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1

Arunan, E. "van der Waals." Resonance 15, no. 7 (July 2010): 584–87. http://dx.doi.org/10.1007/s12045-010-0043-3.

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2

Han, Jianing. "Two-Dimensional Six-Body van der Waals Interactions." Atoms 10, no. 1 (January 24, 2022): 12. http://dx.doi.org/10.3390/atoms10010012.

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Van der Waals interactions, primarily attractive van der Waals interactions, have been studied over one and half centuries. However, repulsive van der Waals interactions are less widely studied than attractive van der Waals interactions. In this article, we focus on repulsive van der Waals interactions. Van der Waals interactions are dipole–dipole interactions. In this article, we study the van der Waals interactions between multiple dipoles. Specifically, we focus on two-dimensional six-body van der Waals interactions. This study has many potential applications. For example, the result may be applied to physics, chemistry, chemical engineering, and other fields of sciences and engineering, such as breaking molecules.
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3

Bernasek, Steven L. "Van der Waals rectifiers." Nature Nanotechnology 8, no. 2 (January 6, 2013): 80–81. http://dx.doi.org/10.1038/nnano.2012.242.

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4

Geim, A. K., and I. V. Grigorieva. "Van der Waals heterostructures." Nature 499, no. 7459 (July 2013): 419–25. http://dx.doi.org/10.1038/nature12385.

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5

Levitov, L. S. "Van Der Waals' Friction." Europhysics Letters (EPL) 8, no. 6 (March 15, 1989): 499–504. http://dx.doi.org/10.1209/0295-5075/8/6/002.

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6

Capozziello, S., S. De Martino, and M. Falanga. "Van der Waals quintessence." Physics Letters A 299, no. 5-6 (July 2002): 494–98. http://dx.doi.org/10.1016/s0375-9601(02)00753-3.

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7

Bärwinkel, Klaus, and Jürgen Schnack. "van der Waals revisited." Physica A: Statistical Mechanics and its Applications 387, no. 18 (July 2008): 4581–88. http://dx.doi.org/10.1016/j.physa.2008.03.019.

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8

Thongyothee, Chawis, and Somchai Chucheepsakul. "Finite Element Modeling of van der Waals Interaction for Elastic Stability of Multi-Walled Carbon Nanotubes." Advanced Materials Research 55-57 (August 2008): 525–28. http://dx.doi.org/10.4028/www.scientific.net/amr.55-57.525.

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The purpose of this study is to assess the effect of van der Waals interactions within multi-walled carbon nanotubes with the three dimensional finite element models. The elastic buckling behaviors of nanotubes are treated under axial compressive force acting on open both ends of nanotubes and considered with various boundary conditions. The analysis is based on the assumptions that the covalent bond of each wall is represented by an elastic beam element while the van der Waals force of adjacent walls are represented by a nonlinear truss element following the Lennard-Jones “6-12” theory. The models of double-walled carbon nanotubes are used to explain the characteristic of multi-walled carbon nanotubes and then results compared with the column theory. The results show that the critical load of nanotubes depends on atomic arrangement, tube length, and number of walls, while the van der Waals force has a small effect on the buckling load for multi-walled carbon nanotubes.
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9

Wu, Yan-Fei, Meng-Yuan Zhu, Rui-Jie Zhao, Xin-Jie Liu, Yun-Chi Zhao, Hong-Xiang Wei, Jing-Yan Zhang, et al. "The fabrication and physical properties of two-dimensional van der Waals heterostructures." Acta Physica Sinica 71, no. 4 (2022): 048502. http://dx.doi.org/10.7498/aps.71.20212033.

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Two-dimensional van der Waals materials (2D materials for short) have developed into a novel material family that has attracted much attention, and thus the integration, performance and application of 2D van der Waals heterostructures has been one of the research hotspots in the field of condensed matter physics and materials science. The 2D van der Waals heterostructures provide a flexible and extensive platform for exploring diverse physical effects and novel physical phenomena, as well as for constructing novel spintronic devices. In this topical review article, starting with the transfer technology of 2D materials, we will introduce the construction, performance and application of 2D van der Waals heterostructures. Firstly, the preparation technology of 2D van der Waals heterostructures in detail will be presented according to the two classifications of wet transfer and dry transfer, including general equipment for transfer technology, the detailed steps of widely used transfer methods, a three-dimensional manipulating method for 2D materials, and hetero-interface cleaning methods. Then, we will introduce the performance and application of 2D van der Waals heterostructures, with a focus on 2D magnetic van der Waals heterostructures and their applications in the field of 2D van der Waals magnetic tunnel junctions and moiré superlattices. The development and optimization of 2D materials transfer technology will boost 2D van der Waals heterostructures to achieve breakthrough results in fundamental science research and practical application.
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10

