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Journal articles on the topic 'Trilayers'

Author: Grafiati

Published: 2 June 2025

Last updated: 31 July 2025

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1

Patrin, K. G., V. Y. Yakovchuk, G. S. Patrin, and S. A. Yarikov. "Magnetism and Magnetoresistance in NiFe/Bi/NiFe Films." Solid State Phenomena 190 (June 2012): 439–42. http://dx.doi.org/10.4028/www.scientific.net/ssp.190.439.

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Interlayer interactions in FeNi/Bi/FeNi trilayers have been experimentally studied. Based on the data of SQUID magnetometry and magnetic resonance investigations, it is shown that the interlayer interaction is determined by a bismuth spacer thickness and temperature. The giant magnetoresistive effect in the trilayer films has been discovered.

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2

Karpe, N., J. B⊘ttiger, A. L. Greer, J. Janting, and K. Kyllesbech Larsen. "On the chemical diffusion in layered thin films containing amorphous Co–Zr, Ni–Zr, and Fe–Zr." Journal of Materials Research 7, no. 4 (1992): 926–33. http://dx.doi.org/10.1557/jmr.1992.0926.

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The chemical diffusion in thin trilayer films of TM–TM100−xZrx–TM with an amorphous middle layer where TM = Co, Ni, or Fe and in amorphous Fe–Zr and Ni–Zr films with composition gradients has been investigated using Rutherford backscattering spectrometry. The growth of the amorphous layer in the trilayers, due to in-diffusion of cobalt and nickel, is initially found to be proportional to the square root of the time, t1/2, and subsequently found to level off before the compositions corresponding to metastable equilibria are reached. Irradiation, with 500 keV Xe+ ions, is found to promote the in

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3

Sacco, Chiara, Alice Galdi, Francesco Romeo, et al. "Comparing Thickness and Doping-Induced Effects on the Normal States of Infinite-Layer Electron-Doped Cuprates: Is There Anything to Learn?" Nanomaterials 12, no. 7 (2022): 1092. http://dx.doi.org/10.3390/nano12071092.

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We grew Sr1-xLaxCuO2 thin films and SrCuO2/Sr0.9La0.1CuO2/SrCuO2 trilayers by reflection high-energy diffraction-calibrated layer-by-layer molecular beam epitaxy, to study their electrical transport properties as a function of the doping and thickness of the central Sr0.9La0.1CuO2 layer. For the trilayer samples, as already observed in underdoped SLCO films, the electrical resistivity versus temperature curves as a function of the central layer thickness show, for thicknesses thinner than 20 unit cells, sudden upturns in the low temperature range with the possibility for identifying, in the no

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4

Lucci, Massimiliano, Ivano Ottaviani, Matteo Cirillo, et al. "Anodization-based process for the fabrication of all niobium nitride Josephson junction structures." Beilstein Journal of Nanotechnology 8 (March 2, 2017): 539–46. http://dx.doi.org/10.3762/bjnano.8.58.

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We studied the growth and oxidation of niobium nitride (NbN) films that we used to fabricate superconductive tunnel junctions. The thin films were deposited by dc reactive magnetron sputtering using a mixture of argon and nitrogen. The process parameters were optimized by monitoring the plasma with an optical spectroscopy technique. This technique allowed us to obtain NbN as well as good quality AlN films and both were used to obtain NbN/AlN/NbN trilayers. Lift-off lithography and selective anodization of the NbN films were used, respectively, to define the main trilayer geometry and/or to sep

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5

Atwa, Mohamed M., Ahmed AlAskalany, Karim Elgammal, Anderson D. Smith, Mattias Hammar, and Mikael Östling. "Trilayer Graphene as a Candidate Material for Phase-Change Memory Applications." MRS Advances 1, no. 20 (2016): 1487–94. http://dx.doi.org/10.1557/adv.2016.237.

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ABSTRACTThere is pressing need in computation of a universal phase change memory consolidating the speed of RAM with the permanency of hard disk storage. A potentiated scanning tunneling microscope tip traversing the soliton separating a metallic, ABA-stacked phase and a semiconducting ABC-stacked phase in trilayer graphene has been shown to permanently transform ABA-stacked regions to ABC-stacked regions. In this study, we used density functional theory (DFT) calculations to assess the energetics of this phase-change and explore the possibility of organic functionalization using s-triazine to

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6

Jing, Zhao-Xuan, Shou-Heng Zhang, and Shandong Li. "Enhancement of high-frequency performances by Al₂O₃ interlayer in FeCoHf/Al₂O₃/FeCoHf trilayers." AIP Advances 12, no. 5 (2022): 055224. http://dx.doi.org/10.1063/5.0089503.

