FDFrancoise Damay

Francoise Damay

*This is an algorithmically generated author record based on publicly available information.

Current Organizations / Institutes

The organizations/institutes from the scholar's latest article


Francoise Damay has a total of 157 co-authors. Here are the top co-authors by number of shared publications:


Latest Publications

  • Open Access

    Origin of the magnetic ground state of Tb 2 Ir 2 O 7

    by Y. Alexanian, E. Lhotel, J. Robert, S. Petit, E. Lefrançois, P. Lejay, A. Hadj-Azzem, F. Damay, J. Ollivier, B. Fåk, et al.

    Magnetic-rare-earth pyrochlore iridates exhibit a rich variety of unconventional phases, driven by the complex interactions within and between the rare-earth and the iridium sublattices. In this study, we investigate the peculiar magnetic state of Tb 2 Ir 2 O 7 , where a component of the Tb 3 + moment orders perpendicular to its local Ising anisotropy axis. By means of neutron diffraction and inelastic neutron scattering down to dilution temperatures, complemented by specific heat measurements, we show that this intriguing magnetic state is fully established at 1.5 K and we characterize its excitation spectrum across a broad range of energies. Our calculations reveal that bilinear interactions between Tb 3 + ions subjected to the Ir molecular field capture several key features of the experiments, but need to be supplemented to fully reproduce the observed behavior.

  • Spin liquid state in the three dimensional pyrochlore-like frustrated magnet MgCrGaO 4

    by U. Jena, S. Kundu, Suheon Lee, Q. Faure, F. Damay, S. Rols, Adam Berlie, S. Petit, Kwang-Yong Choi, P. Khuntia


  • From Triangular Correlated Paramagnet to Multi- q Noncoplanar Spin State in Spinel GeFe 2 O 4

    by L. Chaix, J. Robert, E. Chan, E. Ressouche, S. Petit, C. V. Colin, R. Ballou, J. Ollivier, L.-P. Regnault, E. Lhotel, et al.

    Combining macroscopic measurements, neutron scattering, and modeling, we identify in the GeFe_{2}O_{4} spinel a correlated paramagnetic state resulting from the predominance of third-neighbor antiferromagnetic interactions. These interactions materialize four interlaced families of triangular planes with 120° spins emerging from the underlying pyrochlore lattice. At lower temperatures, a phase transition occurs to a noncoplanar spin structure that is characterized by six propagation vectors. This unusual multi-q order is triggered by the presence of weaker interactions up to the sixth neighbors. The system is remarkably successful in coupling the different triangular planes while maintaining their two-dimensional 120° order. Our Letter highlights the hierarchy of interactions involved in GeFe_{2}O_{4}, which is singular among spinel compounds since first-neighbor interactions are only a small fraction of the dominant third-neighbor ones.


  • Unusual planar anisotropy of the induced magnetism in KTb3F10

    by O. Demortier, S. Petit, B. Fauqué, E. Ressouche, I. Kibalin, J. Robert, R. Sibille, B. Roessli, C. Colin, A. Ivanov, et al.

  • Open Access

    Entropy-stabilized materials as a platform to explore terbium-based pyrochlore frustrated magnets

    by Florianne Vayer, Sylvain Petit, Françoise Damay, Jan Embs, Stéphane Rols, Claire Colin, Elsa Lhotel, Dalila Bounoua, Nita Dragoe, David Bérardan, et al.


  • Open Access

    Following the guidelines for communicating commensurate magnetic structures: real case examples

    by F. Damay

    A few real case examples are presented on how to report magnetic structures, with precise step-by-step explanations, following the guidelines of the IUCr Commission on Magnetic Structures [Perez-Mato et al. (2024). Acta Cryst. B80, 219–234]. Four examples have been chosen, illustrating different types of single-k magnetic orders, from the basic case to more complex ones, including odd-harmonics, and one multi-k order. In addition to acquainting researchers with the process of communicating commensurate magnetic structures, these examples also aim to clarify important concepts, which are used throughout the guidelines, such as the transformation to a standard setting of a magnetic space group.


  • Influence of Dy3+ environment on magnetic anisotropy and magnetocaloric effect in Dy3B2C3O12 (B=In,Sc,Te;C=Ga,Al,Li) garnets

    by F. Damay, S. Petit, D. Sheptyakov, C. V. Colin, E. Suard, S. Rols, J. Embs, U. Stuhr, D. Bounoua, O. Demortier, et al.

