Single-Spin Density Gradient Systems and Micropreparative Ultracentrifugation

Lipoproteins ◽  
1993 ◽  
Author(s):  
John Bauer
1991 ◽  
Vol 37 (6) ◽  
pp. 853-858 ◽  
Author(s):  
Tom P J Dormans ◽  
Dorine W Swinkels ◽  
Jacqueline de Graaf ◽  
Jan C M Hendriks ◽  
Anton F H Stalenhoef ◽  
...  

Abstract Single-spin density-gradient ultracentrifugation (DUC) has proven to be a reproducible method for detection of low-density-lipoprotein (LDL) heterogeneity. Recently another method has been described for this: gradient gel electrophoresis (GGE) of serum, a method that might be more suitable for screening. To gain insight into the relationship of GGE to DUC and into their reproducibility, we determined LDL heterogeneity by DUC and GGE in 41 healthy individuals. In 90.2% (n = 37) of the subjects, the number of LDL subfractions found by both methods agreed. In addition, the density and the relative migration distance of the predominant LDL subfraction observed with the respective methods showed a strong correlation (Pearson correlation, r = 0.85, P less than 0.0001). Although it was not possible to compare for all aspects of LDL heterogeneity, these data suggest that GGE is a valid method of analysis for LDL heterogeneity. In screening programs, it may be necessary to store samples. Therefore, we studied in 24 sera the influence of storage at -80 degrees C for one, four, and 12 weeks on the LDL subfraction distribution detected by each method. LDL heterogeneity was maintained during storage under these conditions.


1979 ◽  
Vol 20 (2) ◽  
pp. 397-403 ◽  
Author(s):  
G. L. Oliver ◽  
J. P. Perdew

2021 ◽  
Author(s):  
Farid Kalhor ◽  
Li-Ping Yang ◽  
Leif Bauer ◽  
Noah F Opondo ◽  
Shoaib Mahmud ◽  
...  

Molecules ◽  
2020 ◽  
Vol 25 (15) ◽  
pp. 3537 ◽  
Author(s):  
Giovanna Bruno ◽  
Giovanni Macetti ◽  
Leonardo Lo Presti ◽  
Carlo Gatti

Despite its role in spin density functional theory and it being the basic observable for describing and understanding magnetic phenomena, few studies have appeared on the electron spin density subtleties thus far. A systematic full topological analysis of this function is lacking, seemingly in contrast to the blossoming in the last 20 years of many studies on the topological features of other scalar fields of chemical interest. We aim to fill this gap by unveiling the kind of information hidden in the spin density distribution that only its topology can disclose. The significance of the spin density critical points, the 18 different ways in which they can be realized and the peculiar topological constraints on their number and kind, arising from the presence of positive and negative spin density regions, is addressed. The notion of molecular spin graphs, spin maxima (minima) joining paths, spin basins and of their valence is introduced. We show that two kinds of structures are associated with a spin–polarized molecule: the usual one, defined through the electron density gradient, and the magnetic structure, defined through the spin density gradient and composed in general by at least two independent spin graphs, related to spin density maxima and minima. Several descriptors, such as the spin polarization index, are introduced to characterize the properties of spin density critical points and basins. The study on the general features of the spin density topology is followed by the specific example of the water molecule in the 3B1 triplet state, using spin density distributions of increasing accuracy.


2021 ◽  
Vol 3 (4) ◽  
Author(s):  
Farid Kalhor ◽  
Li-Ping Yang ◽  
Leif Bauer ◽  
Zubin Jacob

2021 ◽  
Author(s):  
Farid Kalhor ◽  
Li-Ping Yang ◽  
Leif Bauer ◽  
Noah F Opondo ◽  
Sunil Bhave ◽  
...  

Author(s):  
Byung H. Chung ◽  
Jere P. Segrest ◽  
Marjorie J. Ray ◽  
John D. Brunzell ◽  
John E. Hokanson ◽  
...  

1979 ◽  
Vol 44 ◽  
pp. 307-313
Author(s):  
D.S. Spicer

A possible relationship between the hot prominence transition sheath, increased internal turbulent and/or helical motion prior to prominence eruption and the prominence eruption (“disparition brusque”) is discussed. The associated darkening of the filament or brightening of the prominence is interpreted as a change in the prominence’s internal pressure gradient which, if of the correct sign, can lead to short wavelength turbulent convection within the prominence. Associated with such a pressure gradient change may be the alteration of the current density gradient within the prominence. Such a change in the current density gradient may also be due to the relative motion of the neighbouring plages thereby increasing the magnetic shear within the prominence, i.e., steepening the current density gradient. Depending on the magnitude of the current density gradient, i.e., magnetic shear, disruption of the prominence can occur by either a long wavelength ideal MHD helical (“kink”) convective instability and/or a long wavelength resistive helical (“kink”) convective instability (tearing mode). The long wavelength ideal MHD helical instability will lead to helical rotation and thus unwinding due to diamagnetic effects and plasma ejections due to convection. The long wavelength resistive helical instability will lead to both unwinding and plasma ejections, but also to accelerated plasma flow, long wavelength magnetic field filamentation, accelerated particles and long wavelength heating internal to the prominence.


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