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In this study, Hf-doped FeCo alloy films with a high ferromagnetic resonance (FMR) frequency at zero external fields were prepared by a composition gradient sputtering method. In order to further enhance the high-frequency performances, Al2O3 spacers of various thicknesses were inserted in the middle of the FeCoHf film. It is revealed that the Al2O3 interlayer improves the magnetic anisotropy of trilayers, enhances the resistivity, and refines the grain size. As a result, the FMR frequency of the trilayer was enhanced to over 3 GHz, and the permeability was also evidently improved from 41 (sin

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7

Leung, D. K., M. Y. He, and A. G. Evans. "The cracking resistance of nanoscale layers and films." Journal of Materials Research 10, no. 7 (1995): 1693–99. http://dx.doi.org/10.1557/jmr.1995.1693.

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Thin film cracking has been studied for a nanometer brittle/ductile layered system consisting of Si and Cu. Single Si films and Cu/Si/Cu trilayers were fabricated by physical vapor deposition. The films were deposited onto a ductile substrate consisting of stainless steel with a thin polyimide interlayer. Straining of the substrate induced cracking of the Si. Cracking strains ≥1% were observed, particularly in layers ≤100 nm thick. The critical cracking strain was found to depend upon the Si layer thickness, as well as the thickness and elastic/plastic properties of the adjacent ductile layers

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8

Hermosilla Palacios, Martha Alejandra, Jeff Blackburn, Alexis Myers, et al. "Ultrafast Charge Transfer Cascade in a Mixed-Dimensionality Nanoscale Trilayer." ECS Meeting Abstracts MA2024-01, no. 12 (2024): 1014. http://dx.doi.org/10.1149/ma2024-01121014mtgabs.

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Innovation in optoelectronic semiconductor devices is driven by a fundamental understanding of how to move charges and/or excitons (electron-hole pairs) in specified directions for doing useful work, e.g. for making fuels or electricity. The diverse and tunable electronic and optical properties of two-dimensional (2D) transition metal dichalcogenides (TMDCs) and one-dimensional (1D) semiconducting single-walled carbon nanotubes (s-SWCNTs) make them good quantum confined model systems for fundamental studies on charge and exciton transfer across heterointerfaces. In nature, the photosynthetic a

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9

Freitag, Marcus. "Trilayers unravelled." Nature Physics 7, no. 8 (2011): 596–97. http://dx.doi.org/10.1038/nphys2032.

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10

WANG, H. O., P. DAI, H. LIU, et al. "MAGNETIC AND TRANSPORT PROPERTIES OFPr0.7Sr0.3MnO3/La0.5Ca0.5MnO3/Pr0.7Sr0.3MnO3TRILAYERS." International Journal of Modern Physics B 26, no. 23 (2012): 1250132. http://dx.doi.org/10.1142/s0217979212501329.

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All-manganites Pr0.7Sr0.3MnO3/ La0.5Ca0.5MnO3/ Pr0.7Sr0.3MnO3(PSMO/LCMO/PSMO) trilayers were deposited on (001)-oriented single crystal MgO by pulsed laser deposition. The thickness of both PSMO layers was 36 nm while the thickness of LCMO layer varied from 6 to 36 nm. High resolution X-ray diffraction patterns indicated that trilayers were well (001)-oriented grown with high crystalline quality, and that PSMO layers were fully-strain-relaxed while LCMO spacer was partially strained. Studies on transport and magnetic properties of trilayers indicated that metal-insulator transition temperature

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11

Song, Tiancheng, Qi-Chao Sun, Eric Anderson, et al. "Direct visualization of magnetic domains and moiré magnetism in twisted 2D magnets." Science 374, no. 6571 (2021): 1140–44. http://dx.doi.org/10.1126/science.abj7478.

