Ferromagnetism and Ru-Ru distance in SrRuO3 thin film grown on SrTiO3 (111) substrate
© Lee et al.; licensee Springer. 2014
Received: 30 September 2013
Accepted: 1 December 2013
Published: 7 January 2014
Epitaxial SrRuO3 thin films were grown on both (100) and (111) SrTiO3 substrates with atomically flat surfaces that are required to grow high-quality films of materials under debate. The following notable differences were observed in the (111)-oriented SrRuO3 films: (1) slightly different growth mode, (2) approximately 10 K higher ferromagnetic transition temperature, and (3) better conducting behavior with higher relative resistivity ratio, than (100)c-oriented SrRuO3 films. Together with the reported results on SrRuO3 thin films grown on (110) SrTiO3 substrate, the different physical properties were discussed newly in terms of the Ru-Ru nearest neighbor distance instead of the famous tolerance factor.
75.70.Ak; 75.60.Ej; 81.15.Fg
KeywordsSrRuO3 Ferromagnetic transition temperature Ru-Ru nearest neighbor distance Tolerance factor
Due to its low resistivity and good chemical stability, SrRuO3 (SRO) is frequently used as metallic electrodes in epitaxial perovskite-heterostructure capacitors [1, 2]. Film thickness, the amount of lattice mismatch, oxygen vacancy, and Ru vacancy are found to change its physical properties.
Fundamental thickness limit of itinerant ferromagnetism was observed . In addition to thickness being smaller than the critical thickness (t < 10 unit cells), a significant amount of oxygen vacancy was also found to deteriorate its ferromagnetic properties for thicker films (t > > 10 unit cells). Aside from these two factors, the ferromagnetic properties of SRO, especially the ferromagnetic transition temperature, Tc, have been known to be rather robust. While transport properties such as residual resistivity ratio (varying order of magnitude) are very sensitive to a tiny amount of Ru vacancy in SRO thin films grown on (100) SrTiO3 (STO) substrates, the ferromagnetic properties are rather immune to this tiny amount of Ru vacancy . A peculiar orthorhombic-to-tetragonal structural transition with variation of the Ru-O-Ru bond angle was observed depending on the thickness and temperature of the SRO film on STO (001) substrate but this structural transition temperature was not associated with the ferromagnetic transition temperature .
While many previous studies have focused on (100)c-oriented SRO films, the in-plane magnetization of thin films on top of STO (001) substrates was smaller than out-of-plane magnetization and Tc was smaller than that of bulk SRO [5, 6]. The observed small change of ferromagnetic properties in SRO films has been mostly explained simply in terms of lattice mismatch. A free-standing film made by lifting the film off its growth substrate recovered its bulk Tc and bulk saturated magnetic moment [5, 6]. An SRO film having a structure most similar to the bulk SRO was made using a buffer layer and STO (110) substrate, and its magnetic anisotropy was maximum [7–9]. The observed changes in SRO films on STO (110) was explained based on the inherently lower lattice mismatch of the orthorhombic crystal along the cubic substrate’s [1–10] in-plane direction than along the cubic substrate’s  in-plane direction . So, the lattice mismatch of orthorhombic crystal can always be smaller by choosing a cubic (110) substrate instead of a cubic (001) substrate. (In this report, we use pseudocubic notation for SRO films. (110)orthorhombic is equivalent to (100)c in the pseudocubic notation).
Up to now, the tolerance factor, t = (r A + r O )/√2(r B + r O ), was widely regarded as the most dominant factor to determine the structural transition from cubic to lower symmetries and accompanying huge changes in magnetic and electrical properties of many perovskite oxides [10–12]. Smaller t < 1.0 results in a more distorted structure having a smaller Ru-O-Ru bond angle . This factor is but a simple geometrical factor which cares the optimal radius of a sphere inside eight octahedra arranged at right angles and has been quite useful to explain major physical properties such as transport and magnetic properties in cubic, tetragonal, and orthorhombic colossal magnetoresistance. Recently, the structure modification effect on magnetic properties was reported in SrTi1-xFe x O3-δ thin films on STO (001), (110), and (111) substrates . The authors tried to interpret the change of magnetostriction in terms of lattice parameter.
