812 resultados para Distance decay contiguity


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Nous vivons dans une époque où la mobilité internationale est une pratique très courante; ainsi, de plus en plus de partenaires doivent maintenir leurs relations à distance. Le phénomène va de pair avec le développement des nouvelles technologies, qui introduisent de nouvelles formes et de pratiques pour maintenir l’intimité. Cela soulève des questions sur les pratiques de connexion (ou déconnexion) lorsque les couples sont séparés par la distance et le temps. Ce mémoire propose d’explorer comment les femmes dans des relations amoureuses à distance utilisent divers modes d’expression (visuels, textuels, oraux et tactiles) ainsi que plusieurs sens à travers de multiples technologies mobiles, qui lui permettent de reconstruire la présence et l’intimité avec l’autre. Inspiré par le new mobilities paradigm (Sheller & Urry, 2006), ainsi que les concepts de mobile intimacy (Hjorth & Lim, 2012; Elliott & Urry, 2010) et la présence imaginée (Chayko, 2002; Elliott & Urry, 2010), je propose les notions de (dé) connectivité virtuelle, le lieu virtuel, ainsi que la présence/absence technologique. Utilisant une approche méthodologique mixte, venant des données d’entrevues semi-dirigées, de l’autoethnographie, de la recherche création et de journaux de bord multimédias, certaines pratiques de contrôle et de surveillance, des formes émergentes de travail, l’immédiateté et la réciprocité émergent dans une époque d’interconnectivité.

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The D-eigenvalues of a graph G are the eigenvalues of its distance matrix D, and the D-energy ED(G) is the sum of the absolute values of its D-eigenvalues. Two graphs are said to be D-equienergetic if they have the same D-energy. In this note we obtain bounds for the distance spectral radius and D-energy of graphs of diameter 2. Pairs of equiregular D-equienergetic graphs of diameter 2, on p = 3t + 1 vertices are also constructed.

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The D-eigenvalues of a graph G are the eigenvalues of its distance matrix D, and the D-energy ED(G) is the sum of the absolute values of its D-eigenvalues. Two graphs are said to be D-equienergetic if they have the same D-energy. In this note we obtain bounds for the distance spectral radius and D-energy of graphs of diameter 2. Pairs of equiregular D-equienergetic graphs of diameter 2, on p = 3t + 1 vertices are also constructed.

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A sensitive method based on the principle of photothermal phenomena to study the energy transfer processes in organic dye mixtures is presented. A dual beam thermal lens method can be very effectively used as an alternate technique to determine the molecular distance between donor and acceptor in fluorescein–rhodamine B mixture using optical parametric oscillator.

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Variations in the decay times of the characteristic green emissions at 522.7, 551.3, 549.6, 547.6, 542.2, 540.2, 535.9 and 533.5nm from CaF2 :H03+ with concentration are studied at RT and LNT. A pulsed N2 laser beam of power density 1.5 MW cm-2 is used for the excitation. Temperature dependent concentration quenching of the decay times are observed for all the emission bands. But an increase in the decay time due to the reabsorption process is also observed for a few of the above bands.

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Recent measurements of electron escape from a nonequilibrium charged quantum dot are interpreted within a two-dimensional (2D) separable model. The confining potential is derived from 3D self-consistent Poisson-Thomas-Fermi calculations. It is found that the sequence of decay lifetimes provides a sensitive test of the confining potential and its dependence on electron occupation

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We present an imaginary-time path-integral study of the problem of quantum decay of a metastable state of a uniaxial magnetic particle placed in the magnetic field at an arbitrary angle. Our findings agree with earlier results of Zaslavskii obtained by mapping the spin Hamiltonian onto a particle Hamiltonian. In the limit of low barrier, weak dependence of the decay rate on the angle is found, except for the field which is almost normal to the anisotropy axis, where the rate is sharply peaked, and for the field approaching the parallel orientation, where the rate rapidly goes to zero. This distinct angular dependence, together with the dependence of the rate on the field strength, provides an independent test for macroscopic spin tunneling.

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The nonmesonic decay of the hypertriton is calculated based on a hypertriton wave function and 3N scattering states, which are rigorous solutions of three-body Faddeev equations using realistic NN and hyperon-nucleon interactions. The pion exchange together with heavier meson exchanges for the ¿N¿NN transition is considered. The total nonmesonic decay rate is found to be 0.5% of the free ¿ decay rate. Integrated as well as differential decay rates are given. The p- and n-induced decays are discussed thoroughly and it is shown that the corresponding total rates cannot be measured individually.

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