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Journal articles on the topic 'Canted antiferromagnetic state'

Author: Grafiati

Published: 4 June 2021

Last updated: 8 February 2022

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1

Nagai, I., Y. Yoshida, S. I. Ikeda, H. Matsuhata, H. Kito, and M. Kosaka. "Canted antiferromagnetic ground state in Sr3Ir2O7." Journal of Physics: Condensed Matter 19, no. 13 (2007): 136214. http://dx.doi.org/10.1088/0953-8984/19/13/136214.

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2

Nagaev, E. L. "Underdoped manganites: Canted antiferromagnetic ordering or two-phase ferro-antiferromagnetic state?" Journal of Experimental and Theoretical Physics 87, no. 6 (1998): 1214–20. http://dx.doi.org/10.1134/1.558615.

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3

Dean, Philip, Yuji Muro, Toshiro Takabatake, and Peter D. Hatton. "A Spin-Canted Antiferromagnetic Ground State in CeRu2Al10." Journal of the Physical Society of Japan 87, no. 1 (2018): 013706. http://dx.doi.org/10.7566/jpsj.87.013706.

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4

Danilovich, Igor L., Anna V. Merkulova, Igor V. Morozov, et al. "Strongly canted antiferromagnetic ground state in Cu3(OH)2F4." Journal of Alloys and Compounds 776 (March 2019): 16–21. http://dx.doi.org/10.1016/j.jallcom.2018.10.032.

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5

Sonomura, Hirosuke, Tomoyuki Terai, Tomoyuki Kakeshita, et al. "Neutron Diffraction Study on Magnetic Structure in Layered Manganite La_2-2xSr_1+2xMn₂O₇ (x=0.307)." Solid State Phenomena 172-174 (June 2011): 1301–6. http://dx.doi.org/10.4028/www.scientific.net/ssp.172-174.1301.

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Magnetic structure in a layered perovskite manganite, La2-2xSr1+2xMn2O7 (x = 0.307) has been investigated by neutron diffraction measurements. We found that the ground state (at 4 K) has a ferromagnetic structure with magnetic moment of Mn ions being aligned in a direction inclined by 10 degree from the c-axis. The magnetic structure changes to a canted antiferromagnetic one (CAFM-I) at about 20 K and then to another canted antiferromagnetic one (CAFM-II) at about 80 K. Here the magnetic moment lies in the ab-plane in CAFM-II but not in CAFM-I. The magnetic structure then changes to an antifer

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6

Yakubovich, Olga, Galina Kiriukhina, Larisa Shvanskaya, et al. "Canted antiferromagnet superimposed on a buckled kagomé network in RbMn4(PO4)3." Acta Crystallographica Section C Structural Chemistry 74, no. 5 (2018): 641–49. http://dx.doi.org/10.1107/s2053229618006034.

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Rubidium tetramanganese tris(phosphate), RbMn4(PO4)3, has been synthesized as single crystals under hydrothermal conditions. The crystal structure was refined in the space groupPnnm(D2h12). It is argued that the size factorRM/RA,i.e.the ratio of theA+ionic radius to theM2+ionic radius, within the morphotropic seriesAM4(TO4)3corresponds to a specific type of crystal structure. At low temperatures, the antiferromagnet superimposed on a buckled kagomé network in RbMn4(PO4)3experiences a transition into a long-range ordered state with finite spontaneous magnetization. First principles calculations

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7

Umeo, K., H. Yamane, H. Kubo, Y. Muro, and T. Takabatake. "Pressure-induced transition from a canted antiferromagnetic state to a ferromagnetic state in YbRhSb." Journal of Physics: Conference Series 200, no. 1 (2010): 012215. http://dx.doi.org/10.1088/1742-6596/200/1/012215.

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8

Jiang, Jie. "Magnetic Transition and Spin Correlation in Mn Oxides at Low Temperatures." Australian Journal of Physics 51, no. 1 (1998): 131. http://dx.doi.org/10.1071/p96108.

