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Journal articles on the topic 'One to one interaction'

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Published: 4 June 2021

Last updated: 1 February 2022

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1

GUO, HUAIMING, and SHUN-QING SHEN. "EFFECT OF INTERACTION IN ONE-DIMENSIONAL TOPOLOGICAL INSULATOR." International Journal of Modern Physics B 27, no. 07 (March 10, 2013): 1361001. http://dx.doi.org/10.1142/s0217979213610018.

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The one-dimensional interacting topological insulator is studied by means of exact diagonalization method. The topological properties are examined with the existence of the edge states and the quantized berry phase at half-filling. It is found that the topological phases are not only robust to small repulsive interactions but also are stabilized by small attractive interactions and also finite repulsive interaction can drive a topological nontrivial phase into a trivial one while the attractive interaction can drive a trivial phase into a nontrivial one. These results could be realized experimentally using cold atoms trapped in the 1D optical lattice.

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2

Li, Zhou, and Xiangming Hu. "Optomechanical quantum-state transfer beyond one-to-one interaction." Journal of Physics B: Atomic, Molecular and Optical Physics 45, no. 18 (August 30, 2012): 185503. http://dx.doi.org/10.1088/0953-4075/45/18/185503.

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3

Wells, John D., William L. Fuerst, and Joobin Choobineh. "Managing information technology (IT) for one-to-one customer interaction." Information & Management 35, no. 1 (January 1999): 53–62. http://dx.doi.org/10.1016/s0378-7206(98)00076-7.

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4

Boström, M., J. J. Longdell, D. J. Mitchell, and B. W. Ninham. "Resonance interaction between one excited and one ground state atom." European Physical Journal D - Atomic, Molecular and Optical Physics 22, no. 1 (January 1, 2003): 47–52. http://dx.doi.org/10.1140/epjd/e2002-00214-0.

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5

Kolomeisky, Eugene B. "Interaction, disorder, and commensurability in one and nearly one dimension." Physical Review B 48, no. 8 (August 15, 1993): 4998–5003. http://dx.doi.org/10.1103/physrevb.48.4998.

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6

WEI, BO-BO. "TWO ONE-DIMENSIONAL INTERACTING PARTICLES IN A HARMONIC TRAP." International Journal of Modern Physics B 23, no. 18 (July 20, 2009): 3709–15. http://dx.doi.org/10.1142/s0217979209053345.

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In this brief report, two one-dimensional interacting particles interacting with a delta interaction in a harmonic trap is discussed. For strong interactions, we derive the asymptotic expressions for all the energy levels. In addition, the variational method is used to obtain asymptotic ground state energy and wave function. The variational results are compared with the exact solution and they turn out to agree very well.

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7

NAKANO, KYOHEI, ROBERT EDER, and YUKINORI OHTA. "EXACT WAVEFUNCTION OF THE ONE-DIMENSIONAL DOUBLE-EXCHANGE MODEL WITH ONE ELECTRON." International Journal of Modern Physics B 26, no. 30 (October 7, 2012): 1250154. http://dx.doi.org/10.1142/s0217979212501548.

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We study the one-dimensional double-exchange model with L localized spins and one mobile electron. We solve the Schrödinger equation analytically and obtain the energies and wavefunctions for all the eigenstates with spin S = (l-1)/2 exactly. As an application, we compute the single-particle Green's function. We show that, for vanishing exchange interactions between localized spins, the single-particle spectrum is entirely incoherent and the lowest band has an infinite band mass, i.e., the single electron is localized due to its interaction with the spin excitations. For nonvanishing exchange interactions between localized spins, the lower edge of the spectrum acquires a dispersion but the spectrum remains incoherent with no well-defined quasiparticle peak.

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8

Odabaşoğlu, Mustafa, and Orhan Büyükgüngör. "3-Anilinoisobenzofuran-1(3H)-one." Acta Crystallographica Section E Structure Reports Online 62, no. 7 (June 21, 2006): o2943—o2944. http://dx.doi.org/10.1107/s1600536806022537.

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Crystals of the title compound, C14H11NO2, are stabilized by an intermolecular N—H...O hydrogen bond and a weak π–π interaction. N—H...O hydrogen-bond interactions generate C(6) chains. The phthalide section of the molecule is planar and the dihedral angle between the phthalide group and the benzene ring is 78.43 (5)°.

