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Journal articles on the topic 'Magnetism in insulating solids'

Author: Grafiati

Published: 4 June 2021

Last updated: 7 February 2022

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1

Ohtomo, Akira, Suvankar Chakraverty, Hisanori Mashiko, Takayoshi Oshima, and Masashi Kawasaki. "Spontaneous atomic ordering and magnetism in epitaxially stabilized double-perovskites." MRS Proceedings 1454 (2012): 3–13. http://dx.doi.org/10.1557/opl.2012.923.

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ABSTRACTWe report on the atomic ordering of B-site transition-metals and magnetic properties in double-perovskite oxides, La2CrFeO6 (LCFO) and La2VMnO6 (LVMO), which have never been reported to exist in ordered forms. These double-perovskite oxides are particularly interesting because of possible ferromagnetism (expected from the Kanamori-Goodenough rule for LCFO) and half-metallic antiferromagnetism (predicted for LVMO). Using pulsed-laser deposition technique with single solid-solution targets, we have prepared epitaxial films in ordered forms. Despite similar ionic characters of constituent transition-metals in each compound, the maximum B-site order attained was surprisingly high, ∼90% for LCFO and ∼80% for LVMO, suggesting a significant role of epitaxial stabilization in the spontaneous ordering process. Magnetization and valence state characterizations revealed that the magnetic ground state of both compounds was coincidently ferrimagnetic with saturation magnetization of ∼2μBper formula unit, unlike those predicted theoretically. In addition, they were found to be insulating with optical band-gaps of 1.6 eV and 0.9 eV for LCFO and LVMO, respectively. Our results present a wide opportunity to explore novel magnetic properties of binary transition-metal perovskites upon epitaxial stabilization of the ordered phase.

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2

Wang, D. Y., L. Liu, Y. B. Liu, T. Li, Z. Ma, and H. X. Wu. "Heat insulating capacity of Sm2Zr2O7 coating added with high absorptivity solids." Ceramics International 43, no. 2 (2017): 2884–87. http://dx.doi.org/10.1016/j.ceramint.2016.11.068.

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3

Brau, A., J. P. Farges, and F. Ali-Sahraoui. "Investigation versus temperature of highly conducting compacted mixtures of insulating reactive solids." Synthetic Metals 27, no. 3-4 (1988): 71–76. http://dx.doi.org/10.1016/0379-6779(88)90126-9.

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4

MOHN, P., and K. SCHWARZ. "ITINERANT MAGNETISM IN SOLIDS." International Journal of Modern Physics B 07, no. 01n03 (1993): 579–84. http://dx.doi.org/10.1142/s0217979293001219.

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Based on the spin-density functional theory we discuss the essential mechanism of spin-split itinerant electrons which cause the formation of spin-magnetic moments in a solid. The success and the difficulties of the Stoner model of itinerant magnetism is shown for hcp Co. The FSM (fixed spin moment) method allows us to compute the total energy as a function of volume and magnetic moment, E(M, V). These energy surfaces contain the crucial information about magneto-volume instabilities and related phenomena. At finite temperatures collective phenomena such as spin fluctuations are important which can be treated with a Landau—Ginzburg formalism. Results are given for the finite temperature properties of the strongly enhanced Pauli paramagnet fcc Pd and the metamagnetic system YCo2.

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5

Can, T. V., M. A. Caporini, F. Mentink-Vigier, et al. "Overhauser effects in insulating solids." Journal of Chemical Physics 141, no. 6 (2014): 064202. http://dx.doi.org/10.1063/1.4891866.

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6

Verdaguer, Michel, and Alain N. Gleizes. "Magnetism: Molecules to Build Solids." European Journal of Inorganic Chemistry 2020, no. 9 (2020): 723–31. http://dx.doi.org/10.1002/ejic.201901274.

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7

Esquinazi, Pablo, Wolfram Hergert, Daniel Spemann, Annette Setzer, and Arthur Ernst. "Defect-Induced Magnetism in Solids." IEEE Transactions on Magnetics 49, no. 8 (2013): 4668–74. http://dx.doi.org/10.1109/tmag.2013.2255867.

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8

Varret, François, Kamel Boukheddaden, Epiphane Codjovi, and Antoine Goujon. "Molecular Switchable Solids: towards photo-controlled magnetism." Hyperfine Interactions 165, no. 1-4 (2006): 37–47. http://dx.doi.org/10.1007/s10751-006-9244-2.

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9

Esquinazi, P., W. Hergert, D. Spemann, A. Setzer, and A. Ernst. "ChemInform Abstract: Defect-induced Magnetism in Solids." ChemInform 44, no. 23 (2013): no. http://dx.doi.org/10.1002/chin.201323229.

