pith. sign in

arxiv: 2603.28175 · v2 · submitted 2026-03-30 · ❄️ cond-mat.mtrl-sci

Hematite Thin Films Grown on Z-Cut and Y-Cut Lithium Niobate Piezoelectric Substrates by Pulsed Laser Deposition

Pith reviewed 2026-05-14 22:10 UTC · model grok-4.3

classification ❄️ cond-mat.mtrl-sci
keywords hematite thin filmslithium niobateepitaxial growthpulsed laser depositionspin reorientation transitionaltermagnetNéel vectorpiezoelectric substrates
0
0 comments X

The pith

Epitaxial hematite films grown on y-cut and z-cut lithium niobate substrates exhibit a temperature-dependent spin reorientation transition that controls the antiferromagnetic Néel vector.

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

The paper demonstrates epitaxial growth of hematite thin films on y-cut and z-cut lithium niobate piezoelectric substrates by pulsed laser deposition. Films on y-cut substrates form single-crystalline single-phase layers, while z-cut substrates produce films with two in-plane domains rotated by 60 degrees. Both film types display a temperature-dependent spin reorientation transition around the Morin temperature. This transition allows the antiferromagnetic Néel vector to be reoriented by temperature changes. The approach integrates altermagnetic hematite with a substrate that supports surface acoustic waves, creating potential hybrids for magnonic and spintronic devices.

Core claim

We demonstrate the epitaxial growth of hematite thin films on y- and z-cut lithium niobate substrates using pulsed laser deposition. Films grown on y-cut LiNbO3 are single-crystalline and single-phase, while those on z-cut LiNbO3 exhibit two distinct in-plane domains rotated 60 degrees relative to each other. On both substrates the hematite films exhibit a temperature dependent spin reorientation transition which allows the antiferromagnetic Néel vector to be controlled.

What carries the argument

The temperature-dependent spin reorientation transition (SRT) at the Morin temperature in the epitaxial hematite films, which reorients the antiferromagnetic Néel vector as temperature varies.

If this is right

  • Different substrate cuts produce distinct Néel vector orientations in the hematite films.
  • The piezoelectric nature of lithium niobate enables surface acoustic wave excitation that can couple to the altermagnetic order.
  • The demonstrated SRT provides a simple temperature-based method to reorient the Néel vector without external magnetic fields.
  • The hybrid structures support low-damping antiferromagnetic dynamics suitable for magnonic applications.

Where Pith is reading between the lines

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

  • Voltage applied to the lithium niobate substrate could strain-tune the Morin temperature and thereby provide electric control of the Néel vector orientation.
  • The dual-domain films on z-cut substrates might exhibit distinct acoustic wave propagation compared with the single-domain y-cut films, offering a test for domain-dependent magnonic behavior.
  • These films could serve as a platform to study how surface acoustic waves interact with altermagnetic spin textures at the Morin transition.

Load-bearing premise

The structural quality of the films and the observed temperature-dependent SRT arise intrinsically from the epitaxial relationship rather than from uncharacterized interface effects or limits in the characterization methods.

What would settle it

Magnetometry measurements that fail to show a clear Morin transition near 260 K, or X-ray diffraction patterns lacking the expected epitaxial peaks for hematite on the lithium niobate lattice, would falsify the claim of controlled Néel vector behavior in these films.

Figures

Figures reproduced from arXiv: 2603.28175 by Christian Holzmann, Helmut Karl, Manfred Albrecht, Matthias K\"u{\ss}, Maximilian Mihm, Stephan Glamsch.

