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An overlooked series of gas phase diatomic metal oxide ions that are long-lived.

Although the "Golden" years of spectroscopy and the major studies on ionization processes now are behind us, as with many branches of science, much yet remains to be gleaned from such topics that is both full of interest and of significance to present day research. Presented here is one such overlooked example, an observation that relates to both these fields. An analysis is presented for the periodic table concerning the gas-phase thermochemical nature of MO+ and MO2+ ions. Unexpectedly, a pattern of 18 elements has been identified that exhibit the potential for having long-lived MO+ ions. Normally such molecular ions are expected to decay extremely rapidly by dissociative recombination with electrons, but in particular, 12 of this group behave not like molecules but rather as atomic ions. These are the diatomic oxide ions of Sc, Y, La, Zr, Hf, Ce, Pr, Nd, Pm, Gd, Tb, and Th. In the gas phase, they decay by much slower three-body recombination channels. As may be noted, these elements are located in the first two columns of the transition elements, among the earlier rare earths and an actinide. From all the elements, UO2+ is the only dioxide ion that behaves similarly. These findings now elevate the potential importance of these ions and should facilitate their spectral characterization. Moreover, subsequent comparisons with spectra of well-known isoelectronic and isovalent neutral monoxides and other diatomics will help in the stimulation of further theoretical advances. In addition, once characterized, an ease of spectrally monitoring such ionic states will provide a useful analytical tool.

Electrons↗

Real-space imaging of an orbital Kondo resonance on the Cr(001) surface.

The Kondo effect is usually connected with the interaction between a localized spin moment and itinerant electrons. This interaction leads to the formation of a narrow resonance at the Fermi level, which is called the Abrikosov-Suhl or Kondo resonance. Scanning tunnelling microscopy is an ideal technique for real-space investigations of complicated electronic structures and many-body phenomena, such as the formation of the Kondo resonance or d-wave pairing in high-T(c) superconductors. Theory has predicted that similar, Kondo-like many-electron resonances are possible for scattering centres with orbital instead of spin degrees of freedom--the quadruple momenta in uranium-based compounds or two-level systems in metallic glasses are examples of such 'pseudo-Kondo' scattering centres. Here we present evidence for the orbital Kondo resonance on a transition-metal surface. Investigations of an atomically clean Cr(001) surface at low temperature using scanning tunnelling microscopy reveal a very narrow resonance at 26 meV above the Fermi level, and enable us to visualize the orbital character of the corresponding state. The experimental data, together with many-body calculations, demonstrate that the observed resonance is an orbital Kondo resonance formed by two degenerate d(xz), d(yz) surface states.

Journal Article↗

Nanometre-size products of uranium bioreduction.

One strategy that is being pursued to tackle the international problem of actinide contamination of soils, sediments and water is to use microbial activity to 'fix' these radionuclides into an insoluble form that cannot be readily dispersed. Here we show that uraninite (UO(2)) particles formed from uranium in sediments by bacterial reduction are typically less than 2 nanometres across and that the small size has important implications for uraninite reactivity and fate. Because these tiny particles may still be transported in an aqueous environment, precipitation of uranium as insoluble uraninite cannot be presumed to immobilize it.

Anaerobiosis↗

Bioaccumulation of nickel by intercalation into polycrystalline hydrogen uranyl phosphate deposited via an enzymatic mechanism.

A Citrobacter sp. accumulates uranyl ion (UO2(2+)) as crystalline HUO2PO4.4H2O (HUP), using enzymatically generated inorganic phosphate. Ni was not removed by this mechanism, but cells already loaded with HUP removed Ni2+ by intercalative ion-exchange, forming Ni(UO2PO4)2.7H2O, as concluded by x-ray diffraction (XRD) and proton induced x-ray emission (PIXE) analyses. The loaded biomass became saturated with Ni rapidly, with a molar ratio of Ni:U in the cellbound deposit of approx. 1:6; Ni penetration was probably surface-localized. Cochallenge of the cells with Ni2+ and UO2(2+), and glycerol 2-phosphate (phosphate donor for phosphate release and metal bioprecipitation) gave sustained removal of both metals in a flow through bioreactor, with more extensively accumulated Ni. We propose 'Microbially Enhanced Chemisorption of Heavy Metals' (MECHM) to describe this hybrid mechanism of metal bioaccumulation via intercalation into preformed, biogenic crystals, and note also that MECHM can promote the removal of the transuranic radionuclide neptunium, which is difficult to achieve by conventional methods.

