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Competing magnetostructural phases in a semiclassical system

npj Quantum Materialsvolume 2, Article number: 65 (2017) | Download Citation

Abstract

The interplay between charge, structure, and magnetism gives rise to rich phase diagrams in complex materials with exotic properties emerging when phases compete. Molecule-based materials are particularly advantageous in this regard due to their low energy scales, flexible lattices, and chemical tunability. Here, we bring together high pressure Raman scattering, modeling, and first principles calculations to reveal the pressure–temperature–magnetic field phase diagram of Mn[N(CN)2]2. We uncover how hidden soft modes involving octahedral rotations drive two pressure-induced transitions triggering the low → high magnetic anisotropy crossover and a unique reorientation of exchange planes. These magnetostructural transitions and their mechanisms highlight the importance of spin–lattice interactions in establishing phases with novel magnetic properties in Mn(II)-containing systems.

Introduction

The interplay between charge, structure, and magnetism has a profound effect on the functionality of complex materials.1,2,3,4 These interactions are particularly strong in oxides, giving rise to elaborate PTB phase diagrams, often with exotic and/or coexisting states that derive from delicately balanced coupling.5,6,7,8 External perturbations such as pressure, magnetic field, or light, can change important energy scales, driving these flexible materials into new areas of phase space with very different properties. This is interesting because exotic properties tend to emerge when phases compete. While of foundational importance, phase transitions driven by external stimuli can be difficult to realize at experimentally attainable conditions in specific physical systems.9,10,11,12 This is because material energy scales tend to be high relative to the size of an external tuning parameter like pressure or magnetic field. As a result, investigations often focus on metal–insulator transitions in organic or oxide materials13,14,15,16 and superconducting systems.17,18,19 Molecule-based materials, with their flexible lattices, overall low energy scales, and chemical tunability,20,21,22,23 provide an alternate approach to the exploration of pressure- and magnetic field-induced transitions. At the same time, they provide opportunities to isolate spin–lattice interactions and test the chemical aspects of these processes—in this case, the ability of high spin S = 5/2 Mn(II) centers to support novel states of matter.

The M[N(CN)2]2 (M = Ni, Co, Mn, Fe) family of materials provides a superb platform for exploring phases that arise under external stimuli.24,25,26,27,28,29,30,31,32,33 Mn[N(CN)2]2 is a particularly important member of this series.34,35,36,37,38 In the Pnnm structure, the Mn(II) centers are connected by soft N≡C–N ligands that act as magnetic superexchange pathways.27 Below T N = 15.9 K, the system is a weakly canted antiferromagnet.34 Magnetic field drives a spin–flop transition near 0.5 T and a transition to the fully saturated state at 30 T that is supported by dicyanamide distortions.30 A series of room temperature, pressure-induced structural transitions was recently discovered,38 although a full pressure–temperature (PT) phase diagram could not be developed from the data. This prevented an analysis of the thermodynamics and various phase relationships such as the precise connection between the lattice distortions and the low-temperature enhancement of magnetic anisotropy above 0.7 GPa.37 Reaching beyond a simple room temperature understanding of various structural phases is also crucial to exploring mechanistic scenarios. The relationship between the magnetostructural phases and MnN6 octahedral rotations also merits further investigation because unstable rotations and distortions are significant routes to ferroelectricity.39

In this work, we combine high pressure Raman spectroscopy with complementary modeling, lattice dynamics calculations, and prior magnetization30,37 to unveil the extremely rich pressure–temperature–magnetic field (PTB) phase diagram of Mn[N(CN)2]2. We use this phase diagram—which reaches extremes in pressure and magnetic field that are rarely brought together—to untangle the connection between the different competing states. Tracking the series of pressure-induced phase transitions to low temperature reveals a delicate balance between magnetostructural phases, and our analysis of the octahedral rotations reveals the precise mechanism by which the different magnetic states are triggered. Enhanced exchange anisotropy above 0.7 GPa,37 for instance, is driven by softening of the octahedral rotation around b. Compression also stabilizes a previously unexplored soft mode-driven magnetic phase above 2.8 GPa that involves octahedral rotation around a and is predicted to occur with a unique 90° reorientation of the exchange planes. In addition to opening an avenue for closer examination of materials containing high spin S = 5/2 Mn(II),40,41,42 these findings underscore the importance of cooperative structural distortions in the stabilization of novel magnetic phases and help to provide a strategy for the control of functional materials.

