Double perovskites (DP, A2BB’O6) exhibit a breadth of multifunctional properties with a huge potential range of applications, including magneto-optic and spintronic devices. However, spontaneous cation ordering is limited by the similar size and charge of B and B’ cations. We introduce a route to stimulate B-site rock-salt ordering. By growing thin films on (111)-oriented substrates, ‘in-plane’ strain acts on the intrinsically tilted oxygen octahedra of the DP and produces two different B-site cages (in size and shape), stimulating spontaneous cation ordering. For the ferromagnetic insulator La2CoMnO6, clear Co/Mn ordering was achieved by growing on (111)-oriented substrates. The difference in B-site cages was further enhanced when grown under minor (111) in-plane compressive strain, resulting in long-range ordering with a saturation magnetization of 5.8 μB/formula unit (f.u.), close to the theoretical 6 μB/f.u., without antiferromagnetic behavior. Our approach enables the study of many new ordered DPs which have never been made before.
Bi-component perovskites, AA’BB’O6, both artificially grown as ultrashort period perovskite-oxide superlattices and as spontaneously ordered double perovskites (DP), attract high interest due to their potential application in a wide range of devices, such as electrically tunable microwave devices,1 multiferroic solar cells,2 magneto-optic devices3 and spin-filter devices.4 In this materials family, the cations are ordered in either a layered, columnar or rock salt structure. As a result, these materials exhibit a large set of exotic magnetic and ferroelectric properties that are absent in the parent compounds, including improper ferroelectricity (for example, in PbSrTi2O6),5 strongly enhanced dielectric constant (for example, in BaSrTi2O6),6 ferromagnetic semiconducting behavior (for example, in La2NiMnO6),7 multiferroicity (for example, in Bi2NiMnO6)8 and room temperature colossal magnetoresistance (for example, in Sr2FeMoO6).9 In addition, there are many experimentally unexplored bi-component perovskites that are suggested to have fascinating properties. Examples are hybrid improper ferroelectric LaYGa2O6,10 low-band-gap Sr2AlVO6,11 half-metallic ferromagnet Sr2TiCrO612 and half-metallic antiferromagnet La2VCuO6.13 However, to achieve these exciting functionalities, the materials should have a high degree of cation ordering. Unfortunately, the fabrication of ultrashort period superlattices is extremely difficult and a slow growth rate is required, limiting industrial interest. Therefore, to enable the fabrication of bi-component perovskite thin films with perfect ordering and thus realizing their huge potential, one has to look for routes that allow natural formation of these superlattices, that is, fabrication of DP thin films.
Considering DP B-site cation ordering in bulk, the biggest challenge is the similarity of the ionic formal valence (FV) and ionic radius (rB) of the B-site cations. Hence, to achieve spontaneous B-site rock salt ordering in bulk, a distinct difference in FV and rB is necessary.14, 15 Similar constraints apply for thin films, but, in addition, thin film growth is complicated by the presence of multiple multivalent ions in DPs.16, 17 These constraints limit the group of ordered DP thin films significantly, and therefore, to date, only a small number of ordered DP thin films has been fabricated. On the other hand, thin film growth offers an additional set of growth parameters to play with, including anisotropic strain. Optimizing these growth parameters has already shown to enable the growth of spontaneously ordered DP thin film materials that do not exist in bulk.18, 19, 20, 21, 22
Promisingly, for example, recent studies have shown that control of thin film growth kinetics can lead to spontaneous ordering even if the difference in FV and rB is negligible.18, 19, 20, 21, 22 Here, cation ordering can be stimulated by using non-equilibrium growth settings during pulsed laser deposition, that is, a low oxygen pressure (~10−4 mbar), high substrate temperature (>1000 °C) and subsequent quenching to room temperature. It was proposed that ordering may occur under these conditions as the FV difference between B and B’ is enhanced in the surface growth front.22 However, the exact understanding of why B-site ordering takes place was not made clear. Also, the complexity of the growth and reproducibility of the growth remain challenging. In addition, the required high substrate temperature and low pressure during growth are not suitable for many DP compositions, including Sr2FeMoO6, La2CoMnO6 and the highly demanding multiferroic Pb- or Bi-containing DPs.8, 23, 24, 25
Therefore, understanding of what leads to spontaneous B-site ordering in thin films and developing new growth processes that produce this ordering reliably are now required. Here, we start with what is known for bulk A-site ordering, where the presence of two differently sized spaces at the A-sites, as a result of a+a+a+ BO6 octahedral tilting (Glazer’s notation26), produces spontaneous A-site cation ordering in the highly complex A3A’B4O12 system.27 Transferring this route to the B-sites in A2BB’O6 thin films would require the formation of different B-site cages (in shape and volume) in an ordered arrangement. Analogously to the scenario described for the A-sites, we propose here that two different spaces at the B-site can be created in a rock salt ordered manner when the film material contains anti-phase octahedral rotations in combination with induced ‘in-plane’ strain, which is controlled by the orientation of the substrate and the substrate-film misfit. We investigate experimentally whether this approach can enhance or even induce spontaneous B-site ordering.
