SearcharxivSearch

arXiv · 2509.24300

Bose glass in Ca$_2$RuO$_4$ nanofilms

Abstract

Weak localization of bosons can give rise to an exotic quantum phase known as a Bose glass, characterized by the absence of global phase coherence yet finite conductivity. This phase is crucial in understanding the interplay between disorder, interactions, and superconductivity, especially in two-dimensional and strongly correlated systems. Here we report the presence of the Bose glass phase in the weak localization region of ruthenium oxide Ca$_2$RuO$_4$. The electrical resistance exhibits a characteristic logarithmic temperature dependence in this phase, $\rho \sim \ln(1/T)$. Through $\beta$-function scaling analysis, we observed "vertical flow" indicating unconventional scaling behavior associated with localized bosonic states. Our results suggest the existence of bosons-Cooper pairs-persisting up to high temperatures around 220 K and that these bosons undergo weak localization. In the Bose glass phase, vortices are found to have a dual relationship with the localized Cooper pairs, enabling their motion and resulting in finite resistance despite the presence of bosonic order. We identified two quantum critical points: one between the Bose glass and superconducting phases and another between the Bose glass and Mott insulating phases, allowing us to extract the corresponding quantum sheet resistances. We revealed that the ground state of the Ca$_2$RuO$_4$ changes depending on the localization strength. Thinning the Ca$_2$RuO$_4$ corresponds to controlling the electronic correlation by relieving the distortion in RuO$_6$ octahedra. These findings offer significant insights into the interplay between electronic correlations and bosonic transport, with important implications for studying high-temperature superconductors based on perovskite structures.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Hiroyoshi Nobukane, Koki Hirose, Kakeru Isono, Mizuki Higashiizumi, Masahito Sakoda, Korekiyo Takahashi, Satoshi Tanda. 2025-09-29. Bose glass in Ca$_2$RuO$_4$ nanofilms. https://arxiv.org/abs/2509.24300

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

KEEP EXPLORING

Related papers

Competing Interlayer Loop Currents and Superconductivity in the Bilayer $t$-$J_\perp$-$V$ Model

The recent discovery of high-$T_c$ superconductivity in pressurized and thin-film bilayer nickelates, featuring a strong interlayer exchange coupling, and their potential similarities with cuprate superconductors, has made this a very active topic in condensed matter physics. In the present paper we study the strongly correlated one-orbital ($d_{x^2-y^2}$) bilayer $t$-$J_\perp$-$V$ model for nickelates, where $V$ denotes the Coulomb interactions, using a controlled large-$N$ expansion at and beyond the mean-field level. Focusing on the out-of-plane spin exchange interaction ($J_\perp$), we find that it triggers both out-of-plane $s$-wave superconductivity and an out-of-plane bond-order phase ($z$-BOP) instability. The $z$-BOP gives rise to a complex $z$-axis hopping dominated by its imaginary component, which drives out-of-plane currents and induces in-plane ones, spontaneously forming on the vertical plaquettes a loop-current state that breaks time-reversal symmetry. Competition between this loop-current phase and superconductivity yields a dome-shaped superconducting region, with optimal superconductivity occurring near the $z$-BOP quantum critical point. The resulting phase diagram features a pure loop-current region, a low-doping coexistence phase, a pure superconducting state at higher doping, and a correlated metallic state.

cond-mat.str-el

Optically induced metallic state with persistent monoclinic symmetry in NdNiO$_3$

Understanding whether electronic and structural order remain coupled under nonequilibrium conditions is a central challenge in correlated materials. Here, we simultaneously track metallicity and symmetry across the photoinduced insulator-to-metal transition in NdNiO$_3$ using time-resolved optical reflectivity and symmetry-sensitive second-harmonic generation. We find that metallic reflectivity emerges at significantly lower excitation fluence than restoration of the orthorhombic high-temperature symmetry. As a result, optical excitation stabilizes a metastable state that combines the reflectivity of the metallic phase with the monoclinic symmetry of the insulating phase, revealing an optically induced monoclinic metal. Only at substantially higher fluences does the symmetry fully recover to that of the high-temperature phase. These results demonstrate a nonequilibrium decoupling of metallicity and structural symmetry and establish simultaneous multiprobe spectroscopy as a powerful approach for identifying emergent phases in correlated materials.

cond-mat.str-el

Instabilities in self-consistent diagrammatic approaches and how to cure them

While self-consistent diagrammatic approaches are widely used to compute the physical properties of correlated quantum materials, their applicability may get severely hindered precisely in the parameter regions, where the most exciting physics is observed. One of the major issues, referred to as "misleading convergence", is the tendency of iterative schemes to converge to unphysical fixed points for intermediate-to-strong electronic interactions, regardless of numerical accuracy of the computation. Here, we explicitly verify that the origin of this problem in several established self-consistent many-electron approaches, defined in the general diagrammatic framework of the boson-exchange formalism, resides exclusively in the stability condition of the respective iteration schemes, and not in an intrinsic breakdown of their self-consistent diagrammatic description. This insight enables a simple and general remedy, as recently proposed in Phys. Rev. Lett. 137, 016502 (2026): The redefinition of the iterative procedure, by inverting the unstable eigendirections of the Jacobian associated to the fixed point of the self-consistent algorithm. We illustrate the successful outcome of this procedure by means of systematic calculations performed on testbed, exactly solvable, models. Our results demonstrate that the physical fixed point of the diagrammatic schemes we considered can be stabilized, de facto, across the entire parameter range, including the most challenging nonperturbative/strong-coupling regimes.

cond-mat.str-el