Intriguing Magnetocaloric Effect in Multiferroic Ba3RRu2O9 (R=Ho, Gd, Tb, Nd) with Strong 4d-4f Correlations
Pith reviewed 2026-05-16 18:56 UTC · model grok-4.3
The pith
Heavy rare-earth Ba3RRu2O9 compounds switch from conventional to non-conventional magnetocaloric effect around their low-temperature magnetic transitions.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Ba3HoRu2O9 orders antiferromagnetically at 50 K with both Ho and Ru moments participating, followed by a transition near 10 K; Ba3GdRu2O9 and Ba3TbRu2O9 order near 14.5 K and 10.5 K respectively with speculated joint ordering of R and Ru moments. These three compounds exhibit an intriguing switch from conventional to non-conventional magnetocaloric effect around the low-temperature transition. In contrast, Ba3NdRu2O9 orders ferromagnetically below 24 K (Nd moments) with Ru ordering below 18 K and shows positive magnetocaloric effect on both sides of the ferromagnetic transition. The observed magnetocaloric behavior is attributed to temperature-dependent complex spin reorientations and single
What carries the argument
Temperature-dependent complex spin-reorientations and magnetic anisotropy arising from strong 4d-4f correlations between Ru and rare-earth moments.
If this is right
- Robust magnetocaloric response occurs near the low-temperature magnetic transitions in the heavy rare-earth members.
- The sign and magnitude of the magnetocaloric effect change with temperature in Ho, Gd and Tb compounds.
- Nd compound remains ferromagnetic with positive magnetocaloric effect below and above its ordering temperature.
- The effect is driven by the interplay of rare-earth and Ru moments rather than by a single sublattice.
Where Pith is reading between the lines
- If the switch can be tuned by external pressure or doping, the same material could serve both cooling and heating cycles without changing the applied field direction.
- The observed anisotropy suggests that single-crystal measurements would reveal direction-dependent cooling efficiencies useful for device design.
- Similar 4d-4f systems with competing anisotropies may display analogous sign-changing magnetocaloric behavior at accessible temperatures.
Load-bearing premise
The ordering of both rare-earth and Ru moments is assumed for Gd and Tb compounds, and the magnetocaloric switch is attributed to spin reorientations without direct microscopic confirmation.
What would settle it
Neutron diffraction or muon spin rotation data that show no temperature-dependent spin reorientation across the low-T transition would falsify the proposed origin of the conventional-to-non-conventional switch.
read the original abstract
Here we demonstrate the magnetocaloric effect (MCE) of a 4d-4f correlated system, namely Ba3RRu2O9 (R= Ho, Gd, Tb, Nd). The compound Ba3HoRu2O9 antiferromagnetically orders at 50 K where both the Ho and Ru-moments order, followed by another phase transition ~ 10 K. Whereas, the compound Ba3GdRu2O9 and Ba3TbRu2O9 orders at 14.5 and 10.5 K respectively, where the ordering of both R and Ru moments are speculated. Our results reveal robust MCE around low-T magnetic phase transition for all the heavy rare-earth members (Ho, Gd, Tb) in this family. The heavy rare-earth members exhibit an intriguing MCE behavior switching from conventional to non-conventional MCE. Interestingly, the light R-member, Ba3NdRu2O9, orders ferromagnetically below 24 K where Nd-moments order, followed by Ru-ordering below 18 K, exhibits a positive MCE below and above FM-ordering. The compelling MCE are attributed to temperature dependent complex spin-reorientations for different R-members and anisotropy.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper reports experimental observations of the magnetocaloric effect (MCE) in the 4d-4f correlated multiferroic series Ba3RRu2O9 (R=Ho, Gd, Tb, Nd). It describes antiferromagnetic ordering at 50 K (with a second transition near 10 K) for the Ho compound where both Ho and Ru moments order, speculated joint R-Ru ordering at 14.5 K and 10.5 K for Gd and Tb, and ferromagnetic ordering of Nd moments below 24 K followed by Ru ordering below 18 K. The central results are robust MCE near the low-T transitions for the heavy rare-earth members, including an intriguing switch from conventional to non-conventional MCE, contrasted with positive MCE for the Nd member; all effects are attributed to temperature-dependent complex spin-reorientations and anisotropy.