In this paper, we discussed the physical property changes in terms of the nearest neighbor distance of B-site ion instead of the tolerance factor. We found that STO (001) and (111) substrates are ideal to study the change of physical properties of SRO films with Ru-Ru nearest neighbor distance (Ru nn-distance) which changes in order to accommodate the Sr2+ ion. This is because the Ru nn-distance can be differently changed by using different surface directions of the substrates. In the rhombohedral structure of the SRO film on STO (111) substrate, the Ru nn-distance does not change much to accommodate the Sr2+ ion, which might be able to explain the better transport and magnetic properties in this film.
The SRO thin films were grown on STO (001) and STO (111) substrates with a pulsed laser deposition method using a KrF excimer laser [7–9, 14, 15]. For simplicity, we will use ‘the SRO100 film’ and ‘the SRO111 film,’ respectively. Both substrates were initially prepared by etching and heat treatment to create step-and-terrace structures. Laser pulses of 140 to 170 mJ at 2 to 5 Hz were focused on a stoichiometric ceramic target. The substrate temperature and the oxygen partial pressure during deposition were 700°C to 760°C and approximately 100 mTorr, respectively. The thickness of the SRO film was 37 to 38 nm. We used an atomic force microscope (AFM) to check the surface morphology of the treated STO substrate and the SRO films. We performed structural analyses using a high-resolution X-ray diffractometer (HRXRD). The magnetic properties were measured with a superconducting quantum interference device (MPMSXL, Quantum Design, San Diego, CA, USA).
As the STO (111) surface consists of two highly polar layers of SrO34- and Ti4+, thermodynamic mixed termination is preferred to minimize the surface dipole . However, atomically well-defined SrTiO3 (111) substrates with a strong polar interface were recently developed using a rather difficult and selective etching of SrO34- and thermal annealing process . Chang et al. reported that simple annealing of as-polished STO (111) substrates yielded a step-and-terrace surface structure characterized by many bumps with step heights in multiples of 1/2 × d111, indicating mixed termination [16, 17]. To obtain atomically flat SrTiO3 (111) substrates with good step-and-terrace structures with Ti termination, they reported that harsh etching is required; both an ultrasonically agitated buffered hydrofluoric acid (BHF) solution and high-temperature ultrasonic agitation of an STO (111) substrate in deionized water were needed instead of mere soaking in etchants at room temperature. The harsh etching was followed by subsequent thermal annealing in a tube furnace at 1,050°C under an O2 atmosphere for 1 h.
Here, we report the simple preparation of atomically well-defined SrTiO3 (111) substrates and subsequent growth of SRO thin films. The surface roughness, rocking curve width, and transport properties showed that the SRO film grown on the SrTiO3 (111) substrates was of high quality. We compared basically the growth mode, transport properties, surface morphology, and magnetic properties of these films with the SRO film grown on the SrTiO3 (001) substrate with different structure deformation. Due to the additional danger accompanying the use of the ultrasonic agitator with BHF, we etched the STO (111) substrate using two different soaking times at room temperature, followed by annealing the etched substrate in a tube furnace at approximately 1,000°C under an O2 atmosphere for approximately 5 h. (For the STO (001) substrate, the typical soaking time was 15 to 30 s.) We found that simply increasing the BHF soak time worked very well for the STO (111) substrate without resorting to a more complicated method [17, 18]. (Connell et al. found that atomically flat STO (001) substrate can be prepared even without the use of dangerous BHF ).
There are many reasons that affect the different RRR values in epitaxially grown SrRuO3 thin films. Chemical doping like (Ca,Sr)RuO3 or epitaxial strain caused by using different substrates can change the bandwidth (thus transport properties) probably due to different Ru-O-Ru bond angles . If we use the same substrate for thin film growth, there are other factors that affect RRR. Oxygen vacancy and/or Ru vacancy can cause low RRR values and these accompany with expansion of the lattice. For example, a recent review paper correlated the unit cell volume with RRR . According to the review paper, an SRO with an orthorhombic unit cell volume of 240.9 Å3 ((=3.9052 × 3.950 × 4) should have RRR ~ 20. However, in our case, RRRs were 3 and 9 for the SRO100 film and the SRO111 film, respectively. A single-crystalline SRO thin film on STO (110) substrate having an orthorhombic unit cell volume of 240.9 Å3 was reported to have RRR ~ 8 . So, a simple explanation in terms of structural factor such as volume expansion is not enough to explain the different RRR values even though we accept that PLD-grown SRO films have more tendency to have larger lattice volumes and have lower RRR values.
