Search arXivSearch

arXiv · 1302.1608

Inconsistency of the photoemission spectrum with the spectral function in Kondo systems

Abstract

Kondo effect is an example of asymptotic freedom where the antiferromagnetic coupling between a localized magnetic moment and valence electrons, increases with reducing temperature. The electronic spectral function for such a system predicts a narrow Kondo resonance close to Fermi energy below its Kondo temperature 'TK'. The internal energy level structure of the localized magnetic moment introduces sidebands near the Kondo resonance, each with its respective Kondo temperature increasing as the sideband position moves towards higher binding energies. Consequently, the temperature dependence of the resonance features becomes weaker as we go towards higher binding energies. Here, we show a Ce4f photoemission spectral evolution obtained from a prototypical Kondo system CeAl2, departing from the predictions of the spectral function. Our measurements reveal a uniform temperature dependence for all the well screened Ce4f photoemission features (4f1 final state), which are usually interpreted as resonance features, as we reduce the temperature suggesting that the resonance interpretation for the 4f1 final state features is not appropriate. Instead, the spectral evolution is explained simply by the temperature dependence of the strength of the coupling between Ce4f and valence electrons, which remains uniform over the range of 4f1 final state features. As a possible explanation to the observed spectral evolution, we propose the phenomenon of collapse of the Kondo singlet wave function upon photoelectron kinetic energy measurement, analogous to the wave function collapse observed upon measurements performed on an entangled EPR (Einstein, Podolsky, Rosen) pair. Our proposal highlights how experiments studying single particle properties, when performed on a quantum system, give incomplete information about the many-body physics of the system.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

S. Patil, A. Generalov, A. Omar. 2015-10-09. Inconsistency of the photoemission spectrum with the spectral function in Kondo systems. https://doi.org/10.1088/0953-8984%2F25%2F38%2F382205

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Exotic Spin Excitation Continuum in a Weakly Coupled Quantum Chainsaw Antiferromagnet

Collective motions in strongly interacting magnets involve many spins and are often described in terms of integer-spin excitations. However, in certain cases, the collective motion can behave as if these integer excitations break apart into smaller, particle-like entities with unusual properties. Such fractionalized excitations in quantum magnets are commonly associated either with topological order in two dimensions or with criticality in one dimension. It remains unclear how these distinct mechanisms are connected across a dimensional crossover. Here we investigate the Ti-based quantum antiferromagnet, $Cs_{8}LiNa_{3}Ti_{12}F_{48}$, in which $Ti^{3+}$ ($3d^{1}$, $S=1/2$) ions interact antiferromagnetically within distorted kagome planes. Our inelastic neutron scattering study on a single crystal reveals a frustrated network of weakly coupled spin-$1/2$ chainsaws, realizing a regime of dimensional frustration in which interchain couplings fail to establish coherent two-dimensional order. The magnetic excitation spectrum exhibits a strong continuum spanning the full measured momentum and energy phase space. In addition, the dynamic spin correlation function displays rod-like scattering in momentum space, indicating a quasi-one-dimensional nature of the magnetic correlations. These results point to fractionalized excitations with intrinsically directional character, demonstrating that signatures of one-dimensional criticality can persist within a two-dimensional lattice. Our findings establish anisotropic fractionalization as a distinct organizing principle for quantum-disordered states.

cond-mat.str-el

Quantum-interference-driven orbital density wave and high-temperature superconductivity in trilayer nickelates

Intertwined charge-density-wave (CDW) and spin-density-wave (SDW) orders are a hallmark of high-temperature superconducting multilayer nickelates. In trilayer La4Ni3O_{10}, charge correlations develop at temperatures above the onset of long-range spin order, and the characteristic ordering wavevectors satisfy $Q_{cdw} \approx 2Q_{sdw}$. Here, using a density-wave equation with vertex corrections, we show that quantum interference between short-range SDW fluctuations at $q \approx Q_{sdw}$ on the outer NiO2 layers generates an inter-outer-layer bond order at $Q_{cdw} \approx 2 Q_{sdw}$. This bond order induces a pronounced inner-layer-centered orbital order, with antiphase modulations of the Ni $d_{3z^2-r^2}$ and $d_{x^2-y^2}$ occupations, producing strong orbital polarization but only weak total charge modulation. This intertwined bond-and-orbital order accounts for the layer-selective electronic reconstruction inferred from NMR/NQR and is consistent with Raman spectroscopy and scanning tunnelling microscopy measurements. The same orbital and spin fluctuations also cooperate to stabilize $s_{\pm}$-wave superconductivity through $M_z$ mirror-parity selection rules. Our results provide a unified microscopic framework for intertwined density-wave order and high-Tc superconductivity in multilayer nickelates.

cond-mat.str-el

Model Fractional Quantum Hall States on Lattices: Exact Parent Hamiltonians and Routes to Realization

Recent advances in engineered quantum platforms have enabled the realization of bosonic Laughlin states at $ν=1/2$ and brought non-Abelian topological phases within experimental reach. A central theoretical challenge is to develop a unified framework connecting lattice fractional quantum Hall (FQH) model states, exact parent Hamiltonians, and experimentally accessible interactions. We systematically construct Hermitian parent Hamiltonians for which continuum lowest Landau level (LLL) model states sampled on lattice sites are exact zero modes. Using these model manifolds as quantitative references, we find that, within the projected lattice LLL at the flux densities studied, short-range density interactions stabilize Laughlin ground-state manifolds at $ν=1/3$ and $1/4$, while two-body onsite repulsion supports a Moore--Read triplet at $ν=1$. Full multiband calculations reveal a sharp contrast: the Laughlin manifolds remain robust against interband mixing on the studied tori, whereas the Moore--Read triplet becomes less spectrally isolated and eventually undergoes a level crossing with competing states near the interband scale. Our framework provides a theoretical foundation for using lattice model states to guide the search for experimentally accessible Abelian and non-Abelian FQH states.

cond-mat.str-el