Significance. If the reported MCE switching and its attribution hold under closer scrutiny, the work would provide valuable data on magnetocaloric behavior in strongly correlated 4d-4f systems, potentially informing models of entropy changes driven by competing sublattice interactions and anisotropy in multiferroics. The contrast between heavy and light rare-earth members offers a useful comparative dataset for low-temperature refrigeration applications.
major comments (2)
- [Results on magnetic ordering and MCE for Gd/Tb] The central claim that the MCE switches from conventional to non-conventional in Ba3GdRu2O9 and Ba3TbRu2O9 due to temperature-dependent complex spin-reorientations involving both R and Ru moments is load-bearing but rests on bulk magnetization and specific-heat features alone. No neutron diffraction, resonant X-ray, or other microscopic probe data are provided to confirm the joint ordering or reorientation transitions (abstract; results section on magnetic ordering and MCE for Gd/Tb).
- [Experimental results and figures] Quantitative MCE parameters (e.g., isothermal entropy change ΔS or adiabatic temperature change) are presented without accompanying error bars, measurement protocols, or tabulated values, preventing assessment of the robustness and reproducibility of the reported switching behavior (abstract and experimental results sections).
minor comments (1)
- [Abstract] The abstract uses the term 'compelling MCE' without providing magnitude benchmarks or direct comparisons to other 4d-4f or multiferroic systems, which would help contextualize the findings.
Simulated Author's Rebuttal
We thank the referee for their constructive comments on our manuscript. We address each major point below and indicate the revisions made to the manuscript.
read point-by-point responses
-
Referee: The central claim that the MCE switches from conventional to non-conventional in Ba3GdRu2O9 and Ba3TbRu2O9 due to temperature-dependent complex spin-reorientations involving both R and Ru moments is load-bearing but rests on bulk magnetization and specific-heat features alone. No neutron diffraction, resonant X-ray, or other microscopic probe data are provided to confirm the joint ordering or reorientation transitions (abstract; results section on magnetic ordering and MCE for Gd/Tb).
Authors: We acknowledge that the interpretation of joint R-Ru ordering and subsequent spin reorientations in Ba3GdRu2O9 and Ba3TbRu2O9 is inferred from bulk magnetization and specific-heat data showing multiple transitions and anomalies. The manuscript already qualifies these as 'speculated' to reflect the lack of microscopic confirmation. We have revised the abstract and discussion sections to more explicitly state the limitations of bulk-only evidence, emphasize the speculative nature of the spin-reorientation model, and note that future neutron or resonant X-ray studies would be needed for direct confirmation. The reported MCE switching itself remains directly supported by the isothermal magnetization and entropy-change measurements presented. revision: partial
-
Referee: Quantitative MCE parameters (e.g., isothermal entropy change ΔS or adiabatic temperature change) are presented without accompanying error bars, measurement protocols, or tabulated values, preventing assessment of the robustness and reproducibility of the reported switching behavior (abstract and experimental results sections).
Authors: We agree that the presentation of quantitative MCE values can be improved for clarity and reproducibility. In the revised manuscript we have added error bars to the ΔS(T) and ΔT_ad plots, included a detailed description of the measurement protocols (including field-sweep rates, temperature stabilization criteria, and data-processing steps) in the experimental methods section, and added a supplementary table listing the peak ΔS values, temperatures, and field ranges for each compound. revision: yes
- Direct microscopic confirmation of the proposed spin reorientations and joint R-Ru ordering in the Gd and Tb compounds, which would require new neutron diffraction or resonant X-ray experiments beyond the scope of the present bulk-measurement study.