Siemons et al. estimated that the Ru vacancy concentration causing drastic change of RRR is much smaller than a few percent for the range of samples they studied, from the fact that the decrease of the Curie temperature is as small as approximately 10 K . Thus, the effect of a very small amount of Ru vacancy in SRO thin films seems to be critical for RRR but should be much smaller than the effect of strain on the ferromagnetic properties . This is consistent with the observation of robust low-spin configuration for nearly all thin films of SrRuO3.
Figure 4b shows the temperature dependence of the magnetization at 500 Oe after high field cooling at 7 T. [The same specimen was used for these measurements by only changing the field direction with respect to the crystallographic axis - one along the in-plane direction, H//and the other along the surface normal direction, H⟂.] For the SRO111 film, the magnitude of magnetization along the surface normal direction was larger than that along the in-plane direction. This was similar to the observations for the SRO100 film and was interpreted in terms of compressive strain [5, 6]. To estimate the changes in the ferromagnetic transition temperature, we plotted magnetization of the SRO100 film and the SRO film grown on STO (110) substrate on the same plot . From Fig. 4(b), it can be seen that the ferromagnetic transition temperature of the SRO111 film is about 10 K higher than those of the SRO100 film and SRO film grown on STO (110) substrate. These increased ferromagnetic transition temperatures of films grown on a cubic (111) substrate were also reported for manganese oxide [28–30].
Figure 4c shows magnetic hysteresis curves at 5 K for applied fields along two directions. Here, we found that magnetization along the surface normal direction increased more rapidly than that along the in-plane direction. For fields along the surface normal direction, the coercive field was very well defined for both films. The coercive field for the SRO111 film was approximately 0.7 T, which was slightly larger than the value of approximately 0.5 T for the SRO100 film. Finally, we found that the saturated magnetic moments with a 6-T applied field were smaller than 2 μB/Ru. This was in contrast to the observed approximately 3.5 μB/Ru in the SRO film grown on STO (111) substrate . Note that we grew a very high-quality film on top of the STO (111) substrates with step-and-terrace structures.
Similarly, it has not been reported that volume change due to a small amount of Ru vacancy causing subtle change of the Ru-O-Ru bond angle can induce a significant change of spin configuration in SRO [1, 26]. The orthorhombic-to-tetragonal structural transition temperature TOT as a function of the SRO film thickness did not show a correlation with the ferromagnetic transition temperature .
Previously, the difference of RRR and Tc has been explained by oxygen vacancy, Ru vacancy, and surface difference. However, the SRO100 film and the SRO111 film have nearly the same lattice parameters and unit cell volumes because the volume difference between the two films is within the error bar of HRXRD. So, the vacancies could not explain the different RRR and Tc between the two films. Since the films are as thick as approximately 100 unit cells, which is enough to neglect surface dependence, surface effects on its physical properties must be excluded.
Figure 5b,c shows the different effects of strain on the nearest neighbor distance between the adjacent Ru ions (≡Ru nn-distance) depending on the substrate surface orientation. The lattice of the SRO100 film is simply elongated along the c-axis direction while those along the two in-plane lattices shrank. The result is that the Ru nn-distance along the c-axis becomes larger than that of the bulk SRO (3.950 Å > 3.923 Å, approximately 0.69%) and that along two in-plane axes becomes smaller (3.905 Å < 3.923 Å, approximately -0.46%) due to the coherent growth through the epitaxial strain.
If we grow SRO on top of STO (111) substrate, SRO will receive compressive strain. The deformation of SRO occurs in the following way: A Ru pseudocube of SRO consisting of eight Ru ions at each corner will transform to a rhombohedron. By using the in-plane lattice constant and out-of plane lattice constant data in Figure 2, we could get the shape of the rhombus of the rhombohedron: side length of approximately 3.920 Å and angle of approximately 89.56°. In summary, through the rhombohedral distortion, the Ru nn-distance does change very little (approximately 0.003 Å) from its bulk value of 3.923 Å by reducing the Ru-Ru-Ru angle γ from 90° to only approximately 0.44°. Another point is that the ‘Ru cube’ could hold ions larger than the Sr ion at its center since Ru is larger than Ti. (SrTiO3 is cubic. The ‘Ti cube’ has a lattice constant of 3.905 Å.) Thus, the bulk SRO structure was made by decreasing the inner hollow space of the cube by having a buckling angle and thus has an orthorhombic structure. In the SRO111 film, the Ru cube changed to a rhombohedron and its inner hollow volume is closer to the optimum value to have the Sr ion at its center which is a little bit smaller to fill the inner space of the undistorted Ru cube having a lattice constant of approximately 3.923 Åc.