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We study the magnetic transition and spin correlation in Mn oxides at low temperatures. The results indicate that there are antiferromagnetic (AF), spiral (SP), ferromagnetic (FM) and canted (CN) states when T → 0. With temperature increasing, a paramagnetic (PM) state appears. The spin–spin correlation function is also obtained.

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9

Fukuda, Akira, Shinsuke Kozumi, Daiju Terasawa, et al. "Quantum transport study of canted antiferromagnetic phase in the bilayer quantum Hall state." Physica E: Low-dimensional Systems and Nanostructures 34, no. 1-2 (2006): 77–80. http://dx.doi.org/10.1016/j.physe.2006.06.001.

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10

Li, Tian, Jun Peng Liao та Ying Feng Wang. "Solvothermal synthesis and magnetic properties of β-Co2P nanorods". Materials Science-Poland 33, № 2 (2015): 312–16. http://dx.doi.org/10.1515/msp-2015-0049.

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AbstractHexagonal high temperature phase β-Co2P nanorods with a diameter of around 50 nm were synthesized via a mild solvothermal route. The reaction was carried out at 180 °C using cobalt chloride hexahydrate (CoCl2 · 6H2O) as Co source and yellow phosphorous as P source. The composition, structure as well as morphology were characterized by X-ray diffraction (XRD), X-ray photoemission spectroscopy (XPS) and transmission electron microscopy (TEM). The magnetic susceptibility curve indicates that the β-Co2P nanorods show canted antiferromagnetic state, different from the paramagnetic state of

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11

Fanucci, Gail E., J. Krzystek, Mark W. Meisel, Louis-Claude Brunel, and Daniel R. Talham. "Antiferromagnetic Resonance as a Tool for Investigating Magnetostructural Correlations: The Canted Antiferromagnetic State of KMnPO4·H2O and a Series of Manganese Phosphonates." Journal of the American Chemical Society 120, no. 22 (1998): 5469–79. http://dx.doi.org/10.1021/ja974247g.

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12

FANUCCI, G. E., J. KRZYSTEK, M. W. MEISEL, L. C. BRUNEL, and D. R. TALHAM. "ChemInform Abstract: Antiferromagnetic Resonance as a Tool for Investigating Magnetostructural Correlations: The Canted Antiferromagnetic State of KMnPO4×H2O and a Series of Manganese Phosphonates." ChemInform 29, no. 34 (2010): no. http://dx.doi.org/10.1002/chin.199834004.

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13

Fukuda, Akira, Shinsuke Kozumi, Daiju Terasawa та ін. "Erratum to: “Quantum transport study of canted antiferromagnetic phase in the ν=2 bilayer quantum Hall state”". Physica E: Low-dimensional Systems and Nanostructures 39, № 2 (2007): 277. http://dx.doi.org/10.1016/j.physe.2006.12.004.

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14

Sun, Xiao Liang, Jing Shi, Guang Ma, and Jin Li. "Preparation and Ferroelectromagnetic Characteristics of Bi₂SrNdNb₂FeO₁₂ Ceramic." Advanced Materials Research 295-297 (July 2011): 126–30. http://dx.doi.org/10.4028/www.scientific.net/amr.295-297.126.

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The solid solutions of NdFeO3-Bi2SrNb2O9 (1:1ratio) of the Aurivillius-type compounds was prepared by solid-state reaction. The room structural data were obtained from X-ray diffraction (XRD) and confirmed a Three-layered Aurivillius phase. The dielectric measurement showed no anomalies due to the high conductivity of these samples at elevated temperature. From the magnetic measurement the compounds were found to be of canted antiferromagnetic at room temperature. It is revealed that the formation of Fe2+ can be suppressed by the pre-oxidation of Fe2O3，This result may have implications for fur

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15

DaSilva, Jack G., Rodolphe Clérac, and Joel S. Miller. "Pressure Induced Crossover between a Ferromagnetic and a Canted Antiferromagnetic State for [Bis(pentamethylcyclopentadienyl)-iron(III)][Tetracyanoethenide], [FeCp2*][TCNE]." Inorganic Chemistry 52, no. 19 (2013): 11677–83. http://dx.doi.org/10.1021/ic4021959.