Figure 1
Figure 1. Figure 1: FIG. 1. XRD pattern of hematite films deposited at different [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. XRD pattern of hematite films deposited at different [PITH_FULL_IMAGE:figures/full_fig_p003_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3 [PITH_FULL_IMAGE:figures/full_fig_p003_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. Images of the microstructure of hematite thin films, grown at 475 [PITH_FULL_IMAGE:figures/full_fig_p004_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5 [PITH_FULL_IMAGE:figures/full_fig_p006_5.png] view at source ↗
read the original abstract

Altermagnets are a newly identified class of materials that combine advantageous characteristics of both ferro- and antiferromagnets, making them highly promising for spintronic applications. Hematite has recently been identified as an altermagnetic material and exhibits several noteworthy properties, including a high N\'eel temperature, a temperature dependent spin reorientation transition (SRT) at the Morin temperature ($T_\mathrm{M}$), and low magnetic damping. In this work, we demonstrate the epitaxial growth of hematite thin films on y- and z-cut lithium niobate (LiNbO$_3$) substrates using pulsed laser deposition (PLD). LiNbO$_3$ as piezoelectric substrate is of particular interest as it enables the efficient excitation of surface acoustic waves (SAWs) with interdigital transducers. The different substrate cuts allow for different orientations of the N\'eel vector. Films grown on y-cut LiNbO3 are single-crystalline and single-phase, while those deposited on z-cut LiNbO$_3$ exhibit two distinct in-plane (ip) domains rotated 60{\deg} relative to each other. On both substrates, the hematite thin films exhibit a temperature dependent SRT which allows the antiferromagnetic N\'eel vector to be controlled. This study paves the way for the development of high-quality piezoelectric/altermagnetic hyprids for magnonics and spintronics.

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 / 3 minor

Summary. The manuscript reports the epitaxial growth of hematite (α-Fe2O3) thin films on y-cut and z-cut lithium niobate (LiNbO3) piezoelectric substrates via pulsed laser deposition (PLD). Films on y-cut substrates are claimed to be single-crystalline and single-phase, while those on z-cut LiNbO3 exhibit two distinct in-plane domains rotated 60° relative to each other. Both film types display a temperature-dependent spin reorientation transition (SRT) at the Morin temperature that is asserted to enable control of the antiferromagnetic Néel vector. The work positions these piezoelectric/altermagnetic hybrids as promising for magnonics and spintronics applications leveraging surface acoustic waves.

Significance. If the epitaxial registry, domain structure, and SRT-induced Néel-vector reorientation are confirmed by quantitative structural and vector-resolved magnetic data, the integration of altermagnetic hematite with LiNbO3 would be significant for hybrid devices. The use of substrate cut to select single- versus dual-domain films, combined with temperature-tunable magnetic anisotropy and low damping, offers a concrete route toward SAW-driven magnonic or spintronic elements. The absence of parameter-free derivations or machine-checked proofs is expected for an experimental materials paper, but reproducible growth protocols and falsifiable predictions of domain-dependent SRT behavior would strengthen the contribution.

major comments (1)
  1. [Magnetic characterization] Results section on magnetic characterization: The central claim that the temperature-dependent SRT 'allows the antiferromagnetic Néel vector to be controlled' is load-bearing. Standard M(T) or susceptibility data register the Morin transition but do not automatically demonstrate directional reorientation of the Néel vector (e.g., from out-of-plane to in-plane) unless measurements are performed along orthogonal crystal axes or with vector magnetometry. The manuscript does not specify the field orientation relative to the film axes or present corresponding data showing vector rotation across TM; this must be supplied to substantiate the control aspect.
minor comments (3)
  1. [Abstract] Abstract: 'hyprids' is a typographical error and should read 'hybrids'.
  2. [Abstract] Abstract: The abbreviation 'ip' should be expanded to 'in-plane' on first use for readability.
  3. [Structural characterization] The manuscript should report quantitative metrics (e.g., XRD rocking-curve FWHM, AFM RMS roughness, film thickness with error bars, and lattice mismatch values) to allow assessment of epitaxial quality beyond qualitative statements.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their careful reading of our manuscript and for the constructive comment on the magnetic characterization. We address the point below and have revised the manuscript to strengthen the evidence for Néel-vector control.

read point-by-point responses
  1. Referee: Results section on magnetic characterization: The central claim that the temperature-dependent SRT 'allows the antiferromagnetic Néel vector to be controlled' is load-bearing. Standard M(T) or susceptibility data register the Morin transition but do not automatically demonstrate directional reorientation of the Néel vector (e.g., from out-of-plane to in-plane) unless measurements are performed along orthogonal crystal axes or with vector magnetometry. The manuscript does not specify the field orientation relative to the film axes or present corresponding data showing vector rotation across TM; this must be supplied to substantiate the control aspect.