Levelt Sengers, J. M. H., and J. V. Sengers. "van der Waals fund, van der Waals laboratory and Dutch high-pressure science." Physica A: Statistical Mechanics and its Applications 156, no. 1 (March 1989): 1–14. http://dx.doi.org/10.1016/0378-4371(89)90107-6.

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11

Ao, Hong Rui, Ming Dong, Xi Chao Wang, and Hong Yuan Jiang. "Analysis of Pressure Distribution on Head Disk Air Bearing Slider Involved Van der Waals Force." Applied Mechanics and Materials 419 (October 2013): 111–16. http://dx.doi.org/10.4028/www.scientific.net/amm.419.111.

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This paper focuses on the pressure distribution on the surface of slider in hard disk drive when its flying height is in nanoscale. The gas rarefaction effect and van der Waals force are involved in the analysis process. Here the air bearing force model is based on F-K model and we establish the equation of van der Waals force between the head and disk. Using the finite element method, the modified Reynolds equation and the van der Waals force were obtained. The air bearing force on slider before and after the van der Waals force involved were compared. The results illustrate that the effect of van der Waals force on the air bearing force is different according to the slider shapes and flying heights. As a result, van der Waals force plays an important role when the flying height of slider is below 10 nm.
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12

ZHOU, W., Y. HUANG, B. LIU, J. WU, K. C. HWANG, and B. Q. WEI. "ADHESION BETWEEN CARBON NANOTUBES AND SUBSTRATE: MIMICKING THE GECKO FOOT-HAIR." Nano 02, no. 03 (June 2007): 175–79. http://dx.doi.org/10.1142/s1793292007000490.

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A continuum model is developed based on the van der Waals interactions to study the adhesion between multi-wall carbon nanotubes (MWCNT) and substrates. Simple, analytical expressions for the binding energy and pulling force are obtained in terms of the MWCNT radius, number of walls, and parameters in the van der Waals potential. For a 1 cm by 1 cm template with densely packed MWCNTs (50 nm in spacing), the total pulling force can reach 26.6 N and 21.9 N for the graphite and polyethylene substrates, respectively.
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13

Avramenko, Andriy A., Igor V. Shevchuk, and Margarita M. Kovetskaya. "An Analytical Investigation of Natural Convection of a Van Der Waals Gas over a Vertical Plate." Fluids 6, no. 3 (March 15, 2021): 121. http://dx.doi.org/10.3390/fluids6030121.

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The study focused on a theoretical study of natural convection in a van der Waals gas near a vertical plate. A novel simplified form of the van der Waals equation derived in the study enabled analytical modeling of fluid flow and heat transfer. Analytical solutions were obtained for the velocity and temperature profiles, as well as the Nusselt numbers. It was revealed that nonlinear effects considered by the van der Waals equation of state contribute to acceleration or deceleration of the flow. This caused respective enhancement or deterioration of heat transfer. Results for a van der Waals gas were compared with respective computations using an ideal gas model. Limits of the applicability of the simplified van der Waals equations were pinpointed.
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14

Linder, Bruno, and Robert A. Kromhout. "van der Waals induced dipoles." Journal of Chemical Physics 84, no. 5 (March 1986): 2753–60. http://dx.doi.org/10.1063/1.450299.

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15

Han, Xiaodong. "Ductile van der Waals materials." Science 369, no. 6503 (July 30, 2020): 509. http://dx.doi.org/10.1126/science.abd4527.

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16

Wells, B. H., and S. Wilson. "van der Waals interaction potentials." Molecular Physics 66, no. 2 (February 10, 1989): 457–64. http://dx.doi.org/10.1080/00268978900100221.

