The nuclear g factor of the 356-keV level in 196Pt and the internal field on mercury in iron

1968 ◽  
Vol 46 (1) ◽  
pp. 75-78 ◽  
Author(s):  
J. Murray ◽  
T. A. McMath ◽  
J. A. Cameron
Keyword(s):  

1967 ◽  
Vol 45 (5) ◽  
pp. 1813-1819 ◽  
Author(s):  
J. Murray ◽  
T. A. McMath ◽  
J. A. Cameron

The nuclear g factor of the first excited state in 106Pd has been measured by the method of perturbed angular correlations. The perturbing fields used were the internal fields on palladium in dilute iron and cobalt alloys. By comparing the rotation caused by these alloys with the rotation observed when nickel was the host, a measurement of the internal field on palladium in nickel has been obtained.The g factor of the first excited state in 106Pd has been determined to be +0.35 ± 0.03. The internal field on palladium in nickel at room temperature was found to be −174 ± 13 kOe.



1971 ◽  
Vol 49 (21) ◽  
pp. 2646-2650 ◽  
Author(s):  
L. Keszthelyi ◽  
J. A. Cameron ◽  
D. C. Santry

Perturbed angular correlation measurements have been made on the decay of 181Hf implanted in iron. The average integral rotation angle for the 136 keV 9/2+ state of 181Ta is ωτ = 0.051 ± 0.004 rad. For the internal field on Ta in iron of 640 kOe, this gives a nuclear g factor of 0.27 ± 0.04. Alternative explanations of the small rotation are discussed. The E2/M1 mixing ratio of the 136 keV transition was found to be δ = −0.44 ± 0.04.



1975 ◽  
Vol 53 (22) ◽  
pp. 2544-2545 ◽  
Author(s):  
S. A. Wender ◽  
J. A. Cameron

The integral rotation of the 1066 keV 9/2 + level of 65Zn has been measured using the (α,n) reaction in a target of the alloy Ni10Fe90. The average rotation angle measured was ωτ = 150 ± 20 mrad. Using the known lifetime of 829 ± 37 ps and the internal field of −110 ± 25 kOe found for a similar alloy with the 184 keV level of 67Zn, the g factor is g = −0.35 ± 0.10.



1964 ◽  
Vol 12 (02) ◽  
pp. 462-470 ◽  
Author(s):  
F Rodríguez-Erdmann

SummaryAnimals treated in the conventional form to elicit the generalized Shwartzman reaction (gSr) by means of properly spaced injections of endotoxin develop an abrupt consumption of the plasmatic factors of the clotting mechanism, as demonstrated by the reduction of the activity of prothrombin and Ac-G (factor V). These animals show ultimatly characteristic morphological pattern: bilateral cortical necrosis of the kidney. Rabbits treated four hours after the second (‘‘provocative”) endotoxin injection with streptokinase (Varidase/Lederle) in order to activate the fibrinolytic system failed to develop the renal cortical necrosis, but their prothrombin and Ac-G (factor V) level decreased abruptly.Through indirect deduction the intravascular presence of thrombin-like activity is accepted four hours after the “provocative” endotoxin injection.



1970 ◽  
Vol 146 (1) ◽  
pp. 215-219 ◽  
Author(s):  
F.C. Zawislak ◽  
J.D. Bowman
Keyword(s):  


2020 ◽  
Vol 128 (23) ◽  
pp. 235109
Author(s):  
David Ompong ◽  
Godfred Inkoom ◽  
Jai Singh


2021 ◽  
Vol 7 (2) ◽  
pp. 28
Author(s):  
Hamza Cansever ◽  
Jürgen Lindner

The phenomenon of magnetic resonance and its detection via microwave spectroscopy provide insight into the magnetization dynamics of bulk or thin film materials. This allows for direct access to fundamental properties, such as the effective magnetization, g-factor, magnetic anisotropy, and the various damping (relaxation) channels that govern the decay of magnetic excitations. Cavity-based and broadband ferromagnetic resonance techniques that detect the microwave absorption of spin systems require a minimum magnetic volume to obtain a sufficient signal-to-noise ratio (S/N). Therefore, conventional techniques typically do not offer the sensitivity to detect individual micro- or nanostructures. A solution to this sensitivity problem is the so-called planar microresonator, which is able to detect even the small absorption signals of magnetic nanostructures, including spin-wave or edge resonance modes. As an example, we describe the microresonator-based detection of spin-wave modes within microscopic strips of ferromagnetic A2 Fe60Al40 that are imprinted into a paramagnetic B2 Fe60Al40-matrix via focused ion-beam irradiation. While microresonators operate at a fixed microwave frequency, a reliable quantification of the key magnetic parameters like the g-factor or spin relaxation times requires investigations within a broad range of frequencies. Furthermore, we introduce and describe the step from microresonators towards a broadband microantenna approach. Broadband magnetic resonance experiments on single nanostructured magnetic objects in a frequency range of 2–18 GHz are demonstrated. The broadband approach has been employed to explore the influence of lateral structuring on the magnetization dynamics of a Permalloy (Ni80Fe20) microstrip.



Author(s):  
E. Dvoretskaya ◽  
A. Palii ◽  
O. Koplak ◽  
R. Morgunov


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