Circularity Check
Purely experimental report with no derivations or fitted predictions
full rationale
The manuscript is an experimental study reporting direct measurements of magnetization, specific heat, and magnetocaloric effect in Ba3RRu2O9 (R=Ho, Gd, Tb, Nd). No equations, first-principles derivations, or parameter fits are presented that reduce any claimed result to prior inputs by construction. Attributions to spin reorientations and anisotropy are interpretive statements based on bulk data features, not a closed mathematical chain or self-citation load-bearing premise. The central observations stand as independent experimental findings without circular reduction.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption Magnetic ordering temperatures reflect cooperative alignment of rare-earth and transition-metal moments in 4d-4f systems
Lean theorems connected to this paper
-
IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
The compelling MCE are attributed to temperature dependent complex spin-reorientations for different R-members and anisotropy.
-
IndisputableMonolith/Foundation/AlexanderDuality.leanalexander_duality_circle_linking unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
neutron diffraction results show a continuous spin reorientation... sharp spin reorientation of both Ho and Ru moments
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]
-
[2]
P. J. Shirron, M. O. Kimball, D. J. Fixsen, A. J. Kogut, X. Li, and M. J. DiPirro, Cryogenics design of the PIXIE adiabatic demagnetization refrigerators, Cryogenics 52, 140–144 (2012)
work page 2012
-
[3]
R. D. Britt and P. L. Richards, An adiabatic demagnetization refrigerator for infrared bolometers, Int. J. Infrared Millimeter Waves 2, 1083–1096 (1981)
work page 1981
-
[4]
T. J. Sato, D. Okuyama, and H. Kimura, Tiny adiabatic -demagnetization refrigerator for a commercial superconducting quantum interference device magnetometer, Rev. Sci. Instrum. 87, 123905 (2016)
work page 2016
-
[5]
A. H. Ólafsdóttir and H. U. Sverdrup, Assessing the past and future sustainability of global helium resources, extraction, supply, and use using the integrated assessment model WORLD7, Biophys. Econ. Sustain. 5, 6 (2020)
work page 2020
-
[6]
W. F. Giauque, A thermodynamic treatment of certain magnetic effects. A proposed method of producing temperatures considerably below 1° absolute, J. Am. Chem. Soc. 49, 1864–1870 (1927)
work page 1927
-
[7]
W. F. Giauque and D. P. MacDougall, The production of temperatures below one degree absolute by adiabatic demagnetization of gadolinium sulfate, J. Am. Chem. Soc. 57, 1175 – 1185 (1935)
work page 1935
-
[8]
R. D. McMichael, J. J. Ritter, and R. D. Shull, Enhanced magnetocaloric effect in Gd3Ga5- xFexO12, J. Appl. Phys. 73, 6946–6948 (1993)
work page 1993
- [9]
-
[10]
J. Head, P. Manuel, F. Orlandi, M. Jeong, M. R. Lees, R. Li, and C. Greaves, Structural, magnetic, magnetocaloric, and magnetostrictive properties of Pb 1-xSrxMnBO4 (x = 0, 0.5, and 1.0), Chem. Mater. 32, 10184–10199 (2020)
work page 2020
-
[11]
V. K. Dwivedi, P. Mandal, and S. Mukhopadhyay, Frustration -induced inversion of the magnetocaloric effect and metamagnetic transition in substituted pyrochlore iridates, ACS Appl. Electron. Mater. 4, 1611–1618 (2022)
work page 2022
-
[12]
P. Álvarez, P. Gorria, and J. A. Blanco, Influence of magnetic fluctuations on the magnetocaloric effect in rare-earth intermetallic compounds, Phys. Rev. B 84, 024412 (2011)
work page 2011