Results

Revealing structural phase transition mechanisms

Figure 1 displays close-up views of the Raman response of Mn[N(CN)2]2 as a function of pressure at 100 K. The majority of features display traditional compression-induced hardening,38 so we focus on the behavior of the octahedral rotations, the lowest frequency lattice modes, the C≡N–C ligand bend, and the C≡N stretch as most significant. Peak position vs. pressure plots along with a frequency shift and splitting pattern analysis reveal a series of pressure-induced structural phase transitions at 0.2, 1.3, and 3.0 GPa. In order to simplify our discussion of the structural distortions, we designate the phases as α, α′, γ, and δ from lowest to highest pressure. The sharp αα′ transition at P C1 = 0.2 GPa takes place within the orthorhombic Pnnm space group. It involves only local distortions in the MnN6 environment as indicated by a hardening of the 50 cm−1 mode associated with octahedral rotation around c and a change in slope of the 80 cm−1 equatorial out-of-phase N–Mn–N bending mode. The more gradual α′ → γ crossover at P C2 = 1.3 GPa is signaled by the disappearance of the 50 cm−1 octahedral rotation around c and splitting of the 2190 cm−1 C≡N stretch. Finally, the γδ crossover near P C3 = 3.0 GPa is identified by splitting of the mode at 120 cm−1, a significant width enhancement of the C≡N–C bending mode near 680 cm−1 that we attribute to weak splitting, and rigidity in the 2260 cm−1 overtone. As discussed below, P C2 and P C3 have important effects on the crystal symmetry and magnetic properties.38

Fig. 1
Fig. 1

a–c Close-up views of the 100 K Raman spectra of Mn[N(CN2)]2 as a function of pressure. d–f Frequency vs. pressure for the modes displayed in a-c from which we determine the critical pressures. Line and background colors correlate with well-defined phases. Here, blue, green, red, and cyan represent the ambient pressure orthorhombic (Pnnm) α phase and the high pressure α′, γ, and δ phases, respectively. The blending near P C2 and P C3 indicates the range over which the structural distortions take place

We extended these variable pressure Raman scattering measurements and the analysis shown in Fig. 1 to include several temperatures between 100 and 300 K. In each case, we identify a series of three critical pressures. As before, the αα ' transition is sharp whereas the α′ → γ and γδ crossovers take place continuously over much broader pressure ranges. Figure 2 displays the pressure–temperature (PT) phase diagram of Mn[N(CN)2]2. We immediately notice that the phase boundaries corresponding to these structural distortions have positive ∂P/∂T’s. Since (∂P/∂T) V  = −(∂S/∂V) T , the slopes indicate that entropy is increasing—becoming more disordered through each successive structural transition. These phase boundaries drive toward an interesting set of magnetic states at low temperature.

In order to unveil the mechanism behind this series of structural phase transitions, we performed first-principles calculations of Mn[N(CN)2]2 under isotropic compression and compared our predictions with the experimental results (Fig. 3 a, b). Our calculations reveal three octahedral rotational modes (Fig. 3 c–e), two of which strikingly become unstable under pressure. These soft modes drive permanent lattice distortions and are responsible for the structural phase transitions at P C2 and P C3 in Mn[N(CN)2]2. By contrast, the transition at P C1 is a local distortion and therefore is not associated with a soft mode. Thus, while P C2 and P C3 are amenable to x-ray investigation, P C1 can not be resolved by an average structure technique. The soft modes predicted to appear at 49 and 53 cm−1 are unfortunately not observed in our experiments because (i) the features overlap and (ii) the calculated matrix elements are very small (0.018 and 4.43 compared to ≈44 for the 120 cm−1 lattice mode). This highlights the role of predictive theory in unraveling precisely how and why a phase transition takes place.

