Definitions of a single-particle resonance

2006 ◽  
Vol 73 (1) ◽  
Author(s):  
H. T. Fortune
1975 ◽  
Vol 53 (23) ◽  
pp. 2622-2630 ◽  
Author(s):  
S. Kupca ◽  
C. W. Searle

Echoes, following an rf pulse sequence, which originate from excitation and refocusing of elastic modes in powders of various metals were observed in a 10–100 MHz frequency range. The echoes from ferromagnetic and normal metals have many identical properties; differences between them are due to different excitation mechanisms. The experimental evidence suggests that in all cases the echo is formed by refocusing of single particle resonance modes.


2007 ◽  
Vol 650 (2-3) ◽  
pp. 129-134 ◽  
Author(s):  
T. Teranishi ◽  
S. Kubono ◽  
H. Yamaguchi ◽  
J.J. He ◽  
A. Saito ◽  
...  

2002 ◽  
Vol 11 (06) ◽  
pp. 469-473 ◽  
Author(s):  
T. N. LEITE ◽  
N. TERUYA ◽  
H. DIAS

The separation energy and half-life of some heavy proton emitting nuclei, and the single-particle structure of unbound 11 N , have been evaluated by implementing a careful numerical treatment to solve the Schrödinger equation in a continuum discretization context. The basic scheme behind the method consists in using the ground-state proton emitter in connection with an isolated single-particle resonance.


1973 ◽  
Vol 51 (11) ◽  
pp. 1176-1181 ◽  
Author(s):  
J. W. Jury ◽  
J. I. Lodge ◽  
K. H. Lokan ◽  
N. K. Sherman ◽  
R. W. Gellie

Photoneutron energy spectra from 40Ar have been measured at bremsstrahlung end-point energies from 13 to 23 MeV in 1 MeV steps. The differential cross section at 90° for the reaction 40Ar(γ, n0)39Ar revealed some 26 previously unreported excited states of 40Ar in the region below 13 MeV. The envelope of these states suggests a single particle resonance involving the valence 1f7/2 neutrons. The measured total neutron cross section exhibits a marked change from this single particle behavior at about 14 MeV where collective effects begin to dominate and neutrons are emitted to highly excited states of 39Ar.


Author(s):  
J. Frank ◽  
P.-Y. Sizaret ◽  
A. Verschoor ◽  
J. Lamy

The accuracy with which the attachment site of immunolabels bound to macromolecules may be localized in electron microscopic images can be considerably improved by using single particle averaging. The example studied in this work showed that the accuracy may be better than the resolution limit imposed by negative staining (∽2nm).The structure used for this demonstration was a halfmolecule of Limulus polyphemus (LP) hemocyanin, consisting of 24 subunits grouped into four hexamers. The top view of this structure was previously studied by image averaging and correspondence analysis. It was found to vary according to the flip or flop position of the molecule, and to the stain imbalance between diagonally opposed hexamers (“rocking effect”). These findings have recently been incorporated into a model of the full 8 × 6 molecule.LP hemocyanin contains eight different polypeptides, and antibodies specific for one, LP II, were used. Uranyl acetate was used as stain. A total of 58 molecule images (29 unlabelled, 29 labelled with antl-LPII Fab) showing the top view were digitized in the microdensitometer with a sampling distance of 50μ corresponding to 6.25nm.


Author(s):  
Adriana Verschoor ◽  
Ronald Milligan ◽  
Suman Srivastava ◽  
Joachim Frank

We have studied the eukaryotic ribosome from two vertebrate species (rabbit reticulocyte and chick embryo ribosomes) in several different electron microscopic preparations (Fig. 1a-d), and we have applied image processing methods to two of the types of images. Reticulocyte ribosomes were examined in both negative stain (0.5% uranyl acetate, in a double-carbon preparation) and frozen hydrated preparation as single-particle specimens. In addition, chick embryo ribosomes in tetrameric and crystalline assemblies in frozen hydrated preparation have been examined. 2D averaging, multivariate statistical analysis, and classification methods have been applied to the negatively stained single-particle micrographs and the frozen hydrated tetramer micrographs to obtain statistically well defined projection images of the ribosome (Fig. 2a,c). 3D reconstruction methods, the random conical reconstruction scheme and weighted back projection, were applied to the negative-stain data, and several closely related reconstructions were obtained. The principal 3D reconstruction (Fig. 2b), which has a resolution of 3.7 nm according to the differential phase residual criterion, can be compared to the images of individual ribosomes in a 2D tetramer average (Fig. 2c) at a similar resolution, and a good agreement of the general morphology and of many of the characteristic features is seen.Both data sets show the ribosome in roughly the same ’view’ or orientation, with respect to the adsorptive surface in the electron microscopic preparation, as judged by the agreement in both the projected form and the distribution of characteristic density features. The negative-stain reconstruction reveals details of the ribosome morphology; the 2D frozen-hydrated average provides projection information on the native mass-density distribution within the structure. The 40S subunit appears to have an elongate core of higher density, while the 60S subunit shows a more complex pattern of dense features, comprising a rather globular core, locally extending close to the particle surface.


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