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17

Holstein, Barry R. "The van der Waals interaction." American Journal of Physics 69, no. 4 (April 2001): 441–49. http://dx.doi.org/10.1119/1.1341251.

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18

Lu, J. X., and W. H. Marlow. "Nonsingular van der Waals potentials." Physical Review A 52, no. 3 (September 1, 1995): 2141–54. http://dx.doi.org/10.1103/physreva.52.2141.

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19

Wells, B. H., and S. Wilson. "van der Waals interaction potentials." Molecular Physics 55, no. 1 (May 1985): 199–210. http://dx.doi.org/10.1080/00268978500101271.

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20

Wells, Bryan H., and Stephen Wilson. "van der Waals interaction potentials." Molecular Physics 54, no. 4 (March 1985): 787–98. http://dx.doi.org/10.1080/00268978500103161.

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21

Wells, B. H., and S. Wilson. "van der Waals interaction potentials." Molecular Physics 57, no. 1 (January 1986): 21–32. http://dx.doi.org/10.1080/00268978600100021.

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22

Wells, B. H., and S. Wilson. "van der Waals interaction potentials." Molecular Physics 57, no. 2 (February 10, 1986): 421–26. http://dx.doi.org/10.1080/00268978600100331.

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23

Wells, B. H. "Van der Waals interaction potentials." Molecular Physics 61, no. 5 (August 10, 1987): 1283–93. http://dx.doi.org/10.1080/00268978700101791.

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24

Wells, B. H., and S. Wilson. "van der Waals interaction potentials." Molecular Physics 65, no. 6 (December 20, 1988): 1363–76. http://dx.doi.org/10.1080/00268978800101851.

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25

Rajagopal, Aruna, David Kubizňák, and Robert B. Mann. "Van der Waals black hole." Physics Letters B 737 (October 2014): 277–79. http://dx.doi.org/10.1016/j.physletb.2014.08.054.

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26

Han, Zhumin, Xinyuan Wei, Chen Xu, Chi-lun Chiang, Yanxing Zhang, Ruqian Wu, and W. Ho. "Imaging van der Waals Interactions." Journal of Physical Chemistry Letters 7, no. 24 (December 5, 2016): 5205–11. http://dx.doi.org/10.1021/acs.jpclett.6b02749.

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27

Kiessling, M. K. H., and J. K. Percus. "Nonuniform van der Waals theory." Journal of Statistical Physics 78, no. 5-6 (March 1995): 1337–76. http://dx.doi.org/10.1007/bf02180135.

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28

Cole, Milton W., Darrell Velegol, Hye-Young Kim, and Amand A. Lucas. "Nanoscale van der Waals interactions." Molecular Simulation 35, no. 10-11 (August 14, 2009): 849–66. http://dx.doi.org/10.1080/08927020902929794.

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29

Magnasco, Valerio, Giuseppe Figari, and Camilla Costa. "Understanding van der Waals bonding." Journal of Molecular Structure: THEOCHEM 261 (July 1992): 237–53. http://dx.doi.org/10.1016/0166-1280(92)87078-e.

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30

Feil, Sylvia. "Van der Waals: erstmals gemessen." Chemie in unserer Zeit 50, no. 5 (August 17, 2016): 303. http://dx.doi.org/10.1002/ciuz.201680049.

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31

Liu, Chang-Hua, Jiajiu Zheng, Shane Colburn, Taylor K. Fryett, Yueyang Chen, Xiaodong Xu, and Arka Majumdar. "Ultrathin van der Waals Metalenses." Nano Letters 18, no. 11 (October 8, 2018): 6961–66. http://dx.doi.org/10.1021/acs.nanolett.8b02875.

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32

Kilian, H. G. "Filled van der Waals networks." Progress in Colloid & Polymer Science 75, no. 1 (December 1987): 213–30. http://dx.doi.org/10.1007/bf01188373.

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33

Zhang, Ya-ni, Zhuo-ying Song, Dun Qiao, Xiao-hui Li, Zhe Guang, Shao-peng Li, Li-bin Zhou, and Xiao-han Chen. "2D van der Waals materials for ultrafast pulsed fiber lasers: review and prospect." Nanotechnology 33, no. 8 (December 3, 2021): 082003. http://dx.doi.org/10.1088/1361-6528/ac3611.

