scholarly journals The Systems of Volume-Localized Electron Quantum Levels of Charged Fullerenes

2018 ◽  
Vol 2018 ◽  
pp. 1-10 ◽  
Author(s):  
Rafael V. Arutyunyan ◽  
Alexander V. Osadchy

The existence of a system of short-lived, discrete, volume-localized electron quantum levels in positively charged fullerenes is theoretically and numerically demonstrated using the example of fullerenes C60 and C20. Unlike experimentally and theoretically well-studied electron states localized in a thin surface layer, these electron states are due to the flat part of the Coulomb potential of a positively charged fullerene sphere. The energy width of the system of such discrete volume-localized levels depends on the charge and increases with increasing charge. For C60+1, the energy width is 0.16 a.u. and increases up to 0.9 a.u. for fullerene C60+10. Thus, the electrons captured on these discrete levels of fullerene form a sort of short-lived superheavy “nanoatom” or “nanoion,” in which the electrons are localized inside a positively charged spherical “nucleus” with an atomic mass of 240 a.u. for C20 and 720 a.u. for C60. Numerous published papers have demonstrated theoretically and experimentally the existence of metastable positively charged C60 fullerenes with a charge of +10 or more, which suggests the possibility of experimental observation of the considering system of volume-localized electronic states. In conclusion, questions are discussed and estimates are made of the possibility of generating coherent radiation at these transitions.

Author(s):  
yifan yang ◽  
Lorenz S Cederbaum

The low-lying electronic states of neutral X@C60(X=Li, Na, K, Rb) have been computed and analyzed by employing state-of-the-art high level many-electron methods. Apart from the common charge-separated states, well known...


2006 ◽  
Vol 62 (5) ◽  
pp. 775-789 ◽  
Author(s):  
Michel Evain ◽  
Vaclav Petricek ◽  
Yves Moëlo ◽  
Colette Maurel

The structure of synthetic levyclaudite-(Sb), approximately (Pb1 − y Sb y S)1.357[Sn1 − x (Cu2) x S2], has been determined by single-crystal X-ray diffraction on the basis of the (3 + 2)-dimensional superspace approach. This misfit-layer compound, of the cylindrite type, results from the combination of two heavily modulated triclinic Q and H subsystems with a common q wavevector and only one shared reciprocal axis (stacking direction). The Q pseudo-tetragonal layer, ∼(Pb0.70Sb0.30S), derived from the NaCl archetype, is positively charged; the H pseudo-hexagonal layer, ∼(Sn0.85Cu0.30S2), derived from the CdI2 archetype, is negatively charged, owing to the replacement of Sn4+ in an octahedral coordination by Cu+ pairs in an opposite triangular coordination. The analysis shows a strong transverse displacive modulation of the two layers, referred to as a `mondulation', correlated to a maximal Sb site occupation factor in the concavity of the Q layer undulation. The wavelength control of the `mondulation' obeys the vernier principle (14cQ ≅ 13cH ), which would correspond to an energy minimization through a charge transfer density modulation wave, common to all two-dimensional misfit-layer inorganic compounds.


2000 ◽  
Vol 14 (24) ◽  
pp. 2587-2596
Author(s):  
KE-QIU CHEN ◽  
XUE-HUA WANG ◽  
BEN-YUAN GU

Using a effect-barrier height method, we investigate the effect of coupling between normal and lateral degree of freedom of an electron on the localized electronic states at zero and finite magnetic fields perpendicular to interfaces in SL's with structural defect layer within the framework of effective-mass theory. The numerical calculations for GaAs/AlxGa1-xAs material show that minibands, minigaps and localized levels is obviously dependent on the transverse wave number kxy. Magneto-coupling effect brings about not only the splitting of the localized electron levels but also the definite dependence of the minibands, minigaps, localized levels and localization degree on magnetic field and Landau indices. It is believed that applying an appropriate magnetic field may provide a available way to control the minibands, minigaps and localized levels in structural defect superlattice's to match practice requirements.