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9

Creech, Andrea. "Interpersonal behaviour in one-to-one instrumental lessons: An observational analysis." British Journal of Music Education 29, no. 3 (April 2, 2012): 387–407. http://dx.doi.org/10.1017/s026505171200006x.

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This paper explores patterns of interpersonal behaviour amongst teachers and pupils during one-to-one instrumental lessons. It was hypothesised that these patterns might differ in systematic ways, according to an existing model of six interaction ‘types’ developed within a systems theory perspective and based on measures of interpersonal control and responsiveness. Eleven violin teachers and their pupils aged 10–16 were observed. Digital recordings of 23 one-to-one lessons were analysed using the overarching categories of teacher talk, teacher questioning, scaffolding, pupil talk and pupil playing. Behaviour style was found to correspond with the model of interpersonal interaction in instrumental teaching. Highly directive teachers were found to engage most often in scaffolding, while the most responsive teachers allowed space for the pupil voice to be heard and provided more feedback that was attributed to specific strategies or effort. These findings suggest that teachers and pupils may become entrenched in fixed patterns of interaction behaviour that potentially place constraints on teaching and learning outcomes. The implications for practice lie in teachers’ awareness and reflections on their own interaction behaviours. Being cognisant of fixed patterns of behaviour, teachers may choose to re-frame their style of interaction, thus effecting positive changes in teaching and learning.

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10

Lu, G. X., L. Q. Yang, and J. H. Lin. "One-dimensional magnetic interaction in BaMn2Si2O7." Solid State Communications 114, no. 2 (March 2000): 113–16. http://dx.doi.org/10.1016/s0038-1098(00)00011-9.

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11

Kexin Liu, Linfang Shen, Xiaodong Zheng, and Sailing He. "Interaction Between Two One-Way Waveguides." IEEE Journal of Quantum Electronics 48, no. 8 (August 2012): 1059–64. http://dx.doi.org/10.1109/jqe.2012.2202215.

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12

Tachibana, Akitomo, Takayuki Inoue, Tokio Yamabe, and Kenzi Hori. "Vibronic interaction in one-dimensional polymer." International Journal of Quantum Chemistry 30, no. 5 (November 1986): 575–79. http://dx.doi.org/10.1002/qua.560300502.

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13

Mitchell, D. B., Y. Nogami, and N. D. Whelan. "Relativistic versus nonrelativistic Hartree–Fock calculations: solvable examples in one dimension." Canadian Journal of Physics 67, no. 6 (June 1, 1989): 583–86. http://dx.doi.org/10.1139/p89-106.

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Relativistic and nonrelativistic one-dimensional systems of particles of the same mass interacting through instantaneous contact interactions are considered. For the relativistic interaction, we assume a combination of a Lorentz scalar and a vector. The mass and interaction strength are chosen such that the deuteron is simulated; the relativistic and nonrelativistic "deuteron" models have the same binding energy and practically the same structure. The relativistic and nonrelativistic Hartree–Fock equations can both be solved analytically. For certain combinations of the Lorentz scalar and vector interactions, the difference between the relativistic and nonrelativistic results can be appreciable.

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14

Kuchen, Benjamin, Fabio Vazquez, Yolanda Paola Maturano, Gustavo J. E. Scaglia, Licia María Pera, and Martha Dina Vallejo. "Toward application of biocontrol to inhibit wine spoilage yeasts: The use of statistical designs for screening and optimisation." OENO One 55, no. 2 (April 19, 2021): 75–96. http://dx.doi.org/10.20870/oeno-one.2021.55.2.4510.

