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Journal articles on the topic 'Three-Body Effects'

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Author: Grafiati

Published: 10 December 2022

Last updated: 28 January 2023

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1

Garrido, E., D. V. Fedorov, and A. S. Jensen. "Three-body halo fragmentation: polarization effects." Europhysics Letters (EPL) 36, no. 7 (December 1, 1996): 497–502. http://dx.doi.org/10.1209/epl/i1996-00259-y.

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2

Sasakawa, T., S. Ishikawa, Y. Wu, and T.-Y. Saito. "Rho-meson exchange three-body force effects." Physical Review Letters 68, no. 24 (June 15, 1992): 3503–6. http://dx.doi.org/10.1103/physrevlett.68.3503.

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3

Glöckle, W., T. S. H. Lee, and F. Coester. "Relativistic effects in three-body bound states." Physical Review C 33, no. 2 (February 1, 1986): 709–16. http://dx.doi.org/10.1103/physrevc.33.709.

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4

Eyre, D., and H. G. Miller. "Sturmian approximation of three-body continuum effects." Physics Letters B 153, no. 1-2 (March 1985): 5–7. http://dx.doi.org/10.1016/0370-2693(85)91429-7.

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5

Oryu, Shinsho, and Hiroshi Yamada. "Effects of the three-body force in three-nucleon systems." Physical Review C 49, no. 5 (May 1, 1994): 2337–41. http://dx.doi.org/10.1103/physrevc.49.2337.

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6

Arena, N., Seb Cavallaro, G. Fazio, G. Giardina, A. Italiano, M. Herman, M. Bruno, F. Cannata, M. D’Agostino, and M. Lombardi. "Three-body effects in theLi7(d,ααn) reaction." Physical Review C 40, no. 1 (July 1, 1989): 55–58. http://dx.doi.org/10.1103/physrevc.40.55.

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7

Knutson, L. D., and A. Kievsky. "Effects of three-body forces in the3Hbound state." Physical Review C 58, no. 1 (July 1, 1998): 49–57. http://dx.doi.org/10.1103/physrevc.58.49.

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8

Prasad, Anil, and Charles H. K. Williamson. "Three-dimensional effects in turbulent bluff body wakes." Experimental Thermal and Fluid Science 14, no. 1 (January 1997): 9–16. http://dx.doi.org/10.1016/s0894-1777(96)00107-0.

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9

Charlton, M., D. P. van der Werf, R. J. Lewis, P. R. Watkeys, and S. J. Kerrigan. "Three-body effects in positron annihilation on molecules." Journal of Physics B: Atomic, Molecular and Optical Physics 39, no. 17 (August 29, 2006): L329—L334. http://dx.doi.org/10.1088/0953-4075/39/17/l03.

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10

PRASAD, ANIL, and CHARLES H. K. WILLIAMSON. "Three-dimensional effects in turbulent bluff-body wakes." Journal of Fluid Mechanics 343 (July 25, 1997): 235–65. http://dx.doi.org/10.1017/s002211209700579x.