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Abstract 2D van der Waals materials are crystals composed of atomic layers, which have atomic thickness scale layers and rich distinct properties, including ultrafast optical response, surface effects, light-mater interaction, small size effects, quantum effects and macro quantum tunnel effects. With the exploration of saturable absorption characteristic of 2D van der Waals materials, a series of potential applications of 2D van der Waals materials as high threshold, broadband and fast response saturable absorbers (SAs) in ultrafast photonics have been proposed and confirmed. Herein, the photoelectric characteristics, nonlinear characteristic measurement technique of 2D van der Waals materials and the preparation technology of SAs are systematically described. Furthermore, the ultrafast pulsed fiber lasers based on classical 2D van der Waals materials including graphene, transition metal chalcogenides, topological insulators and black phosphorus have been fully summarized and analyzed. On this basis, opportunities and directions in this field, as well as the research results of ultrafast pulsed fiber lasers based on the latest 2D van der Waals materials (such as PbO, FePSe3, graphdiyne, bismuthene, Ag2S and MXene etc), are reviewed and summarized.
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34

Jiandong Qiao, Jiandong Qiao, Fuhong Mei Fuhong Mei, and Yu Ye Yu Ye. "Single-photon emitters in van der Waals materials." Chinese Optics Letters 17, no. 2 (2019): 020011. http://dx.doi.org/10.3788/col201917.020011.

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35

Manning, Gerald S. "Construction of a Universal Gel Model with Volume Phase Transition." Gels 6, no. 1 (February 27, 2020): 7. http://dx.doi.org/10.3390/gels6010007.

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The physical principle underlying the familiar condensation transition from vapor to liquid is the competition between the energetic tendency to condense owing to attractive forces among molecules of the fluid and the entropic tendency to disperse toward the maximum volume available as limited only by the walls of the container. Van der Waals incorporated this principle into his equation of state and was thus able to explain the discontinuous nature of condensation as the result of instability of intermediate states. The volume phase transition of gels, also discontinuous in its sharpest manifestation, can be understood similarly, as a competition between net free energy attraction of polymer segments and purely entropic dissolution into a maximum allowed volume. Viewed in this way, the gel phase transition would require nothing more to describe it than van der Waals’ original equation of state (with osmotic pressure Π replacing pressure P). But the polymer segments in a gel are networked by cross-links, and a consequent restoring force prevents complete dissolution. Like a solid material, and unlike a van der Waals fluid, a fully swollen gel possesses an intrinsic volume of its own. Although all thermodynamic descriptions of gel behavior contain an elastic component, frequently in the form of Flory-style rubber theory, the resulting isotherms usually have the same general appearance as van der Waals isotherms for fluids, so it is not clear whether the solid-like aspect of gels, that is, their intrinsic volume and shape, adds any fundamental physics to the volume phase transition of gels beyond what van der Waals already knew. To address this question, we have constructed a universal chemical potential for gels that captures the volume transition while containing no quantities specific to any particular gel. In this sense, it is analogous to the van der Waals theory of fluids in its universal form, but although it incorporates the van der Waals universal equation of state, it also contains a network elasticity component, not based on Flory theory but instead on a nonlinear Langevin model, that restricts the radius of a fully swollen spherical gel to a solid-like finite universal value of unity, transitioning to a value less than unity when the gel collapses. A new family of isotherms arises, not present in a preponderately van der Waals analysis, namely, profiles of gel density as a function of location in the gel. There is an abrupt onset of large amplitude density fluctuations in the gel at a critical temperature. Then, at a second critical temperature, the entire swollen gel collapses to a high-density phase.
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36

Nejad, Marjan A., and Herbert M. Urbassek. "Adsorption and Diffusion of Cisplatin Molecules in Nanoporous Materials: A Molecular Dynamics Study." Biomolecules 9, no. 5 (May 27, 2019): 204. http://dx.doi.org/10.3390/biom9050204.

