.
Axiom & Free-Parameter Ledger
free parameters (1)
- magnon relaxation time
axioms (2)
- standard math Magnetization dynamics are governed by the Landau-Lifshitz-Gilbert equation.
- domain assumption Diffusive transport can be described by the Boltzmann equation in the relaxation-time approximation.
Lean theorems connected to this paper
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IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
using the Boltzmann transport equation in the relaxation time approximation and perturbation analysis, the magnon-spin and magnon thermal conductivities are obtained... Expanding in Taylor series in G... Δσ(3D)m ≡ 4τe²kBT (K0 − K∞) G / (3π²ℏ² J1 K0 K∞)
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IndisputableMonolith/Foundation/AlexanderDuality.leanalexander_duality_circle_linking unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
in both three- and two-dimensional systems... ellipticity... enhancement or a decrease, depending on whether magnets with a easy or hard perpendicular-to-plane axis
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
Works this paper leans on
-
[1]
L. Landau and E. Lifshitz,On the theory of the dispersion of magnetic permeability in ferromagnetic bodies,Phys. Z. Sowjetunion8,153 (1935)
work page 1935
-
[2]
DOI:10.1016/B978-0-08-044316-4.X0001-1
Mayergoyz I D, Bertotti G, Serpico C.Nonlinear Mag- netization Dynamics in Nanosystems(Elsevier, Oxford, 2009). DOI:10.1016/B978-0-08-044316-4.X0001-1
-
[3]
D. C. Ralph and M. D. Stiles,Spin transfer torques,J. Magn. Magn. Mater.320, 1190 (2008). DOI:10.1016/j.jmmm.2007.12.019
-
[4]
Slonczewski,Current-driven excitation of magnetic multilayers,J
J.C. Slonczewski,Current-driven excitation of magnetic multilayers,J. Magn. Magn. Mater.159, L1 (1996). DOI:10.1016/0304-8853(96)00062-5
-
[5]
Berger,Emission of spin waves by a magnetic mul- tilayer traversed by a current,Phys
L. Berger,Emission of spin waves by a magnetic mul- tilayer traversed by a current,Phys. Rev. B54, 9353 (1996). DOI:10.1103/PhysRevB.54.9353
-
[6]
Q. Shao, P. Li, L. Liu, H. Yang, S. Fukami, A. Razavi, H. Wu, K. Wang, F. Freimuth, Y . Mokrousov, M. D. Stiles, S. Emori, A. Hoffmann, J. Åkerman, K. Roy, J.-P. Wang, S.-H. Yang, K. Garello, and W. Zhang,Roadmap of Spin- Orbit Torques,IEEE Trans. Magn.57, 1 (2021). DOI:10.1109/TMAG.2021.3078583
-
[7]
G. E. W. Bauer, E. Saitoh, and B. J. van Wees,Spin caloritronics,Nat. Mater.11, 391 (2012). DOI:10.1038/nmat3301
-
[8]
A. Bose and A. A. Tulapurkar,Recent advances in the spin Nernst effect, Journal of Magnetism and Magnetic Materials,J. Magn. Magn. Mater.491, 165526 (2019). DOI:10.1016/j.jmmm.2019.165526
-
[9]
Uchida,Transport phenomena in spin caloritronics, Proc
K-I. Uchida,Transport phenomena in spin caloritronics, Proc. Japan Acad., Ser. B97, 69 (2021). DOI:10.2183/pjab.97.004
-
[10]
K-I. Uchida, T. An, Y . Kajiwara, M. Toda, and E. Saitoh,Surface-acoustic-wave-driven spin pumping in Y3Fe5O12/Pt hybrid structure,Appl. Phys. Lett.99, 212501 (2011). https://doi.org/10.1063/1.3662032
-
[11]
L. Dreher, M. Weiler, M. Pernpeintner, H. Huebl, R. Gross, M. S. Brandt, and S. T. B. Goennenwein,Sur- face acoustic wave driven ferromagnetic resonance in nickel thin films: Theory and experiment,Phys. Rev. B 86, 134415(2012). DOI:10.1103/PhysRevB.86.134415
-
[12]
J. Zhu, J. A. Katine, G. E. Rowlands, Y . J. Chen, Z. Duan, J. G. Alzate, P. Upadhyaya, J. Langer, P. K. Amiri, K. L. Wang, and I. N. Krivorotov,dcVoltage-Induced Ferromagnetic Resonance in Magnetic Tunnel Junctions, 8 Phys. Rev. Lett.108, 197203 (2012). https://doi.org/10.1103/PhysRevLett.108. 197203