Blood ◽  
2005 ◽  
Vol 106 (11) ◽  
pp. 2326-2326
Author(s):  
Jose R. Romero ◽  
Sandra M. Suzuka ◽  
Raouf Alami ◽  
Steven N. Feiring ◽  
Eric E. Bouhassira ◽  
...  

Abstract Transgenic mice were generated with human α-chain anti-sickling mutations at contact sites for the HbS polymer. Some of these mice were found to have elevated K-Cl cotransport. Elevation of K-Cl cotransport in patients with homozygous HbS or SC disease increases red cell MCHC and contributes to pathology. In contrast to C57Bl mouse red cells (mRBC) and mRBC expressing only HbA that have little volume-stimulated K-Cl cotransport, we previously reported that HbC under all conditions, and HbS + γ, in the absence of mouse globins, are able to stimulate the activity of K-Cl cotransport in mRBC. These observations support the contention that HbS and HbC stimulate K-Cl cotransport activity in both mouse and human red cells and may do so via the positive charge on the human β-chain. We report here that positively charged α-chains also stimulate K-Cl cotransport in mRBC. Mice expressing α-chain mutants were generated: α49 (HbSavaria, α49S→R, +1 positive charge vs human α) with no human β-globin; α49 and βS; α49 and NY1 (that expresses human α and βS); α49–114, that expresses both α49 and α114 (HbChiapas α114P→R, +2 positive charge vs human α) with no human β-globin; α49–114 and βS; α20 (HbLeLamentin, α20 H→Q, -1 negative charge vs human α) and βS; and α20–114 (that has no average charge difference from human α) with no human β-globin. Mice were bred with α- and β-KO mice and mice expressing the NY1 transgene to produce mice expressing various levels of mutant α, human α, βS, and mouse globins. Density gradients detected increased red cell density relative to wild type mice (C57Bl) in mice expressing α-globins with a positive charge relative to human α. To isolate the effect of charged α-globin, we first examined mice with only mutated α-globins and no βS. We previously measured volume-stimulated K-Cl cotransport in C57Bl and HbAKO mice (that only express HbA) as 2.0±0.9 and 2.4±1.7 mmol/L cells x hr (FU) respectively. We found a similar value (2.4±1.1 FU) in mRBC expressing either 32% or 100% α20–114 with no βS (no charge difference from human α). mRBC expressing α49 at 44 or 100% with no βS had an average value of 12.9±3.3 FU; similarly, mRBC expressing 48% α114-49 with no βS averaged 9.4±1.2 FU. The volume-stimulated K-Cl cotransport was both chloride and okadaic acid sensitive. These results demonstrate that positively charged α-chains stimulate K-Cl cotransport while mutant α-chains without a charge difference do not. We have also examined mRBC expressing α49 or α49–114 with βS or NY1 and found that all mice exhibited increased K-Cl cotransport with the exception of mRBC from founder α49–114βS mice that express 31% mutant α and 9% βS. We conclude that a positive charge in excess of that found on human α can stimulate K-Cl cotransport and result in increased MCHC. In the presence of βS, this effect results in mouse red cells with properties similar to human SC disease and prevents the birth of mice that are fully knocked out, due to polymer formation, despite the presence of anti-sickling mutations. In constrast, mice with α20βS (−1 vs human α) were viable with exclusively human globins. These observations could only have been made by creating mouse models and imply that charge must also be considered when anti-sickling globins are proposed.


1978 ◽  
Vol 234 (6) ◽  
pp. F455-F460 ◽  
Author(s):  
B. M. Brenner ◽  
T. H. Hostetter ◽  
H. D. Humes

The formation of glomerular ultrafiltrate is dependent on the interplay of glomerular pressures and flows as well as the intrinsic permselectivity properties of the glomerular capillary wall. These intrinsic permeability properties serve to exclude macromolecules from the urinary space, based on size as well as net molecular charge discrimination. Neutral dextrans with molecular radii less than 20 A cross the glomerular wall without measurable restriction, whereas dextrans with radii greater than 42 A are almost completely barred. For any given size, negatively charged macromolecules are restricted to a greater extent than neutral molecules. Additionally, positively charged molecules are enhanced in their ability to cross the glomerular wall compared to similarly sized neutral polymers. The concept of a charge barrier, due to fixed negative charges within the glomerular wall, is also supported by morphological studies. Glomerular injury, leading to proteinuria, has been associated with loss of the charge-selective properties of these capillaries. Loss of glomerular fixed negative charges may also result in the foot process fusion and mesangial cell dysfunction often observed in proteinuric states.