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There has recently been a surge in activity concerning the development of three-dimensionality in the wakes of nominally two-dimensional bluff bodies, yielding the realization that end effects can influence the wake vortex shedding pattern over long spanlengths. Much of this work has been focused on low Reynolds numbers (Re), but virtually no studies have investigated to what extent it is possible to control shedding patterns at higher Reynolds numbers, through the use of end manipulation. In the present paper, we demonstrate that it is possible to induce parallel shedding, oblique shedding and vortex dislocations, by manipulation of the end conditions, over a large range of Reynolds number. Such patterns affect the frequency of primary wake instability and its amplitude of fluctuation, as they do at low Reynolds number, although distinct differences are found at the higher Reynolds numbers.We find that imposition of oblique shedding conditions at high Reynolds number leads to a spatial variation of both the oblique shedding angle and shedding frequency across the span, and to sparse dislocations which are not restricted to the spanwise end regions, as they are at low Reynolds numbers (under similar geometrical conditions). In the wake transition regime (Re=190–250), it is confirmed that the spontaneous appearance of vortex dislocations in mode-A shedding precludes the control of shedding patterns using end manipulation. However, it has proven possible to extend the regime of Reynolds number where dislocations ‘naturally’ exist to Re>250, by introducing them artificially through end control, where they would otherwise not occur. The possibility of introducing dislocations and of inducing oblique vortex shedding at higher Reynolds numbers has practical significance, if one can deliberately decorrelate the vortex shedding, and hence reduce the spanwise-integrated unsteady fluid forces on the body.We confirm the existence of a transition in the mode of shedding at Re≈5000 (originally found by Norberg 1987) under conditions where parallel shedding is attempted. This mode transition displays similarities to an inverse of the mode A→mode B transition that is found in the wake transition regime. It is clear that vortex dislocations occur beyond Re=5000, although it is not clear why the flow is unstable to such a mode. Furthermore, there appears to be some support for the suggestion that vortex dislocations may be a feature of the flow for Re at least up to 30×103, as evidenced by the work of Norberg (1994).

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11

Refsgaard, J., H. O. U. Fynbo, O. S. Kirsebom, and K. Riisager. "Three-body effects in the Hoyle-state decay." Physics Letters B 779 (April 2018): 414–19. http://dx.doi.org/10.1016/j.physletb.2018.02.031.

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12

ARGENTINA, MÉDÉRIC, PIERRE COULLET, JEAN-MARC GILLI, MARC MONTICELLI, and GERMAIN ROUSSEAUX. "ROBERT HOOKE'S THREE-BODY PROBLEM." International Journal of Bifurcation and Chaos 19, no. 10 (October 2009): 3435–44. http://dx.doi.org/10.1142/s0218127409024888.

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During the winter 1679, R. Hooke challenged I. Newton to predict the dynamics of an object submitted to a constant radial force. This correspondence made a strong impact on I. Newton, who wrote four years later "De Motu", the real ancestor of "The Principia", published in 1687. R. Hooke's problem can be physically linked to the dynamics of a sphere sliding on an inverted cone due to gravitational effects. If the symmetry axis of the cone is parallel to the gravitational field, the ball executes stable precessions. Breaking this symmetry induces the appearance of chaotic motions. After having derived the equations related to the position of the sphere, we analyze its dynamics, and we perform an approximated Floquet analysis that is compared to our numerical results.

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13

Fedorov, D. V., E. Garrido, and A. S. Jensen. "Three-body halos. III. Effects of finite core spin." Physical Review C 51, no. 6 (June 1, 1995): 3052–65. http://dx.doi.org/10.1103/physrevc.51.3052.

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14

Ghosh Deb, S., and C. Sinha. "Multiphoton effects in three-body recombination for antihydrogen formation." EPL (Europhysics Letters) 88, no. 2 (October 1, 2009): 23001. http://dx.doi.org/10.1209/0295-5075/88/23001.

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15

Ghosh Deb, S., and C. Sinha. "Multiphoton effects in three-body recombination for antihydrogen formation." EPL (Europhysics Letters) 88, no. 4 (November 1, 2009): 49902. http://dx.doi.org/10.1209/0295-5075/88/49902.

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16

Safronov, A. N. "Effects of particle structure in the three-body problem." Theoretical and Mathematical Physics 89, no. 3 (December 1991): 1310–23. http://dx.doi.org/10.1007/bf01017827.

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17

Johnsen, Rainer. "Three-body effects in dissociative recombination of molecular ions." Journal of Physics: Conference Series 204 (January 1, 2010): 012006. http://dx.doi.org/10.1088/1742-6596/204/1/012006.

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18

Kajumov, Sh S., A. M. Mukhamedzhanov, R. Yarmukhamedov, and I. Borb�ly. "Three-body coulomb effects in one-particle transfer reactions." Zeitschrift f�r Physik A Atomic Nuclei 336, no. 3 (September 1990): 297–302. http://dx.doi.org/10.1007/bf01292860.