Overall, the predicted critical pressures are in excellent agreement with the sequence of structure phase transitions displayed in the PT phase diagram (Fig. 2). The octahedral rotation around b (R b in Fig. 3c) is predicted to become imaginary at 2.2 GPa, near the observed α′ → γ crossover at P C2 = 1.3 GPa. The MnN6 rotation about the a axis (R a in Fig. 3d) is predicted to go soft at 3.1 GPa, very close to the γδ crossover at P C3 = 3.0 GPa. Finally, we point out that the ambient structure is already displaced through the octahedral rotation around c (R c in Fig. 3e), and therefore the MnN6 rotational mode observed at 50 cm−1 does not go soft (Fig. 3a, b). Trends in the lattice and localized modes are reproduced as well,38 although small discrepancies arise from carrying out our calculations under constant symmetry.

Fig. 2
Fig. 2

Pressure–temperature phase diagram of Mn[N(CN)2]2 obtained by combining the critical pressures determined by Raman scattering (red points) with magnetic properties data (green points) from  Quintero et al.37 The blue, green, red, and teal regions correspond to the α, α′, γ, and δ phases, respectively. The breadth of the phase boundaries near P C2 and P C3 is indicated by blending between the dotted lines

Fig. 3
Fig. 3

(a) Calculated and (b) experimental frequency vs. pressure trends for the low frequency Raman-active modes of Mn[N(CN)2]2. Colored regions correspond to various phases as labeled, with blended areas indicating gradual crossovers. c–e Displacement patterns for the octahedral rotation modes around b, a, and c

Structural phase transitions trigger new magnetic states

This series of pressure-driven structural distortions has important implications for low temperature magnetism. The connection is readily apparent from the PT phase diagram, where we see that Mn[N(CN)2]2 sports at least two long-range ordered magnetic states that differ in their anisotropy.37 Extrapolating the pressure-induced structural transitions (the edges of which are indicated by dotted lines in Fig. 2) to base temperature reveals that the low pressure edge of the α′ → γ transition directly encounters the magnetic phase boundary. This coincidence suggests that it triggers the anisotropy crossover. Despite the temperature limitations imposed by our in-situ pressure experiments, this sort of direct connection from simple inspection of the phase diagram is not often apparent. Our calculations link the α′ → γ structural phase transition and the magnetic anisotropy crossover as well. Figure 4 displays two of the important angles in the Mn–N≡C–N–Mn superexchange pathway and the corresponding exchange interaction between metal centers (J) as a function of pressure. These values are computed in two different magnetic planes. Strikingly, we predict the development of two unique Mn–N≡C–N–Mn bridges under pressure (in agreement with our spectral findings), an unprecedented change in the Mn–N–C bond angle (by more than ±20°), and a consequent splitting of J in the γ phase. These two different exchange interactions arise due to the octahedral rotations. Although we predict that the system remains orthorhombic, the development of two unique J values is consistent with a change in exchange anisotropy. We therefore conclude that structural distortions across the α′ → γ transition drive the anisotropy enhancement37 in the γ phase.

Fig. 4
Fig. 4

Calculated (a) Mn–N≡C and Mn–N–C angles and (b) J vs. pressure. J 1 (J 2) is the exchange interaction of spins located in the blue (red) plane of (c) the orthorhombic′ γ and (d) monoclinic δ phases. The exchange interactions in both the γ and δ phases support G-type antiferromagnetism on a bipartite lattice. The blue and red magnetic planes (associated with J 1 and J 2) rotate by 90º in a cooperative manner across the structural transition

The temperature dependence of the γδ transition provides compelling evidence for an unexplored low temperature magnetic phase near 3 GPa. Our calculations predict that the 53 cm−1 soft mode [R a ] drives the system to a monoclinic space group, consistent with the appearance of new spectral features. As seen in Fig. 4a, the 120° Mn–N≡C angle splits into two, giving a total of four unique superexchange angles in the δ phase. This is also in line with splitting of the N≡C–N ligand bending mode around 680 cm−1 (Fig. 1b, e). The δ phase thus displays two unique J values (Fig. 4b) that become more distinct under compression. Another intruiging aspect of the γδ transition in Mn[N(CN)2]2 is that it takes place with a 90° reorientation of the exchange planes (Fig. 4c, d). According to our calculations, this unusual exchange plane reorientation is a consequence of the 90° separation of the rotation axes of the R b and R a soft modes that define the structural phases. High pressure magnetization or inelastic neutron scattering may be able to detect these exotic changes in the microscopic spin rearrangement.

