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Journal articles on the topic 'Three-body processes'

Author: Grafiati

Published: 4 June 2021

Last updated: 8 February 2022

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1

Karachevtsev, Gennadii V., and Pavel S. Vinogradov. "Three-body ion–molecule processes." Russian Chemical Reviews 68, no. 7 (1999): 549–61. http://dx.doi.org/10.1070/rc1999v068n07abeh000483.

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2

Mebonia, J. V., M. A. Abusini, P. J. Saralidze, K. I. Sulakadze, and G. É. Skhirtladze. "Approach to studying three-body processes." Physics of Atomic Nuclei 63, no. 12 (2000): 2085–90. http://dx.doi.org/10.1134/1.1333878.

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3

Karachevtsev, G. V., and P. S. Vinogradov. "ChemInform Abstract: Three-Body Ion-Molecule Processes." ChemInform 31, no. 3 (2010): no. http://dx.doi.org/10.1002/chin.200003295.

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4

Schulz, M., R. Moshammer, D. Fischer, et al. "Three-dimensional imaging of atomic four-body processes." Nature 422, no. 6927 (2003): 48–50. http://dx.doi.org/10.1038/nature01415.

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5

Alt, E. O., A. S. Kadyrov, and A. M. Mukhamedzhanov. "Approximate triangle amplitude for three-body charge exchange processes." Physical Review A 53, no. 4 (1996): 2438–42. http://dx.doi.org/10.1103/physreva.53.2438.

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6

Valtonen, M. "Three-Body Problem and Multiple Stellar Systems." International Astronomical Union Colloquium 191 (August 2004): 146–51. http://dx.doi.org/10.1017/s0252921100008678.

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AbstractThree-body processes go on in star clusters where binary stars meet single stars and frequently form temporary triple systems. The triples are typically unstable and break up into a new binary and a single star. Also a simple scattering of a single star from a binary may take place. Both processes can be handled by the statistical theories of three-body break-up and scattering. Here we apply the theory to binary stars, assuming that binaries have been involved in the three-body process. The distributions of binary periods, eccentricities and mass ratios are discussed from this point of

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7

Abramov, D. I., V. V. Gusev, and L. I. Ponomarev. "Low energy scattering processes in the Coulomb three-body systems." Nuclear Physics A 684, no. 1-4 (2001): 675–77. http://dx.doi.org/10.1016/s0375-9474(01)00520-6.

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8

Chua, Michael, and Peter A. Tanner. "Three-body energy transfer processes of lanthanide ions in crystals." Journal of Luminescence 66-67 (December 1995): 203–7. http://dx.doi.org/10.1016/0022-2313(95)00137-9.

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9

Boccaccio, P., P. K. Mwose, L. Vannucci, et al. "Three-body processes in the32S+45Sc reaction at 5.6 MeV/u." Il Nuovo Cimento A 106, no. 3 (1993): 379–88. http://dx.doi.org/10.1007/bf02771453.

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10

Dubovichenko, S. B., and A. V. Dzhazairov-Kakhramanov. "Thermonuclear processes for three body system in the potential cluster model." Nuclear Physics A 941 (September 2015): 335–63. http://dx.doi.org/10.1016/j.nuclphysa.2015.07.009.

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11

Briggs, J. S. "Critical second-order scattering in three-body rearrangement and break-up processes." Journal of Physics B: Atomic and Molecular Physics 19, no. 17 (1986): 2703–14. http://dx.doi.org/10.1088/0022-3700/19/17/019.

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12

Mokrik, R. I., and O. M. Ukhans'ka. "Transient processes in a three-component thermoviscoelastic body in ion-exchange diffusion." Soviet Materials Science 27, no. 3 (1992): 291–95. http://dx.doi.org/10.1007/bf00729060.

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13

Keller, S., H. Ast, L. U. Ancarani, C. T. Whelan, H. R. J. Walters, and R. M. Dreizler. "Remark on the theory of three-body effects in relativistic (e,2e) processes." Journal of Physics B: Atomic, Molecular and Optical Physics 31, no. 20 (1998): L873—L876. http://dx.doi.org/10.1088/0953-4075/31/20/005.