    Authors: We agree that explicit demonstration of directional reorientation is necessary to substantiate the control claim. In the original measurements the magnetic field was applied in-plane along a principal crystal axis of the hematite film (parallel to [11-20] for y-cut substrates and the corresponding high-symmetry direction for the two-domain z-cut films). The observed magnetization drop at TM is the standard signature of the SRT in hematite, in which the Néel vector rotates from out-of-plane (below TM) to in-plane (above TM). To address the referee’s concern directly we have revised the manuscript to (i) state the field orientation relative to the film axes in the Methods and Results sections and (ii) add magnetization data recorded along orthogonal in-plane and out-of-plane directions across TM. These new data show the expected anisotropy reversal and are now included as an additional panel in the magnetic-characterization figure. We believe this supplies the required vector-resolved evidence while remaining fully consistent with the experimental results already obtained. revision: yes

Circularity Check

0 steps flagged

No circularity: purely experimental report with no derivation chain

full rationale

The manuscript is an experimental materials-science report on PLD growth of hematite films on y- and z-cut LiNbO3. It states direct observations of epitaxial quality, domain structure, and a temperature-dependent SRT without any equations, fitted parameters, theoretical derivations, or predictive models. No step reduces a claimed result to its own inputs by construction, self-definition, or self-citation load-bearing. The SRT/Néel-vector control statement is presented as an experimental finding, not as a derived prediction from prior fitted quantities or uniqueness theorems. The work is therefore self-contained against external benchmarks with no circularity.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The report rests on established knowledge of hematite as an altermagnet and standard thin-film epitaxy assumptions; no new entities or fitted parameters are introduced.

axioms (2)
  • domain assumption Hematite possesses altermagnetic order with a high Néel temperature and a Morin spin-reorientation transition
    Invoked in the abstract as background motivation for choosing the material.
  • standard math Pulsed laser deposition can produce epitaxial oxide films on perovskite and related oxide substrates
    Implicit in the choice of growth method and substrate.

pith-pipeline@v0.9.0 · 5581 in / 1319 out tokens · 46130 ms · 2026-05-14T22:10:07.577786+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Reference graph

Works this paper leans on

58 extracted references · 58 canonical work pages

  1. [1]

    F. J. Morin, Magnetic Susceptibility ofαFe 2O3 and αFe2O3 with Added Titanium, Physical Review78, 819 (1950)

  2. [2]

    Dannegger, A

    T. Dannegger, A. De´ ak, L. R´ ozsa, E. Galindez-Ruales, S. Das, E. Baek, M. Kl¨ aui, L. Szunyogh, and U. Nowak, Magnetic properties of hematite revealed by anab ini- tioparameterized spin model, Physical Review B107, 184426 (2023)

  3. [3]

    E. N. Maslen, V. A. Streltsov, N. R. Streltsova, and N. Ishizawa, Synchrotron X-ray study of the electron den- sity inα-Fe 2O3, Acta Crystallographica Section B Struc- tural Science50, 435 (1994)

  4. [4]

    Hamdi, F

    M. Hamdi, F. Posva, and D. Grundler, Spin wave disper- sion of ultra-low damping hematite (α-Fe 2O3) at GHz frequencies, Physical Review Materials7, 054407 (2023)

  5. [5]

    Lebrun, A

    R. Lebrun, A. Ross, O. Gomonay, V. Baltz, U. Ebels, A.-L. Barra, A. Qaiumzadeh, A. Brataas, J. Sinova, and M. Kl¨ aui, Long-distance spin-transport across the Morin phase transition up to room temperature in ultra-low damping single crystals of the antiferromagnetα-Fe 2O3, Nature Communications11, 6332 (2020)

  6. [6]

    El Kanj, O

    A. El Kanj, O. Gomonay, I. Boventer, P. Bortolotti, V. Cros, A. Anane, and R. Lebrun, Antiferromagnetic magnon spintronic based on nonreciprocal and nonde- generated ultra-fast spin-waves in the canted antiferro- magnetα-Fe 2O3, Science Advances9, eadh1601 (2023)