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Spoilage yeasts generate considerable economic losses in the wine industry, and although sulphur dioxide (SO2) is traditionally used for control, its use has become controversial because of its negative effects on health. Biocontrol has emerged as a partial alternative to SO2, and most research has focused on the selection of biocontrol yeasts and/or the mechanisms involved, while little research has been directed to the environmental conditions that make biocontrol effective for application. When there are two or more interacting yeasts, the physicochemical factors that affect their antagonism are many and therefore the application of biocontrol is complex. To reduce SO2, the present study aimed to elucidate biocontrol mechanisms of two yeast interactions and to establish optimal physicochemical conditions for biocontrol of the spoilage yeast during grape must fermentation. Through the use of statistical design, it was possible to find relevant physicochemical factors and optimise them. Wickerhamomyces anomalus “BWa156” developed an active supernatant against ZygoSaccharomyces rouxii “BZr6” while supernatant from Metschnikowia pulcherrima “BMp29” was ineffective. In mixed must fermentations, the first interaction (BWa156 vs. BZr6) showed fewer physicochemical factors impacting biocontrol compared to the second interaction (BMp29 vs. BZr6). However, the fewer factors of the first interaction had a stronger effect on the decline in the spoilage population. Validations showed that the optimal conditions for biocontrol with the first interaction could be predicted. Analysis of the results with BWa156 vs. BZr6 and BMp29 vs. BZr6 suggests that the first interaction is a competition that includes a killer toxin, while the second interaction involves competition for iron resources. Response surface methodology (RSM) allowed a reduction in the number of experiments and permitted to find the optimal biocontrol conditions (SO2: 0 mg mL-1; pH: 3.7; Reducing sugars: 23 °Brix) for the interaction between BWa156 and BZr6.

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15

Ding, Xiaowei, Rende Shui, Shulin Chen, Mowei Shen, and Zaifeng Gao. "Two Equals One: Social Interaction Groups Two Biological Movements as One Unit." Journal of Vision 16, no. 12 (September 1, 2016): 281. http://dx.doi.org/10.1167/16.12.281.

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16

Ding, Xiaowei, Zaifeng Gao, and Mowei Shen. "Two Equals One: Two Human Actions During Social Interaction Are Grouped as One Unit in Working Memory." Psychological Science 28, no. 9 (July 18, 2017): 1311–20. http://dx.doi.org/10.1177/0956797617707318.

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Every day, people perceive other people performing interactive actions. Retaining these actions of human agents in working memory (WM) plays a pivotal role in a normal social life. However, whether the semantic knowledge embedded in the interactive actions has a pervasive impact on the storage of the actions in WM remains unknown. In the current study, we investigated two opposing hypotheses: (a) that WM stores the interactions individually (the individual-storage hypothesis) and (b) that WM stores the interactions as chunks (the chunk-storage hypothesis). We required participants to memorize a set of individual actions while ignoring the underlying social interactions. We found that although the social-interaction aspect was task irrelevant, the interactive actions were stored in WM as chunks that were not affected by memory load (Experiments 1 and 2); however, inverting the human actions vertically abolished this chunking effect (Experiment 3). These results suggest that WM automatically and efficiently used semantic knowledge about interactive actions to store them and support the chunk-storage hypothesis.

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17

Hikida, Michiko, and Jungmin Lee. "Positioning Readers in One-on-One Conferences." Literacy Research: Theory, Method, and Practice 67, no. 1 (July 9, 2018): 180–94. http://dx.doi.org/10.1177/2381336918786887.

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Over the last few decades, scholars have conceptualized academic struggle, including learning disabilities, as socially constructed. When students, especially students of color, are constructed as struggling with school-based literacy, they can experience a variety of negative outcomes including higher dropout rates. In an attempt to unpack how academic struggle was constructed and deconstructed for two fifth-grade readers of color, we conducted a micoanalysis of the interactions between these readers and their teacher in one-on-one reading conferences. We examine how positions of struggle were (de)constructed, and findings suggest that the interactional key of the conferences, which was set by the teacher, seemed to contribute to how the students were positioned as readers within the conferring space.

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18

DING, HANQIN, and JUN ZHANG. "EFFECT OF CORRELATED-HOPPING INTERACTION ON A ONE-DIMENSIONAL EXTENDED HUBBARD MODEL WITH SPIN-EXCHANGE INTERACTION." Modern Physics Letters B 26, no. 07 (March 20, 2012): 1150044. http://dx.doi.org/10.1142/s0217984911500448.

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By using the field-theoretical techniques combining bosonization with renormalization group, we study a one-dimensional (1D) model of interacting electrons with on-site repulsion (U > 0), nearest-neighbor (nn) exchange (J) and correlated-hopping (t2, t3) interactions at weak coupling. In the case of a half-filled band, the two-body interaction t2 does not influence phase diagram of the model, while the presence of three-body interaction t3 makes the physics of the system highly non-trivial. By a Hartree–Fock decoupling, the effects of t3 bring about hopping of pairs, V-like (nn Coulomb interaction) and isotropic exchange terms in the reduced model Hamiltonian. Interestingly, a negative t3 provides a possibility for the occurrence of the triplet superconductivity in 1D system with purely repulsive interactions (U, J > 0). The ground state phase diagram including the insulating and superconducting phases is discussed analytically.