When the SRO film is grown with different strain directions, there are three categories that we might consider as key parameters: (1) Ru-O distance, (2) Ru-O-Ru buckling angle, (3) Ru nn-distance. Previous reports have mainly focused on Ru-O distance and Ru-O-Ru buckling angle, which are in the scheme of the tolerance factor. However, the tolerance factor mostly covers cubic, tetragonal, and orthorhombic structures. In the SRO111 film, we could keep nearly the bulk SRO value of the Ru nn-distance more easily while the Ru nn-distance of the SRO100 film was quite reduced along the in-plane direction. The ability of keeping the Ru nn-distance closer to the bulk value seems to be one of the main factors to obtain higher RRR and Tc in the SRO111 film compared to the SRO100 film. This scenario can be generalized to other cases. The smaller lattice mismatch in SRO/STO (110) compared to SRO/STO (001) means the a smaller disturbance to the original Ru nn-distance [7, 9]. With d1-10 = 3.905 Å/√2 and d110 = 3.905 Å/√2, the Ru nn-distance and Ru-Ru-Ru angle are approximately 3.928 Å and approximately 89.34° along the rhombus side and 3.905 Å and 90° along the rectangular side of SRO (110) film, repectively [7–9]. In summary, the major change of Ru nn-distance from the pseudocubic bulk SRO value of 3.923 Å is approximately -0.018 Å for the SRO (100) film, approximately -0.006 Å and approximately -0.017 Å for the SRO (110) film, and approximately -0.003 Å for the SRO (111) film. Thus, the nearest neighbor distance between B-site ions seems to be as good as the tolerance factor in perovskite thin films and even better if the strain pushes lower symmetry like in rhombohedral structures.
We made high-quality SrRuO3 thin films on SrTiO3 (111) and SrTiO3 (001) substrates with atomically flat surfaces. The SrRuO3 thin films on SrTiO3 (111) substrate showed (1) a slightly different growth mode, (2) approximately 10 K higher ferromagnetic transition temperature, and (3) better conducting behavior with a higher relative resistivity ratio, than (100)c-oriented SrRuO3 films. The oxygen and Ru vacancies are not dominant factors for the difference because of the same unit cell volume for both films. The differences in the magnetic and electrical properties should be interpreted in terms of other factors, probably different structural deformation of the SrRuO3 unit cell. In the SRO111 film, we could nearly keep the bulk SRO value of the Ru nn-distance more easily while the Ru nn-distances of the SRO100 film and of the SRO110 film were quite changed along the in-plane direction. We propose Ru nearest neighbor distance as a new concept, for explaining strain effects in perovskite oxide thin films grown on different surfaces of cubic substrates. Finally, (111)c-oriented SrRuO3 films revealed no signatures of high-spin states of Ru.
aRecent studies on the detailed crystal structure of SRO thin films showed that the crystal structure of the film depended on the thickness, temperature, and type of in-plane strain. A thicker SRO film on a SrTiO3 (001) substrate has a very slight distortion from tetragonal to monoclinic at room temperature.
bWe found that the optimal growth conditions for the SRO111 film in terms of surface morphology were much narrower than those for the SRO100 film.
cThe ideal Ru cube should have a lattice constant larger than 3.923 Å. One may have to make Ba x Sr1-xRuO3 in cubic phase and measure its lattice constant.
The authors thank C. B. Eom, H. N. Lee, and S. S. A. Seo for the critical reading of the manuscript. This research was supported by the Basic Science Research Program through the National Research Foundation of Korea (NRF) funded by the Ministry of Education, Science and Technology (2012R1A1A2008595 and 2012R1A1A2008845) and by the National Research Foundation of Korea (NRF) grant funded by the Korea government (MEST) (NRF-2013-0031010).