-
[13]
T. Nozaki, T. Yamamoto, S. Miwa, M. Tsujikawa, M. Shirai, S. Yuasa, and Y . Suzuki,Recent Progress in the Voltage-Controlled Magnetic Anisotropy Effect and the Challenges Faced in Developing Voltage-Torque MRAM, Micromachines10, 327 (2019). https://doi.org/10.3390/mi10050327
-
[14]
S. I. Kiselev, J. C. Sankey, I. N. Krivorotov, N. C. Emley, R. J. Schoelkopf, R. A. Buhrman, and D. C. Ralph,Mi- crowave oscillations of a nanomagnet driven by a spin- polarized current,Nature425, 380 (2003). https://doi.org/10.1038/nature01967
-
[15]
A. Slavin and V . Tiberkevich,Nonlinear auto-oscillator theory of microwave generation by spin-polarized current, IEEE Trans. Magn.45, 1875 (2009). https://doi.org/10.1109/TMAG.2008.2009935
-
[16]
D. Berkov and N. Gorn,Transition from the macrospin to chaotic behavior by a spin-torque driven magnetiza- tion precession of a square nanoelement,Phys. Rev. B71, 052403 (2005). https://doi.org/10.1103/PhysRevB.71.052403
-
[17]
A. M. Cabanas, M. G. Clerc, D. Laroze, and A. O. Leon, Chaotic patterns and localized states in spin valves, J. Magn. Magn. Mater.476, 589 (2019). DOI:10.1016/j.jmmm.2019.01.027
-
[18]
G. Tatara, H. Kohno, and J. Shibata,Microscopic ap- proach to current-driven domain wall dynamics,Phys. Rep.468, 213 (2008). DOI:10.1016/j.physrep.2008.07.003
-
[19]
A. Fert, N. Reyren and V . Cros,Magnetic skyrmions: advances in physics and potential applications,Nat. Rev. Mater.2, 17031 (2017). DOI:https://doi.org/10.1038/natrevmats. 2017.31
-
[20]
A. Brataas, B. van Wees, O. Klein, G. de Loubens, and M. Viret,Spin insulatronics,Phys. Rep.885, 1 (2020). DOI:https://doi.org/10.1016/j.physrep.2020. 08.006
-
[21]
A. J. Princep, R. A. Ewings, S. Ward, S. Tóth, C. Dubs, D. Prabhakaran, and A. T. Boothroyd,The full magnon spectrum of yttrium iron garnetnpj Quantum Materials2, 63 (2017). DOI:10.1038/s41535-017-0067-y
-
[22]
Y . Nambu, J. Barker, Y . Okino, T. Kikkawa, Y . Shiomi, M. Enderle, T. Weber, B. Winn, M. Graves-Brook, J. M. Tran- quada, T. Ziman, M. Fujita, G. E. W. Bauer, E. Saitoh, and K. Kakurai,Observation of Magnon Polarization,Phys. Rev. Lett.125, 027201 (2020). DOI:10.1103/PhysRevLett.125.027201
-
[23]
D. S. Maior, E. C. Souza, and S. M. Rezende,Magnon energy renormalization in yttrium iron garnet, Phys. Rev. B108, 054406 (2023). DOI:10.1103/PhysRevB.108.054406
-
[24]
H. Bai, H-A. Zhou, W. Li, T. Xu, L. Wang, P. Gargiani, M. Valvidares, and W. Jiang,4f electron−mediated com- pensated magnetism in rare-earth-substituted iron garnet films with perpendicular magnetic anisotropy, Phys. Rev. Applied23, 044062 (2025). DOI:10.1103/PhysRevApplied.23.044062
-
[25]
P. G. Li, S. M. Ng, X. Yuan, F. X. Zhang, H. F. Wong, Z. Chu, P. Cao, C. W. Leung,Spin magnetotransport in rare- earth iron garnet (REIG)/Pt: Effects of modulated bulk and REIG/Pt interfaces, APL Mater.12, 081114 (2024). DOI:10.1063/5.0215071
-
[26]
V . V . Kruglyak, S. O. Demokritov, and D. Grundler, Magnonics,J. Phys. D: Appl. Phys.43, 264001 (2010). DOI:10.1088/0022-3727/43/26/264001
-
[27]
A. V . Chumak, V . I. Vasyuchka, A. A. Serga, and B. Hille- brands,Magnon spintronics,Nat. Phys.11, 453 (2015). DOI:10.1038/nphys3347
-
[28]
B. Flebus, D. Grundler, B. Rana, Y . Otani, I. Barsukov, A. Barman, G. Gubbiotti, P. Landeros, J. Akerman, U. Ebels, P. Pirro, V . E. Demidov, K. Schultheiss, G. Csaba, Q. Wang, F. Ciubotaru, D. E. Nikonov, P. Che, R. Hertel, T. Ono, D. Afanasiev, J. Mentink, T. Rasing, B. Hillebrands, S. V . Kusminskiy, W. Zhang, C. R. Du, A. Finco, T. van der Sar, Y . K...