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16

BALAMURUGAN, S. "HIGH-PRESSURE SYNTHESIS AND PHYSICAL PROPERTIES OF NbSr2(Dy1.5Ce0.5)Cu2O10." Modern Physics Letters B 23, no. 07 (2009): 903–10. http://dx.doi.org/10.1142/s0217984909019132.

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In the present study, we have successfully synthesized and structurally characterized a new 1222-type Dy -based niobio-cuprate for the first time with the chemical formula, NbSr 2( Dy 1.5 Ce 0.5) Cu 2 O 10 by high-pressure and elevated temperature technique under different synthesis conditions. A good quality polycrystalline ceramic sample was prepared at 1723 K and 6 GPa for 2 h. The title compound crystallizes in a tetragonal symmetry of space group I4/mmm with lattice parameters a = b = 3.864(5) Åand c = 28.68(4) Å. The temperature dependence of (low field) magnetic susceptibilities reveals

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17

Nair, Sunil, and A. K. Nigam. "A re-entrant canted antiferromagnetic state in the Mn site substituted manganite La 0.46 Sr 0.54 Mn 0.98 Cr 0.02 O 3." EPL (Europhysics Letters) 84, no. 3 (2008): 37008. http://dx.doi.org/10.1209/0295-5075/84/37008.

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18

Šenjug, Pavla, Jure Dragović, Filip Torić, et al. "Magnetoelectric Multiferroicity and Magnetic Anisotropy in Guanidinium Copper(II) Formate Crystal." Materials 14, no. 7 (2021): 1730. http://dx.doi.org/10.3390/ma14071730.

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Hybrid metal-organic compounds as relatively new and prosperous magnetoelectric multiferroics provide opportunities to improve the polarization, magnetization and magneto-electric coupling at the same time, which usually have some limitations in the common type-I and type-II multiferroics. In this work we investigate the crystal of guanidinium copper (II) formate [C(NH2)3]Cu(HCOO)3 and give novel insights concerning the structure, magnetic, electric and magneto-electric behaviour of this interesting material. Detailed analysis of crystal structure at 100 K is given. Magnetization points to the

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19

Manipatruni, Sasikanth, Dmitri E. Nikonov, Chia-Ching Lin, et al. "Voltage control of unidirectional anisotropy in ferromagnet-multiferroic system." Science Advances 4, no. 11 (2018): eaat4229. http://dx.doi.org/10.1126/sciadv.aat4229.

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Demonstration of ultralow energy switching mechanisms is imperative for continued improvements in computing devices. Ferroelectric (FE) and multiferroic (MF) order and their manipulation promise an ideal combination of state variables to reach attojoule range for logic and memory (i.e., ~30× lower switching energy than nanoelectronics). In BiFeO3(BFO), the coupling between the antiferromagnetic (AFM) and FE order is robust at room temperature, scalable in voltage, stabilized by the FE order, and can be integrated into a fabrication process for a beyond-CMOS (complementary metal-oxide semicondu

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20

Liu, Peitao, and Cesare Franchini. "Advanced First-Principle Modeling of Relativistic Ruddlesden—Popper Strontium Iridates." Applied Sciences 11, no. 6 (2021): 2527. http://dx.doi.org/10.3390/app11062527.

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In this review, we provide a survey of the application of advanced first-principle methods on the theoretical modeling and understanding of novel electronic, optical, and magnetic properties of the spin-orbit coupled Ruddlesden–Popper series of iridates Srn+1IrnO3n+1 (n = 1, 2, and ∞). After a brief description of the basic aspects of the adopted methods (noncollinear local spin density approximation plus an on-site Coulomb interaction (LSDA+U), constrained random phase approximation (cRPA), GW, and Bethe–Salpeter equation (BSE)), we present and discuss select results. We show that a detailed

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21

HIRAYAMA, YOSHIRO. "NUCLEAR-SPIN-BASED MEASUREMENTS OF QUANTUM HALL SYSTEMS." International Journal of Modern Physics B 23, no. 12n13 (2009): 2737–38. http://dx.doi.org/10.1142/s0217979209062281.