Biomass↗

Association of p53, K-ras and proliferating cell nuclear antigen with rat lung lesions following exposure to simulated nuclear fuel particles.

Expression of p53, K-ras, and proliferating cell nuclear antigen (PCNA) and mutations of p53 and K-ras genes in lung lesions of Han/Wistar rats were investigated by immunohistochemistry and direct DNA sequencing following a long-term exposure of animals to neutron-activated UO2 particles. The p53 protein was overexpressed in all five malignant tumors, in 62% of benign tumors, and in 42% of hyperplastic lesions examined. K-ras protein and PCNA levels were only slightly elevated in all types of lung lesions. In three malignant tumors a C-->T transition was detected in codon 288 (human 290) of the p53 gene, but this mutation was not present in seven other tumors analyzed. No mutations were detected in codons 12/13 and 61 of the K-ras gene in any of the five tumors analyzed. Our findings suggest that K-ras overexpression is a rare alteration, whereas p53 protein overexpression (sometimes associated with mutated p53 gene), as assessed with the CM5 antibody, is a relatively common phenomenon in hot particle-induced preneoplastic and neoplastic rat lung lesions.

Animals↗

Investigation of monovalent cation activation of S-adenosylmethionine synthetase using mutagenesis and uranyl inhibition.

S-Adenosylmethionine (AdoMet) synthetase catalyzes the formation of AdoMet from ATP and L-methionine with subsequent hydrolysis of the bound tripolyphosphate intermediate. Maximal activity requires the presence of two divalent and one monovalent cation per active site. Recently, the x-ray structure of the Escherichia coli AdoMet synthetase was solved, and the positions of the two Mg2+ binding sites were identified. Based on additional spherical electron density, the K+ binding site was postulated to be a nearby site where the uranyl heavy atom derivative also bound in the crystal. The side chain of glutamate 42 is within ligation distance of the metals. Mutagenesis of glutamate 42 to glutamine (E42QMetK) abolished monovalent cation activation and produced an enzyme that has kinetic properties virtually identical to those of K(+)-free wild type AdoMet synthetase in both the overall AdoMet synthetase reaction and in the hydrolysis of tripolyphosphate. Thus, there is a approximately 100-fold decrease in the Vmax for AdoMet synthesis and large increases in the Km values for both substrates. In contrast there is only a 2-fold decrease in Vmax for tripolyphosphate hydrolysis. The uranyl ion, UO2(2+), is a competitive inhibitor with respect to K+ (Ki = 350 nM) and is the first ion to bind at this site and inhibit the enzyme. The UO2(2+) inhibition is reversible and tight-binding, and results from UO2(2+) and not UO2(2+)-ATP. Analogous to K+ activation, UO2(2+) predominantly inhibits AdoMet formation rather than tripolyphosphate hydrolysis. The kinetic results indicate that UO2(2+) inhibition is likely to result from interference with productive ATP binding. UO2(2+) remains a tight-binding inhibitor of the E42Q mutant, which suggests that K+ and UO2(2+) have different ligation preferences when bound in the monovalent cation binding pocket. The results support the model that glutamate 42 provides ligands to the K+ and has a major role in monovalent cation binding.

Adenosine Triphosphate↗

The behaviour of uranium-233 oxide and uranyl-233 nitrate in rats.

233UO2 and 233UO2(NO3)2 in aqueous suspension have been administered to rats by pulmonary intubation. The 233U associated with the fraction of the 233UO2 less than 4 nm in diameter translocates from lungs to blood at the same rapid rate as 233U from 233UO2(NO3)2. Identical reactions with blood plasma and lung fluid were observed whether the 233U was administered as less than 4 nm 233UO2 particles or 233UO2(NO3)2. It is suggested that oxidation of UO2 to UO3 occurs followed by the formation of uranyl ion. In blood plasma, approximately 50 per cent of the 233U is bound to transferrin, 25 per cent to citrate and 25 per cent on bicarbonate.

Animals↗

Behaviour of spherical and irregular (U,Pu)O2 particles after inhalation or intratracheal instillation in rat lung and during in vitro culture with bovine alveolar macrophages.