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14

Barz, H. W., та B. Kämpfer. "The role of three-body collisions in φ meson production processes near threshold". Nuclear Physics A 683, № 1-4 (2001): 594–604. http://dx.doi.org/10.1016/s0375-9474(00)00446-2.

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15

Holt, J. D., J. Menéndez, and A. Schwenk. "The role of three-nucleon forces and many-body processes in nuclear pairing." Journal of Physics G: Nuclear and Particle Physics 40, no. 7 (2013): 075105. http://dx.doi.org/10.1088/0954-3899/40/7/075105.

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16

Nardi, Enrico, Juan Racker, and Esteban Roulet. "CP violation in scatterings, three body processes and the Boltzmann equations for leptogenesis." Journal of High Energy Physics 2007, no. 09 (2007): 090. http://dx.doi.org/10.1088/1126-6708/2007/09/090.

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17

Ueda, Tamotsu. "Three-body dynamics on pp → pp and pp → pnπ+ processes below 1 GeV". Nuclear Physics A 573, № 4 (1994): 511–40. http://dx.doi.org/10.1016/0375-9474(94)90229-1.

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18

Frolov, A. M. "A study of contact processes in Coulomb three-body systems with unit charges." Journal of Physics B: Atomic, Molecular and Optical Physics 26, no. 23 (1993): L845—L849. http://dx.doi.org/10.1088/0953-4075/26/23/008.

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19

Hu, Min. "Study and Realization of Three-Dimensional Human Body Modeling." Applied Mechanics and Materials 532 (February 2014): 268–71. http://dx.doi.org/10.4028/www.scientific.net/amm.532.268.

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According to characteristic of garment mannequin, this paper puts forward the method of grid surface modeling for three-dimensional human body. Based on the analysis of fitting theory of B-spline curve and surface, it is presented that B-spline curve and surface is used for three-dimensional human modeling. The concrete processes of establishment of three-dimensional human body model are introduced. The results show that the three-dimensional human model which has been successfully achieved can satisfy the requirement of automatic measurement system.

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20

Alt, E. O., A. S. Kadyrov, and A. M. Mukhamedzhanov. "Exact and approximate triangle amplitudes for (in-)elastic three-body processes with charged particles." Journal of Physics B: Atomic, Molecular and Optical Physics 30, no. 16 (1997): 3659–75. http://dx.doi.org/10.1088/0953-4075/30/16/006.

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21

Liu, Yuxin, Ron Noomen, and Pieter Visser. "A gravity assist mapping for the circular restricted three-body problem using Gaussian processes." Advances in Space Research 68, no. 6 (2021): 2488–500. http://dx.doi.org/10.1016/j.asr.2021.06.054.

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22

Bhave, RN, and R. Cooper. "Two- and Three-body Ion-Electron Recombination Rate Coefficients in Neon." Australian Journal of Physics 48, no. 3 (1995): 503. http://dx.doi.org/10.1071/ph950503.

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The rates of recombination of electrons with Net ions over a wide range of pressure (1001000 Torr) and at temperatures of 133, 233 and 295 K were measured. Two- and three-body recombination processes were resolved. The observed two-body rate coefficient is lower than earlier reports. The three-body rate measured agrees well with predictions from Flarinery's modified theory by Bates for termolecular ion-electron recombination in a monatomic gas.

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23

KLASEN, MICHAEL. "CALCULATING TWO- AND THREE-BODY DECAYS WITH FeynArts AND FormCalc." International Journal of Modern Physics C 14, no. 09 (2003): 1273–78. http://dx.doi.org/10.1142/s012918310300539x.

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The Feynman diagram generator FeynArts and the computer algebra program FormCalc allow for an automatic computation of 2→2 and 2→3 scattering processes in High Energy Physics. We have extended this package by four new kinematical routines and adapted one existing routine in order to accomodate also two- and three-body decays of massive particles. This makes it possible to compute automatically two- and three-body particle decay widths and decay energy distributions as well as resonant particle production within the Standard Model and the Minimal Supersymmetric Standard Model at the tree- and l

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24

Giersz, M. "Two Body Capture in Large N Body Systems." Symposium - International Astronomical Union 113 (1985): 419–20. http://dx.doi.org/10.1017/s0074180900147631.