2019 ◽  
Vol 74 (4) ◽  
pp. 281-286 ◽  
Author(s):  
Victor P. Stepanov

AbstractThe potential dependence of the contact angle between a gold electrode and lithium, sodium, potassium, rubidium, and caesium chloride melts was studied using the meniscus weight method to establish the patterns of wettability of solid surfaces by ionic melts when changing the composition of the salt phase and the jump of the electric potential. It is found that the forms of the contact angle versus the potential curve of Au change from a convex to a camel-like shape with two maxima upon replacing the lithium chloride with the caesium chloride melt. This phenomenon is explained by the assumption that the adsorption of the halide anions at the positively charged electrode surface has a chemical rather than electrostatic character. The adsorption process is accompanied by a charge transfer through the interface and the formation of covalent bonds between the adsorbent and adsorbate.


2020 ◽  
Vol 11 (1) ◽  
Author(s):  
Wassilios Papawassiliou ◽  
Aleksander Jaworski ◽  
Andrew J. Pell ◽  
Jae Hyuck Jang ◽  
Yeonho Kim ◽  
...  

AbstractDetecting the metallic Dirac electronic states on the surface of Topological Insulators (TIs) is critical for the study of important surface quantum properties (SQPs), such as Majorana zero modes, where simultaneous probing of the bulk and edge electron states is required. However, there is a particular shortage of experimental methods, showing at atomic resolution how Dirac electrons extend and interact with the bulk interior of nanoscaled TI systems. Herein, by applying advanced broadband solid-state 125Te nuclear magnetic resonance (NMR) methods on Bi2Te3 nanoplatelets, we succeeded in uncovering the hitherto invisible NMR signals with magnetic shielding that is influenced by the Dirac electrons, and we subsequently showed how the Dirac electrons spread inside the nanoplatelets. In this way, the spin and orbital magnetic susceptibilities induced by the bulk and edge electron states were simultaneously measured at atomic scale resolution, providing a pertinent experimental approach in the study of SQPs.


2001 ◽  
Vol 19 (1) ◽  
pp. 117-119 ◽  
Author(s):  
Dai Zhen-Hong ◽  
Sun Jin-Zuo ◽  
Zhang Li-De ◽  
Li Zuo-Hong ◽  
Huang Shi-Yong ◽  
...  

2010 ◽  
Vol 28 (1) ◽  
pp. 223-232 ◽  
Author(s):  
D. B. Muldrew

Abstract. In this study, ball lightning (BL) is assumed to have a solid, positively-charged core. According to this underlying assumption, the core is surrounded by a thin electron layer with a charge nearly equal in magnitude to that of the core. A vacuum exists between the core and the electron layer containing an intense electromagnetic (EM) field which is reflected and guided by the electron layer. The microwave EM field applies a ponderomotive force (radiation pressure) to the electrons preventing them from falling into the core. The energetic electrons ionize the air next to the electron layer forming a neutral plasma layer. The electric-field distributions and their associated frequencies in the ball are determined by applying boundary conditions to a differential equation given by Stratton (1941). It is then shown that the electron and plasma layers are sufficiently thick and dense to completely trap and guide the EM field. This model of BL is exceptional in that it can explain all or nearly all of the peculiar characteristics of BL. The ES energy associated with the core charge can be extremely large which can explain the observations that occasionally BL contains enormous energy. The mass of the core prevents the BL from rising like a helium-filled balloon – a problem with most plasma and burning-gas models. The positively charged core keeps the negatively charged electron layer from diffusing away, i.e. it holds the ball together; other models do not have a mechanism to do this. The high electrical charges on the core and in the electron layer explains why some people have been electrocuted by BL. Experiments indicate that BL radiates microwaves upon exploding and this is consistent with the model. The fact that this novel model of BL can explain these and other observations is strong evidence that the model should be taken seriously.


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