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10

Esquinazi, Pablo, Wolfram Hergert, Daniel Spemann, Annette Setzer, and Arthur Ernst. "ChemInform Abstract: Defect-Induced Magnetism in Solids." ChemInform 45, no. 1 (2013): no. http://dx.doi.org/10.1002/chin.201401236.

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11

Can, T. V., Q. Z. Ni, and R. G. Griffin. "Mechanisms of dynamic nuclear polarization in insulating solids." Journal of Magnetic Resonance 253 (April 2015): 23–35. http://dx.doi.org/10.1016/j.jmr.2015.02.005.

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12

Ritz, Ethan T., Sabrina J. Li, and Nicole A. Benedek. "Thermal expansion in insulating solids from first principles." Journal of Applied Physics 126, no. 17 (2019): 171102. http://dx.doi.org/10.1063/1.5125779.

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13

Illas, F., J. Casanovas, M. A. García-Bach, R. Caballol, and O. Castell. "Towards anab initiodescription of magnetism in ionic solids." Physical Review Letters 71, no. 21 (1993): 3549–52. http://dx.doi.org/10.1103/physrevlett.71.3549.

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14

Illas, F., J. Casanovas, M. A. García-Bach, R. Caballol, and O. Castell. "Towards anAb InitioDescription of Magnetism in Ionic Solids." Physical Review Letters 72, no. 16 (1994): 2669. http://dx.doi.org/10.1103/physrevlett.72.2669.

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15

Demers, Hendrix, and Raynald Gauvm. "The Effect of Charging on Electron Diffusion in Solids." Microscopy and Microanalysis 7, S2 (2001): 668–69. http://dx.doi.org/10.1017/s143192760002941x.

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The studies of insulating specimen by using scanning electron microscopy (SEM) or associated microanalytical techniques such as electron probe microanalysis (EPMA), Auger electron spectroscopy (AES), etc., is limited by the charging phenomena. Different techniques have been found to minimize this problem: coating the specimen with a conductor, working at low energy [1], etc. But for a better knowledge of this effect, we have started a study of the mechanisms of charging as well as its effect on the electrons trajectories in the case of an insulating specimen. with the success, in past years, of Monte Carlo (MC) simulation of electron scattering in solid specimens [2], we have been developing a new Monte Carlo program for the simulation of the electron trajectory in insulators.With this program, we want to understand the effect of the trapping charge on a insulating specimen. The new MC will be constructed by adding a succession of refined model. in each step, the model goes deeper in the mechanisms for the charging phenomena.

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16

Chien, C. L. "Magnetism and Giant Magneto-Transport Properties in Granular Solids." Annual Review of Materials Science 25, no. 1 (1995): 129–60. http://dx.doi.org/10.1146/annurev.ms.25.080195.001021.

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17

Muraleedharan, K., J. K. Srivastava, V. R. Marathe, and R. Vijayaraghavan. "On the re-entrant magnetism in the insulating diluted spinel Co0.5Zn0.5Fe2O4." Journal of Physics C: Solid State Physics 18, no. 27 (1985): 5355–59. http://dx.doi.org/10.1088/0022-3719/18/27/021.

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18

Pylaeva, Svetlana, Konstantin L. Ivanov, Marc Baldus, Daniel Sebastiani, and Hossam Elgabarty. "Molecular Mechanism of Overhauser Dynamic Nuclear Polarization in Insulating Solids." Journal of Physical Chemistry Letters 8, no. 10 (2017): 2137–42. http://dx.doi.org/10.1021/acs.jpclett.7b00561.

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19

Albrecht, Martin, and Jun-ichi Igarashi. "Local-Orbital Based Correlatedab initioBand Structure Calculations in Insulating Solids." Journal of the Physical Society of Japan 70, no. 4 (2001): 1035–44. http://dx.doi.org/10.1143/jpsj.70.1035.

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20

Yildirim, N., S. M. Shaler, D. J. Gardner, R. Rice, and D. W. Bousfield. "Cellulose Nanofibril (CNF) Reinforced Starch Insulating Foams." MRS Proceedings 1621 (2014): 177–89. http://dx.doi.org/10.1557/opl.2014.1.

