Gadolinium oxyorthogermanate Gd2GeO5: An efficient solid refrigerant material for magnetic cryocoolers
Graphical abstract
Introduction
In recent years, the cooling requirements for T < 20 K temperatures are growing terrifically, such as in space detectors, scanners, and spintronic devices, as well as in creating cryogenic environments for quantum computing and liquifying helium and hydrogen [[1], [2], [3], [4]]. The adiabatic demagnetization refrigeration (ADR) technique that exploits the magnetocaloric effect is thus becoming increasingly popular, which describes the changes of adiabatic temperature and magnetic entropy following changes of magnetic fields [1,[5], [6], [7], [8]]. Magnetic refrigeration can offer an energy savings of up to 30% compared to traditional gas compressors by developing proper refrigeration procedures, and possesses characterizations of high efficiency and reliability, low microphonics and thermophonics [9]. Besides, the thermodynamic responses are highly reversible, thus suitable for a diverse array of large-scale utilization.
The research of magnetic refrigeration is an ongoing endeavour, which consists of designing prototypes of refrigerators, as well as searching for suitable refrigerants. The applicable magnetocaloric materials should be of good chemical stability, easy fabrication, high resistance to mechanical corrosion, high thermal conductivity, as well as good durability without fracturing or degradation in the thermal, pressure and magnetic cycles [7,8]. More specifically, the desirable characteristics of magnetocaloric materials should include low magnetic ordering temperature (typically 1–2 K below the lowest limit of the desired operating temperature window), large magnetic ions densities with weak crystal-field effect, as well as low electronic and lattice specific heat so that the internal heat load is minimized during the magnetic cycle [1]. In addition, the large magnetic entropy change shall be readily acquired within the lowest possible field changes, which can lower the economic cost significantly.
According to the above-mentioned criteria, the gadolinium compounds shall be prominent alternatives under consideration in the sense of magnetic entropy retaining [1,10,11]. The spin-orbit coupling in Gd3+ ions vanish up to the first order, and thus the splitting of the (2S + 1)-degenerate spin multiplets due to crystal-field interactions is relatively insignificant [12,13]. Consequently, the magnetic ordering transition is generally suppressed to a very low temperature, and the full reservation of magnetic entropy Rln8 per ion is available for temperatures of 2–20 K.
As a valid instance, the gadolinium gallium garnet Gd3Ga5O12 (GGG) has long been the benchmark material for cryogenic magnetic refrigerant materials, which shows a high magnetic density and broad magnetic transition due to frustrated spin arrangements. The maximum isothermal magnetic entropy change for GGG is 0.30 J K−1 cm−3 (42.4 J K−1 kg−1) under an applied field change of 9 T [1,[14], [15], [16]]. However, the magnetocaloric effect of GGG is far from satisfactory in terms of utilization efficiency of Gd3+ spin entropy. Further investigation of materials that shows a more pronounced magnetocaloric effect is appealing. A compromise is necessary to control the magnetic density and suppress the magnetic ordering simultaneously [17,18]. Therefore, we focus on the gadolinium oxyorthogermanate Gd2GeO5 with compacted spin centres and limited magnetic-passive elements Ge, which is clearly advantageous in regard to magnetic density.
Below, we investigate the magnetic and thermodynamic parameters of Gd2GeO5 through bulk magnetization and heat capacity measurements. Analysis of the magnetization isotherms reveals moderate antiferromagnetic interactions between isotropic Gd3+ spins, which endows the system with remarkably high magnetocaloric effects. The lack of magnetic ordering down to T < 2 K, and the sufficient low phonon contributions of heat capacity suggest that the Gd2GeO5 may be quite impressive for use in helium-free magnetic cryocoolers.
Section snippets
Materials and methods
The polycrystalline powders were obtained using a traditional solid-state reaction process. Stoichiometric amounts of the Gd2O3 (5 N, Adamas, pre-dried at 1173 K for 24 h) and GeO2 (4 N, Energy chemical) were thoroughly grinded in an agate mortar. The mixtures were then pressed into a tablet of φ-1.8 cm under 2 tons of pressure, put in muffle furnace and heated to 1373 K at a rate of 5 K/h for 24 h. A second heating to 1673 K for 20 h durations was conducted to obtain the phase pure samples.