-
[29]
S. A. Bender and Y . Tserkovnyak,Interfacial spin and heat transfer between metals and magnetic insulators, Phys. Rev. B91, 140402(R) (2015). DOI:10.1103/PhysRevB.91.140402
-
[30]
C. Ulloa, A. Tomadin, J. Shan, M. Polini, B. J. van Wees, and R. A. Duine,Nonlocal Spin Transport as a Probe of Viscous Magnon Fluids, Phys. Rev. Lett.123, 117203 (2019). DOI:10.1103/PhysRevLett.123.117203
-
[31]
J. Zheng, S. Bender, J. Armaitis, R. E. Troncoso, and R. A. Duine,Green’s function formalism for spin transport in metal-insulator-metal heterostructures,Phys. Rev. B96, 174422 (2017). DOI:10.1103/PhysRevB.96.174422
-
[32]
J. Gao, C-H. Lambert, R. Schlitz, M. Fiebig, P. Gam- bardella, and Saül Vélez,Magnon transport and ther- moelectric effects in ultrathin Tm3Fe5O12/Pt nonlocal de- vices,Phys. Rev. Research4, 043214 (2022). DOI:10.1103/PhysRevResearch.4.043214 9
-
[33]
L. J. Cornelissen, K. J. H. Peters, G. E. W. Bauer, R. A. Duine, and B. J. van Wees,Magnon spin transport driven by the magnon chemical potential in a magnetic insulator, Phys. Rev. B94, 014412 (2016). DOI:10.1103/PhysRevB.94.014412
-
[34]
O. Alves Santos and B. J. van Wees,Magnon Confinement in an All-on-Chip YIG Cavity Resonator Using Hybrid YIG/Py Magnon Barriers, Nano Lett.23, 9303 (2023). DOI:10.1021/acs.nanolett.3c02388
-
[35]
T. Yu, C. Cai, G. E. W. Bauer,Chirality enables thermal magnon transistors, Sci. China Phys. Mech. Astron.67, 247511 (2024). DOI:10.1007/s11433-023-2294-1
-
[36]
D. K. de Wal, R. L. Mena, M. Zohaib, and B. J. van Wees, Gate control of magnon spin transport in unconventional magnon transistors based on the van der Waals antiferro- magnet CrPS4, Phys. Rev. B110, 224434 (2024). DOI:10.1103/PhysRevB.110.224434
-
[37]
X.-Y . Wei, O. Alves Santos, C. H. Sumba Lusero, G. E. W. Bauer, J. Ben Youssef, and B. J. van Wees,Giant magnon spin conductivity in ultrathin yttrium iron garnet films, Nat. Mater.21, 1352 (2022). DOI:10.1038/s41563-022-01369-0
-
[38]
G. E. W. Bauer, P. Tang, M. Elyasi, Y . M. Blanter, and B. J. van Wees,Soft magnons in anisotropic ferromagnets, Phys. Rev. B108, 064431 (2023). DOI:10.1103/PhysRevB.108.064431
-
[39]
T. Wimmer, M. Althammer, L. Liensberger, N. Vliet- stra, S. Geprägs, M. Weiler, R. Gross, and H. Huebl, Spin Transport in a Magnetic Insulator with Zero Effec- tive Damping,Phys. Rev. Lett.123, 257201 (2019). DOI:10.1103/PhysRevLett.123.257201
-
[40]
J. Gückelhorn, T. Wimmer, M. Müller, S. Geprägs, H. Huebl, R. Gross, and M. Althammer,Magnon transport in Y3Fe5O12/Pt nanostructures with reduced effective magne- tization,Phys. Rev. B104, L180410 (2021). DOI:10.1103/PhysRevB.104.L180410
-
[41]
Y . Yin, Y . Liu, Y . Liu, and X. Wan,Influence of magnon renormalization and interband coupling on the spin See- beck effect in YIG, Phys. Rev. B110, 144413 (2024). DOI:10.1103/PhysRevB.110.144413
-
[42]
J. Liu, X-Y . Wei, G. E. W. Bauer, J. Ben Youssef, and B. J. van Wees,Electrically induced strong modulation of magnon transport in ultrathin magnetic insulator films, Phys. Rev. B103, 214425 (2021). DOI:10.1103/PhysRevB.103.214425
-
[43]