Discussion

Pressure and temperature are not the only tuning parameters that support new states of matter in Mn[N(CN)2]2. Applied magnetic field drives a spin–flop transition35 and ultimately a transition to the fully polarized state that is stabilized by lattice distortions.36 Here, field suppresses the quantum fluctuations associated with the canted antiferromagnetic state to saturate the magnetization above 30 T. Bringing these results together with our current effort yields an extraordinarily rich PTB phase diagram (Fig. 5) with a surprising number of competing magnetostructural phases. This complexity arises from the delicate balance of interactions in Mn[N(CN)2]2, making it possible for small external perturbations to modify the important energy scales and mixing processes and driving the system into new phases with unique properties. The low → high anisotropy transition with pressure and field (taking the system from Heisenberg to Ising-like) is an especially nice illustration of pressure/field complementarity. The ability to explore materials in these extreme environments is obviously very unusual. What makes this particular PTB phase diagram especially fascinating is the prospect that these phases may host emergent properties at experimentally-realizable conditions. An important aspect of the phase diagram in Fig. 5 is that the majority of transitions depend upon external stimuli rather than thermal fluctuations. We argue here that the mechanism for the pressure-induced transitions in Mn[N(CN)2]2 at T = 0 K depends on quantum fluctuations which are enhanced by softening of the phonon modes. Of course, high spin Mn(II) is typically described as a semi-classical or solely classical ion because spin is large (S = 5/2), single ion anisotropy is low, and quantum fluctuations (which go as 1/S) tend to be small—especially compared to Mn(III) and Mn(IV).43 That said, dicyanimide is a high anisotropy ligand and is intimately involved in establishing the different Neél states under pressure. Moreover, our calculations predict that Dzyaloshinskii-Moriya interactions grow with decreasing bond angle (Fig. 4a). The magnetostructural phase diagram and mechanisms revealed here thus suggest that a number of the states and phase transitions in Mn[N(CN)2]2 may have unexpected complexity—especially above P C3, where we predict a unique reorientation of exchange planes.

Fig. 5
Fig. 5

Pressure–temperature–magnetic field phase diagram of Mn[N(CN)2]2 created by combining our findings with prior magnetic and vibrational properties work.30,35,37,38 The color scheme in pressure space matches that in prior figures, and blended areas denote extended transition regimes. The structural and magnetic phases are labeled

We emphasize that the magnetostructural coupling mechanisms discussed here are intrinsic to molecular materials and, in addition to being important features of Mn[N(CN)2]2, likely underlie the properties of hybrid transition metal–organic materials—many of which also contain Mn(II). Multiferroic [(CH3)2NH2]Mn(HCOO)3 is a superb example.44,45,46,47 Mn(TCNE)[C4(CN)8]1/2 and Mn1−x Co x WO4, which display a pressure-induced antiferromagnetic → ferrimagnetic transition and an eccentric spin cycloid respectively, also merit investigation in this regard.40,42 The competing phases in these and other materials41,48,49,50,51 suggest that Mn(II)-containing systems may provide an interesting new platform for exploring novel states of matter, some of which may even host quantum properties.

Methods

Polycrystalline Mn[N(CN)2]2 was synthesized as described previously24 and loaded into a diamond anvil cell with an annealed ruby ball to determine pressure.52 Tests of loading conditions (either neat or with vacuum grease, liquid argon, or KBr as pressure media) demonstrate consistent results due to the soft nature of the material. Raman measurements were performed with a 532 nm diode pumped solid state laser, with < 1 mW power to prevent sample damage. Raman spectra were collected with a resolution of 0.5 cm−1, integrated between 60 and 120 s, and averaged three times. An open-flow helium cryostat provided temperature control. In order to apply pressure in situ at low temperature, the diamond anvil cell was placed inside of a cryostat, the thermal contact of which limited our temperature range to 100 K. Pressure was raised to 5 GPa and fully released after each compression so that the material could relax. Standard peak fitting procedures were employed as appropriate.

