Results 251 to 260 of about 3,973,142 (304)
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Energy loss functions for electron energy loss spectroscopy
Surface Science, 1999Losses to surface excitations affect experimental data in several different kinds of spectroscopies and have been considered in detail by various workers. We discuss and compare calculations using commonly assumed response functions. The boundary (begrenzung) effect, originating in the orthogonality of surface and bulk eigenmodes, manifests interesting
T. Nagatomi, R. Shimizu, R.H. Ritchie
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Energy loss and energy loss straggling for heavy ions
Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms, 1987Abstract Energy loss distributions are reported for low velocity (υ ∼ 0.8 υ0) ions 9 ⩽ Z1 ⩽ 20 after passage through thin C and Al targets. For carbon targets, the energy loss straggling is enhanced for Z1-values near the nodal point of the Z1-oscillation in stopping.
W.N. Lennard, H. Geissel
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Energy loss in general relativity
Physical Review D, 1987Implicit assumptions regarding continuity in energy-loss calculations in general relativity are examined. The Arnowitt-Deser-Misner energy integral is treated in a new manner as a universal vehicle for energy loss. Two explicit examples are given: the electric dipole radiation flux is computed using general relativity as well as the gravitational ...
, Cooperstock, , Lim
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Electrical Engineering, 1931
PRACTICALLY the full text of this paper is published in this issue of Electrical Engineering, pp. 898–900. (A.I.E.E. Paper No. 31–139)
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PRACTICALLY the full text of this paper is published in this issue of Electrical Engineering, pp. 898–900. (A.I.E.E. Paper No. 31–139)
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Energy-loss spectrometer for low-energy pion scattering
Nuclear Instruments and Methods, 1974Abstract The performance of an energy-loss spectrometer is reported together with a detailed discussion of the basic parameters of such a system and in particular the second-order aberrations. The system we have constructed consists of two uniform-field 70° bending sectors in a configuration symmetrical to first order, with an image point in the ...
R.BARBINI +4 more
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Quasi-energies, loss-energies and stochasticity
Reports on Mathematical Physics, 1991Abstract We review the concepts of quasi-energy and loss-energy by discussing examples of simple time-dependent quantum systems such as a free particle with time-varying mass, a one-dimensional harmonic oscillator with time-dependent frequency and a damped harmonic oscillator.
Karner, G., Man'ko, V.I., Streit, Ludwig
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Computed tomography using proton energy loss
Physics in Medicine & Biology, 1981An experiment has been performed to demonstrate the feasibility of proton computed tomography. The proton energy loss was used to measure the projections of the relative stopping power of the phantom. High quality reconstructions were obtained from scans of 19 cm and 30 cm diameter performance phantoms.
K M, Hanson +7 more
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Energy loss minimization for vehicular energy network routing
Proceedings of the Workshop on Electric Vehicle Systems, Data, and Applications, 2016Recently, vehicular energy network (VEN) has been proposed to transport energy over a large geographical area by means of electric vehicles (EVs) over a road network. In the near future, an abundance of EVs, plentiful generation of renewables, and mature wireless energy transfer and vehicular communication technologies will expedite the realization of ...
Lam, AYS, Li, VOK
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1991
Atoms moving in a solid lose energy due to interaction with electrons. This phenomenon, referred to as electronic or inelastic energy loss, can be due to excitation or ionization in both of the colliding atoms, leading to a change in kinematics, which may be handled as discussed in Chap. 2.
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Atoms moving in a solid lose energy due to interaction with electrons. This phenomenon, referred to as electronic or inelastic energy loss, can be due to excitation or ionization in both of the colliding atoms, leading to a change in kinematics, which may be handled as discussed in Chap. 2.
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1990
On the way from the ion irradiation to the observation of the developed track three distinct fields exist, associated with different degrees of complexity (Figure 2–1):
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On the way from the ion irradiation to the observation of the developed track three distinct fields exist, associated with different degrees of complexity (Figure 2–1):
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