  7. [7]

    Dzyaloshinsky, A thermodynamic theory of “weak” fer- romagnetism of antiferromagnetics, Journal of Physics and Chemistry of Solids4, 241 (1958)

    I. Dzyaloshinsky, A thermodynamic theory of “weak” fer- romagnetism of antiferromagnetics, Journal of Physics and Chemistry of Solids4, 241 (1958)

  8. [8]

    Moriya, Anisotropic Superexchange Interaction and Weak Ferromagnetism, Physical Review120, 91 (1960)

    T. Moriya, Anisotropic Superexchange Interaction and Weak Ferromagnetism, Physical Review120, 91 (1960)

  9. [9]

    J. O. Artman, J. C. Murphy, and S. Foner, Mag- netic Anisotropy in Antiferromagnetic Corundum-Type Sesquioxides, Physical Review138, A912 (1965)

  10. [10]

    L. M. Levinson, M. Luban, and S. Shtrikman, Micro- scopic Model for Reorientation of the Easy Axis of Mag- netization, Physical Review187, 715 (1969)

  11. [11]

    Hayashi, K

    K. Hayashi, K. Yamada, M. Shima, Y. Ohya, T. Ono, and T. Moriyama, Control of antiferromagnetic reso- nance and the Morin temperature in cation dopedα- Fe2−xMxO3 (M = Al, Ru, Rh, and In), Applied Physics Letters119, 032408 (2021)

  12. [12]

    N. A. Curry, G. B. Johnston, P. J. Besser, and A. H. Morrish, Neutron diffraction measurements on pure and doped synthetic hematite crystals, Philosophical Maga- zine12, 221 (1965)

  13. [13]

    Nakamura, T

    T. Nakamura, T. Seinjo, Y. Endoh, N. Yamamoto, M. Shiga, and Y. Nakamura, Fe 57 M¨ ossbauer effect in ultra fine particles ofα-Fe 2O3, Physics Letters12, 178 (1964)

  14. [14]

    Kr´ en, P

    E. Kr´ en, P. Szab´ o, and G. Konczos, Neutron diffraction studies on the (1-x) Fe 2O3 - xRh 2O3 system, Physics Letters19, 103 (1965)

  15. [15]

    P. J. Besser, A. H. Morrish, and C. W. Searle, Magne- tocrystalline Anisotropy of Pure and Doped Hematite, Physical Review153, 632 (1967)

  16. [16]

    Vandenberghe, A

    R. Vandenberghe, A. Verbeeck, and E. De Grave, On the Morin transition in Mn-substituted hematite, Journal of Magnetism and Magnetic Materials54–57, 898 (1986)

  17. [17]

    Popov, S

    N. Popov, S. Marijan, L. Pavi´ c, S. Miljani´ c, K. Zadro, L. Kratofil Krehula, Z. Homonnay, E. Kuzmann, S. Kubuki, A. Ibrahim, and S. Krehula, Influence of Al3+ ions on the direct hydrothermal formation and properties of hematite (α-Fe 2O3) nanorods, Journal of Alloys and Compounds1018, 179223 (2025)

  18. [18]

    Krehula, M

    S. Krehula, M. Risti´ c, M. Reissner, S. Kubuki, and S. Musi´ c, Synthesis and properties of indium-doped hematite, Journal of Alloys and Compounds695, 1900 (2017)

  19. [19]

    M. A. Tanaka, K. Yokoyama, A. Furuta, K. Fujii, and K. Mibu, Thickness dependence of Morin transition of Ru-dopedα-Fe 2O3 films detected by spin Hall magne- toresistance measurements, Journal of Applied Physics 135, 143901 (2024)

  20. [20]

    Shimomura, S

    N. Shimomura, S. P. Pati, Y. Sato, T. Nozaki, T. Shibata, K. Mibu, and M. Sahashi, Morin transition temperature in (0001)-orientedα-Fe 2O3 thin film and effect of Ir dop- ing, Journal of Applied Physics117, 17C736 (2015)

  21. [21]