To understand how two different B-sites can be created, we first discuss the effect of ‘in-plane’ strain on non-distorted BO6 for different substrate orientations (see Figures 1a and b). First of all, for the most conventionally used orientation, the (001), a perovskite under compressive in-plane strain has four reduced in-plane B-O bonds (dB-O) and two elongated out-of-plane dB-O (Figure 1a). On the other hand, for the rarely studied (111)-oriented perovskites under compressive strain, all six dB-O elongate to preserve the unit cell volume. (Figure 1b)
Secondly, we include octahedral rotations, as they are present in the majority of DP-oxides.28 The rotations of the octahedra result in a zig-zag pattern of the -O-B-O-B- chain, as depicted in Figures 1c and d. For (001)-oriented films, the rotation axes are either parallel or perpendicular to the substrate surface (Figure 1c). Therefore, although the octahedra are tilted, the effect of strain is expected to be the same on all tilted BO6 octahedra, independent of the type of rotation (in-phase or anti-phase). For (111)-oriented films, one set of BO6 octahedra tilts towards the substrate surface plane (the in-plane direction), while the nearest neighboring set of BO6 octahedra tilts toward the substrate surface normal (the out-of-plane direction) as illustrated in Figure 1d. Hence, the effect of in-plane strain on the two sets of octahedra is different, resulting in B-site cages of different orientation and volume. The difference between the octahedra depends on the magnitude of the strain and the magnitude of the octahedral tilting. A typical volume difference between the two octahedra would be between 0.3–3%. Both octahedra are tilted similar with respect to the out-of-plane direction. Therefore, applying in-plane strain on these octahedra results in a shape and volume change that is the same for both octahedra. Note that cation displacements are not taken into account. Since the two different B-site cages are nearest neighbors, they are then arranged in a rock salt fashion, which is the most frequently found arrangement of B cations in ordered A2BB’O6.15 Having small differences between B and B’, such as in valence state, ionic radius and electronegativity, is expected to stimulate an ordered occupation of the B-site cages instead of forming a random arrangement.
To test the above hypothesis about the formation of two different B-site cages stimulating B-site cation ordering, we have grown the ferromagnetic insulator La2CoMnO6 (monoclinic space group P21/n, amonoclinic=0.553 nm, bmonoclinic=0.549 nm, cmonoclinic=0.778 nm and βmonoclinic=89.95° giving apc=0.389 nm, where pc denotes pseudocubic) on various (001)- and (111)-oriented substrates with different strain states (see Figure 2a).29
La2CoMnO6 is used here as a model system, since it offers some significant advantages. First of all, bulk La2CoMnO6 has an a−a−c+ tilting pattern (Glazer’s notation26). Having rotations along all three orthogonal axis of which two rotations are anti-phase, a clear difference in B-site space as a result of strain can be expected. (Note that the volumes of MnO6 and CoO6 in bulk ordered La2CoMnO6 have a difference of ~13%.29) Secondly, it is a challenge to achieve full Co/Mn ordering as both ordered and disordered La2CoMnO6 exist in bulk. Ordered La2CoMnO6 can occur as a result of internal charge transfer from Mn to Co, giving Mn4+ and Co2+ (ΔFV=2 and ΔrB=11.5 pm).29, 30, 31 However, disordered La2CoMnO6 contains Co3+/Mn3+ (ΔFV=0 and ΔrB=3.5 pm) and is energetically (0.2 eV) slightly more favorable than Co2+/Mn4+.29, 30, 32 As a result, a very high degree of Co/Mn ordering in thin films has not been achieved to date. Using the formation of two different B-site spaces as an extra driving force to create Co/Mn ordering, we expect that highly ordered La2CoMnO6 films can be achieved on (111)-oriented substrates. Since this driving force is absent for films on (001)-oriented substrates, a low degree of cation ordering is expected in these cases.