First-principles calculations were performed based on density-functional theory within the generalized gradient approximation GGA + U scheme53 with the Perdew–Becke–Erzenhof parametrization54 as implemented in the Vienna ab initio simulation package.55,56 We employed the Dudarev57 implementation with on-site Coulomb interaction U = 5 eV to treat the localized d electron states of Mn. Within GGA + U this choice gives excellent agreement between the calculated (4.66 μB) and experimental magnetic moments (4.65 μB).34 The projector augmented wave potentials58,59 explicitly include 13 valence electrons for manganese (3p 63d 54s 2), 5 for nitrogen (2s 22p 3), and 4 for carbon (2s 22p 2). Structural optimizations were performed for a 22-atom unit-cell with a 6 × 6 × 6 Monkhorst-Pack k-point mesh. Raman mode frequencies were computed using the frozen phonon method to capture soft-modes driven by pressure. To find the minimum-energy configuration of the soft modes with pressure, we added one (under ~2 GPa) or two unstable soft modes (under ~3–5 GPa) in the ground state structure and moved the atoms according to the conjugate-gradient algorithm until the Hellman-Feynman forces were less than 1.0 meV/Å. Interestingly, when we added the two soft modes to the Pnnm ground state under the higher pressures (3–5 GPa), only the R a soft mode leading to the monoclinic δ phase remains after the relaxation. A Heisenberg-type spin Hamiltonian (\({\cal H} = - \mathop {\sum}\nolimits_{\langle i,j\rangle } J_{i,j}S_i \cdot S_j\)) was employed to estimate the exchange interactions. As a point of comparison, the calculated J value at ambient conditions (−0.12 meV) is in good agreement with the experimental value (−0.07 meV).34,35


Data Availability

Relevant data is available upon request from the corresponding authors, Jan Musfeldt (email: musfeldt@utk.edu) or Jun Hee Lee (email: junhee@unist.ac.kr).

Additional information

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Acknowledgements

This work was supported by the National Science Foundation [DMR-1707846 (JLM, UT) and DMR-1703003 (JLM, EWU)], the Petroleum Research Fund [52052-ND10 (JLM, UT)], and the Department of Energy, Office of Science, Basic Energy Sciences, Materials Sciences and Engineering Division (RF). The research at UNIST (JHL, MSK) was supported by Basic Science Research Program through the National Research Foundation of Korea (NRF) funded by the Ministry of Science, ICT & Future Planning (2015R1C1A1A01055760) and Creative Materials Discovery Program through the National Research Foundation of Korea (NRF) funded by the Ministry of Science and ICT (2017M3D1A1040828). Work at the National Synchrotron Light Source at Brookhaven National Laboratory was funded by the Department of Energy (DE-AC98-06CH10886). The use of the U2A beamline was supported by COMPRES under NSF Cooperative Agreement EAR 11-57758 and CDAC (DE-FC03-03N00144). This research used resources of the National Energy Research Scientific Computing Center, a DOE Office of Science User Facility supported by the Office of Science of the U.S. Department of Energy under Contract No. DE-AC02-05CH11231.

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Affiliations

  1. Department of Chemistry, University of Tennessee, Knoxville, TN, 37996, USA

    • Kenneth R. O’Neal
    •  & Janice L. Musfeldt
  2. School of Energy and Chemical Engineering, Ulsan National Institute of Science and Technology, Ulsan, 44919, Korea

    • Jun Hee Lee
    •  & Maeng-Suk Kim
  3. Department of Chemistry and Biochemistry, Eastern Washington University, Cheney, WA, 99004, USA

    • Jamie L. Manson
  4. Department of Civil and Environmental Engineering, The George Washington University, Washington, DC, 20052, USA

    • Zhenxian Liu
  5. Materials Science and Technology Division, Oak Ridge National Lab, Oak Ridge, TN, 37830, USA

    • Randy S. Fishman
  6. Department of Physics, University of Tennessee, Knoxville, TN, 37996, USA

    • Janice L. Musfeldt

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Contributions

This project was conceived by J.L.M. (UT), J.H.L., R.S.F., Z.L., and K.R.O. The sample was synthesized by J.L.M. (EWU), spectroscopic measurements were performed by K.R.O., Z.L., and J.L.M. (UT), and first-principles calculations and predictions based on density-functional theory were carried out by J.H.L., M.K., and R.S.F. All authors discussed the data. The manuscript was written by K.R.O., J.H.L., R.S.F., and J.L.M. (UT), and all authors commented on the document.

Competing interests

The authors declare no competing financial interests.

Corresponding authors

Correspondence to Jun Hee Lee or Janice L. Musfeldt.

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DOI

https://doi.org/10.1038/s41535-017-0065-0