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ABSTRACTIn this study, biodegradable foams were produced using cellulose nanofibrils (CNFs) and starch (S). The availability of high volumes of CNFs at lower costs is rapidly progressing with advances in pilot-scale and commercial facilities. The foams were produced using a freeze-drying process with CNF/S water suspensions ranging from 1 to 7.5 wt. % solids content. Microscopic evaluation showed that the foams have a microcellular structure and that the foam walls are covered with CNF`s. The CNF's had diameters ranging from 30 nm to 100 nm. Pore sizes within the foam walls ranged from 20 nm to 100 nm. The materials` densities ranging from 0.012 to 0.082 g/cm3 with corresponding porosities between 93.46% and 99.10%. Thermal conductivity ranged from 0.041 to 0.054 W/m-K. The mechanical performance of the foams produced from the starch control was extremely low and the material was very friable. The addition of CNF's to starch was required to produce foams, which exhibited structural integrity. The mechanical properties of materials were positively correlated with solids content and CNF/S ratios. The mechanical and thermal properties for the foams produced in this study appear promising for applications such as insulation and packaging.

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21

Morozovska, A. N., E. A. Eliseev, M. D. Glinchuk, and R. Blinc. "Surface-induced magnetism of the solids with impurities and vacancies." Physica B: Condensed Matter 406, no. 9 (2011): 1673–88. http://dx.doi.org/10.1016/j.physb.2011.01.039.

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22

Cullen, J. "Effect of dipolar coupling on the magnetism of disordered solids." Journal of Applied Physics 61, no. 8 (1987): 4413–15. http://dx.doi.org/10.1063/1.338393.

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23

Volnianska, O., and P. Boguslawski. "Magnetism of solids resulting from spin polarization of p orbitals." Journal of Physics: Condensed Matter 22, no. 7 (2010): 073202. http://dx.doi.org/10.1088/0953-8984/22/7/073202.

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24

Lohmann, Mark, Tang Su, Ben Niu, et al. "Probing Magnetism in Insulating Cr2Ge2Te6 by Induced Anomalous Hall Effect in Pt." Nano Letters 19, no. 4 (2019): 2397–403. http://dx.doi.org/10.1021/acs.nanolett.8b05121.

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25

Choi, Taeyoung, and Jay A. Gupta. "Building blocks for studies of nanoscale magnetism: adsorbates on ultrathin insulating Cu2N." Journal of Physics: Condensed Matter 26, no. 39 (2014): 394009. http://dx.doi.org/10.1088/0953-8984/26/39/394009.

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26

BASKARAN, G. "High temperature superconductivity from magnetism - The Resonating Valence Bond State." International Journal of Modern Physics B 01, no. 03n04 (1987): 697–719. http://dx.doi.org/10.1142/s0217979287001080.

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In this talk the Resonating Valence Bond (RVB) state of the Mott- Hubbard insulator and the high temperature superconductivity resulting from doping are described as the possible mechanisms for the insulating and high temperature superconducting properties of undoped and doped La2CuO4 and other high Tc oxides. We describe in detail two microscopic approaches to the understanding of the RVB superconductivity- one is a simple mean field theory and the other is a gauge theory.

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27

Farges, J. P., A. Brau, and F. ALI Sahraoui. "Conducting Organic Composites of Two Insulating Reactive Solids: A Thermopower Study." Molecular Crystals and Liquid Crystals Incorporating Nonlinear Optics 186, no. 1 (1990): 143–49. http://dx.doi.org/10.1080/00268949008037204.

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28

Malyshkin, Vladislav, and Arthur R. McGurn. "Computer-simulation study of the thermal conductivity of amorphous insulating solids." Physical Review B 54, no. 5 (1996): 2980–83. http://dx.doi.org/10.1103/physrevb.54.2980.

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29

Pylaeva, Svetlana, Patrick Marx, Gurjot Singh, Thomas D. Kühne, Michael Roemelt, and Hossam Elgabarty. "Organic Mixed-Valence Compounds and the Overhauser Effect in Insulating Solids." Journal of Physical Chemistry A 125, no. 3 (2021): 867–74. http://dx.doi.org/10.1021/acs.jpca.0c11296.

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30

CHIEN, C. L. "ChemInform Abstract: Magnetism and Giant Magneto-Transport Properties in Granular Solids." ChemInform 27, no. 2 (2010): no. http://dx.doi.org/10.1002/chin.199602335.

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31

Solovyev, I. V., A. I. Liechtenstein, and K. Terakura. "Is Hund's Second Rule Responsible for the Orbital Magnetism in Solids?" Physical Review Letters 80, no. 26 (1998): 5758–61. http://dx.doi.org/10.1103/physrevlett.80.5758.

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32

Mahanti, S. D., T. A. Kaplan, Hyunju Chang, and J. F. Harrison. "Magnetism in the insulating parents of the high‐Tcsuperconductors: Well or ill understood?" Journal of Applied Physics 73, no. 10 (1993): 6105–7. http://dx.doi.org/10.1063/1.352715.