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Nuclear magnetic resonance (NMR) is widely used in the physical, chemical, and biological sciences. However, conventional NMR techniques based on induction-detection have drawbacks of low-sensitivity and the need of a relatively large sample. It is not suitable to investigate single or double layers (or their nanostructure), which is essential in studying quantum Hall (QH) effects. In this presentation, I discussed a resistively-detected technique to overcome the low-sensitivity limitation of conventional NMR and its application to QH systems. Resistively-detected nuclear-spin-based measuremen

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22

Yuan, Wei, Qiong Zhu, Tang Su, et al. "Experimental signatures of spin superfluid ground state in canted antiferromagnet Cr2O3via nonlocal spin transport." Science Advances 4, no. 4 (2018): eaat1098. http://dx.doi.org/10.1126/sciadv.aat1098.

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23

Śliwa, Ewelina I., Urszula Śliwińska-Hill, Barbara Bażanów, Miłosz Siczek, Julia Kłak, and Piotr Smoleński. "Synthesis, Structural, and Cytotoxic Properties of New Water-Soluble Copper(II) Complexes Based on 2,9-Dimethyl-1,10-Phenanthroline and Their One Derivative Containing 1,3,5-Triaza-7-Phosphaadamantane-7-Oxide." Molecules 25, no. 3 (2020): 741. http://dx.doi.org/10.3390/molecules25030741.

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A series of water-soluble copper(II) complexes based on 2,9-dimethyl-1,10-phenanthroline (dmphen) and mixed-ligands, containing PTA=O (1,3,5-triaza-7-phosphaadamantane-7-oxide) have been synthesized and fully characterized. Two types of complexes have been obtained, monocationic [Cu(NO3)(O-PTA=O)(dmphen)][PF6] (1), [Cu(Cl)(dmphen)2][PF6] (2), and neutral [Cu(NO3)2(dmphen)] (3). The solid-state structures of all complexes have been determined by single-crystal X-ray diffraction. Magnetic studies for the complex 1–3 indicated a very weak antiferromagnetic interaction between copper(II) ions in c

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24

Rõõm, T., J. Viirok, L. Peedu, et al. "Magnetoelastic distortion of multiferroic BiFeO3 in the canted antiferromagnetic state." Physical Review B 102, no. 21 (2020). http://dx.doi.org/10.1103/physrevb.102.214410.

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25

Kharitonov, Maxim. "Canted Antiferromagnetic Phase of theν=0Quantum Hall State in Bilayer Graphene". Physical Review Letters 109, № 4 (2012). http://dx.doi.org/10.1103/physrevlett.109.046803.

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26

Fukuda, A., A. Sawada, S. Kozumi та ін. "Magnetotransport study of the canted antiferromagnetic phase in bilayerν=2quantum Hall state". Physical Review B 73, № 16 (2006). http://dx.doi.org/10.1103/physrevb.73.165304.

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27

Jani, Hariom, Jiajun Linghu, Sonu Hooda та ін. "Reversible hydrogen control of antiferromagnetic anisotropy in α-Fe2O3". Nature Communications 12, № 1 (2021). http://dx.doi.org/10.1038/s41467-021-21807-y.

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AbstractAntiferromagnetic insulators are a ubiquitous class of magnetic materials, holding the promise of low-dissipation spin-based computing devices that can display ultra-fast switching and are robust against stray fields. However, their imperviousness to magnetic fields also makes them difficult to control in a reversible and scalable manner. Here we demonstrate a novel proof-of-principle ionic approach to control the spin reorientation (Morin) transition reversibly in the common antiferromagnetic insulator α-Fe2O3 (haematite) – now an emerging spintronic material that hosts topological an

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28

Kharitonov, Maxim. "Edge excitations of the canted antiferromagnetic phase of theν=0quantum Hall state in graphene: A simplified analysis". Physical Review B 86, № 7 (2012). http://dx.doi.org/10.1103/physrevb.86.075450.

