Results 211 to 220 of about 175,843 (264)
Creep Modeling and Influencing Factor Analysis of Ultradeep Salt Cavern Gas Storage. [PDF]
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Deformed state lattice planning
2017 IEEE/RSJ International Conference on Intelligent Robots and Systems (IROS), 2017Search-based planning that uses a state lattice has been successfully applied in many applications but its utility is limited when confronted with complex problems represented by a lattice with many nodes and edges with high branching factor. However, in many seemingly complex problems, proper “form-fitting” can reduce the number of nodes and edges ...
Zhongqiang Ren +2 more
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Nuclear Physics A, 1968
Abstract We have attempted to explain the energy spectrum and transition rates in 42 Ca by considering admixtures of deformed and shell-model states for the low-lying levels. Using three variational parameters (the deformation parameters) and two fitted parameters (effective charge and f 7 2 - d 3 2 energy splitting), we have ...
B.H. Flowers, L.D. Skouras
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Abstract We have attempted to explain the energy spectrum and transition rates in 42 Ca by considering admixtures of deformed and shell-model states for the low-lying levels. Using three variational parameters (the deformation parameters) and two fitted parameters (effective charge and f 7 2 - d 3 2 energy splitting), we have ...
B.H. Flowers, L.D. Skouras
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q-deformed Coherent States on a Circle
Czechoslovak Journal of Physics, 2004zbMATH Open Web Interface contents unavailable due to conflicting licenses.
Kowalski, Krzysztof +1 more
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Multiphonon vibrational states in deformed nuclei
Physical Review C, 1994The $^{154}\mathrm{Gd}$ nucleus was studied by \ensuremath{\gamma}-ray spectroscopy following the (\ensuremath{\alpha},2n) reaction at an energy of 26 MeV. We identified the double-phonon K=${4}^{+}$ \ensuremath{\gamma}\ensuremath{\gamma} vibrational band in this nucleus at 1645.8 keV.
, Wu +5 more
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The Steady State of Deformation
Journal of the Geotechnical Engineering Division, 1981The steady state of deformation for any mass of particles is that state in which the mass is continuously deforming at constant volume, constant normal effective stress, constant shear stress, and constant velocity. The steady state of deformation is achieved only after all particle orientation has reached a statistically steady-state condition and ...
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Ground-state properties of the deformable jellium
Physical Review A, 1989A self-consistent calculation is done to evaluate relevant ground-state properties of the electron gas in the deformable-jellium model. We get the melting point of the Wigner crystal and the ground-state energy per particle at all densities. The single-particle state function in the Slater determinant is expanded in a basis of periodic functions.
, Méndez-Moreno, , Ortíz, , Moreno
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Physica Scripta, 1983
Experimental information on multi-quasiparticle isomers is compared, with special emphasis on the hafnium isotopes. New results for 174Hf are presented. The co-existence of deformation-aligning and rotation-aligning influences is considered. Residual interactions are studied as a function of the number of quasiparticles, with large effects being ...
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Experimental information on multi-quasiparticle isomers is compared, with special emphasis on the hafnium isotopes. New results for 174Hf are presented. The co-existence of deformation-aligning and rotation-aligning influences is considered. Residual interactions are studied as a function of the number of quasiparticles, with large effects being ...
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Deformation of the nucleon and delta in excited states
Physical Review Letters, 1985A quark model for baryons, in which the valence quarks are moving in a deformable mean field, is considered. A q-q interaction, consisting of one-gluon-exchange and one-pion-exchange potentials, is diagonalized exactly in the model space of deformed orbitals.
, Murthy, , Bhaduri
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Deformation states in nanocrystals
Physics of the Solid State, 2000The limitations of the classical description of static deformations in crystals in nanometric regions are demonstrated. The problem is formulated on the basis of the phonon Hamiltonian supplemented with point force sources of the monopole and dipole types.
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