Towards a 32-electron principle: Pu@Pb12 and related systems.
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Biomedical subjects
Publications and source records attributed to Pekka Pyykkö.
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It is predicted that solid gold cyanide, AuCN, could have an alternative infinite trigonal-sheet crystal structure, of almost the same energy as the known hexagonally-packed infinite-chain structure.
The acetylene-like linear HThThH structure is calculated to lie almost degenerate to its rhombic alternative. Its unsupported Th-Th triple bond would be the first one of its kind.
A system of additive covalent radii is proposed for sigma(2) pi(4) triple bonds involving elements from Be to E 112 (eka-mercury). Borderline cases with weak multiple bonding are included. Only the elements in Group 1, the elements Zn-Hg in Group 12 and Ne in Group 18 are then totally excluded. Gaps are left at late actinides and some lanthanides. The standard deviation for the 324 included data points is 3.2 pm.
Quantum chemical calculations, based on multiconfigurational wave functions and including relativistic effects, show that the U(2)2+ system has a large number of low-lying electronic states with S of 0 to 2 and Lambda ranging from zero to ten. These states share a very small bond length of about 2.30 A, compared to 2.43 A in neutral U2. The Coulomb explosion to 2 U+ lowers the energy by only 1.6 eV and is separated by a broad barrier.
Quantum chemical calculations predict the existence of new molecular species with general formula MH12, where M is a group 6 atom. The previous MHn species had n values up to 9. The new systems with n = 12 would be a new record for metal hydrides.
Gold is an element whose unique properties are strongly influenced by relativistic effects. A large body of appropriate calculations now exist and their main conclusions are summarized. The theoretical interpretation of the aurophilic attraction is discussed in detail.
DsC and DsCO are calculated to be very similar to PtC and PtCO, suggesting that even the latest 6d elements resemble the corresponding 5d elements chemically.
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High-energy nitrogen-rich pentazolides of groups 6 and 13-16 are studied theoretically. Many of them have experimentally known azide analogues. Our highest nitrogen-to-element ratio of 40:1 is achieved in the systems [M(N5)8](2-) (M=Cr, Mo, W). The thermodynamic and kinetic stability of the studied systems grows with the negative charge on the system and is highest for tetra-pentazolides and hexa-pentazolides of B, Al, and Si. Systems such as B(N5)4- or Si(N5)6(2-) are examples of the most stable candidates for these new species. N(N5)2- is a candidate for a new all-nitrogen system. Neutral and positive systems were less stable. Pentazole derivatives of "dinuclear" C2Hn and N2Hn systems were investigated and were found to be of comparable stability as their "mononuclear" analogues. Pentazole derivatives of benzene, the C6H(6-n)(N5)n (n=2, 3, 6) systems, have a similar stability as the experimentally known phenylpentazole. A borazine analogue, N3B3H3(N5)3 is predicted to be one of the most stable systems of this family.
Quantum chemical calculations suggest that group 4 tetra-azides M(N(3))(4), where M = Ti, Zr, Hf, and Th, are stable species. They present a unique structural feature; namely, the M-N-N-N fragments are linear. These species are energetically more stable than the corresponding isomers with general formula eta(5)-N(5) -M-eta(7)-N(7), and the Th species, Th(N(3))(4), is the most stable of all. Possible mixed nitride azides NMN(3) were also investigated.
RHF, DFT and MP2 calculations are reported for the compounds [H5Pt-TlHn]n-, n = 0-2. These serve as analogues for the experimentally known [(NC)5Pt-Tl(CN)n](n-)-species. The very short bond between platinum and thallium is discussed.
The chemical properties of gold are strongly influenced by relativistic effects. One example is the large electronegativity of Au, which qualitatively explains the stability of (solid or liquid) cesium auride, Cs(+)Au(-), and other systems with Au(-) ions. An especially impressive compound is CsAu.NH(3), the structure and bonding of which are discussed. Future possibilities for finding further aurides are outlined.
Mercury tetrahydride (D4h) is calculated to have similar bond lengths and vibrational frequencies as the already known HgH2 and to lie energetically 200 kJ mol-1 above HgH2 + H2, in a local well, about 40 kJ mol-1 below a transition state.
Calculations with the linearized augmented plane wave method indicate that several high-density forms of sulfur trioxide should be accessible at pressures above 29 GPa, with densities up to 1.7 times larger than the presently known forms of solid SO3.
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