Elsevier

Physics Letters A

Volume 380, Issue 38, 7 September 2016, Pages 3107-3110
Physics Letters A

Coupled magnetic and elastic properties in LaPr(CaSr)MnO manganites

https://doi.org/10.1016/j.physleta.2016.06.056Get rights and content

Highlights

  • Chemical pressure through doping enhances ferromagnetism in the same way as the application of a magnetic field.

  • The enhancement of the FM phase fraction on cooling is preceded by a strong lattice contraction.

  • The magnetic properties are linked to structural changes in phase separated manganites.

Abstract

We investigate a series of manganese oxides, the La0.225Pr0.4(Ca1xSrx)0.375MnO3 system. The x=0 sample is a prototype compound for the study of phase separation in manganites, where ferromagnetic and charge ordered antiferromagnetic phases coexist. Replacing Ca2+ by Sr2+ gradually turns the system into a homogeneous ferromagnet. Our results show that the material structure plays a major role in the observed magnetic properties. On cooling, at temperatures below 100 K, a strong contraction of the lattice is followed by an increase in the magnetization. This is observed both through thermal expansion and magnetostriction measurements, providing distinct evidence of magneto-elastic coupling in these phase separated compounds.

Introduction

The study of manganese based perovskites, known as manganites, has fascinated the scientific community for the last two decades. This interest was triggered by the discovery of the colossal magnetoresistance effect [1], a huge reduction of the electrical resistivity on application of a magnetic field, which was explained in terms of the interplay between the double exchange mechanism and quenched disorder [2]. In addition, the competition between very different phases with similar ground state energies, namely an insulating charge ordered antiferromagnetic (CO-AFM) and a metallic ferromagnetic (FM) state, leads to complex phase diagrams [3], and to the occurrence of a phase separated state [4], [5], where both phases can spontaneously coexist in meso- or nanoscopic scales [6], [7], [8]. Phase separation (PS) in manganites has became a very important topic of investigation in the physics of strongly correlated electron systems, and a similar phenomenology is found in the high Tc cuprates [9], particularly in the underdoped regime, as well as in magnetocaloric materials, such as Gd5Ge4 [10].

A prototype compound to investigate the phenomenon of phase separation in manganites is La5/8yPryCa3/8MnO3, which has been thoroughly studied in the literature [11], [12], [13], [14]. It is a mixture of the optimized colossal magnetoresistive compound La0.625Ca0.375MnO3, with the Pr based system, Pr0.625Ca0.375MnO3, known to have a robust CO-AFM state at low temperatures. The intermediate mixture, La0.225Pr0.40Ca0.375MnO3, becomes charge ordered and highly insulating below 230 K, and orders antiferromagnetically below 180 K. Phase separation manifests itself at lower temperatures, below 80 K, where FM metallic clusters which nucleate within the CO-AFM matrix yield a sizable magnetization even in low applied magnetic fields.

In this work we performed additional doping to the above mentioned phase separated compound, La0.225Pr0.40Ca0.375MnO3, by replacing the alkaline-earth Ca2+ with larger Sr2+ ions. This substitution introduce structural distortions that gradually increases the exchange coupling [15], thus promoting the FM phase at low temperatures, eventually leading to a homogeneous FM ground state. Our objective is to correlate the macroscopic magnetic response of the system with its structural behavior, obtained from thermal expansion and magnetostriction measurements. The results clearly show that the formation of FM clusters on cooling occurs at temperatures just below a strong lattice contraction of the material, giving evidence of the coupling between structural and magnetic degrees of freedom in phase separated manganites.

Section snippets

Experimental

Polycrystalline samples of La0.225Pr0.4(Ca1xSrx)0.375MnO3, with 0x1, were synthesized by a citrate–nitrate decomposition method [16], using 99.9% purity reactants (oxides and soluble salts). After the mixed solution was dried at 100 °C, thermal treatments were made at 500 °C for 5 hours and at 1400 °C for 16 hours. The powder was compacted into pellets of 5×2×2 mm3 using a pressure 8 t/cm2. The pellets were finally sintered at 1400 °C for 2 hours. The resulting average grain size is ∼2 μm.

Results and discussion

Fig. 1 shows the room temperature x-ray diffraction intensity of La0.225Pr0.4(Ca1xSrx)0.375MnO3, with x=0.05. Rietveld refinements were carried out with the FULLPROF program, with an orthorhombic Pnma space group. The reliability factors of the Rietveld analysis [18] are RBragg=9.04, RF=9.81, and χ2=1.57. The inset shows an enlarged plot of specific areas of the diffractogram, so that the calculated and observed profiles are clearly visible. The lower trace in the main panel is a plot of the

Conclusions

To summarize, our results demonstrate that magneto-structural coupling plays a major role in the balance between competing phases in phase separated manganites. Chemical pressure through doping and the application of an external magnetic field have a similar effect, enhancing the FM phase fraction of the compound. Sr doping in the La0.225Pr0.4(Ca1xSrx)0.375MnO3 system increases the cell volume, and at the same time reduces the distortion of the Mn–O–Mn bond angle, which favors the FM double

Acknowledgements

This research was supported by the bilateral cooperation FAPERJ-CONICET, the Brazilian agencies CNPq and CAPES (Science without borders program), and by the Brazilian Synchrotron Light Laboratory (LNLS). We acknowledge the useful help of Fabiano Yokaichiya and Helio Salim Amorim with the analysis of the x-ray data. LFC acknowledges the UK EPSRC.

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