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Related papers: Important role of alkali atoms in A4C60

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We derive numerical tight-binding hopping parameters to describe conduction-band dispersion in arbitrary orientational phases of $A_3$C$_{60}$. The parameters are obtained by direct Fourier inversion of the spectra from self-consistent…

Condensed Matter · Physics 2009-10-22 S. C. Erwin , E. J. Mele

The polymer phases of AC60 form distinct crystal structures characterized by the mutual orientations of the (C60-)n chains. We show that the direct electric quadrupole interaction between chains always favors the orthorhombic structure Pmnn…

Materials Science · Physics 2009-10-31 K. H. Michel , A. V. Nikolaev

In high Tc superconductors the magnetic and electronic properties are determined by the probability that valence electrons virtually jump from site to site in the CuO2 planes, a mechanism opposed by on-site Coulomb repulsion and favored by…

Although C$_{60}$ is a molecular crystal with a bandgap E$_g$ of ~2.5 eV, we show that E$_g$ is strongly affected by injected charge. In sharp contrast to the Coulomb blockade typical of quantum dots, E$_g$ is {\it reduced} by the Coulomb…

Materials Science · Physics 2009-11-10 Z. H. Lu , C. C. Lo , C. J. Huang , M. W. C. Dharma-wardana , Marek Z. Zgierski

Band theory predicts both K3C60 and K4C60 to be metals; various experimental probes show that while K3C60 is indeed metallic, K4C60 appears to be insulating. The standard view of this apparent failure of the single-particle picture is that…

Condensed Matter · Physics 2009-10-22 Steven C. Erwin , Christoph Bruder

It is demonstrated that the fullerene shell affects dramatically the radiative and Auger vacancy decay of an endohedral atom A@C60. The collectivized electrons of the C60 shell add new possibilities for radiative and non-radiative decays…

Atomic Physics · Physics 2022-06-13 M. Ya. Amusia , A. S. Baltenkov

We present first-principles band calculations as well as structural optimization of the orthorhombic K$_1$C$_{60}$ polymerized phase. We found three-dimensional inter-fullerene bonding/anti-bonding characters consisting of $t_{1u}$…

Materials Science · Physics 2007-05-23 T. Ogitsu , K. Kusakabe , S. Tsuneyuki , Y. Tateyama

The restoration of metallicity in the high-temperature, cubic phase of Li4C60 represents a remarkable feature for a member of the A4C60 family (A = alkali metal), invariably found to be insulators. Structural and resonance technique…

Strongly Correlated Electrons · Physics 2009-11-13 M. Riccò , M. Belli , D. Pontiroli , M. Mazzani , T. Shiroka , D. Arcon , A. Zorko , S. Margadonna , G. Ruani

The binding energy of A3C60, a conductor, is described well by an ionic solid type calculation. This succeeds because there is little overlap between molecular wave functions on neighbouring sites, so that electrons are practically…

Materials Science · Physics 2007-05-23 K. Ranjan , Sarbpreet Singh , K. Dharamvir , V. K. Jindal

We consider transitions of electron holes (vacancies in otherwise filled shells of atomic systems) in multiply-charged ions that, due to level-crossing of the holes, have frequencies within the range of optical atomic clocks. Strong E1…

Atomic Physics · Physics 2011-07-21 J. C. Berengut , V. A. Dzuba , V. V. Flambaum , A. Ong

We study a one-dimensional chain of identical atoms with two electronic orbitals and two electrons per atom, subject to an external oscillating pressure that periodically modulates the lattice spacing. This leads to time-dependent intra-…

Mesoscale and Nanoscale Physics · Physics 2025-11-18 Anwesha Chattopadhyay

The orientation of individual C60 molecules adsorbed on Cu(100) is reversibly switched when the tip of a scanning tunneling microscope is approached to contact the molecule. The probability of switching rises sharply upon displacing the tip…

Materials Science · Physics 2009-11-13 N. Neel , L. Limot , J. Kroeger , R. Berndt

Recent studies of the backbending phenomenon in medium light weight nuclei near A~60 expanded greatly our interest about how the single particle orbits are nonlinearly affected by the collective motion. As a consequence we have applied a…

Nuclear Theory · Physics 2015-06-26 S. U. El-Kameesy , H. H. Alharbi , y , H. A. Alhendi

We demonstrate that the Auger decay rate in an endohedral atom is very sensitive to the atom's location in the fullerene cage. Two additional decay channels appear in an endohedral system: (a) the channel due to the change in the electric…

Atomic and Molecular Clusters · Physics 2015-05-20 Andrey V. Korol , Andrey V. Solov'yov

Fullerene solids doped with alkali metals (A$_3$C$_{60}$, A = K, Rb, Cs) exhibit a superconducting transition temperature ($T_c$) as high as 40 K, and their unconventional superconducting properties have been a subject of debate. With…

Superconductivity · Physics 2023-10-24 Jianyu Li , Zhangkai Cao , Jiahao Su , Ruipeng Wang , Haipeng Li , Yusuke Nomura , Xiaosen Yang , Ho-Kin Tang

The multiplet structure induced by the Coulomb interactions in C$_{60}^{n-}$ ($n = 1 - 12$) is analyzed. The partially ocuppied LUMO gives rise to a set of levels which fill a relatively wide band ( $\approx 2-3$ eV ). A large ($\sim 1$ eV)…

Condensed Matter · Physics 2009-10-22 F. Guinea , J. Gonzalez , M. A. H. Vozmediano

Interchain hopping in systems of coupled chains of correlated electrons is investigated by exact diagonalizations and Quantum-Monte-Carlo methods. For two weakly coupled Hubbard chains at commensurate densities (e.g. n=1/3) the splitting at…

Condensed Matter · Physics 2016-08-31 D. Poilblanc , H. Endres , F. Mila , M. G. Zacher , S. Capponi , W. Hanke

The alkali halides are ionic compounds. Each alkali atom donates an electron to a halogen atom, leading to ions with full shells. The valence band is mainly located on halogen atoms, while, in a traditional picture, the conduction band is…

Materials Science · Physics 2023-10-24 Christopher C. Leon , Abhishek Grewal , Klaus Kuhnke , Klaus Kern , Olle Gunnarsson

We present numerical evidence that the hopping of electrons between chains described by the $t-J$ model is coherent in the integrable cases ($J=0$ and $J=2$) and essentially incoherent otherwise. This effect is {\it not} related to the…

Condensed Matter · Physics 2009-10-28 Frederic Mila , Didier Poilblanc

By calculation and analysis of the bare conduction bands in a large number of hole-doped high-temperature superconductors, we have identified the energy of the so-called axial-orbital as the essential, material-dependent parameter. It is…

Condensed Matter · Physics 2009-10-31 E. Pavarini , I. Dasgupta , T. Saha-Dasgupta , O. Jepsen , O. K. Andersen
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