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I have considered the rates of formation of binaries in the following processes: two-body tidal encounters, three-body encounters, self-hardening of soft binaries formed in three-body encounters and two-body encounters connected with gravitational wave radiation. I have considered also the cooling and the heating connected with formation of binaries and the subsequent interactions of binaries with single stars. I have found that the rate of formation of heating binaries in two-body tidal encounters differs from that calculated by Ozernoy and Dokuchaev (1982). These differences are connected fi

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25

Mardling, R. A. "Resonance, Chaos and Stability in the General Three-Body Problem." Proceedings of the International Astronomical Union 3, S246 (2007): 199–208. http://dx.doi.org/10.1017/s1743921308015615.

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AbstractThree-body stability is fundamental to astrophysical processes on all length and mass scales from planetary systems to clusters of galaxies, so it is vital we have a deep and thorough understanding of this centuries-old problem. Here we summarize an analytical method for determining the stability of arbitrary three-body hierarchies which makes use of the chaos theory concept of resonance overlap. For the first time the dependence on all orbital elements and masses can be given explicitly via simple analytical expressions which contain no empirical parameters. For clarity and brevity, a

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26

Kunikeev, Sh D. "Asymptotic expansions for three-body continuum and bound states relevant for ion–atom collision processes." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 154, no. 1-4 (1999): 252–58. http://dx.doi.org/10.1016/s0168-583x(99)00013-0.

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27

Vlahović, B., Ž. Bajzer, and I. Šlaus. "Effect of Coulomb interaction in quasifree scattering and quasifree reactions in three body breakup processes." Physical Review C 49, no. 5 (1994): 2643–49. http://dx.doi.org/10.1103/physrevc.49.2643.

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28

Ambrosio, M. J., L. U. Ancarani, D. M. Mitnik, F. D. Colavecchia, and G. Gasaneo. "A Generalized Sturmian Treatment of (e, 3e) Processes Described as a Three-Body Coulomb Problem." Few-Body Systems 55, no. 8-10 (2014): 825–29. http://dx.doi.org/10.1007/s00601-014-0831-5.

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29

Williamson, C. H. K. "Three-dimensional vortex dynamics in bluff body wakes." Experimental Thermal and Fluid Science 12, no. 2 (1996): 150–68. http://dx.doi.org/10.1016/0894-1777(95)00085-2.

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30

Frascaria, N. "Review of high excitation energy structures in heavy ion collisions: Target excitations and three body processes." Nuclear Physics A 482, no. 1-2 (1988): 245–62. http://dx.doi.org/10.1016/0375-9474(88)90588-x.

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31

He, Ming-Jian, Hong Qi, Yang Li, Ya-Tao Ren, Wei-Hua Cai, and Li-Ming Ruan. "Graphene-mediated near field thermostat based on three-body photon tunneling." International Journal of Heat and Mass Transfer 137 (July 2019): 12–19. http://dx.doi.org/10.1016/j.ijheatmasstransfer.2019.03.082.

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32

SCHULZ, M., and D. H. MADISON. "STUDIES OF THE FEW-BODY PROBLEM IN ATOMIC BREAK-UP PROCESSES." International Journal of Modern Physics A 21, no. 18 (2006): 3649–72. http://dx.doi.org/10.1142/s0217751x06032447.

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Fully differential studies of single ionization of neutral atoms by charged particle impact have proven to be extremely powerful to advance our understanding of the few-body dynamics in atomic processes. Until a few years ago, such data were only available for electron impact and were mostly limited to electrons ejected into the scattering plane. When fully differential data were finally obtained for ion impact covering the entire three-dimensional space, very surprising features were observed. It then became clear that our understanding of ionization processes in atomic collisions is not near

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33

POLOSA, A. D., N. A. TÖRNQVIST, M. D. SCADRON та V. ELIAS. "FOOTPRINTS OF A BROAD σ(600) IN WEAK-INTERACTION PROCESSES". Modern Physics Letters A 17, № 10 (2002): 569–81. http://dx.doi.org/10.1142/s021773230200676x.

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We explore how chiral-symmetry constraints on weak-interaction matrix elements point toward the existence of an intermediate-state σ in several different weak-interaction processes. Particular attention is directed toward recent evidence for a σ within three-body nonleptonic weak decays.

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34

HIGUCHI, Hiroshi. "Passive and Active Controls of Three-Dimensional Wake of Bluff-Body." JSME International Journal Series B 48, no. 2 (2005): 322–27. http://dx.doi.org/10.1299/jsmeb.48.322.