To date, achieving cation ordering in La2CoMnO6 in both bulk and thin films requires high growth temperatures (for example, >1100 °C in bulk) as well as high oxygen pressures.33, 34, 35 As a result, the non-equilibrium DP thin film growth method, using low oxygen pressures, cannot be used for La2CoMnO6. In La2CoMnO6, low oxygen pressures lead to oxygen vacancies, which are associated with cation disorder.30 Additionally, the magnetic Curie temperature (TC) and the saturation magnetization (Ms) of La2CoMnO6 strongly depend on the cation ordering, making the magnetic behavior a good indicator for the presence of cation ordering.17, 36 Bulk ordered La2Co2+Mn4+O6 has a ferromagnetic-to-paramagnetic transition temperature (TC) of ~230 K, while a TC of ~80–150 K is often related to the disordered La2Co3+Mn3+O6 phase.30, 36 Furthermore, fully ordered La2CoMnO6 has a theoretical spin-only Ms of 6 μB/formula unit (f.u.).30 The introduction of disorder at the B-site as a result of antisites or anti-phase boundaries leads to antiferromagnetic (AFM) Co2+-O-Co2+ and Mn4+-O-Mn4+ superexchange interactions, lowering both Ms and TC.30 Moreover, the TC and Ms decrease by the introduction of oxygen vacancies arising from the formation of Mn3+ which lowers the degree of ordering.17, 30, 37
To study the influence of both the magnitude of strain and the substrate orientation, thin La2CoMnO6 films were grown by pulsed laser deposition on three different perovskite-oxide substrates (LaAlO3, (La,Sr)(Al,Ta)O3 (LSAT) and SrTiO3) with two different orientations, either (001) or (111). The mismatch between substrate and ordered La2CoMnO6 is depicted in Figure 2a. To avoid any influence of the growth parameters on cation ordering, all films were grown under the same growth conditions. The growth settings were optimized for films on (111)-oriented SrTiO3 to achieve coherently-grown, single-phase La2CoMnO6. To minimize the effect of spontaneous bulk ordering, we used a growth temperature which was 50–100 °C lower than in previous investigations of La2CoMnO6 film growth.17, 31, 33, 34, 36, 38, 39, 40 The films were deposited in the thickness range of 20–60 nm, which is sufficiently low to allow only minimal in-plane relaxations on the SrTiO3 and LSAT substrates, but not too low to result in a TC reduction.41, 42, 43
A ceramic La2CoMnO6 target was synthesized by conventional solid-state reaction. A stoichiometric mixture of Co3O4 (Alfa Aesar, Lancashire, UK), MnO2 (Alfa Aesar) and La2O3 (Sigma Aldrich, Dorset, UK) was ground and subsequently calcined at 900 °C for 10 h under oxygen flow. After cool down the mixture was ground and pressed into a 1 inch pellet. The pellet was sintered at 1200 °C for 17 h under oxygen flow. Single-phase La(Co,Mn)O3 was confirmed by powder X-ray diffraction (XRD, Bruker D8 theta/theta diffractometer, Cu Kα radiation (Bruker AXS GmbH, Karlsruhe, Germay)).
Thin film fabrication
As substrates, we used TiO2 terminated (001)-and (111)-oriented SrTiO3 (a=0.3905 nm),44, 45 thermally treated (001)-and (111)-oriented LSAT (a=0.387 nm)46 and thermally treated (111)-oriented LaAlO3 (apc=0.382 nm)47 single-crystal substrates (Crystec GmbH, Berlin, Germany). The films were grown by pulsed laser deposition at a substrate temperature of 710 °C with a repetition rate of 1 Hz and a fluence of 1.5 J cm−2. To ensure oxygen stoichiometry, the films were grown at 0.15 mbar flowing O2, annealed in 500 mbar O2 at 700 °C for 30 min directly after deposition and slowly cooled afterwards (−5 °C min−1 to 400 °C followed by −10 °C min−1 to room temperature) while maintaining 500 mbar O2 background pressure.
Characterization of structure and physical properties
Structural analysis of the films was done by XRD (high-resolution Panalytical Empyrean vertical diffractometer, Cu Kα radiation, Panalytical, Kassel, Germany). Magnetic property measurements were performed using a superconducting quantum interference device (SQUID magnetometer, Quantum Design, San Diego, CA, USA), with a temperature range of 5–300 K and up to 4 T.