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Imaging twisty magnets Twisting monolayers of graphene with respect to each other has led to a number of unusual correlated states. This approach has inspired researchers to try their hand at twisting two-dimensional (2D) magnets, but such experiments have proven a difficult challenge. Song et al . made structures out of layers of the 2D magnet chromium triiodide with a small twist angle (see the Perspective by Lado). Using nitrogen vacancy centers in diamond as a magnetometer, the authors imaged the magnetic domains in both twisted monolayer and twisted trilayer structures. For twisted trilay

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12

Lu, Ning, Hongyan Guo, Lu Wang, Xiaojun Wu, and Xiao Cheng Zeng. "van der Waals trilayers and superlattices: modification of electronic structures of MoS2 by intercalation." Nanoscale 6, no. 9 (2014): 4566–71. http://dx.doi.org/10.1039/c4nr00783b.

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We perform a comprehensive first-principles study of the electronic properties of van der Waals (vdW) trilayers via intercalating a two-dimensional (2D) monolayer (ML = BN, MoSe<sub>2</sub>, WS<sub>2</sub>, or WSe<sub>2</sub>) between a MoS<sub>2</sub> bilayer to form various MoS<sub>2</sub>/ML/MoS<sub>2</sub> sandwich trilayers.

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13

Cucolo, A. M., and P. Prieto. "A Comparative Study of Different Tunnel Barriers for C-Axis Oriented Y(Ho)Ba2Cu3O7 Based Trilayer Structures." International Journal of Modern Physics B 11, no. 32 (1997): 3833–47. http://dx.doi.org/10.1142/s0217979297001969.

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We report on the structural and electrical characterization of c-axis oriented Y(Ho)Ba2Ca3O7 -based trilayer structures with different insulating layers. A comparative study of Y2O3 , SrTiO3 and PrBa2Cu3O7 barriers is carried out. Structural characterization demonstrates the epitaxial growth of the heterostructures with sharp interfaces between the different layers. Resistivity and ac susceptibility dependences on temperature indicate no degradation of the superconducting properties of the bottom and top electrodes. Josephson effect and quasi-particle tunneling are observed in the YBa2Cu3O7/Y2

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14

Stajic, J. "Skyrmions emerge in trilayers." Science 349, no. 6245 (2015): 279. http://dx.doi.org/10.1126/science.349.6245.279-c.

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15

BI, K., and Y. G. WANG. "INFLUENCE OF INTERFACE AND POLARIZATION ON MAGNETOELECTRIC COUPLING IN Ni-LEAD ZIRCONIUM TITANATE-Ni TRILAYERS DERIVED BY ELECTROLESS DEPOSITION." Surface Review and Letters 19, no. 03 (2012): 1250030. http://dx.doi.org/10.1142/s0218625x12500308.

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Magnetoelectric (ME) coupling in layered structures of magnetostrictive and piezoelectric phases are mediated by mechanical deformation and depends strongly on the interface conditions. Ni -lead zirconium titanate- Ni trilayers with neither electrodes nor bonding layers have been derived by electroless deposition. The structure of the electroless deposited Ni layer was characterized by X-ray diffraction. The cross-section of the Ni/PZT layers was investigated using scanning electron microscopy. The value of ME voltage coefficient (αE,31) increases as the interface roughness increases. The maxi

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16

BADER, S. D. "MAGNETO-OPTIC CHARACTERIZATIONS OF SUPERLATTICES AND WEDGED SANDWICHES WITH OSCILLATORY INTERLAYER MAGNETIC COUPLING." International Journal of Modern Physics B 07, no. 01n03 (1993): 414–18. http://dx.doi.org/10.1142/s0217979293000883.

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Three examples of magnetic coupling across metallic spacer layers are considered. Fe/Nb sputtered superlattices are observed to have as many as five antiferromagnetic oscillations, but a weak magnetoresistive anomaly. Epitaxial trilayers of Fe/Mo/Fe grown on Mo(100) and Co/Cu/Co grown on Cu(100) are observed to have short- and long-period oscillations, respectively. The trilayers are grown with wedged spacer layers and characterized in-situ by means of the magneto-optic Kerr effect.

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17

Prischepa, Serghej L., V. N. Kushnir, C. Cirillo, C. Attanasio, and M. Yu Kupriyanov. "Superconducting Critical Temperature and Magnetic Inhomogeneities in Superconductor/Ferromagnet/Superconductor Trilayers." Solid State Phenomena 190 (June 2012): 409–12. http://dx.doi.org/10.4028/www.scientific.net/ssp.190.409.