- Koster G, Klein L, Siemons W, Rijnders G, Dodge JS, Eom CB, Blank DHA, Beasley MR: Structure, physical properties, and applications of SrRuO3 thin films. Rev Mod Phys 2012, 84: 253–298. 10.1103/RevModPhys.84.253View ArticleGoogle Scholar
- Auciello O, Foster CM, Ramesh R: Processing technologies for ferroelectric thin films and heterostructures. Annu Rev Mater Sci 1998, 28: 501–531. 10.1146/annurev.matsci.28.1.501View ArticleGoogle Scholar
- Chang YJ, Kim CH, Phark S-H, Kim YS, Yu J, Noh TW: Fundamental thickness limit of itinerant ferromagnetic SrRuO3 thin films. Phys Rev Lett 2009, 103: 057201.View ArticleGoogle Scholar
- Vailionis A, Siemons W, Koster G: Room temperature epitaxial stabilization of a tetragonal phase in ARuO3 (A = Ca and Sr) thin films. Appl Phys Lett 2008, 93: 051909. 10.1063/1.2967878View ArticleGoogle Scholar
- Gan Q, Rao RA, Eom CB, Garrett JL, Lee M: Direct measurement of strain effects on magnetic and electrical properties of epitaxial SrRuO3 thin films. Appl Phys Lett 1998, 72: 978–980. 10.1063/1.120603View ArticleGoogle Scholar
- Gan Q, Rao RA, Eom CB: Control of the growth and domain structure of epitaxial SrRuO3 thin films by vicinal (001) SrTiO3 substrates. Appl Phys Lett 1997, 70: 1962–1964. 10.1063/1.118792View ArticleGoogle Scholar
- Jung CU, Yamada H, Kawasaki M, Tokura Y: Magnetic anisotropy control of SrRuO3 films by tunable epitaxial strain. Appl Phys Lett 2004, 84: 2590–2592. 10.1063/1.1695195View ArticleGoogle Scholar
- Lee BW, Jung CU: Modification of magnetic properties through the control of growth orientation and epitaxial strain in SrRuO3 thin films. Appl Phys Lett 2010, 96: 102507. 10.1063/1.3334727View ArticleGoogle Scholar
- Lee BW, Jung CU: Coherent growth behavior of an orthorhombic (Ca, Sr)SnO3 thin films on a cubic SrTiO3 (110) substrate. J Korean Phys Soc 2012, 61: 795–798. 10.3938/jkps.61.795View ArticleGoogle Scholar
- Tokura Y, Tomioka Y: Colossal magnetoresistive manganites. J Magn Magn Mater 1999, 200: 1. 10.1016/S0304-8853(99)00352-2View ArticleGoogle Scholar
- Salamon MB, Jaime M: The physics of manganites: structure and transport. Rev Mod Phys 2001, 73: 583. 10.1103/RevModPhys.73.583View ArticleGoogle Scholar
- Imada M, Fujimori A, Tokura Y: Metal-insulator transition. Rev Mod Phys 1998, 70: 1039. 10.1103/RevModPhys.70.1039View ArticleGoogle Scholar
- Kim DH, Aimon NM, Bi L, Florez JM, Dionne GF, Ross CA: Magnetostriction in epitaxial SrTi1-xFe x O3-δ perovskite films with x = 0.13 and 0.35. J Phys Condens Matter 2013, 25: 026002. 10.1088/0953-8984/25/2/026002View ArticleGoogle Scholar
- Lee BW, Jung CU, Kawasaki M, Tokura Y: Tuning of magnetism in SrRuO3 thin films on SrTiO3 (001) substrate by control of the twin and strain amount in the buffer layer. J Appl Phys 2008, 104: 103909. 10.1063/1.3028277View ArticleGoogle Scholar
- Kim NG, Kumar N, Park YA, Hur N, Jung CU, Jung JH: Application of magnetic fields for a low temperature growth of high-quality SrRuO3 thin films. J Phys D Appl Phys 2008, 41: 125005. 10.1088/0022-3727/41/12/125005View ArticleGoogle Scholar
- Sekigughi S, Fujimoto M, Nomura M, Cho S-B, Tanaka J, Nishihara T, Kang M-G, Park H-H: Atomic force microscopy observation of SrTiO3 polar surface. Solid State Ion 1998, 108: 73–79. 10.1016/S0167-2738(98)00021-6View ArticleGoogle Scholar