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19

Scott, Thomas, and David W. Riggins. "Work Interaction in Quasi-One-Dimensional Flows." Journal of Propulsion and Power 16, no. 6 (November 2000): 1053–59. http://dx.doi.org/10.2514/2.5675.

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20

Frederico, T., V. S. Timóteo, and Lauro Tomio. "Renormalization of the one-pion-exchange interaction." Nuclear Physics A 653, no. 2 (July 1999): 209–21. http://dx.doi.org/10.1016/s0375-9474(99)00234-1.

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21

De Greve, Jean-Pierre. "Interaction Beyond the Main Sequence: One Recipe?" Symposium - International Astronomical Union 151 (1992): 41–50. http://dx.doi.org/10.1017/s0074180900122041.

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We investigate the different aspects that govern the interaction of post-main-sequence evolution of binaries, using a new, homogeneous set of computations. The set describes the evolution of both components through the phase of mass transfer, till the end of the core helium burning of the primary. The mass range is 9 to 40 Mo, the mass ratios are 0.9 and 0.6 (and introducing 0.99 as a newcomer). Both for small and large masses we discuss the consequences of non-conservative mass transfer. Using a simple concept for the fraction β of transferred matter, we look to its value at the onset of mass transfer for various mass ratios and periods. Exploration of the phase space of interacting binaries reveals the influence of the various parameters on the dimensions of the resulting systems after mass transfer. Special attention is given to binaries with mass ratios very close to one. Their secondaries evolve directly into yellow supergiants such as observed in the LMC.

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22

Lukiyanets, B. A., and N. K. Tovstyuk. "Screened interelectron interaction in one-dimensional crystal." Journal of Physical Studies 1, no. 2 (1997): 251–56. http://dx.doi.org/10.30970/jps.01.251.

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23

Li, You-Quan, Shi-Jian Gu, and Zu-Jian Ying. "One-dimensionalSU(3) bosons with -function interaction." Journal of Physics A: Mathematical and General 36, no. 11 (March 6, 2003): 2821–38. http://dx.doi.org/10.1088/0305-4470/36/11/312.

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24

Lubinsky, Mark S. "One Clinician's View of Clinician/Researcher Interaction." Genetics in Medicine 2, no. 1 (January 2000): 49. http://dx.doi.org/10.1097/00125817-200001000-00022.

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25

Lee, Eun Kyung, Eok Kyun Lee, and Soonchil Lee. "Temperature-dependent RKKY interaction in one dimension." Journal of Physics: Condensed Matter 6, no. 5 (January 31, 1994): 1037–46. http://dx.doi.org/10.1088/0953-8984/6/5/013.

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26

Thomas, K. J., J. T. Nicholls, N. J. Appleyard, M. Y. Simmons, M. Pepper, D. R. Mace, W. R. Tribe, and D. A. Ritchie. "Interaction effects in a one-dimensional constriction." Physical Review B 58, no. 8 (August 15, 1998): 4846–52. http://dx.doi.org/10.1103/physrevb.58.4846.

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27

Fazlutdinov, N. K. "One-dimensional lattice models with nonsummable interaction." Theoretical and Mathematical Physics 63, no. 2 (May 1985): 535–38. http://dx.doi.org/10.1007/bf01017912.

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28

Zolądek, H. "One-dimensional random walk with self-interaction." Journal of Statistical Physics 47, no. 3-4 (May 1987): 543–50. http://dx.doi.org/10.1007/bf01007525.

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29

Šeba, P. "The generalized point interaction in one dimension." Czechoslovak Journal of Physics 36, no. 6 (June 1986): 667–73. http://dx.doi.org/10.1007/bf01597402.

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30

Ding, Hanqin, and Jun Zhang. "Superconductivity in a one-dimensional correlated quantum system." Modern Physics Letters B 30, no. 19 (July 20, 2016): 1650231. http://dx.doi.org/10.1142/s0217984916502316.