H. Taghinejad, K. Yamakawa, X. Huang, Y . Lyu, L. P. Cairns, S. Husain, R. Ramesh, and J. G. Analytis,Low- Field Regime of Magnon Transport in PLD-Grown YIG Films, Nano Lett.25, 6438 (2025). DOI:10.1021/acs.nanolett.4c06592
-
[44]
M. A. Myhre, V . Brehm, T. Delvaux, A. Brataas, and A. Qaiumzadeh,Thickness-dependent magnon spin transport in antiferromagnetic insulators: Crossover from quasi-three-dimensional to quasi-two-dimensional regimes, arXiv:2509.03941 DOI:10.48550/arXiv.2509.03941
-
[45]
W. P. Sterk, H. Y . Yuan, A. Rückriegel, B. Z. Rameshti, and R. A. Duine,Green’s function formalism for nonlo- cal elliptical magnon transport, Phys. Rev. B104, 174404 (2021). DOI:10.1103/PhysRevB.104.174404
-
[46]
J. Zheng, A. Rückriegel, S. A. Bender, and R. A. Duine, Ellipticity and dissipation effects in magnon spin valves, Phys. Rev. B 101, 094402 (2020). DOI:10.1103/PhysRevB.101.094402
-
[47]
A. O. Leon and M. G. Clerc, Spin-transfer-driven nano- oscillators are equivalent to parametric resonators, Phys. Rev. B91, 014411 (2015). DOI:10.1103/PhysRevB.91.014411
-
[48]
H. J. Mikeska,Solitons in a one-dimensional magnet with an easy plane,J. Phys. C11, L29 (1978). DOI:https://doi.org/10.1088/0022-3719/11/1/ 007
-
[49]
I. V . Barashenkov and E. V . Zemlyanaya,Stable Com- plexes of Parametrically Driven, Damped Nonlinear Schrödinger Solitons, Phys. Rev. Lett. 83, 2568 (1999). DOI:10.1103/PhysRevLett.83.2568
-
[50]
M. G. Clerc, S. Coulibaly, D. Laroze, A. O. Leon, and A. S. Núñez,Alternating spin-polarized current induces parametric resonance in spin valves, Phys. Rev. B91, 224426 (2015). DOI:10.1103/PhysRevB.91.224426 [51]Dissipative magnetic breathers induced by time- modulated voltages, A. O. Leon, M. G. Clerc, and D. Altbir, Phys. Rev. E98, 062213 (2018). DOI:10...
-
[51]
S. Streib, N. Vidal-Silva, K. Shen, and G. E. W. Bauer,Magnon-phonon interactions in magnetic insula- tors,Phys. Rev. B99, 184442 (2019). DOI:10.1103/PhysRevB.99.184442
-
[52]
A. Rückriegel, P. Kopietz, D. A. Bozhko, A. A. Serga, and B. Hillebrands,Magnetoelastic modes and lifetime of magnons in thin yttrium iron garnet films,Phys. Rev. B 89, 184413 (2014). DOI:10.1103/PhysRevB.89.184413
-
[53]
J. Barker, and G. E. W. BauerThermal Spin Dynamics of Yttrium Iron GarnetPhys. Rev. Lett.117, 217201 (2016). DOI:10.1103/PhysRevLett.117.217201 10
-
[54]
H. Urra, J. F. Marín, M. Páez-Silva, M. Taki, S. Coulibaly, L. Gordillo, and M. A. García-Ñustes,Localized Fara- day patterns under heterogeneous parametric excitation, Phys. Rev. E99, 033115 (2019). DOI:10.1103/PhysRevE.99.033115
-
[55]
N. V . Alexeeva, I. V . Barashenkov, and G. P. Tsironis, Impurity-Induced Stabilization of Solitons in Arrays of Parametrically Driven Nonlinear Oscillators, Phys. Rev. Lett.84, 3053 (2000). DOI:10.1103/PhysRevLett.84.3053
-
[56]
F. De Lucia, P. Parra-Rivas, C. Mas Arabí, P-J. Sazio, S- P. Gorza, and F. Leo,Parametrically driven Kerr cavity solitons, N. Englebert, Nat. Photonics15, 857 (2021). DOI:10.1038/s41566-021-00858-z
-
[57]
I. V . Barashenkov, M. M. Bogdan and V . I. Korobov,Sta- bility Diagram of the Phase-Locked Solitons in the Para- metrically Driven, Damped Nonlinear Schrödinger Equa- tion, EPL15, 113 (1991). DOI:10.1209/0295-5075/15/2/001 11
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