- Chang J, Park Y-S, Kim S-K: Atomically flat single-terminated SrTiO3 (111) surface. Appl Phys Lett 2008, 92: 152910. 10.1063/1.2913005View ArticleGoogle Scholar
- Biswas A, Rossen PB, Yang C-H, Siemons W, Jung M-H, Yang IK, Ramesh R, Jeong YH: Universal Ti-rich termination of atomically flat SrTiO3 (001), (110), (111) surfaces. Appl Phys Lett 2011, 98: 051904. 10.1063/1.3549860View ArticleGoogle Scholar
- Connell JG, Isaac BJ, Ekanayake GB, Strachan DR, Seo SSA: Preparation of atomically flat SrTiO3 surfaces using a deionized-water leaching and thermal annealing procedure. Appl Phys Lett 2012, 101: 251607. 10.1063/1.4773052View ArticleGoogle Scholar
- Vailionis A, Siemons W, Koster G: Strained-induced single-domain growth of epitaxial SrRuO3 layers on SrTiO3: a high-temperature X-ray diffraction study. Appl Phys Lett 2007, 91: 071907. 10.1063/1.2771087View ArticleGoogle Scholar
- Choi KJ, Baek SH, Jang HW, Belenky LJ, Lyubchenko M, Eom C-B: Phase-transition temperature of strained single-crystal SrRuO3 thin films. Adv Mater 2010, 22: 759–762. 10.1002/adma.200902355View ArticleGoogle Scholar
- Grutter A, Wong F, Arenholz E, Liberati M, Vailionis A, Suzuki Y: Enhanced magnetism in epitaxial SrRuO3 thin films. Appl Phys Lett 2010, 96: 082509. 10.1063/1.3327512View ArticleGoogle Scholar
- Hong W, Lee HN, Yoon M, Christen HM, Lowndes DH, Suo Z, Zhang Z: Persistent step-flow growth of strained films on vicinal substrates. Phys Rev Lett 2005, 95: 095501.View ArticleGoogle Scholar
- Yoon M, Lee HN, Hong W, Christen HM, Zhang Z, Suo Z: Dynamic of step bunching in heteroepitaxial growth on vicinal substrates. Phys Rev Lett 2007, 99: 055503.View ArticleGoogle Scholar
- Lopez de la Torre MA, Sefroui Z, Arias D, Varela M, Villegas JE, Ballesteros C, Leon C, Santamaria J: Electron–electron interaction and weak localization effects in badly metallic SrRuO3. Phys Rev B 2001, 63: 052403.View ArticleGoogle Scholar
- Mathieu R, Jung CU, Yamada H, Asamitsu A, Kawasaki M, Tokura Y: Determination of the intrinsic anomalous Hall effect of SrRuO3. Phys Rev B 2005, 72: 064436.View ArticleGoogle Scholar
- Siemons W, Koster G, Vailionis A, Yamamoto H, Blank DHA, Beasley MR: Dependence of the electronic structure of SrRuO3 and its degree of correlation on cation off-stoichiometry. Phys Rev B 2007, 76: 075126.View ArticleGoogle Scholar
- Lee J-H, Murugavel P, Ryu H, Lee D, Jo JY, Kim JW, Kim HJ, Kim KH, Jo Y, Jung M-H, Oh YH, Kim Y-W, Yoon J-G, Chung J-S, Noh TW: Epitaxial stabilization of a new multiferroic hexagonal phase of TbMnO3 thin films. Adv Mater 2006, 18: 3125–3129. 10.1002/adma.200601621View ArticleGoogle Scholar
- Lee J-H, Murugavel P, Lee D, Noh TW, Jo Y, Jung M-H, Jang KH, Park J-G: Multiferroic properties of epitaxially stabilized hexagonal DyMnO3 thin films. Appl Phys Lett 2007, 90: 012903. 10.1063/1.2429021View ArticleGoogle Scholar
- Lee D, Lee J-H, Murugavel P, Jang SY, Noh TW, Jo Y, Jung M-H, Ko Y-D, Chung J-S: Epitaxial stabilization of artificial hexagonal GdMnO3 thin films and their magnetic properties. Appl Phys Lett 2007, 90: 182504. 10.1063/1.2735546View ArticleGoogle Scholar
- Chang SH, Chang YJ, Jang SY, Jeong DW, Jung CU, Kim Y-J, Chung J-S, Noh TW: Thickness-dependent structural phase transition of strained SrRuO3 ultrathin films: the role of octahedral tilt. Phys Rev B 2011, 84: 104101.View ArticleGoogle Scholar
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