The multiple scattering of 4.5 MeV electrons

The multiple scattering of 4.5 MeV electrons by foils of aluminium, copper, molybdenum, silver and platinum has been determined, using a photographic method to measure the variation of scattered electron intensity with angle. It was found that the results were in good agreement with the Moliere theory into the region of plural scattering, this being the upper limit of angles covered by the observations.

2014 ◽  
Vol 641-642 ◽  
pp. 179-182 ◽  
Author(s):  
Jin Liang Chen

Through grey estimation of the parameters of logistic equation, a grey logistic forecasting model is established. The effective irrigation area in Liaoning Province was simulated by the model. The simulation results had good agreement with the available data, with a correlation of 0.95. The effective irrigation area was predicted to be 1.583 million hectares in 2018, very close to the predicted upper limit of 1.588 million hectares. Thus, there is little potential for the development of the effective irrigation area, rendering the structural adjustment of agricultural resources very necessary.


2017 ◽  
Vol 19 (1) ◽  
pp. 91-95
Author(s):  
B. Z. Azmi ◽  
Y. T. Ling ◽  
M. Hashim ◽  
W. M. M. Yunus ◽  
M. M. Moksin

The recently developed pyroelectric spectroscopic technique has been used to measure the thermal diffusivity of solids. The method has been applied to conductors and insulator where by the thermal wave is measured at various lateral distances on the sample between laser illuminated line and pyroelectric sensor position. The thermal diffusivity is obtained from the gradient of the plot of thermal wave signal versus the lateral distance. A good agreement to the previously reported thermal diffusivity value has been obtained for aluminium, copper and spray paint that is 0.809 cm2s-1, 1.128 3cm2s-1 and 1.547 x 10-3 cm2s-1 respectively.


1994 ◽  
Vol 159 ◽  
pp. 333-334
Author(s):  
H.-J. Röser ◽  
K. Meisenheimer ◽  
M. Neumann ◽  
R.G. Conway

Previously we have studied the jet of the quasar 3C 273 at optical and radio frequencies. In our first set of X-ray data with 17.2 ksec integration time obtained with the ROSAT HRI, the jet is easily visible extending out from the bright quasar core. The total number of counts in the jet lies in the range 200 to 300, depending on the details of the background model. This corresponds to an X-ray flux fv(2.9 × 1017 Hz) = 65 … 140 nJy (lower limit, synchrotron radiation α = −0.8 … upper limit, bremsstrahlung α = 0, NHI = 1.8 × 1020 cm−2), in good agreement with the value derived from the EINSTEIN observations.


The apparatus described in part I has been employed to determine the energy of the excited states of the nucleus 17 O by observations on the protons from the reaction 16 O ( d , p ) 17 O, and on the α-particles from the reaction 19 F( d , α) 17 O . The protons from the first reaction were observed a t five angles of emission with respect to the primary beam, and the α-particles from the second at four angles. Thirteen excited states of 17 O were observed, evidence for ten of which was given by both reactions. The values for the energy in the different excited states, derived from both reactions and at different angles of observation, are in good agreement. The Q -values of the reactions 16 O( d , p ) 17 O and 19 F( d , α) 17 O , in which the 17 O nucleus is formed in its ground state, are 1.928 and 10.042 MeV, respectively. The Q -value for the reaction 16 O( d , α) 14 N was found to be 3.09 MeV, and the existence of two excited states of 14 N was established. Ten excited states of 20 F were observed in a study of the proton groups from the reaction 19 F( d , p ) 20 F.


1989 ◽  
Vol 44 (3) ◽  
pp. 189-194
Author(s):  
P. Kizler ◽  
P. Lamparter ◽  
S. Steeb

Xanes spectra of the amorphous Fe80B20- and Ni80B20-alloys have been investigated using the electron multiple scattering theory of Durham et al. The calculations were based on several models for the structure of amorphous Fe80B20 and Ni80B20. Very good agreement between theoretical and experimental XANES curves was met. Opposite to former expectations for obtaining information on bond angles by XANES, this study shows that XANES points to more complex features of the structure than can be expressed in terms of bond angles.


1955 ◽  
Vol 8 (1) ◽  
pp. 98 ◽  
Author(s):  
JA McDonell ◽  
MA Hanson ◽  
PR Wilson

The energy loss distributions for 1 MeV electrons traversing aluminium foils of various thicknesses have been investigated experimentally. Several of the foils were of thicknesses such that the distributions were expected to show considerable effects due to multiple scattering. It was found that the most probable energy losses were in good agreement with those predicted by the calculations of Hebbard and Wilson (1955).