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The effect of ferromagnetic layer inhomogeneity on the superconducting resistive transition in Superconductor/Ferromagnet/Superconductor (S/F/S) trilayers is studied. The critical temperature, Tc, and the resistive transition shape versus the F layer thickness, dF, in Nb/Cu0.41Ni0.59/Nb and Nb/Pd0.81Ni0.19/Nb trilayers were analyzed. It is shown that the Tc(dF) dependence is sensitive to the Ni concentration variation along the F layer for thickness of dF corresponding to the π-superconducting state and to the 0-π crossover thickness.

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18

Kim, J. W., J. H. Kim, M. N. Janal, and Y. Zhang. "Damage Maps of Veneered Zirconia under Simulated Mastication." Journal of Dental Research 87, no. 12 (2008): 1127–32. http://dx.doi.org/10.1177/154405910808701210.

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Zirconia-based restorations often fracture from chipping and/or delamination of the porcelain veneers. We hypothesized that veneer chipping/delamination is a result of the propagation of near-contact-induced partial cone cracks on the occlusal surface under mastication. Masticatory loading involves the opposing tooth sliding along the cuspal inner incline surface with an applied biting force. To test this hypothesis, we cemented flat porcelain-veneered zirconia plates onto dental composites and cyclically loaded them (contact–slide–liftoff) at an inclination angle as a simplified model of zirc

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19

Wang, Zijun, Xingqiao Ma, Houbing Huang, Hongwen Xiao, and Tianfu Li. "Micromagnetic Simulation of Domain Walls in Exchange Spring Trilayers." Advances in Condensed Matter Physics 2014 (2014): 1–5. http://dx.doi.org/10.1155/2014/301063.

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Chiral domain wall structures in ferromagnetic exchange spring soft/hard/soft and hard/soft/hard trilayers were investigated with micromagnetic simulation, which enables us to fully characterize the nucleation and growth of buried domain walls in layered ferromagnetic thin films. Simulated results show that the trilayers are both exchange coupled and presenting chiral spin structures. Detailed features of field-dependent domain walls evolution in the spring magnets are also revealed. In process of remagnetization, the spin structure of soft/hard/soft is energetically more stable than that of h

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20

Fonseca, T. L., and N. S. Almeida. "Equilibrium configuration of magnetic trilayers." Physical Review B 57, no. 1 (1998): 76–79. http://dx.doi.org/10.1103/physrevb.57.76.

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21

Lee, S. F., C. Yu, W. T. Shih, Y. Liou, and Y. D. Yao. "Properties of Nb/Co trilayers." Journal of Magnetism and Magnetic Materials 209, no. 1-3 (2000): 231–33. http://dx.doi.org/10.1016/s0304-8853(99)00696-4.

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22

Chui, S. T., and J. R. Cullen. "Spin Transmission in Metallic Trilayers." Physical Review Letters 74, no. 11 (1995): 2118–21. http://dx.doi.org/10.1103/physrevlett.74.2118.

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23

Mazalski, Piotr, Iosif Sveklo, Zbigniew Kurant, et al. "XAS and XMCD studies of magnetic properties modifications of Pt/Co/Au and Pt/Co/Pt trilayers induced by Ga+ions irradiation." Journal of Synchrotron Radiation 22, no. 3 (2015): 753–59. http://dx.doi.org/10.1107/s1600577515002933.

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Magnetic and magneto-optical properties of Pt/Co/Au and Pt/Co/Pt trilayers subjected to 30 keV Ga+ion irradiation are compared. In two-dimensional maps of these properties as a function of cobalt thickness and ion fluence, two branches with perpendicular magnetic anisotropy (PMA) for Pt/Co/Pt trilayers are well distinguished. The replacement of the Pt capping layer with Au results in the two branches still being visible but the in-plane anisotropy for the low-fluence branch is suppressed whereas the high-fluence branch displays PMA. The X-ray absorption spectra and X-ray magnetic circular dich

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24

Khusainov, M. G., M. M. Khusainov, and Y. N. Proshin. "Superconducting Probe of Electronic Correlations and Exchange Field Based on the Proximity Effect in F/S Nanostructures." Solid State Phenomena 190 (June 2012): 413–16. http://dx.doi.org/10.4028/www.scientific.net/ssp.190.413.