Scanning transmission electron microscopy
Samples were prepared for scanning transmission electron microscopy (STEM) investigations by a focused ion beam lift-out procedure using a FEI Nova Nanolab 200 DualBeam instrument (FEI, Hillsboro, OR, USA). Final polishing of the sections was performed using a 5 kV Ga beam. In some cases, additional final polishing was performed using 500 V Ar+ ions in a Gatan PIPS (Gatan Inc., Pleasanton, CA, USA). The STEM measurements were performed using two instruments. Most of the data was recorded using a Nion UltraSTEM 100 (NION, Kirkland, WA, USA) operated at 100 kV accelerating voltage with a probe semiconvergence angle of 30 mrad, and equipped with a Gatan Enfina Spectrometer with an acceptance semiangle of 32 mrad. High-angle annular dark field images were recorded with a detector with an effective inner angle of ~78 mrad. annular bright field (ABF) images were recorded with an angular range on the detector of 16–30 mrad, and simultaneously recorded low-angle annular dark field images were recorded with an angular range of 33–180 mrad. Additional data was recorded using a JEOL ARM200CF (JEOL Ltd., Akishima, Japan) operated at 200 kV accelerating voltage and a probe convergence semiangle of 29 mrad, and equipped with a Gatan GIF Quantum ER with DualEELS using a 2.5 mm entrance aperture and 2 cm camera length to give an acceptance semiangle of 36 mrad. High-quality images were created by repeated scanning of the same area using a relatively short pixel dwell time of a few μs, followed by subsequent alignment and summation, either using a simple rigid registration technique using the SDSD plugin for Digital Micrograph48 (Gatan Inc.) or using a non-rigid registration technique to also remove non-linear scan-distortion and higher frequency electronic interference.49 Determination of atomic column positions was then performed using the Image Analysis routine for Digital Micrograph (kindly provided by Dr Bernhard Schaffer, Gatan GmbH), followed by further analysis using conventional spreadsheets. Electron energy loss (EEL) spectrum images were processed by firstly removing noise using principal component analysis,50 followed by elemental mapping using Gatan Digital Micrograph. For the determination of oxidation states, standard spectra were acquired from samples of crushed powders of CoO (Co2+), LiCoO2 (Co3+), Mn2O3 (Mn3+) and MnO2 (Mn4+) (Sigma Aldrich Co.) under identical optical conditions to those used for the acquisition of the data from the La2CoMnO6 films, with both core-loss and low-loss data sets acquired from each area. As before, principal component analysis was used to reduce noise, and then the edge of interest was extracted by the fitting of an appropriate background before the edge. These were then transformed to a single-scattering distribution using Fourier-log deconvolution51 to remove the effects of thickness and multiple scattering. A similar procedure was performed on real Mn and Co L2,3 edges in the sample (where low-loss data were available for the deconvolution). Care needed to be taken with the extraction of the Co edges from the La2CoMnO6 samples, since the weak Mn L1 edge lies just before the Co L2,3 edge and the perturbation from this needed subtraction after background fitting. This then allowed the direct comparison of the real edges to those from standards.
Results and discussion
Structural analysis of the films was done by XRD. Figure 2b shows the out-of-plane diffraction patterns of the films grown on the (111)-oriented substrates (reflections are indexed based on pseudocubic symmetry). The films were grown fully epitaxial and no impurity phases were observed. Thickness fringes for films on SrTiO3 and LSAT were clearly visible indicating high film quality with well-defined interfaces. No superlattice peaks as a result of cation ordering were observed along . However, taking only cation ordering into account and no A-site displacement, these peaks are expected to be within the noise level due to the similar scattering factors of Co and Mn.18, 52
Asymmetric X-ray reciprocal space maps were taken to verify the strain state of the films (see Figures 2c and d for La2CoMnO6 on LSAT (111) and (001)). La2CoMnO6 on both SrTiO3 and LSAT substrates appeared to be fully in-plane strained, independent of the orientation. On the other hand, the misfit between La2CoMnO6 and LaAlO3 was too large (−2.7 %) to accommodate the stress in the film and, as a result, the film was fully relaxed. This result is consistent with the absence of thickness fringes in the out-of-plane diffraction pattern (see Figure 2b).
To verify the insulating state of the La2CoMnO6 films, four-point transport measurements for all samples were performed between 10–300 K. All samples showed insulating behavior with a very high resistivity (ρ) (~1012 Ω-cm) at room temperature, independent of substrate and orientation.
To gain insight into the presence of cation ordering, we measured the magnetization (M) versus temperature (T) and applied magnetic field (H). Figures 3a and b show the in-plane normalized field cooled M(T) (H=200 Oe) for the (001) and (111)-oriented films, respectively. The TC values were determined as the minima of dM/dT (see Table 1). The corresponding in-plane M(H) loops at 5 K along the direction are shown in Figures 3c and d. To enhance the clarity of the M(H) data, we subtracted the paramagnetic background that was only present for the films on SrTiO3. An overview of the main outcomes is shown in Table 1.
