scholarly journals Deuteron Stripping Cross Section from 13C at Deuteron Energies below 350 keV

1998 ◽  
Vol 51 (6) ◽  
pp. 913 ◽  
Author(s):  
M. M. Nagadi ◽  
A. A. Naqvi ◽  
S. Kidwai ◽  
M. A. Al-Ohali ◽  
F. Z. Khiari
Keyword(s):  
Cross Section ◽  
Deuteron Stripping

THE DEUTERON STRIPPING ANOMALY AT THRESHOLD OF ANALOGUE CHANNEL AND THE 3 - p WAVE NEUTRON STRENGTH FUNCTION

2002 ◽  
Vol 17 (20) ◽  
pp. 1315-1322 ◽  
Author(s):  
HORIA COMISEL ◽  
CORNEL HATEGAN
Keyword(s):  
Experimental Data ◽  
Cross Section ◽  
Strength Function ◽  
Empirical Approach ◽  
P Wave ◽  
The Cross ◽  
Deuteron Stripping ◽  
Analyzing Power

We prove in this paper that the magnitude of anomaly in deuteron stripping reactions on A ≈ 80–110 mass target nuclei, at threshold of analogue channel, is proportional to the 3 - p wave neutron strength function. The result is obtained from analysis, within an empirical approach and computational frameworks, of the cross-section and analyzing power experimental data related to this (d,p) anomaly.

The theory of the deuteron stripping reaction

1952 ◽  
Vol 215 (1122) ◽  
pp. 385-398 ◽  
Keyword(s):  
Wave Function ◽  
Cross Section ◽  
Absolute Magnitude ◽  
Bound State ◽  
Matrix Formalism ◽  
Mathematical Technique ◽  
Reaction Proceeds ◽  
The Cross ◽  
Deuteron Stripping ◽  
Two Sides

The differential cross-section for deuteron stripping reactions at energies several million electron volts above the Coulomb barrier is calculated by a method which is essentially that of Butler as regards physical assumptions and line of argument, but which employs a different mathematical technique and notation at many points, for reasons of clarity and exactitude. The procedure is assimilated into the S -matrix formalism. The essence of the method is the smooth joining up of the wave function for the nucleon stripped off, and the derivative of this wave function, on the two sides of the surface of the target nucleus. The formula obtained is discussed, to show how the various factors arise from the successive physical stages by which the reaction proceeds. New features are ( a ) the cross-section is now given explicitly for the case in which the stripped nucleon is captured into a virtual state, as well as for the case of a bound state, as hitherto; ( b ) the factor determining the absolute magnitude of the cross-section is given explicitly in a form which would permit of estimates being made of it.

The stripping theory of deuteron reactions and the inelastic scattering of deuterons

1957 ◽  
Vol 238 (1215) ◽  
pp. 448-472 ◽  
Keyword(s):  
Inelastic Scattering ◽  
Cross Section ◽  
Approximate Expression ◽  
Proton Interaction ◽  
Zero Range ◽  
Deuteron Stripping ◽  
Nuclear Levels ◽  
Derivatives Of ◽  
Logarithmic Derivatives ◽  
Nuclear Constants

The wave functions for the deuteron stripping process are constructed in a concise form, using the approximations of Butler (1951). The resulting theoretical cross-section for ( d, p ) reactions is determined in terms of the nuclear constants, namely, the reduced widths and the logarithmic derivatives of the target nucleus. The interaction between the neutron and the proton after the stripping has taken place is introduced, and it is shown that the inelastic scattering of deuterons is then predicted. Using the zero-range approximation for the neutron-proton interaction the differential cross-section for ( d, d' ) reactions is obtained. However, the formula is complicated and unsuitable for comparison with experimental results. An approximate expression is derived for the cross-section and comparison is made with the data available on the 24 Mg ( d, d' ) 24 Mg* reaction, but it seems improbable that ( d, d' ) reactions will prove to be useful for determining spins and parities of nuclear levels.

XUV Absorption Spectra of Carbon Ions

1988 ◽  
Vol 102 ◽  
pp. 71-73
Author(s):  
E. Jannitti ◽  
P. Nicolosi ◽  
G. Tondello
Keyword(s):  
Absorption Spectra ◽  
Cross Section ◽  
Theoretical Calculations ◽  
Photoionization Cross Section ◽  
Carbon Ions

AbstractThe photoabsorption spectra of the carbon ions have been obtained by using two laser-produced plasmas. The photoionization cross-section of the CV has been absolutely measured and the value at threshold, σ=(4.7±0.5) × 10−19cm2, as well as its behaviour at higher energies agrees quite well with the theoretical calculations.

Elastic Scattering in Electron Microscopy

1973 ◽  
Vol 31 ◽  
pp. 252-253
Author(s):  
J. Langmore ◽  
M. Isaacson ◽  
J. Wall ◽  
A. V. Crewe
Keyword(s):  
Electron Microscopy ◽  
Elastic Scattering ◽  
Cross Section ◽  
Quantum Noise ◽  
Dark Field ◽  
Elastic Cross Section ◽  
Biological Molecules ◽  
Dark Field Microscopy ◽  
Field Systems ◽  
Effects Of Radiation

High resolution dark field microscopy is becoming an important tool for the investigation of unstained and specifically stained biological molecules. Of primary consideration to the microscopist is the interpretation of image Intensities and the effects of radiation damage to the specimen. Ignoring inelastic scattering, the image intensity is directly related to the collected elastic scattering cross section, σɳ, which is the product of the total elastic cross section, σ and the eficiency of the microscope system at imaging these electrons, η. The number of potentially bond damaging events resulting from the beam exposure required to reduce the effect of quantum noise in the image to a given level is proportional to 1/η. We wish to compare η in three dark field systems.