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The proximity effect and competition between the BCS and LOFF states are studied in the Cooper limit for thin F/S and F/S/F nanostructures, where F is a ferromagnet and S is a superconductor. The dependences of the critical temperature Tc on the exchange field I, electron correlations λf, and the thickness df of the F layer are derived for F/S bilayers and F/S/F trilayers. Two new π-phase superconducting states with electronelectron repulsion in the F layers of F/S/F trilayers are predicted. A 2D LOFF state in F/S/F trilayers is possible only in the presence of a weak magnetic field and the ap

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25

Xu, Xiaotao, Xi He, Anthony T. Bollinger, Xiaoyan Shi, and Ivan Božović. "Atomic-Layer Engineering of La2−xSrxCuO4—La2−xSrxZnO4 Heterostructures." Nanomaterials 13, no. 15 (2023): 2207. http://dx.doi.org/10.3390/nano13152207.

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The fabrication of trilayer superconductor-insulator-superconductor (SIS) Josephson junctions with high-temperature superconductor (HTS) electrodes requires atomically perfect interfaces. Therefore, despite great interest and efforts, this remained a challenge for over three decades. Here, we report the discovery of a new family of metastable materials, La2−xSrxZnO4 (LSZO), synthesized by atomic-layer-by-layer molecular beam epitaxy (ALL-MBE). We show that LSZO is insulating and epitaxially compatible with an HTS compound, La2−xSrxCuO4 (LSCO). Since the “parent” compound La2ZnO4 (LZO) is easie

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26

Dilbeck, Tristan, Sean P. Hill, and Kenneth Hanson. "Harnessing molecular photon upconversion at sub-solar irradiance using dual sensitized self-assembled trilayers." Journal of Materials Chemistry A 5, no. 23 (2017): 11652–60. http://dx.doi.org/10.1039/c7ta00317j.

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27

Fako, Edvin, Ana S. Dobrota, Igor A. Pašti, Núria López, Slavko V. Mentus, and Natalia V. Skorodumova. "Lattice mismatch as the descriptor of segregation, stability and reactivity of supported thin catalyst films." Physical Chemistry Chemical Physics 20, no. 3 (2018): 1524–30. http://dx.doi.org/10.1039/c7cp07276g.

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28

Zaytseva, I., M. Z. Cieplak, A. Abal'oshev, et al. "Magnetoresistance of Si/Nb/Si Trilayers." Acta Physica Polonica A 118, no. 2 (2010): 406–8. http://dx.doi.org/10.12693/aphyspola.118.406.

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29

Fominov, Ya V., A. A. Golubov, and M. Yu Kupriyanov. "Triplet proximity effect in FSF trilayers." Journal of Experimental and Theoretical Physics Letters 77, no. 9 (2003): 510–15. http://dx.doi.org/10.1134/1.1591981.

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30

Hall, P. M., F. L. Howland, Y. S. Kim, and L. H. Herring. "Strains in Aluminum-Adhesive-Ceramic Trilayers." Journal of Electronic Packaging 112, no. 4 (1990): 288–302. http://dx.doi.org/10.1115/1.2904381.

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In many of today’s high speed, high density circuits, there is a need to remove large amounts of heat. To facilitate this removal of heat, it is common to adhere a sheet of a high thermal conductivity material (such as aluminum or copper) to the substrate (which may be alumina ceramic). This can result in large expansion mismatches which cause stresses and bowing, with the possibility of delamination, cracking, stressing solder joints, loss of hermeticity, or shorting of a metal lid to wire bonds inside a cavity. One approach to this problem is to use a compliant adhesive to decouple the mater

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31

Uzdin, V. M., and C. Demangeat. "Pinhole defects in Fe/Cr trilayers." Journal of Magnetism and Magnetic Materials 165, no. 1-3 (1997): 458–61. http://dx.doi.org/10.1016/s0304-8853(96)00591-4.

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32

Arrott, A. S. "Micromagnetics of uneven ultrathin film trilayers." Journal of Applied Physics 79, no. 8 (1996): 4973. http://dx.doi.org/10.1063/1.361607.

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33

Wiese, N., T. Dimopoulos, M. Rührig, J. Wecker, H. Brückl, and G. Reiss. "Antiferromagnetically coupled CoFeB∕Ru∕CoFeB trilayers." Applied Physics Letters 85, no. 11 (2004): 2020–22. http://dx.doi.org/10.1063/1.1792375.