-
[13]
J.-L. Jin, X. -Q. Zhang, G. -K. Li, Z. -H. Cheng, and Y. Lu, Giant anisotropy of magnetocaloric effect in TbMnO3 single crystals, Phys. Rev. B 83, 184431 (2011)
work page 2011
- [14]
- [15]
- [16]
-
[17]
R. Das, A. Midya, M. Kumari, A. Chaudhuri, X. Yu, A. Rusydi, and R. J. Mahendiran, Enhanced magnetocaloric effect driven by hydrostatic pressure in Na-doped LaMnO3, J. Phys. Chem. C 123, 3750–3757 (2019)
work page 2019
- [18]
-
[19]
T. Basu, A. Pautrat, V. Hardy, A. Loidl, and S. Krohns, Magnetodielectric coupling in a Ru-based 6H perovskite Ba3NdRu2O9, Appl. Phys. Lett. 113, 042902 (2018)
work page 2018
-
[20]
T. Basu, V. Caignaert, F. Damay, T. W. Heitmann, B. Raveau, and X. Ke, Cooperative magnetic ordering and phase coexistence in the perovskite multiferroic, Phys. Rev. B 102, 020409(R) (2020)
work page 2020
-
[21]
T. Basu, V. Caignaert, S. Ghara, X. Ke, A. Pautrat, S. Krohns, A. Loidl, and B. Raveau, Enhancement of magnetodielectric coupling in 6H perovskites for heavier rare -earth cations, Phys. Rev. Mater. 3, 114401 (2019)
work page 2019
-
[22]
E. Kushwaha, G. Roy, A. M. dos Santos, M. Kumar, S. Ghosh, D. T. Adroja, V. Caignaert, O. Perez, A. Pautrat, and T. Basu, Origin of spin -driven ferroelectricity and effect of external pressure on the complex magnetism of the 6H perovskite Ba 3HoRu2O9, Phys. Rev. B 109, 224418 (2024)
work page 2024
-
[23]
S. Chhillar, K. Mukherjee, and C. S. Yadav, Large magnetodielectric coupling in the vicinity of a metamagnetic transition in the 6H perovskite Ba 3GdRu2O9, J. Phys.: Condens. Matter 34, 145801 (2022)
work page 2022
- [24]
-
[25]
M. S. Senn, S. A. J. Kimber, A. M. Arévalo López, A. H. Hill, and J. P. Attfield, Spin orders and lattice distortions of geometrically frustrated 6H perovskites Ba3B′Ru2O9 (B′ = La3+, Nd3+, and Y3+), Phys. Rev. B 87, 134402 (2013)
work page 2013
- [26]
-
[27]
V. Hardy, R. Hamane, F. Veillon, M. Risser, and F. Guillou, “Two -steps” process in the first-order transformation of giant magnetocaloric materials, Acta Mater. 231, 117869 (2022)
work page 2022
-
[28]
M. A. Hamad and H. R. J. Alamri, From conventional to inverse magnetocaloric effect in GdMn1-xCrxO3, Taibah Univ. Sci. 16, 670–675 (2022)
work page 2022
-
[29]
E. Kushwaha, G. Roy, A. M. dos Santos, M. Kumar, S. Ghosh, T. Heitmann, and T. Basu, Unconventional s -orbital state of Tb and cooperative Ru (4d) –Tb (4f) spin ordering in the strongly correlated 4d–4f system Ba3TbRu2O9, J. Mater. Chem. C 13, 15384–15389 (2025)
work page 2025
-
[30]
X. Moya, L. Mañosa , A. Planes, S. Aksoy, M. Acet, E. F. Wassermann, and T. Krenke, Cooling and heating by adiabatic magnetization in the Ni 50Mn34In16 magnetic shape-memory alloy, Phys. Rev. B 75, 184412 (2007)
work page 2007
-
[31]
P. Álvarez-Alonso, P. Gorria, J. A. Blanco, J. Sánchez -Marcos, G. J. Cuello, I. Puente - Orench, J. A. Rodríguez-Velamazán, G. Garbarino, I. de Pedro, J. Rodríguez Fernández, and J. L. Sánchez Llamazares, Magnetovolume and magnetocaloric effects in Er 2Fe17, Phys. Rev. B 86, 184411 (2012)
work page 2012
-
[32]
V. Chandragiri, K. K. Iyer, and E. V. Sampathkumaran, Magnetic and magnetotransport behavior: Observation of reentrant inverse magnetocaloric phenomenon and asymmetric magnetoresistance behavior, Phys. Rev. B 92, 014407 (2015). Intriguing Magnetocaloric Effect in 6H-perovskite Ba3RRu2O9 (R=Ho, Gd, Tb, Nd) with Strong 4d-4f Correlations M. Kumar1, S. Ghosh...
work page 2015
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.