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19

Brida, I., F. M. Nunes, and B. A. Brown. "Effects of deformation in the three-body structure of." Nuclear Physics A 775, no. 1-2 (August 2006): 23–34. http://dx.doi.org/10.1016/j.nuclphysa.2006.06.012.

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20

Eyre, D., and H. G. Miller. "Sturmian projection and anL2discretization of three-body continuum effects." Physical Review C 32, no. 3 (September 1, 1985): 727–37. http://dx.doi.org/10.1103/physrevc.32.727.

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21

TWEED, R. J., C. TANNOUS, and P. MARCHALANT. "Modelling of three-body effects in a double continuum." Le Journal de Physique IV 03, no. C6 (November 1993): C6–107—C6–116. http://dx.doi.org/10.1051/jp4:1993610.

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22

Bauer, Gernot, Nadezhda Gribova, Alexander Lange, Christian Holm, and Joachim Gross. "Three-body effects in triplets of capped gold nanocrystals." Molecular Physics 115, no. 9-12 (August 29, 2016): 1031–40. http://dx.doi.org/10.1080/00268976.2016.1213909.

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23

Mukhamedzhanov, A. M., and I. Borbely. "Three-body Coulomb effects in neutral-particle-exchange singularity." Few-Body Systems 5, no. 1 (1988): 21–30. http://dx.doi.org/10.1007/bf01080470.

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24

Yang, G. H., and W. M. Garrison. "A comparison of microstructural effects on two-body and three-body abrasive wear." Wear 129, no. 1 (January 1989): 93–103. http://dx.doi.org/10.1016/0043-1648(89)90282-2.

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25

Abouelmagd, Elbaz I., and Juan L. G. Guirao. "On the perturbed restricted three-body problem." Applied Mathematics and Nonlinear Sciences 1, no. 1 (January 28, 2016): 123–44. http://dx.doi.org/10.21042/amns.2016.1.00010.

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AbstractIn this survey paper we offer an analytical study regarding the perturbed planar restricted three-body problem in the case that the three involved bodies are oblate. The existence of libration points and their linear stability are explored under the effects of the perturbations in Coriolis and centrifugal forces. The periodic orbits around these points are also studied under these effects. Moreover, the elements of periodic orbits around these points are determined.

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26

Hicks, Matthew, Douglas Hanes, and Helané Wahbeh. "Expectancy Effect in Three Mind-Body Clinical Trials." Journal of Evidence-Based Complementary & Alternative Medicine 21, no. 4 (July 7, 2016): NP103—NP109. http://dx.doi.org/10.1177/2156587216652572.

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Expectancy, arguably the prime component of the placebo effect, has been shown to significantly modify the effects of many treatments. Furthermore, various forms of mind-body interventions have demonstrated effective improvements in outcomes. The aim of this study was to examine the relationship between pretreatment expectations and symptom reduction in a secondary analysis of 3 mind-body intervention programs. An adjusted correlation and regression analysis compared data from a 6-question expectancy questionnaire to a self-reported clinical impression of change score. Only 1 of the 6 expectancy questions in 1 of the 3 studies reached significance ( B = 0.087; P = .025). The combined data from all 3 studies did not reveal significant expectancy effects. The positive effects of mindfulness meditation appear to be independent of an expectancy effect.

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27

Rouvellou, B., S. Rioual, J. Röder, A. Pochat, J. Rasch, Colm T. Whelan, H. R. J. Walters, and R. J. Allan. "Coulomb three-body effects in electron-impact ionization of argon." Physical Review A 57, no. 5 (May 1, 1998): 3621–26. http://dx.doi.org/10.1103/physreva.57.3621.