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Using molecular dynamics simulations, the adsorption and diffusion of cisplatin drug molecules in nanopores is investigated for several inorganic materials. Three different materials are studied with widely-varying properties: metallic gold, covalent silicon, and silica. We found a strong influence of both the van der Waals and the electrostatic interaction on the adsorption behavior on the pore walls, which in turn influence the diffusion coefficients. While van der Waals forces generally lead to a reduction of the diffusion coefficient, the fluctuations in the electrostatic energy induced by orientation changes of the cisplatin molecule were found to help desorb the molecule from the wall.
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37

Gonzalez, R. I., J. Mella, P. Díaz, S. Allende, E. E. Vogel, C. Cardenas, and F. Munoz. "Hematene: a 2D magnetic material in van der Waals or non-van der Waals heterostructures." 2D Materials 6, no. 4 (July 1, 2019): 045002. http://dx.doi.org/10.1088/2053-1583/ab2501.

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38

Motoc, I., G. R. Marshall, R. A. Dammkoehler, and J. Labanowski. "Molecular Shape Descriptors. 1. Three-Dimensional Molecular Shape Descriptor." Zeitschrift für Naturforschung A 40, no. 11 (November 1, 1985): 1108–13. http://dx.doi.org/10.1515/zna-1985-1106.

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The paper presents and illustrates a method which uses numerical integration of the van der Waals envelope(s) to calculate with desired accuracy the molecular van der Waals volume and the three-dimensional molecular shape descriptor defined as the twin-number [OV(α, β); NOV(β, α), where OV and NOV represent the overlapping and, respectively, the nonoverlapping van der Waals volumes of the molecules α and ß superimposed according to appropriate criteria.
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39

Avramenko, A. A., I. V. Shevchuk, Yu Yu Kovetskaya, and N. P. Dmitrenko. "An Integral Method for Natural Convection of Van Der Waals Gases over a Vertical Plate." Energies 14, no. 15 (July 27, 2021): 4537. http://dx.doi.org/10.3390/en14154537.

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This paper focuses on a study of natural convection in a van der Waals gas over a vertical heated plate. In this paper, for the first time, an approximate analytical solution of the problem was obtained using an integral method for momentum and energy equations. A novel simplified form of the van der Waals equation for real gases enabled estimating the effects of the dimensionless van der Waals parameters on the normalized heat transfer coefficients and Nusselt numbers in an analytical form. Trends in the variation of the Nusselt number depending on the nature of the interaction between gas molecules and the wall were analyzed. The results of computations for a van der Waals gas were compared with the results for an ideal gas.
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40

Zhao, Lu, Lijuan Zhang, Houfu Song, Hongda Du, Junqiao Wu, Feiyu Kang, and Bo Sun. "Incoherent phonon transport dominates heat conduction across van der Waals superlattices." Applied Physics Letters 121, no. 2 (July 11, 2022): 022201. http://dx.doi.org/10.1063/5.0096861.

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Heat conduction mechanisms in superlattices could be different across different types of interfaces. Van der Waals superlattices are structures physically assembled through weak van der Waals interactions by design and may host properties beyond the traditional superlattices limited by lattice matching and processing compatibility, offering a different type of interface. In this work, natural van der Waals (SnS)1.17(NbS2)n superlattices are synthesized, and their thermal conductivities are measured by time-domain thermoreflectance as a function of interface density. Our results show that heat conduction of (SnS)1.17(NbS2)n superlattices is dominated by interface scattering when the coherent length of phonons is larger than the superlattice period, indicating that incoherent phonon transport dominates through-plane heat conduction in van der Waals superlattices even when the period is atomically thin and abrupt, in contrast to conventional superlattices. Our findings provide valuable insights into the understanding of the thermal behavior of van der Waals superlattices and devise approaches for effective thermal management of superlattices depending on the distinct types of interfaces.
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41

Peng, Qing, Xinjie Ma, Xiaoyu Yang, Shuai Zhao, Xiaoze Yuan, and Xiaojia Chen. "Assessing Effects of van der Waals Corrections on Elasticity of Mg3Bi2−xSbx in DFT Calculations." Materials 16, no. 19 (September 29, 2023): 6482. http://dx.doi.org/10.3390/ma16196482.