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We construct a one-dimensional (1D) theoretical model to clarify the occurrence of superconductivity. The weak-coupling (WC) theory allows a determination of the phase diagram. The constrained hopping induces additional two-body and three-body interactions. At half-filling, the three-body interaction is responsible for the triplet superconducting (TS) correlation. Away from half-filling, the two-body interaction works, favoring the singlet superconducting (SS) correlation. The results are expected to provide an insignificant insight into the superconductivity mechanism.

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31

최은지. "Aspects of Interaction in One-to-one Korean Language Class for Marriage Immigrant." EONEOHAG ll, no. 74 (April 2016): 141–65. http://dx.doi.org/10.17290/jlsk.2016..74.141.

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32

Ovchinnikov, A. A., and A. V. Zabrodin. "One-particle density matrix of a one-dimensional Fermi gas with strong interaction." Physics Letters A 151, no. 8 (December 1990): 420–24. http://dx.doi.org/10.1016/0375-9601(90)90915-b.

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33

Lee, Cheng-Yang. "Symmetries and unitary interactions of mass dimension one fermionic dark matter." International Journal of Modern Physics A 31, no. 35 (December 18, 2016): 1650187. http://dx.doi.org/10.1142/s0217751x16501876.

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The fermionic fields constructed from Elko have several unexpected properties. They satisfy the Klein–Gordon but not the Dirac equation and are of mass dimension one instead of three-half. Starting with the Klein–Gordon Lagrangian, we initiate a careful study of the symmetries and interactions of these fermions and their higher-spin generalizations. We find, although the fermions are of mass dimension one, the four-point fermionic self-interaction violates unitarity at high-energy so it cannot be a fundamental interaction of the theory. Using the optical theorem, we derive an explicit bound on energy for the fermion–scalar interaction. It follows that for the spin-half fermions, the demand of renormalizability and unitarity forbids four-point interactions and only allows for the Yukawa interaction. For fermions with spin [Formula: see text], they have no renormalizable or unitary interactions. Since the theory is described by a Klein–Gordon Lagrangian, the interaction generated by the local [Formula: see text] gauge symmetry which contains a four-point interaction, is excluded by the demand of renormalizability. In the context of the Standard Model, these properties make the spin-half fermions natural dark matter candidates. Finally, we discuss the recent developments on the introduction of new adjoint and spinor duals which may allow us to circumvent the unitarity constraints on the interactions.

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34

Suresh, K. "TIPS ON...Improving one to one interactions." BMJ 325, no. 7355 (July 13, 2002): 15Sa—15. http://dx.doi.org/10.1136/bmj.325.7355.s15a.

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35

Suresh, Kallur. "Tips on… Improving one to one interactions." BMJ 325, Suppl S2 (August 1, 2002): 0208281. http://dx.doi.org/10.1136/sbmj.0208281.

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36

LIU, BOYANG, and JIANGPING HU. "ONE-LOOP RENORMALIZATION GROUP ANALYSIS OF BOSE–FERMI MIXTURES." International Journal of Modern Physics B 26, no. 32 (December 11, 2012): 1250197. http://dx.doi.org/10.1142/s0217979212501974.

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A weakly interacting Bose–Fermi mixture model was investigated using Wisonian renormalization group (RG). This model includes one boson–boson interaction term and one boson–fermion interaction term. The scaling dimensions of the two interaction coupling constants were calculated as 2-D at tree level and the flow equations were derived at one-loop level. We find that in the flow equations the contributions from the fermion loops go to zero as the length scale approaches infinity. In three-dimensional case two fixed points are calculated. One is the Gaussian fixed point and the other one is Wilson–Fisher fixed point. We observe that the boson–fermion interaction decouples at the Wilson–Fisher fixed point. We also find that under RG transformation the boson–fermion interaction coupling constant runs to negative infinity with a small negative initial value, which indicates a boson–fermion pairing instability. Furthermore, the possibility of emergent supersymmetry in this model was discussed.

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37

Pemberton, Steven. "Choose one: fast, correct, or pleasurable." Interactions 9, no. 2 (March 2002): 128–27. http://dx.doi.org/10.1145/505103.505143.