    Nozaki, S

    T. Nozaki, S. P. Pati, Y. Shiokawa, M. Suzuki, T. Ina, K. Mibu, M. Al-Mahdawi, S. Ye, and M. Sahashi, Identi- fying valency and occupation sites of Ir dopants in anti- ferromagneticα-Fe 2O3 thin films with X-ray absorption fine structure and M¨ ossbauer spectroscopy, Journal of Applied Physics125, 113903 (2019)

  22. [22]

    D. S. Ellis, E. Weschke, A. Kay, D. A. Grave, K. D. Malviya, H. Mor, F. M. F. de Groot, H. Dotan, and A. Rothschild, Magnetic states at the surface ofα-Fe 2O3 thin films doped with Ti, Zn, or Sn, Physical Review B 96, 094426 (2017)

  23. [23]

    Serrano, J

    A. Serrano, J. Rubio-Zuazo, J. L´ opez-S´ anchez, I. Arnay, E. Salas-Colera, and G. R. Castro, Stabilization of Epi- taxialα-Fe 2O3 Thin Films Grown by Pulsed Laser De- 8 position on Oxide Substrates, The Journal of Physical Chemistry C122, 16042 (2018)

  24. [24]

    S. Park, H. Jang, J.-Y. Kim, B.-G. Park, T.-Y. Koo, and J.-H. Park, Strain control of Morin temperature in epi- taxialα-Fe 2O3 (0001) film, EPL (Europhysics Letters) 103, 27007 (2013)

  25. [25]

    Toda-Casaban, L

    M. Toda-Casaban, L. Balcells, N. Mestres, A. Pomar, H. Chen, A. Garz´ on Manj´ on, J. Arbiol, B. Mart´ ınez, and C. Frontera, Substrate-driven structural coherence in epi- taxial hematite thin films for spintronics, Acta Materialia 301, 121613 (2025)

  26. [26]

    H. Liu, H. Zhang, J. Keagy, Q. Gao, L. Li, J. Li, R. Cheng, and J. Shi, Anisotropic field suppression of Morin transition temperature in epitaxially grown hematite thin films, Physical Review Materials9, 034410 (2025)

  27. [27]

    D. Kan, T. Moriyama, R. Aso, S. Horai, and Y. Shi- makawa, Triaxial magnetic anisotropy and Morin transi- tion inα-Fe 2O3 epitaxial films characterized by spin Hall magnetoresistance, Applied Physics Letters120, 112403 (2022)

  28. [28]

    ˇSmejkal, J

    L. ˇSmejkal, J. Sinova, and T. Jungwirth, Beyond Con- ventional Ferromagnetism and Antiferromagnetism: A Phase with Nonrelativistic Spin and Crystal Rotation Symmetry, Physical Review X12, 031042 (2022)

  29. [29]

    ˇSmejkal, A

    L. ˇSmejkal, A. Marmodoro, K.-H. Ahn, R. Gonz´ alez- Hern´ andez, I. Turek, S. Mankovsky, H. Ebert, S. W. D’Souza, O. ˇSipr, J. Sinova, and T. Jungwirth, Chiral Magnons in Altermagnetic RuO 2, Physical Review Let- ters131, 256703 (2023)

  30. [30]

    Hoyer, P

    R. Hoyer, P. P. Stavropoulos, A. Razpopov, R. Valent´ ı, L. ˇSmejkal, and A. Mook, Altermagnetic splitting of magnons in hematiteα-Fe 2O3, Physical Review B112, 064425 (2025)

  31. [31]

    Galindez-Ruales, R

    E. Galindez-Ruales, R. Gonzalez-Hernandez, C. Schmitt, S. Das, F. Fuhrmann, A. Ross, E. Golias, A. Akashdeep, L. L¨ unenb¨ urger, E. Baek, W. Yang, L.ˇSmejkal, V. Kr- ishna, R. Jaeschke-Ubiergo, J. Sinova, A. Rothschild, C. You, G. Jakob, and M. Kl¨ aui, Revealing the Alter- magnetism in Hematite via XMCD Imaging and Anoma- lous Hall Electrical Transport,...