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33

Avci, Can Onur, Ethan Rosenberg, Lucas Caretta, et al. "Interface-driven chiral magnetism and current-driven domain walls in insulating magnetic garnets." Nature Nanotechnology 14, no. 6 (2019): 561–66. http://dx.doi.org/10.1038/s41565-019-0421-2.

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34

Kalnin, Yu H., and P. Zapol. "Effective diffusion coefficient and diffusion-controlled reactions in insulating solids with defects." Radiation Effects and Defects in Solids 137, no. 1-4 (1995): 295–97. http://dx.doi.org/10.1080/10420159508222738.

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35

Cross, L. Eric. "Flexoelectric effects: Charge separation in insulating solids subjected to elastic strain gradients." Journal of Materials Science 41, no. 1 (2006): 53–63. http://dx.doi.org/10.1007/s10853-005-5916-6.

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36

Shukla, Rishabh, Anil Jain, M. Miryala, et al. "Spin Dynamics and Unconventional Magnetism in Insulating La(1–2x)Sr2xCo(1–x)NbxO3." Journal of Physical Chemistry C 123, no. 36 (2019): 22457–69. http://dx.doi.org/10.1021/acs.jpcc.9b05423.

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37

Chang, Po-Chun, Venkata Ramana Mudinepalli, Shi-Yu Liu, et al. "Interfacial exchange coupling-modulated magnetism in the insulating heterostructure of CoO /yttrium iron garnet." Journal of Alloys and Compounds 875 (September 2021): 159948. http://dx.doi.org/10.1016/j.jallcom.2021.159948.

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38

Volnianska, O., and P. Boguslawski. "ChemInform Abstract: Magnetism of Solids Resulting from Spin Polarization of P Orbitals." ChemInform 41, no. 40 (2010): no. http://dx.doi.org/10.1002/chin.201040230.

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39

Sch�tz, G., and P. Fischer. "Circularly polarized X-rays probing nuclear magnetic moments and magnetism of solids." Zeitschrift f�r Physik A Hadrons and Nuclei 341, no. 2 (1992): 227–34. http://dx.doi.org/10.1007/bf01298485.

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40

Albrecht, Martin. "Local-orbital-based correlated ab initio band structure calculations in insulating solids: LiF." Theoretical Chemistry Accounts: Theory, Computation, and Modeling (Theoretica Chimica Acta) 107, no. 2 (2002): 71–79. http://dx.doi.org/10.1007/s00214-001-0305-y.

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41

Bedell, Kevin S., Isaac F. Silvera, and Neil S. Sullivan. "Spin-Polarized Quantum Fluids and Solids." MRS Bulletin 18, no. 8 (1993): 38–43. http://dx.doi.org/10.1557/s0883769400037751.

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The spin-polarized phases of the quantum fluids and solids, liquid 3He, solid 3He, and spin-aligned hydrogen have generated considerable excitement over the past fifteen years. The introduction of high magnetic fields (B ∼ 10–30 T) in conjunction with low temperatures (T ≲ 100 mK) has given rise to opportunities for exploring some of the new phases predicted for these materials. There is a broad range of physical phenomena that can be accessed in this regime of parameter space—unconventional superfluidity, unusual magnetic ordering, Bose-Einstein condensation and Kosterlitz-Thouless transitions, to name a few. This is most surprising since this plethora of complicated states of matter are present in some of the most uncomplicated materials. The rich variety of phases found in these materials are all examples of collective phenomena of quantum many-body systems, and they serve as prototypes for developing an understanding of magnetism and order/disorder processes in other systems, and for the design and characterization of new materials.

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42

Thapliyal, Prakash C., and Kirti Singh. "Aerogels as Promising Thermal Insulating Materials: An Overview." Journal of Materials 2014 (April 27, 2014): 1–10. http://dx.doi.org/10.1155/2014/127049.

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Aerogels are solids with high porosity (<100 nm) and hence possess extremely low density (∼0.003 g/cm3) and very low conductivity (∼10 mW/mK). In recent years, aerogels have attracted more and more attention due to their surprising properties and their existing and potential applications in wide range of technological areas. An overview of aerogels and their applications as the building envelope components and respective improvements from an energy efficiency perspective including performance is given here. This overview covers thermal insulation properties of aerogels and studies regarding structural features which will be helpful in buildings envelope. The improvements of thermal insulation systems have future prospects of large savings in primary energy consumption. It can be concluded that aerogels have great potential in a wide range of applications as energy efficient insulation, windows, acoustics, and so forth.

