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Introduction
This document is part of Subvolume B2 'Tables of Excitations from Reactions with Charged Particles. Part 2: Z = 37 - 62' of Volume 19 'Nuclear States...
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54-Xenon
This document is part of Subvolume B2 'Tables of Excitations from Reactions with Charged Particles. Part 2: Z = 37 - 62' of Volume 19 'Nuclear States...
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43-Technetium
This document is part of Subvolume B2 'Tables of Excitations from Reactions with Charged Particles. Part 2: Z = 37 - 62' of Volume 19 'Nuclear States...
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The Structure Functions F2 c , F L and F L c in the Framework of the k T Factorization
We present the perturbative parts of the structure functions F2 c and F L...
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Deep Inelastic J/ψ Production at HERA in the Colour Singlet Model with k T -Factorization
We consider J/ψ meson production in ep deep inelastic scattering in the colour singlet model using the k T...
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One-Loop Corrections to Polarization Observables
We review the physics of polarization observables in high energy reactions in general and discuss the status of NLO one–loop corrections to these...
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Medical Applications of Accelerated Ions
Accelerated ions have significant advantages for radiotherapy. From the physical side these are the inverse depth dose profile (the increase of the...
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Weak Interaction Studies by Precision Experiments in Nuclear Beta Decay
The framework and formalism related to the study of symmetries and the structure of the weak interaction in nuclear β-decay are presented and...
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Experiments with Radioactive Nuclear Beams
These lectures concern experiments with radioactive ion beams. After a brief historical overview, the different production methods for radioactive...
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4 × 4 Transfer Matrix T p for Dielectric Helical Films
Dielectric helical thin films (DHTF’s) are described by a homogeneous rotation of an arbitrarily oriented symmetric dielectric function tensor ɛ...
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Polaritons in Semiconductor Layer Structures
The infrared optical response of layered structures composed of polar semiconductor materials is strongly influenced by resonant excitation of...
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Coherent Elastic Nuclear Resonant Scattering
In the field of x-ray diffraction, the intensity and the direction of scattered waves are determined by the properties of the individual scatterers...
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Zincblende-Structure Materials (III–V)
The following chapters will provide different examples including various semiconductor materials of contemporary interest and with diverse...
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5. Simulation of Active and Nonlinear Photonic Nano-Materials in the Finite-Difference Time-Domain (FDTD) Framework
A numerical method is presented that unites three-dimensional finite-differnce time-domain (FDTD) computer simulations of active, nonlinear photonic...
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13. Parallel Implementation Strategiesfor Algorithms from Scientific Computing
Many applications from scientific computing are computationally intensive and can therefore benefit from a realization on a parallel or a distributed...
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Measurement of the $b\bar{b}$ Production Cross Section in 920 GeV Fixed-Target Proton-Nucleus Collisions at the HERA-B Detector
The $b\bar{b}$ production cross section has been measured using...
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BaBar Experiment Status and Recent Results
The BaBar detector at SLAC PEP-II asymmetric B-Factory has collected between 1999 and 2002 a data sample of 88 millions...
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Heavy Quarks on the Lattice
I review the basic ideas behind lattice QCD calculations that involve charm and bottom quarks. I report on the progress in getting the correct...
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Appendix B: The Relation between Minkowski and Euclidean Actions
The Minkowski action leads to canonical quantization and it is used to calculate matrix elements of the evolution operator e...
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5 The Confinement of SU(3) Color Charges
If we wish to describe color confinement in terms of the Meissner effect of a dual superconductor, we need to adapt the Landau-Ginzburg model to the...