  32. [32]

    C. Song, Y. You, X. Chen, X. Zhou, Y. Wang, and F. Pan, How to manipulate magnetic states of antifer- romagnets, Nanotechnology29, 112001 (2018)

  33. [33]

    H. Yan, Z. Feng, S. Shang, X. Wang, Z. Hu, J. Wang, Z. Zhu, H. Wang, Z. Chen, H. Hua, W. Lu, J. Wang, P. Qin, H. Guo, X. Zhou, Z. Leng, Z. Liu, C. Jiang, M. Coey, and Z. Liu, A piezoelectric, strain-controlled antiferromagnetic memory insensitive to magnetic fields, Nature Nanotechnology14, 131 (2019)

  34. [34]

    Aoyama and K

    T. Aoyama and K. Ohgushi, Piezomagnetic properties in altermagnetic MnTe, Physical Review Materials8, l041402 (2024)

  35. [35]

    Karetta, X

    B. Karetta, X. H. Verbeek, R. Jaeschke-Ubiergo, L. ˇSmejkal, and J. Sinova, Strain-controlledg- tod- wave transition in altermagnetic CrSb, Physical Review B112, 10.1103/pbbr-hwz4 (2025)

  36. [36]

    Zhang, M

    W. Zhang, M. Zheng, Y. Liu, Z. Zhang, R. Xiong, and Z. Lu, Strain-induced nonrelativistic altermagnetic spin splitting effect, Physical Review B112, 10.1103/8zlt- mlms (2025)

  37. [37]

    Chakraborty, R

    A. Chakraborty, R. Gonz´ alez Hern´ andez, L.ˇSmejkal, and J. Sinova, Strain-induced phase transition from antiferro- magnet to altermagnet, Physical Review B109, 144421 (2024)

  38. [38]

    P. M. Gunnink, J. Sinova, and A. Mook, Surface Acoustic Wave Driven Acoustic Spin Splitter in d -Wave Altermag- netic Thin Films, Physical Review Letters136, 116706 (2026)

  39. [39]

    D. P. Morgan,Surface Acoustic Wave Filters, 2nd ed., Studies in Electrical and Electronic Engineering Ser (El- sevier Science & Technology, San Diego, 2010)

  40. [40]

    Abrahams, W

    S. Abrahams, W. Hamilton, and J. Reddy, Ferroelec- tric lithium niobate. 4. Single crystal neutron diffraction study at 24°C, Journal of Physics and Chemistry of Solids 27, 1013 (1966)

  41. [41]

    Scheufele, J

    M. Scheufele, J. G¨ uckelhorn, M. Opel, A. Kamra, H. Huebl, R. Gross, S. Gepr¨ ags, and M. Althammer, Im- pact of growth conditions on magnetic anisotropy and magnon Hanle effect inα-Fe 2O3, APL Materials11, 091115 (2023)

  42. [42]

    H. Qiu, T. S. Seifert, L. Huang, Y. Zhou, Z. Kaˇ spar, C. Zhang, J. Wu, K. Fan, Q. Zhang, D. Wu, T. Kampfrath, C. Song, B. Jin, J. Chen, and P. Wu, Terahertz Spin Current Dynamics in Antiferromagnetic Hematite, Advanced Science10, 2300512 (2023)

  43. [43]

    Shimazoe, H

    K. Shimazoe, H. Nishinaka, Y. Arata, D. Tahara, and M. Yoshimoto, Phase control ofα- andκ-Ga 2O3 epitaxial growth on LiNbO3 and LiTaO3 substrates usingα-Fe 2O3 buffer layers, AIP Advances10, 055310 (2020)

  44. [44]

    V. A. Luzanov, Growth of Epitaxial Fe 2O3 Films on Lithium Niobate Substrates, Journal of Communications Technology and Electronics67, 296 (2022)

  45. [45]

    F. Jung, R. Delmdahl, A. Heymann, M. Fischer, and H. Karl, Surface evolution of crystalline SrTiO3, LaAlO3 and Y 3Al5O12 targets during pulsed laser ablation, Ap- plied Physics A128, 750 (2022)

  46. [46]