Taking a closer look at the M(T) data, a well-defined magnetic transition was found ~200 K for La2CoMnO6 on (111)-oriented substrates. On the (001)-oriented substrates, a minimum in the dM/dT was also present, but at much lower temperatures, around 120 K. Moreover, a clear tail is present in the M(T) curve above TC, which is likely the result of a large proportion of Co–O–Co and Mn–O–Mn bonds leading to AFM/paramagnetic superexchange interaction.35, 53, 54 In addition, M(H) shows a slight biloop behavior (Figure 3d) with a much lower MS. This suggests the presence of disordered magnetic domains with a variance of magnetic coupling due to cation disordering.
The clear difference in TC found between the (001) and the (111)-oriented films, ~120 K and ~200 K, respectively, indicates that the substrate orientation strongly influences the magnetic properties of the film and likely the B-site cation arrangement. In previous studies, the high TC was ascribed to Co/Mn ordering, while the low TC was believed to result from cation disorder, with the presence of Mn3+ and Co3+ and/or oxygen vacancies playing an important role.25, 30, 37 A reduction in Co/Mn ordering in our (001)-oriented film is in full agreement with the hypothesis as the creation of two different B-site spaces would be absent for these films.
To understand the M(T) behavior in more detail, we fitted the paramagnetic susceptibility (χ) of La2CoMnO6 on LSAT (111), the highest TC sample, to a Curie–Weiss Law in the temperature range of 216–250 K (inset in Figure 3a, shown by the solid black line). A paramagnetic Curie temperature (θ) of 213±0.3 K was found. Moreover, we used the expression M~(TC−T)β, where β is the critical exponent, to fit the M(T) curves for comparison with simple mean field theory for spontaneous magnetization near TC (inset Figure 3a, blue solid line). β and TC were found to be 0.34±0.01 and 211±1 K, respectively. The values found for TC and θ are similar indicating ferromagnetic behavior of La2CoMnO6 on LSAT (111). The TC is slightly lower than that observed in bulk La2CoMnO6. However, biaxial strain and a relatively low film thickness may reduce TC as they can affect the magnetic ordering, the B-O bond length and/or B-O-B’ bond angle.55, 56 The value found for β was 0.34 which is close to a three dimensional isotropic Heisenberg ferromagnet. Similar behavior has been suggested for ordered La2NiMnO6.35 The observation of high-quality ferromagnetic behavior indicates that the film has a very high degree of Co/Mn ordering.
While M(T) data show clear differences between (001)- and (111)-oriented films, the M(H) loops show clear differences in Ms and coercive field (Hc) between La2CoMnO6 on LSAT (111) and the other films (Figures 3c and d). The La2CoMnO6 films on (001) and (111) SrTiO3, (001) LSAT and (111) LaAlO3 showed a Ms of ~3.5–4 μB/f.u. with a Hc of 9–13 kOe. These Ms values are much lower than for ordered La2CoMnO6, suggesting the presence of Co/Mn disorder. However, Ms does not give any insight on the type of disorder. On the other hand, since the TC’ values differ significantly between the (001) and (111)-oriented films, the Co/Mn (dis)order is likely to be different. The presence of disorder is also in agreement with the enhancement in Hc compared to (partially) ordered La2CoMnO6 reported in previous studies (5–7 kOe).36, 39 The enhancement in Hc can be explained by the presence of anti-phase domains.
La2CoMnO6 on LSAT (111) showed a much higher Ms compared to all other films studied, Ms~5.8 μB/f.u., which is close to the theoretical maximum value of 6 μB/f.u. for fully ordered La2CoMnO6, as well as a relatively low Hc ~6 kOe, indicating a high degree of Co/Mn order. In comparison to previously reported ordered La2CoMnO6 films, our films on LSAT (111) showed a clear saturation in magnetization above 25 kOe. In previous studies, saturation was not even observed up to 40 kOe, probably due to the presence of AFM interactions.25, 36, 39 As the absence in saturation was not taken into account for determining the Ms in those studies, the actual Ms is likely to be lower than reported, and therefore also the Co/Mn ordering. In addition, from the M(H) loop, there is no evidence for the presence of other magnetic domains resulting from B-site cation disordering or the presence of antisite defects.54 As our films on LSAT (111) show a clear saturation in the magnetization with a Ms of ~5.8 μB/f.u. in combination with a high TC and a well-defined M(H) loop, a high degree of Co/Mn ordering has been achieved in these films.