Characterizations
Crystallography
Fig. 1 depicts the powder X-ray diffraction pattern collected at room temperature, which confirms the monoclinic lattice with a = 9.3259(6) Å, b = 7.0975(5) Å, c = 6.8440(5) Å and β = 105.3983(11) °. The systematic reflection positions are consistent with space group P21/c (no.14) with all atoms in general positions 4e, as determined by the Rietveld refinements converged at a final Rp = 0.0167, Rwp = 0.0238 and goodness of fit of 5.0, respectively. The final atomic coordinates, Wyckoff
Summary
To conclude, we have experimentally determined the magnetocaloric effect and thermodynamic parameters of a solid refrigerant material, gadolinium oxyorthogermanate Gd2GeO5, through magnetization and heat capacity measurements. An isotropic antiferromagnetic exchange coupling with energy scale εex = JexS2 ≈ 2.6 K is estimated from analysing the magnetization isotherms, in agreement with the DFT calculations. A remarkably large −ΔSM (B, T) of 0.36 J K−1 cm−3, and an RCP of 4.34 J cm−3 are
Author contributions
Z. Yang: Conceptualization, Investigation, Writing - Original Draft, and Funding acquisition. S. Qin, J. Zhang, D. Lu, H. Zhao and C. Kang: Investigation. H. Cui, Y. Long and Y.J. Zeng: Supervision and Funding acquisition.
Declaration of competing interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
Acknowledgements
This work was supported by the Science, Technology, and Innovation Commission of Shenzhen Municipality [grant numbers JCYJ20190808152217447, JCYJ20180305125212075, JCYJ20210324095611032, and JCYJ20180507182246321]; the National Natural Science Foundation of China [grant numbers 51925804, 11934017, and 11921004]; the National Key R&D Program of China [grant numbers 2021YFA1400300, 2018YFE0103200 and 2018YFA0305700]; the Beijing Natural Science Foundation [grant number Z200007]; and the Chinese
References (47)
- et al.
Materials for magnetic refrigeration between 2 K and 20 K
Cryogenics
(1982) - et al.
Magnetocaloric effect: from materials research to refrigeration devices
Prog. Mater. Sci.
(2018) - et al.
Magnetocaloric materials and the optimization of cooling power density
Cryogenics
(2014) - et al.
Optimum operating regimes of common paramagnetic refrigerants
Cryogenics
(2011) Refrigeration to below 20 K
Cryogenics
(1970)- et al.
Excellent cryogenic magnetocaloric performances in ferromagnetic Sr2GdNbO6 double perovskite compound
Mater. Today Phys.
(2021) - et al.
Giant refrigerant capacity in Gd-based amorphous/nanocrsytalline composite fibers
Mater. Today Phys.
(2021) - et al.
Structure and luminescence of Gd2GeO5 and Dy2GeO5
J. Less Common. Met.
(1985) On a generalised approach to first and second order magnetic transitions
Phys. Lett.
(1964)- et al.
Magnetic, magnetocaloric and thermoelectric investigations of perovskite LaFeO3 compound: first principles and Monte Carlo calculations
Comput. Theor. Chem.
(2021)
Scaling laws for the magnetocaloric effect in second order phase transitions: from physics to applications for the characterization of materials
Int. J. Refrig.
Magnetocaloric materials for energy efficient cooling
J. Phys. D Appl. Phys.
Advanced materials for magnetic cooling: fundamentals and practical aspects
Appl. Phys. Rev.
Magnetic refrigeration: a review of a developing technology
Adv. Cryog. Eng.
Magnetic refrigeration Design technologies: state of the art and general perspectives
Energies
Magnetic interactions in the tripod kagome antiferromagnet Mg2Gd3Sb3O14 probed by static magnetometry and high-field ESR spectroscopy
Phys. Rev. B
Magnetism and Magnetic Materials
Sensitivity of magnetic properties to chemical pressure in lanthanide garnets Ln3A2X3O12, Ln = Gd, Tb, Dy, Ho, A = Ga, Sc, In, Te, X = Ga, Al, Li
J. Phys. Condens. Matter
Enhancement of the magnetocaloric effect driven by changes in the crystal structure of Al-doped GGG, Gd3Ga5-xAlxO12 (0<=x<=5)
J. Phys. Condens. Matter
Magnetocaloric effect in a frustrated Gd-garnet with No long-range magnetic order
Inorg. Chem.
A dense metal-organic framework for enhanced magnetic refrigeration
Adv. Mater.
Large magnetocaloric effect in gadolinium borotungstate Gd3BWO9
J. Mater. Chem. C
EXPGUI, a graphical user interface for GSAS
J. Appl. Crystallogr.
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