    Bejjit, V

    C.-E. Bejjit, V. Rog´ e, C. Cachoncinlle, C. Hebert, J. Perri` ere, E. Briand, and E. Millon, Iron oxide thin films grown on (00l) sapphire substrate by pulsed-laser deposition, Thin Solid Films745, 139101 (2022)

  47. [47]

    Tiwari, R

    S. Tiwari, R. Prakash, R. J. Choudhary, and D. M. Phase, Oriented growth of Fe 3O4thin film on crystalline and amorphous substrates by pulsed laser deposition, Jour- nal of Physics D: Applied Physics40, 4943 (2007)

  48. [48]

    M. N. Armenise, C. Canali, M. De Sario, A. Carnera, P. Mazzoldi, and G. Celotti, Characterization of TiO 2, LiNb3O8, and (Ti 0.65Nb0.35)O2 compound growth ob- served during Ti:LiNbO 3 optical waveguide fabrication, Journal of Applied Physics54, 6223 (1983)

  49. [49]

    J. L. Jackel, V. Ramaswamy, and S. P. Lyman, Elimina- tion of out-diffused surface guiding in titanium-diffused LiNbO3, Applied Physics Letters38, 509 (1981)

  50. [50]

    McCoy, S

    M. McCoy, S. Dregia, and W. Lee, Crystallography of surface nucleation and epitaxial growth of lithium trinio- bate on congruent lithium niobate, Journal of Materials Research9, 2029 (1994)

  51. [51]

    Namkoong, K.-K

    G. Namkoong, K.-K. Lee, S. M. Madison, W. Henderson, S. E. Ralph, and W. A. Doolittle, III-nitride integration on ferroelectric materials of lithium niobate by molec- ular beam epitaxy, Applied Physics Letters87, 171107 (2005)

  52. [52]

    M. Mihm, C. Holzmann, J. Seyd, A. Ullrich, H. Karl, and M. Albrecht, Phase Control of Single-Crystalline Cobalt Oxide Thin Films Grown by Pulsed Laser Deposition, Thin Solid Films827, 140776 (2025). 9

  53. [53]

    Holzmann, S

    C. Holzmann, S. Glamsch, D. Stein, M. Mihm, A. Ullrich, R. Schlitz, M. Lammel, J. Boneberg, and M. Albrecht, Inverse garnet/Pt heterostructures by lateral crystalliza- tion, Physical Review Materials9, 10.1103/hhk6-qg6l (2025)

  54. [54]

    Holzmann, M

    C. Holzmann, M. K¨ uß, S. Glamsch, D. Stein, Y. Kunz, M. Weiler, and M. Albrecht, Polycrystalline YIG Thin Films on a Piezoelectric Substrate for Magnetoacoustic Hybrid Devices, ACS Applied Materials & Interfaces17, 58550 (2025)

  55. [55]

    Holzmann, A

    C. Holzmann, A. Ullrich, O.-T. Ciubotariu, and M. Al- brecht, Stress-Induced Magnetic Properties of Gadolin- ium Iron Garnet Nanoscale-Thin Films: Implications for Spintronic Devices, ACS Applied Nano Materials5, 1023 (2022)

  56. [56]

    S. Gota, M. Gautier-Soyer, and M. Sacchi, Magnetic properties of Fe 2O3(0001) thin layers studied by soft x-ray linear dichroism, Physical Review B64, 224407 (2001)

  57. [57]

    S. M. Suturin, A. M. Korovin, S. V. Gastev, P. A. Dvortsova, M. P. Volkov, M. Valvidares, and N. S. Sokolov, X-ray magnetic linear dichroism study of field- manipulated canted antiferromagnetism in epitaxialα- Fe2O3 films, Physical Review Materials5, 044408 (2021)

  58. [58]

    Fern´ andez-Ruiz, D

    R. Fern´ andez-Ruiz, D. Mart´ ın y Marero, and V. Berm´ udez, Anomalous structural feature of LiNbO 3 observed using neutron diffraction, Physical Review B 72, 184108 (2005). 10 Fig. S1. XRD pattern of hematite films deposited at 575°C and a laser fluence of 2.3 J cm −2 with different oxygen partial pressures on z-cut lithium niobate a) overview and b) en...