To get a better understanding of the La2CoMnO6 structure, chemical ordering and the resulting magnetic behavior, we compared the films grown on SrTiO3 (111) and LSAT (111) using analytical STEM. Both films showed very good epitaxy and a well-defined interface with the substrate as shown in the high-angle annular dark field image La2CoMnO6 on LSAT and the low angle annular dark field image for La2CoMnO6 on SrTiO3 (Figures 4a and e), which is in agreement with our XRD results. Moreover, the characteristic partial Al-Ta ordering in the LSAT substrate is clearly visible.57 Please note that these images have an exceptionally high signal to noise level without global or local distortions due to the acquisition of a sequence of short exposure scans followed by the application of rigid and non-rigid registration procedures, as described in detail in the ‘Experimental section’. Therefore these data are suited to use for quantitative analysis of atomic positions.
To determine the type of ordering, spatially resolved electron energy loss spectroscopy spectrum imaging was undertaken on both samples. A clear difference in B-site ordering between the two films was present. For the film grown on (111) LSAT, the superimposed electron energy loss spectroscopy spectrum imaging maps of Mn and Co showed a clear rock salt ordering pattern, indicating that the bulk of the film has a high degree of long-range rock salt ordering (Figure 4b). Furthermore, the high degree of cation ordering is in agreement with the extracted electron energy loss spectroscopy (EELS) spectra from this region, which match well to standard spectra for Co2+ and Mn4+ (Figures 4c and d). This is consistent with previous measurements that suggest that atomic ordering is associated with strong charge ordering.30 For the film grown on (111) SrTiO3, the ordering is less clearly visible (Figure 4f). However, some columns still clearly have more Co or Mn, and the EEL spectra still match well to standard spectra for Co2+ and Mn4+ (Figures 4g and h), suggesting that a high degree of local ordering of Mn and Co is still present in the film on SrTiO3 (111), even if cation ordering does not persist over length scales longer than several nanometers, suggesting a nanoscale ordering domain structure. Multiple nanosized anti-phase domains have been inferred in other DPs as well.58 Moreover, a short-range ordered structure would also clarify the significantly reduced Ms as a result of the AFM Co2+-Co2+ and Mn4+-Mn4+ interactions at the anti-phase domains boundaries. However, since the degree of local cation order remained very high, only a minor reduction of TC is present.59
Our hypothesis states that the presence of anti-phase octahedral rotations would be required to enhance cation ordering. For both films, the oxygen maps in the bulk of the film show a clear zig-zag pattern along the direction consistent with the expected octahedral tilt pattern, as shown in Figure 5a for La2CoMnO6 on LSAT. This pattern is also seen in ABF STEM images of the interface for La2CoMnO6 on SrTiO3 (111) (Figure 5b). Quantification of the ABF STEM images of the La2CoMnO6 film on SrTiO3 show that anti-phase rotation along the pc and pc immediately starts at the interface and increases in strength over a few (111)pc planes until it reaches a plateau with a total tilt angle of ±8° (Figure 5c). See Supplementary Information for simulations that confirm this intuitive interpretation of the ABF images. (See supporting information for details regarding the interpretation of the ABF images.) The presence of octahedral tilting in both films is consistent with the presence of cation ordering.
To understand the absence of long-range ordering in La2CoMnO6 on SrTiO3 (111), we also investigated the pseudocubic layer spacing by doing quantitative measurements of the spacing between the A-site layers (d) along the out-of-plane direction, as the d-spacing is linked to the size and shape of the B-site cage.
In the SrTiO3 substrate, A-site layers are spaced with the expected d-spacing of ~2.25 Å. In the La2CoMnO6 film on SrTiO3, these spacings develop a pattern of alternating short and long d-spacings, as shown in Figure 5e, where the alternating spacing increases over about 20 (111)pc layers to values of around 2.32 and 2.18 Å. As this modulation of A-site d-spacings correlates very well with the trend in tilting pattern, it is clear that d-spacing and octahedral tilting are coupled. This is in agreement with the results for bulk ordered La2CoMnO6, where a modulation of alternate spacings of (101)monoclinic planes of 2.37 and 2.14 Å is present.29 Comparing the d-spacings with the bulk values, it is clear that the observed modulation in the film on SrTiO3 (111) is approaching the bulk values, but did not reach the full modulation after 20 (111)pc layers.