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38

Walker, Ashley Marie, Yaxing Yao, Christine Geeng, Roberto Hoyle, and Pamela Wisniewski. "Moving beyond 'one size fits all'." Interactions 26, no. 6 (October 30, 2019): 34–39. http://dx.doi.org/10.1145/3358904.

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39

Lezkan, Alexandra, Steven G. Manuel, J. Edward Colgate, Roberta L. Klatzky, Michael A. Peshkin, and Knut Drewing. "Multiple Fingers – One Gestalt." IEEE Transactions on Haptics 9, no. 2 (April 1, 2016): 255–66. http://dx.doi.org/10.1109/toh.2016.2524000.

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40

SCHULZ, H. J. "CORRELATED FERMIONS IN ONE DIMENSION." International Journal of Modern Physics B 05, no. 01n02 (January 1991): 57–74. http://dx.doi.org/10.1142/s0217979291000055.

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A brief introduction to the bosonization method for interacting one-dimensional fermion systems is given. Using these results, the long-distance decay of correlation functions in the one-dimensional Hubbard model is determined exactly for arbitrary bandfilling and correlation strength, using the exact solution of Lieb and Wu. For infinite U the results are generalized to the case of nonzero nearest-neighbour interaction. The behaviour of thermodynamic quantities, of the frequency-dependent conductivity, and of the thermopower is also discussed, in particular in the proximity of the metal-insulator transitions occurring for half- and quarter-filling. The one-dimensional Luttinger liquid is shown to be unstable in the presence of interchain hopping. The results for the metal-insulator transition are compared with other scenarios developed in higher dimensions.

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41

Salmanov, A. G., I. Yа Kotsyumbas, and V. V. Trokhymchuk. "One World — One Health." International Journal of Antibiotics and Probiotics 2, no. 1 (April 20, 2018): 8–17. http://dx.doi.org/10.31405/ijap.2-1.18.01.

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The «One Health» concept is gathering momentum and over the next years, International Journal Antibiotics and Probiotics will be publishing a series of articles to help encourage that process. Written by specialists in a range of fields, the articles will consider the meaning of One Health, the interactions between animal and human health and how a collaborative and interdisciplinary approach could help to solve emerging global problems. Governments and scientists worldwide recognised that greater interdisciplinary collaboration was required to prevent and control zoonoses and antimicrobial resistance, and that such collaboration should include not only physicians and veterinarians, but also wildlife specialists, including environmentalists, among others. The expression One Health was proposed as a concept to foster such interdisciplinary collaboration. It has been adopted with great enthusiasm by the veterinary profession and by the international agencies charged with control of zoonoses, most notably the Food and Agriculture Organization (FAO), the World Health Organization (WHO), and the World Organization for Animal Health (OIE). Worldwide, the veterinary profession has promoted the concept of One Health to address such issues as food. It is clear that no one discipline or sector of society has enough knowledge and resources to prevent the emergence or resurgence of diseases in today’s globalised world.

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42

Sloos, Marjoleine. "One rule, two frequency effects." Papers in Historical Phonology 4 (April 27, 2019): 1–21. http://dx.doi.org/10.2218/pihph.4.2019.3014.

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The low-mid unrounded front vowel /ɛː/ in German (as in Bären) has been subject to change since Old High German. It slowly merged with the high-mid unrounded front vowel /eː/, but a reversal seems to have emerged recently. This paper investigates both historical and current change of the Bären vowel. Historical change is investigated through literature-based research; current change is examined through corpus-based research. This paper takes the approach of studying both grammatical context and frequency of use. The two major insights of this study are (i) that the BÄREN vowel has been subject to change for a long time and is still variable, and (ii) that frequency effects interact with grammar in an unexpected way. This interaction shows us how to proceed with hybrid grammar-lexicon modelling and I advocate a combined model of Optimality Theory and Exemplar Theory to account for this type of grammar-frequency interactions.

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43

Sebastián, Miguel Ángel. "Borderline Experiences One Cannot Undergo." Crítica (México D. F. En línea) 47, no. 140 (December 6, 2015): 31–42. http://dx.doi.org/10.22201/iifs.18704905e.2015.495.