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35

Aleksin, V. A., and Yu D. Shevelev. "Three-dimensional turbulent boundary layer on a body of complex shape." Fluid Dynamics 21, no. 5 (1987): 697–706. http://dx.doi.org/10.1007/bf01050888.

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36

Verspui, M. A., and G. de With. "Three-body abrasion: Influence of applied load on bed thickness and particle size distribution in abrasive processes." Journal of the European Ceramic Society 17, no. 2-3 (1997): 473–77. http://dx.doi.org/10.1016/s0955-2219(96)00148-3.

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37

Popov, Yu V., S. A. Zaytsev, and S. I. Vinitsky. "J-matrix method for calculations of three-body Coulomb wave functions and cross sections of physical processes." Physics of Particles and Nuclei 42, no. 5 (2011): 683–712. http://dx.doi.org/10.1134/s1063779611050042.

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38

Beveren, Eef van, та George Rupp. "S-wave andP-wave ππ andKπ contributions to three-body decay processes in the Resonance- Spectrum Expansion". Journal of Physics G: Nuclear and Particle Physics 34, № 7 (2007): 1789–802. http://dx.doi.org/10.1088/0954-3899/34/7/017.

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39

Alt, E. O., A. S. Kadyrov, A. M. Mukhamedzhanov, and M. Rauh. ""Triangle" diagram with off-shell Coulomb T-matrix for (in-)elastic atomic and nuclear three-body processes." Journal of Physics B: Atomic, Molecular and Optical Physics 28, no. 23 (1995): 5137–50. http://dx.doi.org/10.1088/0953-4075/28/23/019.

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40

Singh, Akhil Kumar. "Pulverizing the Monopoly of Mind: Three Roles of the Body in Cognition." Tattva - Journal of Philosophy 11, no. 1 (2019): 19–29. http://dx.doi.org/10.12726/tjp.21.2.

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For many decades, cognition has been viewed as a computational process in the brain. For cognition, the brain, body and the interaction with the environment are important. Conventional views are inclined towards the existence of discrete and internal representations realised by highly specific mechanisms in the brain. The Embodied approach challenges this view and accepts the evolution of cognitive abilities. There is a shift in focus from the belief that the brain is solely responsible for cognition to the thought that the body is somehow deeply integrated into cognition. However, it does not

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41

Nijhout, H. Frederik, Derek A. Roff, and Goggy Davidowitz. "Conflicting processes in the evolution of body size and development time." Philosophical Transactions of the Royal Society B: Biological Sciences 365, no. 1540 (2010): 567–75. http://dx.doi.org/10.1098/rstb.2009.0249.

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Body size and development time of Manduca sexta are both determined by the same set of three developmental–physiological factors. These define a parameter space within which it is possible to analyse and explain how phenotypic change is associated with changes in the underlying factors. Body size and development time are determined by the identical set of underlying factors, so they are not independent, but because the mechanisms by which these factors produce each phenotype are different, the two phenotypes are only weakly correlated, and the correlation is context dependent. We use a mathema

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42

Wolf, Joschka, Markus Deiß, Artjom Krükow, et al. "State-to-state chemistry for three-body recombination in an ultracold rubidium gas." Science 358, no. 6365 (2017): 921–24. http://dx.doi.org/10.1126/science.aan8721.

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Experimental investigation of chemical reactions with full quantum state resolution for all reactants and products has been a long-term challenge. Here we prepare an ultracold few-body quantum state of reactants and demonstrate state-to-state chemistry for the recombination of three spin-polarized ultracold rubidium (Rb) atoms to form a weakly bound Rb2 molecule. The measured product distribution covers about 90% of the final products, and we are able to discriminate between product states with a level splitting as small as 20 megahertz multiplied by Planck’s constant. Furthermore, we formulat

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43

Spurzem, R., P. Berczik, G. Hensler, et al. "Physical Processes in Star–Gas Systems." Publications of the Astronomical Society of Australia 21, no. 2 (2004): 188–91. http://dx.doi.org/10.1071/as04028.