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43

Klein, D. R., D. MacNeill, J. L. Lado, et al. "Probing magnetism in 2D van der Waals crystalline insulators via electron tunneling." Science 360, no. 6394 (2018): 1218–22. http://dx.doi.org/10.1126/science.aar3617.

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Magnetic insulators are a key resource for next-generation spintronic and topological devices. The family of layered metal halides promises varied magnetic states, including ultrathin insulating multiferroics, spin liquids, and ferromagnets, but device-oriented characterization methods are needed to unlock their potential. Here, we report tunneling through the layered magnetic insulator CrI3 as a function of temperature and applied magnetic field. We electrically detect the magnetic ground state and interlayer coupling and observe a field-induced metamagnetic transition. The metamagnetic transition results in magnetoresistances of 95, 300, and 550% for bilayer, trilayer, and tetralayer CrI3 barriers, respectively. We further measure inelastic tunneling spectra for our junctions, unveiling a rich spectrum consistent with collective magnetic excitations (magnons) in CrI3.

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44

Zeng, Hui, Meng Wu, Hui-Qiong Wang, Jin-Cheng Zheng, and Junyong Kang. "Tuning the Magnetism in Boron-Doped Strontium Titanate." Materials 13, no. 24 (2020): 5686. http://dx.doi.org/10.3390/ma13245686.

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The magnetic and electronic properties of boron-doped SrTiO3 have been studied by first-principles calculations. We found that the magnetic ground states of B-doped SrTiO3 strongly depended on the dopant-dopant separation distance. As the dopant–dopant distance varied, the magnetic ground states of B-doped SrTiO3 can have nonmagnetic, ferromagnetic or antiferromagnetic alignment. The structure with the smallest dopant-dopant separation exhibited the lowest total energy among all configurations considered and was characterized by dimer pairs due to strong attraction. Ferromagnetic coupling was observed to be stronger when the two adjacent B atoms aligned linearly along the B-Ti-B axis, which could be associated with their local bonding structures. Therefore, the symmetry of the local structure made an important contribution to the generation of a magnetic moment. Our study also demonstrated that the O-Ti-O unit was easier than the Ti-B-Ti unit to deform. The electronic properties of boron-doped SrTiO3 tended to show semiconducting or insulating features when the dopant–dopant distance was less than 5 Å, which changed to metallic properties when the dopant–dopant distance was beyond 5 Å. Our calculated results indicated that it is possible to manipulate the magnetism and band gap via different dopant–dopant separations.

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45

Bennemann, K. H. "Ultra-fast dynamics in solids: non-equilibrium behaviour of magnetism and atomic structure." Annalen der Physik 18, no. 7-8 (2009): 480–560. http://dx.doi.org/10.1002/andp.200810354.

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46

Kimel, Alexey V., Andrei Kirilyuk, Fredrik Hansteen, Roman V. Pisarev, and Theo Rasing. "Nonthermal optical control of magnetism and ultrafast laser-induced spin dynamics in solids." Journal of Physics: Condensed Matter 19, no. 4 (2007): 043201. http://dx.doi.org/10.1088/0953-8984/19/4/043201.

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47

DENG, S., A. SIMON, and J. KÖHLER. "NORMAL STATE CHARACTERISTICS OF SUPERCONDUCTORS." International Journal of Modern Physics B 21, no. 18n19 (2007): 3082–85. http://dx.doi.org/10.1142/s0217979207043956.

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The normal states of simple elemental metal and complex compound superconductors have been studied by using first principle methods and model analysis. The flat/steep band electronic structure and the peak-like structure of electron-phonon coupling have been found as two universal characteristics. A new Hamiltonian is proposed to describe the electronic structure of insulating solids.

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48

Djurišić, Aleksandra B., and E. Herbert Li. "Modeling the index of refraction of insulating solids with a modified lorentz oscillator model." Applied Optics 37, no. 22 (1998): 5291. http://dx.doi.org/10.1364/ao.37.005291.

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49

Rogulis, U., and E. Kotomin. "Non-steady-state tunnelling recombination in insulating solids, controlled by defect diffusion and rotation." Radiation Effects and Defects in Solids 111-112, no. 1-2 (1989): 191–205. http://dx.doi.org/10.1080/10420158908212994.

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50

Hong, Nguyen Hoa, Joe Sakai, and François Gervais. "Magnetism due to oxygen vacancies and/or defects in undoped semiconducting and insulating oxide thin films." Journal of Magnetism and Magnetic Materials 316, no. 2 (2007): 214–17. http://dx.doi.org/10.1016/j.jmmm.2007.02.081.

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