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Representationalism maintains that the phenomenal character of an experience is fully determined by its intentional content. Representationalism is a very attractive theory in the project of naturalizing consciousness, on the assumption that the relation of representation can itself be naturalized. For this purpose, representationalists with naturalistic inclinations typically appeal to teleological theories of mental content. Not much attention has been paid, however, to the interaction between representationalism and teleological theories of content. This paper will provide reasons to think that such an interaction is not felicitous. In particular, I will argue that those who endorse the conjunction of these two theories are committed to the existence of impossible experiences.

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44

Dedmon, Robert E. "Broadening our perspectives as physicians: one world-one medicine-one health." Asian Biomedicine 4, no. 3 (June 1, 2010): 497–98. http://dx.doi.org/10.2478/abm-2010-0063.

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Abstract There are no passengers on spaceship earth. We are all crew ! (Marshall Mcluhan). Understanding the emergence of new zoonotic agents requires knowledge of pathogen biodiversity in wildlife, human-wildlife interactions, anthropogenic pressures on wildlife populations, and changes in society and human behavior [1].

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45

Гайсак, І. І., and В. С. Морохович. "SPIN-SPIN INTERACTION IN ONE PARTICLE DIRAC EQUATION." Scientific Herald of Uzhhorod University.Series Physics 4 (June 25, 1999): 66–68. http://dx.doi.org/10.24144/2415-8038.1999.4.66-68.

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46

Al-Zaidee, Salah Rohaima. "Slab-beam Interaction in One-way Floor Systems." Journal of Engineering 24, no. 3 (March 1, 2018): 122. http://dx.doi.org/10.31026/j.eng.2018.03.10.

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This study focuses on the slab-beam interaction in one-way systems. In the context of this study, slab-beam interaction means how beam deflection can affect moment distribution in one-way slabs. This interaction is usually neglected in the traditional approximate analysis that is adopted in engineering practice and design codes. Slab positive moments have been considered as indicators on the accuracy of approximate methods, as they overestimate negative moments while underestimating positive moments. After proposing of effecting parameters in slab-beam interaction including of panel length and width, beam dimensions, and slab thickness, Buckingham’s theorem has been adopted to transform the dimensional-model into a non-dimensional qualitative one. Different case studies with finite element models have been adopted to generate points on the proposed qualitative non-dimensional model. Finally, linear regression analyses have been adopted to develop the corresponding quantitative models. Case studies and corresponding regression analysis indicate that non-dimensional parameters adopted in the model are related linearly with a correlation coefficient in the range of 0.97 and that an error up to 250% may be noted due to neglecting the slab-beam interaction. Therefore, a condition related to the relative stiffness of supporting beams should be added to the current conditions for the approximated methods to be more accurate and more compatible with those adopted in the analysis of two-way systems.

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Lin, Yong Wen, Xiao Chuan You, and Zhuo Zhuang. "One Method of Fluid-Solid Coupled Interaction Simulation." Advanced Materials Research 33-37 (March 2008): 1095–100. http://dx.doi.org/10.4028/www.scientific.net/amr.33-37.1095.

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In this article we presented a method of Fluid-Solid coupled simulation via FLUNET and ABAQUS in problems such as Aero/Hydro-Elasticity problems. UDF (user define function) script file in the Fluent software was utilized as the ‘Connecting File’ between FLUENT and ABAQUS for Aero-Elastic computations. Firstly, the fluid field was computed by Navier-Stokes Equation and the structure movement was directly integrated by the dynamics Equation, respectively. Then, the ‘Connecting File’ exchanged the computed data through the fluid and structure’s interface. The next analysis step continued. Analysis of the computed results showed that this coupling method designed for aero-elastic system was feasible and can be also used for other Fluid-Structure Coupling problems.

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Percus, J. K., and Guihua Zhang. "One-dimensional lattice gas with second-neighbor interaction." Physical Review A 42, no. 2 (July 1, 1990): 731–36. http://dx.doi.org/10.1103/physreva.42.731.

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Qiu-Lan, Zhang. "One-Dimensional Two-Component Bosons with Attractive Interaction." Chinese Physics Letters 24, no. 12 (December 2007): 3300–3303. http://dx.doi.org/10.1088/0256-307x/24/12/003.

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Ciattoni, A., A. Degasperis, and E. DelRe. "A one- and two-dimensional nonlinear pulse interaction." Physical Review E 61, no. 5 (May 1, 2000): R4714—R4717. http://dx.doi.org/10.1103/physreve.61.r4714.

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