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28

Hubbert, J. C., and V. N. Bringi. "The Effects of Three-Body Scattering on Differential Reflectivity Signatures." Journal of Atmospheric and Oceanic Technology 17, no. 1 (January 2000): 51–61. http://dx.doi.org/10.1175/1520-0426(2000)017<0051:teotbs>2.0.co;2.

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29

Gregory, Jonathon K., and David C. Clary. "Three‐body effects on molecular properties in the water trimer." Journal of Chemical Physics 103, no. 20 (November 22, 1995): 8924–30. http://dx.doi.org/10.1063/1.470082.

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30

Tau, M., L. Reatto, R. Maglis, P. A. Egelstaff, and F. Barocchi. "Three-body potential effects in the structure of fluid krypton." Journal of Physics: Condensed Matter 1, no. 39 (October 2, 1989): 7131–48. http://dx.doi.org/10.1088/0953-8984/1/39/025.

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31

Malhotra, R. "Three-body effects in the PSR 1257+12 planetary system." Astrophysical Journal 407 (April 1993): 266. http://dx.doi.org/10.1086/172511.

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32

Hahn, Yukap. "Plasma density effects on the three-body recombination rate coefficients." Physics Letters A 231, no. 1-2 (June 1997): 82–88. http://dx.doi.org/10.1016/s0375-9601(97)00287-9.

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33

Vilela Mendes, R. "Collision states and scar effects in charged three-body problems." Physics Letters A 233, no. 4-6 (September 1997): 265–73. http://dx.doi.org/10.1016/s0375-9601(97)00557-4.

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34

Thomas, Cristina Urdaneta, and M. Muthukumar. "Three‐body hydrodynamic effects on viscosity of suspensions of spheres." Journal of Chemical Physics 94, no. 7 (April 1991): 5180–89. http://dx.doi.org/10.1063/1.460555.

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35

Stachowiak, G. B., and G. W. Stachowiak. "The effects of particle characteristics on three-body abrasive wear." Wear 249, no. 3-4 (May 2001): 201–7. http://dx.doi.org/10.1016/s0043-1648(01)00557-9.

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36

Blaisten-Barojas, Estela, and Hans C. Andersen. "Effects of three-body interactions on the structure of clusters." Surface Science Letters 156 (June 1985): A324. http://dx.doi.org/10.1016/0167-2584(85)90441-4.

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37

Blaisten-Barojas, Estela, and Hans C. Andersen. "Effects of three-body interactions on the structure of clusters." Surface Science 156 (June 1985): 548–55. http://dx.doi.org/10.1016/0039-6028(85)90617-x.

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38

Bacca, S., N. Barnea, W. Leidemann, and G. Orlandini. "Three-body Force Effects on the Longitudinal Response Function of4He." EPJ Web of Conferences 3 (2010): 04009. http://dx.doi.org/10.1051/epjconf/20100304009.

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39

Sarrett, D. C., K. J. M. Söderholm, and C. D. Batich. "Water and Abrasive Effects on Three-body Wear of Composites." Journal of Dental Research 70, no. 7 (July 1991): 1074–81. http://dx.doi.org/10.1177/00220345910700071201.

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40

Singh, J., and T. O. Amuda. "Perturbation effects in the generalized circular restricted three-body problem." Indian Journal of Physics 92, no. 11 (June 29, 2018): 1347–55. http://dx.doi.org/10.1007/s12648-018-1227-z.

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41

Zrnic, D. S., G. Zhang, V. Melnikov, and J. Andric. "Three-Body Scattering and Hail Size." Journal of Applied Meteorology and Climatology 49, no. 4 (April 1, 2010): 687–700. http://dx.doi.org/10.1175/2009jamc2300.1.