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As a promising room-temperature thermoelectric material, the elastic properties of Mg3Bi2−xSbx (0 ≤ x ≤ 2), in which the role of van der Waals interactions is still elusive, were herein investigated. We assessed the effects of two typical van der Waals corrections on the elasticity of Mg3Bi2−xSbx nanocomposites using first-principles calculations within the frame of density functional theory. The two van der Waals correction methods, PBE-D3 and vdW-DFq, were examined and compared to PBE functionals without van der Waals correction. Interestingly, our findings reveal that the lattice constant of the system shrinks by approximately 1% when the PBE-D3 interaction is included. This leads to significant changes in certain mechanical properties. We conducted a comprehensive assessment of the elastic performance of Mg3Bi2−xSbx, including Young’s modulus, Poisson’s ratio, bulk modulus, etc., for different concentration of Sb in a 40-atom simulation box. The presence or absence of van der Waals corrections does not change the trend of elasticity with respect to the concentration of Sb; instead, it affects the absolute values. Our investigation not only clarifies the influence of van der Waals correction methods on the elasticity of Mg3Bi2−xSbx, but could also help inform the material design of room-temperature thermoelectric devices, as well as the development of vdW corrections in DFT calculations.
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42

TAO, JIANMIN, JOHN P. PERDEW, and ADRIENN RUZSINSZKY. "LONG-RANGE VAN DER WAALS INTERACTION." International Journal of Modern Physics B 27, no. 18 (July 10, 2013): 1330011. http://dx.doi.org/10.1142/s0217979213300119.

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Van der Waals interaction is an elusive many-body effect arising from instantaneous charge fluctuations. Fundamental understanding of this effect plays an important role in computational chemistry, physics and materials science. In this article, recent advances in the evaluation of van der Waals coefficients, in particular the higher-order ones, are reviewed.
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43

Igor Smirnov. "MRET treated water as a tool to mitigate mRNA jab side effects: A review." Open Access Research Journal of Biology and Pharmacy 2, no. 1 (August 30, 2021): 029–36. http://dx.doi.org/10.53022/oarjbp.2021.2.1.0032.

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The viral RNA (ribonucleic acid) was found in virtually every organ in the body, which means the spike proteins as well. There are antibodies (like the “vaccine” is supposed to create) but they’re irrelevant because, based on a study from Japan, we now know that the spike S1 protein is what does the damage. That means the spike proteins created by the mRNA will be in every organ as well, and we now know it is the spike proteins that do the damage. Another significant mRNA jab side effect was found by Israeli researchers. They discovered a link between Pfizer’s COVID-19 vaccine and a rare blood disease called thrombotic thrombocytopenic purpura (TTP). Any formation of proteins depends on Van der Waals interactions. The Van der Waals forces depend in its turn on dielectric property of the protein molecules and water since all biochemistry needs water environment. It is practically impossible to change dielectric property/electrical charge of the proteins, but it is quite easy to modify dielectric property of water. There are research data indicating relation between dielectric constant of the human body tissue (TDC) and temperature: 35° C - 74.9 F/m (TDC) and 40° C - 73.2 F/m (TDC). It shows that normal homeostasis of the human body is allowed at certain range of electrodynamic van der Walls interactions following the small range of tissue dielectric property about 75 - 73 F/m. It allows us to suggest that dielectric property of human body tissue is very important physiological parameter. Considering mentioned above ideas, it allows us to hypothesize that most of biochemical proteins building mechanisms in a healthy human body require certain physiological range “window” of van der Waals interactions and hydrogen bonding between proteins molecules and water - salt medium. In theory, this physiological “window” of van der Waals weak electromagnetic forces may be significantly different from the range of electrodynamic van der Waals interactions required for life sustains formations of DNA/RNA proteins of viruses. Thus, modification of water - based medium electrodynamic parameters of the human tissues that are favorable for the homeostasis of the body (in the range of physiological “window”) can lead to significant change of van der Walls interactions and hydrogen bonding that may result in the inhibition and interruption of proper formation of spike proteins chains. Such scenario obviously disables coronavirus life sequence of attachment and fusion with human cell membranes. We suggest such agent which can interrupt pathogenic microorganism’s life sequence is MRET (Molecular Resonance Effect technology) water with anomalous electrodynamic characteristics. MRET water can be consumed on the regular basis by human subjects to prevent infections of pathogenic microorganisms.
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44

Tang, Yugang, and Ying Liu. "Effect of van der Waals force on wave propagation in viscoelastic double-walled carbon nanotubes." Modern Physics Letters B 32, no. 24 (August 27, 2018): 1850291. http://dx.doi.org/10.1142/s0217984918502913.