A similar effect in d-spacings is seen for La2CoMnO6 on LSAT (111) (Figure 5d). In the area analyzed, significant Al-Ta ordering was present in the LSAT substrate, resulting in a period doubling of (111)pc planes in the substrate. Therefore, for ease of comparison, the spacing of (111)pc planes in LSAT is calculated by halving the actual plane spacing. This averaged spacing is very uniform in LSAT with a constant value of 2.23 Å. In La2CoMnO6, a bimodal distribution of (111)pc layer spacings builds up immediately at the interface, similar as for the film on SrTiO3. However, the bimodality of layer spacings for La2CoMnO6 on LSAT (111) is much stronger approaching bulk values of 2.14 and 2.37 Å at ~20 layers away from the interface.
Our data clearly show that the d-spacing modulation in La2CoMnO6 on LSAT is larger than on SrTiO3. This is in agreement with the higher degree of ordering observed on LSAT. The small compressive strain sets up a pattern of co-operative octahedral tilting and A-site layer spacing modulation resulting in a large difference in the size of the B-site cages within the octahedra in each alternating layer along the growth direction. The pronounced difference in B-site cages then has the simple consequence that the smaller Mn4+ ions are attracted to the smaller octahedra and the larger Co2+ ions to the larger ones, giving the observed ordering pattern and resulting properties.
The minor tensile strain of SrTiO3 appears to slightly suppress the out-of-plane d-spacing modulation. This suppression may be due to the change in orientation of the monoclinic La2CoMnO6 unit cell (amonoclinic=0.553 nm, bmonoclinic=0.549 nm) with respect to the out-of-plane direction when moving from compressive (on LSAT) to tensile strain (on SrTiO3). The growth of La2CoMnO6 on (111) could proceed with a number of different orientations of the monoclinic unit cell with respect to the substrate. Firstly, any of the directions in the monoclinic cell equivalent to cubic could appear as the out-of-plane direction. By analyzing the lattice mismatch between the three directions equivalent to <110>cubic directions in the interface plane, it is possible to find the orientation that gives the lowest mismatch and therefore lowest strain (the same principle was used previously for predicting domain assemblages, for example by MacLaren et al.).60 It is found that of the four distinct <111>cubic directions, monoclinic gives the smallest interface misfit with −0.61%, −0.61 % and −0.36% misfit along the three in-plane <110>cubic directions for the film grown on LSAT. There are then three rotational variants of this orientation, with the monoclinic direction with the low −0.36% misfit along any of the three crystallographically equivalent <110>cubic in the substrate at the interface. Thus, a domain structure of three crystallographically equivalent variants would be expected with the monoclinic direction in-plane in all cases for films grown on LSAT. For films grown on SrTiO3, the misfit is lower and the strain is lowest for  and orientations of the film normal (0.27, −0.14 and 0.34% for the three in-plane directions in both cases). The lack of a strong constraint from SrTiO3 would therefore allow the nucleation of a more complex domain structure, which may also reduce the driving force for strong elemental and magnetic ordering. This could also explain the difference in d-spacing modulation between the films on LSAT (111) and SrTiO3 (111) (Figures 5d and e).
Growth of La2CoMnO6 on both LSAT and SrTiO3 substrates produced a very small concentration of precipitates at the substrate/film interface (Figure 6). The precipitates on SrTiO3 are, on average, slightly larger (~10 nm, Figure 6a) compared to those on LSAT (~2–5 nm, Figure 6b). Nevertheless, the precipitates rarely grow large or persist for any significant thickness of the film. On the basis of a combination of EELS and atomic resolution high-angle annular dark-field STEM imaging, the precipitates are most likely to be rock salt structured CoO, with the CoO directed out-of-plane (Figures 6b and c). As this phase was not observed by XRD, the volume fraction is very small. The particles being CoO agrees with the observed impurity phase seen in XRD by Egoavil et al.39. The presence of CoO is consistent with the fact that the first few layers of La2CoMnO6 were Mn-rich and Co-poor with Mn:Co ratios up to 70%:30% as determined by EELS quantification. However, since La2Co1−xMn1+xO6 also has a ferromagnetic TC ~210 K, no effect on the M(T) has been observed.61, 62 The deviation in stoichiometry also means that the ideal rock salt ordering is disturbed in those first few layers near the interface (Figure 6d), which is consistent with previous studies.39 The formation of CoO and La2Mn1+xCo1−xO6 can be explained by the fact that the in-plane strained lattice sites are too small for Co2+ in the first few layers, until the octahedral tilting and A-site spacing modulation has built up to the bulk-like values, as shown in Figures 5d and e. This also explains why the ideal ordered La2CoMnO6 structure forms readily, as shown in Figure 6d. Furthermore, the ordered La2CoMnO6 grows over the top of the CoO defects leaving the bulk of the film as the ideal rock salt ordered DP structure.