Spherical and irregularly shaped mixed (U,Pu) oxide particles were administered to rats by inhalation and by intratracheal instillation. The lung retention of the particles was independent of particle shape and of the route of administration. Only a small percentage of the administered radioactivity was found in other organs. Detailed electron microscopic studies showed particles within membrane-enclosed vacuoles as well as lying free in the cytoplasm.

Administration, Inhalation↗

Translocation of plutonium from rat and monkey lung after inhalation of industrial plutonium oxide and mixed uranium and plutonium oxide.

This study was designed to compare the translocation from lung of the Pu contained in the pure and mixed industrial oxides PuO2 and (U,Pu)O2. The latter had a Pu content of 20% w/w. For this purpose, young adult male rats and male and female baboons were exposed to a single inhalation of these oxides. Two baboons were exposed to the reference PuO2, i.e. 239PuO2. Rats were killed under anaesthesia 1, 15, 30, 90 and 180 days after exposure, and baboons, also under anaesthesia, 1 year thereafter. The results indicate that lung retention of Pu was independent of the oxide inhaled, but was smaller in rat (12-15% of the initial pulmonary burden, 6 months after exposure) than in baboon (56-80% of this burden, 1 year after exposure). In rat, Pu translocation kinetics were similar for the two industrial oxides, but as from day 15 after inhalation until 6 months thereafter, measurement of Pu deposits in the liver and skeleton showed that translocation of Pu from the mixed oxide was 2-3 times greater than that from the industrial Pu oxide. In baboon, the largest amounts of Pu were retained in the lung and thoracic lymph nodes for the three oxides inhaled. Pu translocation to the liver, skeleton and kidneys, and also urinary Pu excretion, were greater after inhalation of the mixed oxide than after inhalation of the industrial and reference Pu oxides. Nevertheless, the amount of mixed oxide Pu translocated to these sites and excreted in urine remained under 3% of the initial pulmonary burden.

Administration, Inhalation↗

Comparison of the amount of nuclides released from the spent fuel in contact with and without a compacted bentonite block.

A spent LWR fuel specimen between Ca-bentonite blocks was leached in a simulated bentonite-saturated granitic water (SBGW) for 165 days and its results were compared with those of a specimen leached without a bentonite block. The amounts of Cs, Sb, Sr, Eu, Am, U and Pu released from a 4.3 mm thickness of a fuel pellet with a 50,400 MWD/MTU burn-up in the SBGW without a bentonite block were 2.2, 0.25, 0.15, 0.02, 0.01, 0.01 and approximately 5 x 10(-4)% of their inventories, respectively. However, the amounts of nuclides released from the specimen between the 1.4 Mg/m(3) bentonite blocks were decreased by three times at least. Moreover, the concentrations of the nuclides in the leachate were very low because most of them were retained in the bentonite blocks.

Bentonite↗

Powder aerosols generated by accidents: pressurized release experiments.

Safety assessments and environmental impact statements for facilities require an estimation of airborne releases. Aerosols generated by accidents are being investigated to develop the source terms for these releases. A severe accidental release event could be a pressurized powder release. Pressurized powder release experiments performed in static air measured the mass airborne and particle size distribution of these aerosols as a function of source size and containment pressure. Both containment pressure and source size were significant in pressurized powder releases. Release in static air can be estimated using the relationships developed in this work. Weight percent of the source powder airborne ranged from approximately 2 to 24%. Mass median aerodynamic equivalent diameters of the airborne particles ranged from 5 to 19 microns. All of the pressurized releases produced a significant fraction of respirable particles 10 microns AED and less.

Accidents, Occupational↗

Actions of some cations on the electrical properties and mechanical threshold of frog sartorius muscle fibers.

With the use of a point voltage-clamp technique, the effects of Zn(2+), UO(2) (2+), tetraethylammonium, and several other homologous quaternary ammonium ions on the electrical properties of the frog sartorius muscle and its mechanical threshold were studied. None of the agents separated the voltage thresholds for mechanical activation and delayed rectification. However, Zn(2+), UO(2) (2+), and TEA, which are known to potentiate the twitch, caused some inhibition of the normal increase in potassium conductance during delayed rectification. Zn(2+) and UO(2) (2+) also slowed the rate of development of the outward current. A strength-duration relation was studied for depolarization pulses capable of initiating contraction. With a depolarizing pulse of 2.5 msec the mechanical threshold is about -13 mv at about 20 degrees C. UO(2) (2+), 0.5 microM, which markedly reduced the outward current produced by such a short pulse, did not raise the mechanical threshold. All findings indicate that there is no direct causal relation between delayed rectification and mechanical activation.