    In the framework of the general phase diagram published recently for a pseudospin S=1/2 on a hyperkagome network [Kibalin et al., Phys. Rev. Res. 2, 033509 (2020)], four Dy3B2C3O12 garnets with different species on the B and C sites, namely, Dy3Sc2Al3O12 (DyScAl), Dy3Te2Li3O12 (DyTeLi), Dy3Sc2Ga3O12 (DyScGa), and Dy3In2Ga3O12 (DyInGa), have been studied by neutron powder diffraction and inelastic neutron scattering, to investigate the impact of B and C substitutions on the Dy3+ dodecahedral oxygen environment and crystal field, and thus on the Dy3+ spin magnetic anisotropy. In the four compounds, the magnetic ground state is a multiaxis antiferromagnetic order similar to that of Dy3Al5O12, characterized by an ordered moment close to the theoretical maximum, ∼6µB. The gap between the ground state and the first excited crystal electric field level varies from ∼3.2 meV (DyInGa) up to 11.2 meV (DyScAl), confirming the rather strong Ising character of the Dy3+ moment in those garnets. For a better understanding of the impact of the distortion of the oxygen environment on the Dy3+ magnetic anisotropy, point-charge calculations were then performed, mapping a magnetic anisotropy diagram versus a wide range of distortions. Results show that Ising-like behaviors mostly predominate, associated with large gx, gy, or gz Landé values, whose stable area is determined by the shape of the DyO8 cage. Magnetic entropy calculations confirm that the magnetocaloric effect increases sharply near those boundaries and validate the use of dysprosium garnets for low temperature, low magnetic field adiabatic demagnetization refrigeration cryostats.


  • Enhanced magnetism and suppressed magnetoelastic coupling induced by electron doping in Ca1− x Y x MnReO6

    by A S Cavichini, M T D Orlando, M C A Fantini, R Tartaglia, C W Galdino, F Damay, F Porcher, E Granado

    The Ca2MnReO6 double perovskite is a spin–orbit-assisted Mott insulator with exotic magnetic properties, including a largely non-collinear Mn2+ spin arrangement and nearly orthogonal coupling between such spins and the much smaller Re 5d magnetic moments. Here, the electron-doped compound Ca1−x Y x MnReO6 (x = 0.1, 0.2 and 0.3) is reported and a detailed investigation is conducted for x = 0.3. Neutron and x-ray powder diffraction confirm that nearly full chemical order is maintained at the Mn and Re sites under the Y substitution at the Ca site. X-ray absorption measurements and an analysis of the Mn–O/Re–O bond distances show that the Mn oxidation state remains stable at +2 whereas Re is reduced upon doping. The electron doping increases the magnetic ordering temperature from T c = 121 to 150 K and also enhances significantly the ferromagnetic component of the Mn spins at the expense of the antiferromagnetic component at the base temperature (T = 3 K). The lattice parameter anomalies at T c observed in the parent compound are suppressed by the electron doping. The possible reasons for the enhanced magnetism and the suppressed magnetoelastic coupling in Ca1.7Y0.3MnReO6 are discussed.

  • Observation of surface magnons and crystalline electric field shifts in superantiferromagneticNdCu2nanoparticles

    by E. M. Jefremovas, M. de la Fuente Rodríguez, F. Damay, B. Fåk, A. Michels, J. A. Blanco, L. F. Barquín

    An ensemble of superantiferromagnetic NdCu2 nanoparticles has been produced to perform a detailed analysis of magnetic excitations using inelastic neutron scattering. Neutron diffraction measurements indicate a mean nanoparticle size of 〈D〉≈13 nm, where the bulk commensurate antiferromagnetic structure is retained at the nanoparticle core. Magnetic measurements evidence the interaction among the magnetic moments located at the nanoparticle surface to be strong enough to establish a spin glass behavior. Specific heat analyses show a broad Schottky contribution, revealing the existence of a crystalline electric field. Inelastic neutron scattering analyses disclose that the splitting of the crystalline electric field levels associated with the Nd3+ ions, as well as the spin-wave excitations that emerged below the Néel transition (TN≈6 K) in polycrystalline NdCu2 are maintained in the nanoparticle state. We have been able to isolate the scattering contribution arising from the nanoparticle surface where both crystalline electric field splitting and the collective magnetic excitations are well-defined despite the symmetry breaking. Quantitative analyses of this surface scattering reveal that finite-size effects and microstrain lead to a partial inhibition of the transitions from the ground state to the first excited level, as well as a positive shift (∼15%) of the energy associated to collective magnon excitations.


  • Open Access

    Field-temperature phase diagram of the enigmatic Nd2(Zr1−xTix)2O7 pyrochlore magnets

    by M. Léger, E. Lhotel, E. Ressouche, K. Beauvois, F. Damay, C. Paulsen, A. Al-Mawla, E. Suard, M. Ciomaga Hatnean, G. Balakrishnan, et al.

    By combining neutron scattering and magnetization measurements down to 80 mK, we determine the (H,T) phase diagram of the Nd2(Zr1−xTix)2O7 pyrochlore magnet compounds. In those samples, Zr is partially substituted by Ti, hence tuning the exchange parameters and testing the robustness of the various phases. In all samples, the ground state remains all in/all out, while the field induces phase transitions toward new states characterized by two in–two out or one out–three in/one in–three out configurations. These transitions manifest as metamagnetic singularities in the magnetization versus field measurements. Strikingly, it is found that moderate substitution reinforces the stability of the all in/all out phase: the Néel temperature, the metamagnetic fields along with the ordered magnetic moment, are higher in substituted samples with x< 10%.