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Abstract The three-body scattering signature is an appendage seen on weather radar displays of reflectivity behind strong storm cells. It is caused by multiple scattering between hydrometeors and the ground. The radar equation for this phenomenon is reexamined and corrected to include the coherent wave component producing 3 dB more power than previously reported. Furthermore, the possibility to gauge hail size causing this phenomenon is explored. A model of forward scattering by spherical hail and accepted values of ground backscattering cross sections are used in an attempt to reconcile the reflectivity in this signature with observations. This work demonstrates that the signature can be caused by small- (<10 mm) to moderate- (20 mm) sized hail. An effort to gauge hail size by comparing the direct return from hail with the three-body scattered return is made. The theory indicates fundamental ambiguities in size retrieval resulting from resonant effects. Although theory eliminates the number of hailstones per unit volume, the shape of hail size distribution and the cross section of ground contribute additional uncertainty to the retrieval.

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42

Kumar, Raghul Manosh, Subodh Adhikari, Benjamin Emerson, Christopher A. Fugger, and Timothy Lieuwen. "Blowoff of bluff body flames: Transient dynamics and three dimensional effects." Combustion and Flame 244 (October 2022): 112245. http://dx.doi.org/10.1016/j.combustflame.2022.112245.

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43

Sidhisoradej, Wiwat, Supot Hannongbua, and David Ruffolo. "Three-body Effects in Calcium(II)-ammonia Solutions: Molecular Dynamics Simulations." Zeitschrift für Naturforschung A 53, no. 5 (May 1, 1998): 208–16. http://dx.doi.org/10.1515/zna-1998-0518.

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Abstract Molecular dynamics simulations have been performed with and without three-body corrections at an average temperature of 240 K using a flexible ammonia model. The system consists of one calcium ion and 215 ammonia molecules. The calcium(II)-ammonia interactions were newly developed, based on ab initio calculations with a basis set of double zeta quality. The role of three-body interactions on the structural and dynamical properties of the solution has been investigated. The presence of three-body corrections leads to the reduction of the first shell coordination number of Ca(II) in liquid ammonia from 9 to 8, the increase of the size of the solvation shell by 0.33 A and the disappearance of the sec-ond solvation shell.

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44

Schapotschnikow, Philipp, and Thijs J. H. Vlugt. "Understanding interactions between capped nanocrystals: Three-body and chain packing effects." Journal of Chemical Physics 131, no. 12 (September 28, 2009): 124705. http://dx.doi.org/10.1063/1.3227043.

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45

Madsen, J. N., and K. Taulbjerg. "Ionization in ion-atom collisions: off-shell and three-body effects." Physica Scripta T73 (January 1, 1997): 137–43. http://dx.doi.org/10.1088/0031-8949/1997/t73/044.

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46

Wierzchowski, S. J., Z. H. Fang, D. A. Kofke, and J. L. Tilson. "Three-body effects in hydrogen fluoride: survey of potential energy surfaces." Molecular Physics 104, no. 4 (February 20, 2006): 503–13. http://dx.doi.org/10.1080/00268970500424321.

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47

Ermisch, K., A. M. van den Berg, R. Bieber, M. Hagemann, V. M. Hannen, M. N. Harakeh, M. A. de Huu, et al. "Investigation of effects beyond two-body forces in three-nucleon systems." Nuclear Physics A 689, no. 1-2 (June 2001): 337–40. http://dx.doi.org/10.1016/s0375-9474(01)00849-1.

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48

Oryu, S., S. Nemoto, and H. Yamada. "Effects of a new three-body force in N–d scattering." Nuclear Physics A 689, no. 1-2 (June 2001): 373–76. http://dx.doi.org/10.1016/s0375-9474(01)00858-2.

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49

Nabi, Sk Noor, and Saurabh Basu. "Three body interaction effects on the phase diagram of spinor bosons." Journal of Physics: Conference Series 759 (October 2016): 012034. http://dx.doi.org/10.1088/1742-6596/759/1/012034.

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50

Kalantan-Nayestanaki, N. "Searh for three-body force effects in elastic proton-deuteron scattering." Nuclear Physics A 737 (June 2004): 185–89. http://dx.doi.org/10.1016/j.nuclphysa.2004.03.061.

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