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34

Bhattacharyya, A. S., S. Kumar, A. Sharma, et al. "Metallization and APPJ treatment of bismaleimide." High Performance Polymers 29, no. 7 (2016): 816–26. http://dx.doi.org/10.1177/0954008316659123.

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Bismaleimide (BMI) resins are a new breed of thermosetting resins used mainly for high-temperature applications and have major usage in aerospace. Fourier transform infrared (FTIR) studies have shown signatures of imide, C–N–C stretching, maleimide, and N–H stretching. These BMI polymer coatings were deposited on aluminum (Al) and mild steel substrates by sprinkling powers followed by baking. Thermogravimetric analysis and differential scanning calorimetric studies showed the degradation temperature of these polymers around 370°C. Al coatings were deposited on BMI that is previously deposited

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35

Terentieva, Larisa A., Elena L. Parfenova, Mansur G. Khusainov, and Yurii N. Proshin. "Proximity Effect as a Probe of Electronic Correlations and Exchange Field in Dirty Ferromagnet/Superconductor Nanostructures." Solid State Phenomena 152-153 (April 2009): 457–61. http://dx.doi.org/10.4028/www.scientific.net/ssp.152-153.457.

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We investigate the interplay between the BCS and 2D Larkin-Ovchinnikov-Fulde-Ferrell (LOFF) states in the dirty thin ferromagnetic metal/superconductor (FM/S) nanostructures. For the FM/S bilayers we have derived the dependencies of critical temperature on the FM layer exchange field, electronic correlations and thickness. Moreover, in the corresponding FM/S/FM trilayers we predict two new π phase superconducting states with electron-electron repulsion in the FM layers. The 2D modulated LOFF states are possible in such trilayers only in presence of a weak magnetic field and at suitable paramet

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36

Cho, Chungyeon, Yixuan Song, Ryan Allen, Kevin L. Wallace, and Jaime C. Grunlan. "Stretchable electrically conductive and high gas barrier nanocomposites." Journal of Materials Chemistry C 6, no. 8 (2018): 2095–104. http://dx.doi.org/10.1039/c7tc05495e.

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By alternately depositing trilayers of polyethylene oxide, double-walled carbon nanotubes stabilized in polyacrylic acid, and graphene oxide via layer-by-layer assembly, elastomeric conductive multilayers with a high gas barrier were prepared.

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Miranda, Pedro, Antonia Pajares, Fernando Guiberteau, Francisco L. Cumbrera, and Brian R. Lawn. "Contact fracture of brittle bilayer coatings on soft substrates." Journal of Materials Research 16, no. 1 (2001): 115–26. http://dx.doi.org/10.1557/jmr.2001.0021.

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Contact-induced fracture modes in trilayers consisting of a brittle bilayer coating on a soft substrate were investigated. Experiments were performed on model transparent glass/sapphire/polycarbonate structures bonded with epoxy adhesive, to enablein situobservation during the contact. Individual layer surfaces were preferentially abraded to introduce uniform flaw states and so allowed each crack type to be studied separately and controllably. Fracture occurred by cone cracking at the glass top surface or by radial cracking at the glass or sapphire bottom surfaces. Critical loads for each crac

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38

BI, K., H. HONG, W. WU, and Y. G. WANG. "ELECTROLESS DEPOSITION OF NICKEL ON LEAD ZIRCONIUM TITANATE CERAMICS: PREPARATION, MAGNETIC AND MAGNETOELECTRIC PROPERTIES." Surface Review and Letters 19, no. 06 (2012): 1250061. http://dx.doi.org/10.1142/s0218625x12500618.

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The Ni layers with good soft magnetic properties have been successfully electroless deposited on PZT layers. To study the thermodynamics and kinetics of electroless Ni -deposition, the effect of bath parameters such as pH and temperature has been discussed. The structural, magnetic and magnetostrictive properties of Ni layers deposited at various pH and temperature are characterized by X-ray diffraction, transmission electron microscopy, vibrating sample magnetometer and standard strain-gauge technique. The grain size, deposition rate, magnetic properties and magnetostrictive properties of Ni

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39

Ipaves, Bruno, João F. Justo, and Lucy V. C. Assali. "Functionalized few-layer silicene nanosheets: stability, elastic, structural, and electronic properties." Physical Chemistry Chemical Physics 24, no. 15 (2022): 8705–15. http://dx.doi.org/10.1039/d1cp05867c.