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In this paper, the influence of van der Waals force on the wave propagation in viscoelastic double-walled carbon nanotubes (DWCNTs) is investigated. The governing equations of wave motion are derived based on the nonlocal strain gradient theory and double-walled Timoshenko beam model. The effects of viscosity, van der Waals force, as well as size effects on the wave propagation in DWCNTs are clarified. The results show that effects of van der Waals force on waves in inner and outer layers of DWCNTs are different. Flexural wave (FW) in outer layer and shear wave (SW) in inner layer are sensitive to van der Waals force, and display new phenomena. This new finding may provide some useful guidance in the acoustic design of nanostructures with DWCNTs as basic elements.
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45

Samanta, G. C., and R. Myrzakulov. "Cosmological models constructed by van der Waals fluid approximation and volumetric expansion." International Journal of Geometric Methods in Modern Physics 14, no. 12 (November 24, 2017): 1750183. http://dx.doi.org/10.1142/s0219887817501833.

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The universe modeled with van der Waals fluid approximation, where the van der Waals fluid equation of state contains a single parameter [Formula: see text]. Analytical solutions to the Einstein’s field equations are obtained by assuming the mean scale factor of the metric follows volumetric exponential and power-law expansions. The model describes a rapid expansion where the acceleration grows in an exponential way and the van der Waals fluid behaves like an inflation for an initial epoch of the universe. Also, the model describes that when time goes away the acceleration is positive, but it decreases to zero and the van der Waals fluid approximation behaves like a present accelerated phase of the universe. Finally, it is observed that the model contains a type-III future singularity for volumetric power-law expansion.
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46

Duan, Shijie, Ming Yang, Suyuan Zhou, Longhui Zhang, Jinsen Han, Xu Sun, Guang Wang, et al. "Efficient terahertz generation from van der Waals α-In2Se3." Chinese Optics Letters 22, no. 1 (2024): 013202. http://dx.doi.org/10.3788/col202422.013202.

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47

Stöhr, Martin, Troy Van Voorhis, and Alexandre Tkatchenko. "Theory and practice of modeling van der Waals interactions in electronic-structure calculations." Chemical Society Reviews 48, no. 15 (2019): 4118–54. http://dx.doi.org/10.1039/c9cs00060g.

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Opening the black box of van der Waals-inclusive electronic structure calculations: a tutorial-style introduction to van der Waals dispersion interactions, state-of-the-art methods in computational modeling and complementary experimental techniques.
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48

Abdullina, Dina U., Elena A. Korznikova, Volodymyr I. Dubinko, Denis V. Laptev, Alexey A. Kudreyko, Elvira G. Soboleva, Sergey V. Dmitriev, and Kun Zhou. "Mechanical Response of Carbon Nanotube Bundle to Lateral Compression." Computation 8, no. 2 (April 10, 2020): 27. http://dx.doi.org/10.3390/computation8020027.

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Structure evolution and mechanical response of the carbon nanotube (CNT) bundle under lateral biaxial compression is investigated in plane strain conditions using the chain model. In this model, tensile and bending rigidity of CTN walls, and the van der Waals interactions between them are taken into account. Initially the bundle in cross section is a triangular lattice of circular zigzag CNTs. Under increasing strain control compression, several structure transformations are observed. Firstly, the second-order phase transition leads to the crystalline structure with doubled translational cell. Then the first-order phase transition takes place with the appearance of collapsed CNTs. Further compression results in increase of the fraction of collapsed CNTs at nearly constant compressive stress and eventually all CNTs collapse. It is found that the potential energy of the CNT bundle during deformation changes mainly due to bending of CNT walls, while the contribution from the walls tension-compression and from the van der Waals energies is considerably smaller.
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49

Apostol, M. "On the Van der Waals equation." Open Access Journal of Mathematical and Theoretical Physics 1, no. 5 (October 15, 2018): 215–17. http://dx.doi.org/10.15406/oajmtp.2018.01.00037.

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50

Quevedo, Hernando, María N. Quevedo, and Alberto Sánchez. "Geometrothermodynamics of van der Waals systems." Journal of Geometry and Physics 176 (June 2022): 104495. http://dx.doi.org/10.1016/j.geomphys.2022.104495.

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