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981.
The unified treatment of the Dirac monopole, the Schwinger monopole, and the Aharonov-Bohm problem by Barut and Wilson is revisited via a path integral approach. The Kustaanheimo-Stiefel transformation of space and time is utilized to calculate the path integral for a charged particle in the singular vector potential. In the process of dimensional reduction, a topological charge quantization rule is derived, which contains Dirac's quantization condition as a special case.

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982.
Measurements of slow, singly charged fragments in the target rapidity region have been performed for proton and pion induced reactions with various nuclei at 200 GeV/c. Multiplicity, angular and energy distributions are examined and used to study the effects of rescattering in the nuclear medium. Data are compared to a geometric cascade model and to simulations with the VENUS 3.11 and the FRITIOF 1.7 Monte Carlo codes.  相似文献   
983.
The Prins cyclization of an aldehyde 1 with a homoallylic alcohol 2 , affording tetrahydro‐2H‐pyrans 4 via the oxonium ion 3 as central intermediate, was conceptually transferred to (alk‐3‐enyloxy)acrylates 6 , which form a related oxonium ion 7 upon treatment with acids (Scheme 1). The scope and utility of this modification of the Prins‐type cyclization of oxonium ions is discussed exemplarily by means of the syntheses of ten tetrahydro‐2H‐pyran and tetrahydrofuran derivatives, featuring diverse substitution patterns as well as different degrees of molecular complexity. These target structures include (±)‐ethyl (2RS)‐2‐[(2RS,4SR,6RS)‐ and (2SR,4RS,6SR)‐2‐tetahydro‐4‐hydroxy‐6‐methylpyran‐2‐yl]propanoate ( 23 ), (±)‐ethyl [(2RS, 3RS)‐tetrahydro‐3‐isopropenylfuran‐2‐yl]acetate ( 32 ), (±)‐ethyl (2Z)‐3‐(tetrahydro‐2,2‐dimethylfuran‐3‐yl)acrylate ( 37 ), (±)‐(3aRS,6RS, 7aRS)‐octahydro‐7a‐methylbenzofuran‐6‐yl formate ( 42 ), (±)‐ethyl (2RS,3RS,4aRS,8SR,8aRS)‐hexahydro‐2,5,5,8‐tetramethyl‐7‐oxo‐2H,5H‐pyrano[4,3‐b]pyran‐3‐carboxylate ( 48 ), and (±)‐ethyl (2RS,3RS,6SR)‐tetrahydro‐6‐(2‐methoxy‐2‐oxoethyl)‐3‐methyl‐2H‐pyran‐2‐carboxylate ( 53 ) (see Schemes 3 and 5–8). Besides the stereochemistry and mechanistic details of this versatile oxonium‐ion cyclization, the synthesis of suitable starting materials is also described.  相似文献   
984.
Ligand-directed 2D and 3D Ag(I) coordination networks are self-assembled from the rigid, topologically related tri-amino ligands cis-3,5-diaminopiperidine (cis-dapi) and cis,trans-1,3,5-triaminocyclohexane (trans-tach), yielding two networks of differing dimensionality including a 3D network of unprecedented topology comprising helical channels.  相似文献   
985.
986.
We have investigated the applicability of CNDO/S-type methods for the calculation of optical spectra of molecules with the special implication that the calculations should not only describe the intense, dipole-allowed transitions which dominate the one-photon absorption spectrum but also those transitions which are one-photon forbidden in first-order approximation. We show that such a method is well suited to predict dipole allowed and dipole forbidden transitions at a similar level of accuracy if double excited configurations are taken into account. In spite of the lack of perfect pairing in NDO methods there are still two types of states which exhibit a different sensitivity towards correlation effects. Therefore, the approximation by which we describe the R-dependence of the Coulomb repulsion gains much more importance than in cases where mainly dipole allowed transitions are of interest. These findings confirm results obtained earlier from theories for which the pairing theorem is valid. The calculated data show an excellent stability with respect to further increase of the number of configurations if at least about 200 energy selected configurations are taken into account.  相似文献   
987.
988.
989.
A sum rule for ionization potentials, similar to the Manne-Åberg theorem, is derived in the framework of a many-body Green's-function formalism. This sum rule is shown to be valid under mainly two conditions: (i) the constant term and the affinity poles of the self-energy part have to be neglected; (ii) the final state wavefunction has to be separable in a free-electron and an (N ? 1)-electron part. The latter assumption is discussed in connection with the sudden approximation which is not used for the derivation of the new sum rule.  相似文献   
990.
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