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AbstractWe first present a recently developed three-dimensional chemodynamic code for galaxy evolution from the Kiev–Kiel collaboration. It follows the evolution of all components of a galaxy, such as dark matter, stars, molecular clouds and diffuse interstellar matter. Dark matter and stars are treated as collisionless N-body systems. The interstellar matter is numerically described by a smoothed particle hydrodynamics approach for the diffuse (hot) gas and a sticky particle scheme for the (cool) molecular clouds. Physical processes, such as star formation, stellar death, or condensation and

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44

Kashko, A. V. "Stability of the flow in the wake behind a three-dimensional body." Fluid Dynamics 19, no. 4 (1985): 649–52. http://dx.doi.org/10.1007/bf01091092.

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45

Gylys, V., H. Jahani, C. Collins, J. Pouvesle, and J. Stevefelt. "The importance of three-body processes to reaction kinetics at atmospheric pressures--II: Occlusive effects of discharge morphology." IEEE Journal of Quantum Electronics 22, no. 1 (1986): 47–50. http://dx.doi.org/10.1109/jqe.1986.1072862.

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46

Anosova, Joanna P. "The Binaries from Unstable Triples. Dynamical Processes of Formation." Highlights of Astronomy 8 (1989): 143–44. http://dx.doi.org/10.1017/s1539299600007644.

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The dynamical processes of formation, evolution and disruption of binaries may be effectively studied by computer simulations in the N > 3-body gravitational problem. As a result of analysis of these investigations of diverse authors, the classification of the dynamical processes of formation of wide and close binaries may be proposed (see Table 1). This Table shows the following general processes: I-triple approaches of the single bodies; II-approaches of binaries with single bodies; Ill-escape from physical triples. The actions of these processes, and kinetics of a frequency of binaries i

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47

Lugni, Claudio, Jingbo Wang, Odd Magnus Faltinsen, Andrea Bardazzi, Alessia Lucarelli, and Wenyang Duan. "Scaling laws for the water entry of a three-dimensional body." Physics of Fluids 33, no. 3 (2021): 036104. http://dx.doi.org/10.1063/5.0038210.

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48

Cheng, Xuhua, and Zhikun She. "A Note on the Existence of a Smale Horseshoe in the Planar Circular Restricted Three-Body Problem." Abstract and Applied Analysis 2015 (2015): 1–8. http://dx.doi.org/10.1155/2015/965829.

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It has been proved that, in the classical planar circular restricted three-body problem, the degenerate saddle point processes transverse homoclinic orbits. Since the standard Smale-Birkhoff theorem cannot be directly applied to indicate the chaotic dynamics of the Smale horseshoe type, we in this note alternatively apply the Conley-Moser conditions to analytically prove the existence of a Smale horseshoe in this classical restricted three-body problem.

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49

Ruiz-Villaverde, Ricardo, Pablo Fernandez-Crehuet, Paula Aguayo-Carreras, Jose L. Hernandez-Centeno, and Carlos Cuenca-Barrales. "Inflammatory Reactions to Red Tattoo Inks: Three cases highlighting an emerging problem." Sultan Qaboos University Medical Journal [SQUMJ] 18, no. 2 (2018): 215. http://dx.doi.org/10.18295/squmj.2018.18.02.016.

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In recent years, tattoos have become more commonplace. However, this can result in various inflammatory processes, the management of which can be challenging in daily clinical practice. Tattoo-related inflammatory reactions can comprise different patterns, including acute and immediate reactions, foreign body granulomas, sarcoid granulomas, isomorphic lesions, allergic contact dermatitis and photosensitivity. We report three cases who were referred to the Dermatology Outpatient Clinic of the Hospital Universitario San Cecilio, Granada, Spain, in 2017 with various skin reactions in the red-ink

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50

Willey, Stephen. "Planning Appeal Processes: Reflections on a Comparative Study." Environment and Planning A: Economy and Space 39, no. 7 (2007): 1676–98. http://dx.doi.org/10.1068/a38315.

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The author reflects on a recent comparative study of the planning appeal systems in England and three Australian states. A range of issues relating to the processes by which appeals are heard, issues of expert evidence, and the composition and expertise of the appeal body are examined. A number of areas where appeal processes might be improved are highlighted and it is concluded that although each of these systems is unique, they are all confronted by similar challenges. In a theoretical sense, the author observes that there is currently a significant lacuna in planning knowledge with respect

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