2009 ◽  
Vol 23 (23) ◽  
pp. 4755-4765 ◽  
Author(s):  
HAMID EZ-ZAHRAOUY ◽  
ABDELILAH BENYOUSSEF

The effect of several eavesdroppers intercept-resend attacks on the quantum error and mutual information between honest parties of a quantum channel chain is investigated within the BB84 (Bennett and Brassard, 1984). The quantum error and the mutual information are computed for arbitrary number of attacks. It is found that the quantum error and the secured–no secured transition depend strongly on the number N of eavesdroppers and their probabilities of intercepting attacks. For N = 3, numerical calculations show that the quantum error exhibits three kinds of different behaviors as a function of the probability of attack ω1of the first eavesdropper namely: (i) the quantum error remains constant for sufficiently small ω1, (ii) exhibits a plateau for intermediate values of ω1, (iii) increases, passes through a maximum and decreases when increasing ω1. However, depending on the probabilities of attack, phase diagrams present several kinds of topologies, in good agreement with the quantum error behavior. Moreover, in the particular case where all eavesdroppers intercept with identical probabilities ω, the quantum error increases as a nonlinear function with the number of eavesdroppers before reaching an upper limit of ≈ 0.475 for sufficiently large N. Besides, it is shown that the secured–no secured transition occurs under the effect of the number of eavesdroppers.


2015 ◽  
Vol 120 (2) ◽  
pp. 1215-1228 ◽  
Author(s):  
X. Li ◽  
R. S. Selesnick ◽  
D. N. Baker ◽  
A. N. Jaynes ◽  
S. G. Kanekal ◽  
...  

1994 ◽  
Vol 58 (390) ◽  
pp. 1-20 ◽  
Author(s):  
G. T. R. Droop

AbstractThe triple-chain pyriboles jimthompsonite, clinojimthompsonite, and probably chesterite and its monoclinic polytype occur in Lewisian amphibolite-facies ultramafic rocks near Achmelvich, N.W. Scotland. These minerals are intergrown with one another and with amphiboles in prismatic porphyroblasts up to 3 cm long, which are associated with chlorite, carbonate, magnetite and, in some cases, talc. Rocks containing triple-chain silicates have been found at three localities, in each case outcropping in a layer < 1.5 m thick. Clinojimthompsonite is the most abundant triple-chain silicate and generally forms euhedral wedge-shaped overgrowths, measuring up to 1 mm in the b-axis direction, on the {010} faces of actinolite cores. The mineral assemblages are probably of Inverian age.The identification of the triple-chain phases is based mainly on cleavage angle, extinction angle, backscattered electron intensity and, in the case of clinojimthompsonite, on X-ray diffraction data. Microprobe analyses support the identifications. The triple-chain silicates have compositions lying in the system MgO-FeO-SiO2-H2O, with only trace amounts of other components.The cell dimensions of the coarsest clinojimthompsonite are: a = 9.862 ± 0.002 Å, b = 27.184 ± 0.020 Å, c = 5.298 ± 0.004 Å, β = 109.61° ± 0.14° V = 1337.9 ± 1.8 Å3, and its optical properties are as follows: α = 1.600 β = 1.619 γ = 1.628 (all ± 0.001) and optic axial plane = (010). The 2Vα of clinojimthompsonite = 67 ±2°.Back-scattered electron microscopy reveals that although substantial volumes of single-phase clinojimthompsonite are common, (010) intergrowths of Mg,Fe-amphiboles, jimthompsonite polytypes and chesterite polytypes occur locally on scales down to 0.1 µm and probably smaller, indicating considerable chain-width disorder.The triple-chain pyriboles are not pseudomorphous after amphibole and probably grew during prograde Inverian metamorphism. Chemographic constraints suggest that they could have formed from forsterite-bearing assemblages, possibly as the result of infiltration of CO2-rich fluid. Thermodynamic calculations for associated high-variance ultramafic rocks place an upper limit of c. 600–700°C on the temperature of metamorphism.The large number of chemically similar pyriboles and their disposition within compound prisms suggests that crystallization was kinetically controlled. A simple ‘template’ model is propesed to explain the observed patterns, in which the identity of the Mg,Fe-pyribole nucleating at any point on a preexisting actinolite or Mg,Fe-pyribole substrate is controlled by silicate-chain width and/or symmetry (ortho vs. clino), depending on the orientation of the substrate crystal face.


1995 ◽  
Vol 408 ◽  
Author(s):  
S. V. Beiden ◽  
G. Y. Guo ◽  
W. M. Temmerman ◽  
Z. Szotek ◽  
G. A. Gehring ◽  
...  

AbstractWe have implemented the fully relativistic and spin-polarized extension of the O(N) real space locally self-consistent multiple scattering formalism [1]. Here we present preliminary results for the spin and orbital magnetic moments and magneto-crystalline anisotropy in iron metal. The spin and orbital moments are in good agreement with the results of conventional electronic structure methods. In addition we present preliminary results for the magnetocrystalline anisotropy obtained in the frozen potential approximation.


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