With a good understanding of the Co/Mn ordering of La2CoMnO6 on SrTiO3 (111) and LSAT (111), we are now able to infer the type of (dis)order in the films on LaAlO3 (111), SrTiO3 (001) and LSAT (001). First of all, since the magnetic behavior of La2CoMnO6 on LaAlO3 (111) and SrTiO3 (111) is comparable, a similar type of Co-Mn ordering can be expected, that is, short-range ordering with nanometer sized anti-phase domains. The absence of long-range cation ordering on LaAlO3 can be explained by the absence of induced in-plane strain as a result of a too large in-plane mismatch. As a consequence, the strain-induced effect required to promote the formation of two different B-site cages was absent. However, one may still expect the formation of the out-of-plane A-site d-spacing modulation as for the film on SrTiO3, which arises as a natural result of the octahedral tilting due to growing along the  direction.
A drastic change in the magnetic behavior of La2CoMnO6 was found by changing the orientation of the substrate from (111) to (001). For the (001)-oriented films, both a low TC and a low Ms with large HC were found, as well as a clear tail in the M(T) was present indicating the presence of AFM interactions. This strongly suggests a highly disordered or randomly ordered cation structure on the B-site. In addition, the reduced TC may indicate the presence of oxygen vacancies.30 Note that the formation of oxygen vacancies can depend on the film growth direction, even though the film growth conditions are the same.63 Recently, calculations have shown that oxygen vacancies are more likely to form in La2CoMnO6 when Co and Mn are mainly in the 3+ oxidation state,63 which would be expected for a random distribution of Co and Mn ions on the B-sites. Moreover, the presence of oxygen vacancies would also stimulate an increase in the formation of Mn3+, that is, increasing the degree of Co/Mn disorder.30 Therefore, the films grown on the (001) substrates are likely to be highly disordered and oxygen vacancy rich.
Finally, with the understanding of the differences in nature of cation (dis)order for the various samples, we now focus on why these different types of ordering occur. Therefore, we return to the hypothesis that states that two different octahedra, that is, two different B-site cages, can be formed when growing distorted perovskites on (111)-oriented substrates and thereby driving cation ordering. The hypothesis is in full agreement with our results as a significant increase in Co/Mn ordering in films on (111)-oriented substrates was observed compared to the films on (001)-oriented substrates. For the (001)-oriented films cation ordering was not stimulated by the substrate orientation. Since in this study, cation ordering was not stimulated by the growth conditions, no cation ordering was detected in the (001)-oriented La2CoMnO6 films.
To conclude, spontaneous B-site rock salt cation ordering can be stimulated in DP thin films by coherent growth along the  direction. This is because the combination of internal octahedral rotations of the DP and the in-plane strain from the (111)-oriented substrate induces the formation of two differently sized B-site spaces in a rock salt arrangement. A clear increase in Co/Mn rock salt ordering was achieved by growing on (111)-oriented substrates, including on SrTiO3 and LSAT. In addition, we have shown that cation ordering is strongly enhanced in La2CoMnO6 under a minor in-plane compressive strain when grown on a suitable (111)-oriented substrate, resulting in long-range Co/Mn ordered films with a Ms of 5.8 μB/f.u. Since the growth on (111)-oriented substrates can stimulate cation ordering and the driving force is insensitive to growth conditions, our work opens up the possibility of the realization of a whole range of new, high-quality functional DP thin films for a range of applications such as magneto-optic, spin-filter and magnetoelectric devices.
This work was supported by the European Research Council (ERC) (Advanced Investigator grant ERC-2009-AdG-247276-NOVOX), the EPSRC (Equipment Account Grant EP/K035282/1) and the Isaac Newton Trust (Minute 13.38(k)). LJ thank the support of the European Union Seventh Framework Programme under Grant Agreement 312483—ESTEEM2 (Integrated Infrastructure Initiative-I3). SuperSTEM is the UK National Facility for Aberration Corrected STEM funded by EPSRC.
JEK and JLMD designed the project. JEK and EDJ have grown the films. JEK and EDJ have done the XRD measurements; JEK, EMC and EDJ have done the magnetic measurements. DK and DHM acquired the STEM images and spectral data, with technical input and oversight from QMR. Additional STEM images and spectral data were acquired at Glasgow by IM. LJ performed the non-rigid registration of the STEM data sets. STEM data analysis was performed by TMY, BS, BAM, DK and DHM under the leadership of IM. JB performed STEM image simulations to validate the conclusions made in the STEM data analysis. All authors contributed to the discussions and writing of the article.
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