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29

Bijelić, Jelena, Dalibor Tatar, Manisha Sahu, Zvonko Jagličić, and Igor Djerdj. "Size reduction-induced properties modifications of antiferromagnetic dielectric nanocrystalline Ba2NiMO6 (M = W, Te) double perovskites." Oxford Open Materials Science 1, no. 1 (2020). http://dx.doi.org/10.1093/oxfmat/itaa003.

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Abstract The main objective of this work was to synthesize phase pure double perovskites Ba2NiTeO6 (BNTO) and Ba2NiWO6 (BNWO) in nanocrystalline form and to reveal the impact of nanocrystallinity on their magnetic and dielectric properties. The studied double perovskites were synthesized in nanocrystalline form by employing a citrate sol-gel route. A detailed investigation of their structure and properties using X-ray powder diffraction, scanning electron microscopy, Raman spectroscopy technique, energy-dispersive X-ray spectroscopy, SQUID magnetometry and electrical measurements is carefully

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30

Zhu, Tong, Fabio Orlandi, Pascal Manuel, et al. "Directed synthesis of a hybrid improper magnetoelectric multiferroic material." Nature Communications 12, no. 1 (2021). http://dx.doi.org/10.1038/s41467-021-25098-1.

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AbstractPreparing materials which simultaneously exhibit spontaneous magnetic and electrical polarisations is challenging as the electronic features which are typically used to stabilise each of these two polarisations in materials are contradictory. Here we show that by performing low-temperature cation-exchange reactions on a hybrid improper ferroelectric material, Li2SrTa2O7, which adopts a polar structure due to a cooperative tilting of its constituent TaO6 octahedra rather than an electronically driven atom displacement, a paramagnetic polar phase, MnSrTa2O7, can be prepared. On cooling b

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31

Metoki, Naoto. "Neutron Scattering Study on UTGa5 and NpTGa5." MRS Proceedings 986 (2006). http://dx.doi.org/10.1557/proc-986-0986-oo02-04.

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AbstractThe results of our recent neutron scattering studies on actinide ‘115’ compounds are reviewed. The itinerant many-body f-electron system and cross over to the localized character are realized only in actinide system. Actinide ‘115’ family is very interesting, because we can grow high quality single crystals of many iso-structural compounds with different number and character of f electrons and valence d electrons. Variety of the ground state have been reported, e.g. paramagnetic, itinerant magnetism, and heavy fermion superconductivity in PuCoGa5. Very recently we have intensively stud

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32

Tiwari, Jeetendra Kumar, Birendra Kumar, Harish Chandr Chauhan, and Subhasis Ghosh. "Magnetism in quasi-two-dimensional tri-layer La2.1Sr1.9Mn3O10 manganite." Scientific Reports 11, no. 1 (2021). http://dx.doi.org/10.1038/s41598-021-93290-w.

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AbstractThe tri-layer La$$_{3-3x}$$ 3 - 3 x Sr$$_{1+3x}$$ 1 + 3 x Mn$$_{3}$$ 3 O$$_{10}$$ 10 manganites of Ruddlesden–Popper (RP) series are naturally arranged layered structure with alternate stacking of ω-MnO$$_2$$ 2 (ω = 3) planes and rock-salt type block layers (La, Sr)$$_2$$ 2 O$$_2$$ 2 along c-axis. The dimensionality of the RP series manganites depends on the number of perovskite layers and significantly affects the magnetic and transport properties of the system. Generally, when a ferromagnetic material undergoes a magnetic phase transition from ferromagnetic to paramagnetic state, the

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33

Kiryukhin, V., D. Casa, B. Keimer, et al. "X-Ray Induced Insulator-Metal Transitions in CMR Manganites." MRS Proceedings 494 (1997). http://dx.doi.org/10.1557/proc-494-65.

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ABSTRACTIn this work we report a study of the photoinduced insulator-to-metal transition in manganese oxide perovskites of the formula Pr1-xCaxMnO3. The transition is closely related to the magnetic field induced insulator-to-metal transition (CMR effect) observed in these materials. It is accompanied by a dramatic change in the magnetic properties and lattice structure: the material changes from an insulating charge-ordered canted antiferromagnet to a ferromagnetic metal. We present an investigation of the transport and structural properties of these materials over the course of the transitio

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