Animals↗

An experimental test of new theoretical models for the electrokinetic properties of biological membranes. The effect of UO2++ and tetracaine on the electrophoretic mobility of bilayer membranes and human erythrocytes.

For a large smooth particle with charges at the surface, the electrophoretic mobility is proportional to the zeta potential, which is related to the charge density by the Gouy-Chapman theory of the diffuse double layer. This classical model adequately describes the dependence of the electrophoretic mobility of phospholipid vesicles on charge density and salt concentration, but it is not applicable to most biological cells, for which new theoretical models have been developed. We tested these new models experimentally by measuring the effect of UO2++ on the electrophoretic mobility of model membranes and human erythrocytes in 0.15 M NaCl at pH 5. We used UO2++ for these studies because it should adsorb specifically to the bilayer surface of the erythrocyte and should not change the density of fixed charges in the glycocalyx. Our experiments demonstrate that it forms high-affinity complexes with the phosphate groups of several phospholipids in a bilayer but does not bind significantly to sialic acid residues. As observed previously, UO2++ adsorbs strongly to egg phosphatidylcholine (PC) vesicles: 0.1 mM UO2++ changes the zeta potential of PC vesicles from 0 to +40 mV. It also has a large effect on the electrophoretic mobility of vesicles formed from mixtures of PC and the negative phospholipid phosphatidylserine (PS): 0.1 mM UO2++ changes the zeta potential of PC/PS vesicles (10 mol % PS) from -13 to +37 mV. In contrast, UO2++ has only a small effect on the electrophoretic mobility of either vesicles formed from mixtures of PC and the negative ganglioside GM1 or erythrocytes: 0.1 mM UO2++ changes the apparent zeta potential of PC/GM1 vesicles (17 mol % GM1) from -11 to +5 mV and the apparent zeta potential of erythrocytes from -12 to -4 mV. The new theoretical models suggest why UO2++ has a small effect on PC/GM1 vesicles and erythrocytes. First, large groups (e.g., sugar moieties) protruding from the surface of the PC/GM1 vesicles and erythrocytes exert hydrodynamic drag. Second, charges at the surface of a particle (e.g., adsorbed UO2++) exert a smaller effect on the mobility than charges located some distance from the surface (e.g., sialic acid residues).

Electrophoresis↗

Influence of macrophages on microdistribution of inhaled UO2 aerosol in rat lung.

Following the inhalation of an aerosol of UO2 (mass median aerodynamic diameter = 3 microns and geometric standard deviation = 1.6) the lungs of male albino rats were populated by foci containing UO2 particles. A method of neutron-induced autoradiography on Lexan plastic was used to reveal these foci in thin sections cut from the lung. For masses of UO2 in the lung that differed by more than a factor of 10 (39 to 450 micrograms) the number of foci per g of lung increased, but not in proportion to the mass of UO2 deposited. This limited increase in the number of foci was considered to result from physiological limitations on the number of alveolar macrophages available for engulfing the UO2 particles.

Aerosols↗

Further experiments to study whether localised fission fragment irradiation of rat lung causes tumours.

Male albino rats inhaled an aerosol of 235UO2 (mass median aerodynamic diameter = 2.8 micrometers and geometric standard deviation = 1.6). Approximately 20 h or 7 d post-inhalation the rats were exposed briefly to 10(12) slow neutrons cm-2 in a nuclear reactor, causing the retained 235UO2 particles of approximate mass 40 or 400 micrograms to emit fission fragments which irradiated the lungs. The mean absorbed doses from the fission fragments were either 80 ot 800 cGy approximately and in addition the lungs were exposed to a background of alpha-rays throughout the rats' life-time from the retained 235UO2 which gave mean doses of about half that from the fission fragments. The animals were kept for their life-time and killed when they became moribund. Malignant tumours were found in the lungs (squamous cell carcinoma and adenocarcinoma) which were probably induced by the alpha-rays rather than the fission fragments. Because of insufficient numbers of animals in the experimental groups, however, some statistical uncertainty exists as to whether the fission fragments were in fact less effective than the alpha-rays per unit absorbed dose in causing malignant tumours of the lung.

Adenocarcinoma↗