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This paper presents an ab initio investigation, performed in the framework of density functional theory, on the properties of functionalized few-layer silicene nanosheets, denoted as Si2X2 bilayers and Si4X2 trilayers with X = B, N, Al, and P.

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40

Chzhan, A. V., S. Ya Kiparisov, V. A. Seredkin, G. S. Patrin, and M. G. Pal’chik. "Magnetic properties of Co-P-based trilayers." Bulletin of the Russian Academy of Sciences: Physics 73, no. 8 (2009): 1161–63. http://dx.doi.org/10.3103/s1062873809080425.

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Patrin, G. S., V. Yu Yakovchuk, D. A. Velikanov, K. G. Patrin, and S. A. Yarikov. "Interlayer interactions in FeNi/Bi/FeNi trilayers." Bulletin of the Russian Academy of Sciences: Physics 76, no. 2 (2012): 177–79. http://dx.doi.org/10.3103/s1062873812020207.

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42

Prischepa, Serghej L., Carla Cirillo, Carmine Attanasio, et al. "Resistive Transitions in S/F/S Trilayers." Solid State Phenomena 152-153 (April 2009): 478–81. http://dx.doi.org/10.4028/www.scientific.net/ssp.152-153.478.

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The phase transition of Nb/Cu0.41Ni0.59/Nb triple layers from the normal to the superconducting state has been studied experimentally by measuring the temperature dependence of the electrical resistance, R(T). It is shown that the shape of the R(T) curves is different depending on the Cu0.41Ni0.59 thickness. To explain the experimental data we developed a qualitative model which makes more evident the interconnection between the superconducting phase transition and the 0 to  crossover in SFS structures.

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43

Kobyakov, A. V., G. S. Patrin, I. A. Turpanov, et al. "Interlayer Coupling in Co/Ge/Co Trilayers." Solid State Phenomena 168-169 (December 2010): 273–76. http://dx.doi.org/10.4028/www.scientific.net/ssp.168-169.273.

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The interlayer coupling in Co/Ge/Co trilayer films has been experimentally studied by the SQUID magnetometry and electron magnetic resonance. It has been found that the interlayer coupling is temperature-dependent. The values of the exchange constants have been determined.

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44

Yang, L. H., M. Shaughnessy, L. Damewood, C. Y. Fong, and Kai Liu. "Half-metallic hole-doped Mn/Si trilayers." Journal of Physics D: Applied Physics 46, no. 16 (2013): 165502. http://dx.doi.org/10.1088/0022-3727/46/16/165502.

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45

Wüchner, S., J. Voiron, D. Givord, D. Boursier, and J. J. Préjean. "Complex magnetization processes of exchange coupled trilayers." Journal of Applied Physics 75, no. 10 (1994): 6682–84. http://dx.doi.org/10.1063/1.356894.

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46

Laperre, J., and W. Thys. "Mode coupling in solid/liquid/solid trilayers." Journal of the Acoustical Society of America 96, no. 3 (1994): 1643–50. http://dx.doi.org/10.1121/1.411388.

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47

Jungbauer, M., S. Hühn, M. Michelmann, E. Goering, and V. Moshnyaga. "Exchange bias in La0.7Sr0.3MnO3/SrMnO3/La0.7Sr0.3MnO3 trilayers." Journal of Applied Physics 113, no. 17 (2013): 17D709. http://dx.doi.org/10.1063/1.4798349.

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48

Prischepa, S. L., C. Cirillo, C. Bell, et al. "Resistive transitions in Nb/Cu0.41Ni0.59/Nb trilayers." JETP Letters 88, no. 6 (2008): 375–79. http://dx.doi.org/10.1134/s0021364008180070.

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Sinclair, G. J., G. A. Jones, P. J. Grundy, and K. O'Grady. "Magnetization reversal in CoCrPt thin film trilayers." Journal of Physics D: Applied Physics 28, no. 9 (1995): 1785–90. http://dx.doi.org/10.1088/0022-3727/28/9/005.

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50

Herce, H. D., and C. R. Proetto. "Quantum phase transitions in Coulomb-coupled trilayers." Solid State Communications 118, no. 8 (2001): 395–400. http://dx.doi.org/10.1016/s0038-1098(01)00140-5.

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