A New Approach to the Demonstration of Oxidase-Localization Using Tannic Acid Or Catechin

1973 ◽  
Vol 31 ◽  
pp. 698-699
Author(s):  
V. Mizuhira ◽  
Y. Futaesaku
Keyword(s):  
Cross Section ◽  
Tannic Acid ◽  
Elastic Fiber ◽  
The Other ◽  
New Approach ◽  
Tissue Block ◽  
Active Reaction ◽  
The Cross

Previously we reported that tannic acid is a very effective fixative for proteins including polypeptides. Especially, in the cross section of microtubules, thirteen submits in A-tubule and eleven in B-tubule could be observed very clearly. An elastic fiber could be demonstrated very clearly, as an electron opaque, homogeneous fiber. However, tannic acid did not penetrate into the deep portion of the tissue-block. So we tried Catechin. This shows almost the same chemical natures as that of proteins, as tannic acid. Moreover, we thought that catechin should have two active-reaction sites, one is phenol,and the other is catechole. Catechole site should react with osmium, to make Os- black. Phenol-site should react with peroxidase existing perhydroxide.

Electron Irradiation Effects in Polyoxymethylene Crystals Grown Inside Trioxane Crystals

1971 ◽  
Vol 29 ◽  
pp. 78-79
Author(s):  
J. P. Colson ◽  
D. H. Reneker
Keyword(s):  
Cross Section ◽  
Cross Sections ◽  
Detailed Examination ◽  
The Other ◽  
Electron Micrograph ◽  
Irradiation Effects ◽  
Threefold Axis ◽  
Typical Sample ◽  
Polymer Crystals ◽  
Chain Axis

Polyoxymethylene (POM) crystals grow inside trioxane crystals which have been irradiated and heated to a temperature slightly below their melting point. Figure 1 shows a low magnification electron micrograph of a group of such POM crystals. Detailed examination at higher magnification showed that three distinct types of POM crystals grew in a typical sample. The three types of POM crystals were distinguished by the direction that the polymer chain axis in each crystal made with respect to the threefold axis of the trioxane crystal. These polyoxymethylene crystals were described previously.At low magnifications the three types of polymer crystals appeared as slender rods. One type had a hexagonal cross section and the other two types had rectangular cross sections, that is, they were ribbonlike.

Freeze-Fracture Replication of Frozen Outer Segments of Rat Retinal Rods

1969 ◽  
Vol 27 ◽  
pp. 392-393
Author(s):  
Thomas S. Leeson ◽  
C. Roland Leeson
Keyword(s):  
Electron Microscopy ◽  
Cross Section ◽  
Outer Segment ◽  
Freeze Fracture ◽  
X Ray Diffraction ◽  
X Ray ◽  
Outer Segments ◽  
Retinal Rods ◽  
Temperature Electron ◽  
Freeze Etching

Numerous previous studies of outer segments of retinal receptors have demonstrated a complex internal structure of a series of transversely orientated membranous lamellae, discs, or saccules. In cones, these lamellae probably are invaginations of the covering plasma membrane. In rods, however, they appear to be isolated and separate discs although some authors report interconnections and some continuities with the surface near the base of the outer segment, i.e. toward the inner segment. In some species, variations have been reported, such as longitudinally orientated lamellae and lamellar whorls. In cross section, the discs or saccules show one or more incisures. The saccules probably contain photolabile pigment, with resulting potentials after dipole formation during bleaching of pigment. Continuity between the lamina of rod saccules and extracellular space may be necessary for the detection of dipoles, although such continuity usually is not found by electron microscopy. Particles on the membranes have been found by low angle X-ray diffraction, by low temperature electron microscopy and by freeze-etching techniques.

A quantitative approach to inner shell losses

1978 ◽  
Vol 36 (1) ◽  
pp. 526-527 ◽  
Author(s):  
R.D. Leapman ◽  
P. Rez ◽  
D.F. Mayers
Keyword(s):  
Energy Transfer ◽  
Cross Section ◽  
Cross Sections ◽  
Accurate Determination ◽  
Background Intensity ◽  
Core Excitation ◽  
Quantitative Basis ◽  
Cross Section Differential ◽  
Bound Electrons

Microanalysis by EELS has been developing rapidly and though the general form of the spectrum is now understood there is a need to put the technique on a more quantitative basis (1,2). Certain aspects important for microanalysis include: (i) accurate determination of the partial cross sections, σx(α,ΔE) for core excitation when scattering lies inside collection angle a and energy range ΔE above the edge, (ii) behavior of the background intensity due to excitation of less strongly bound electrons, necessary for extrapolation beneath the signal of interest, (iii) departures from the simple hydrogenic K-edge seen in L and M losses, effecting σx and complicating microanalysis. Such problems might be approached empirically but here we describe how computation can elucidate the spectrum shape.The inelastic cross section differential with respect to energy transfer E and momentum transfer q for electrons of energy E0 and velocity v can be written as

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