Hugo Keller
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Hugo Keller has a total of 103 co-authors. Here are the top co-authors by number of shared publications:
- Annette Bussmann-Holder
Max-Planck Institute for Solid State Research
13 shared publications - Rustem Khasanov
Kazan State Medical Academy – branch of the Russian Medical Academy of Continuing Professional Education
5 shared publications - Arndt Simon
Max-Planck-Institute for Solid State Research, Heisenbergstr. 1, D-70569 Stuttgart, Germany
4 shared publications - Alexander Shengelaya
Department of Physics, Ivane Javakhishvili Tbilisi State University, Tbilisi, Georgia
3 shared publications - Antonio Bianconi
Institute of Crystallography National Research Council CNR Via Salaria Km 29.3 00015 Monterotondo Rome Italy
3 shared publications K. Conder
Laboratory for Developments and Methods, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland
3 shared publications
Latest Publications
- 1 November 2026
- Published by AIP Publishing in Low Temperature Physics
- Vol. 52 (11) , 1286-1295
1986 A landmark in the research of superconductivity: From elemental and simple crystalline systems to complex oxide ceramics (Topical review)
Celebrating 40 years of superconductivity in ceramic oxides, we review the history and milestones, beginning in 1986, the year of the discovery, until today. While the first years after the discovery were marked by almost daily news on cuprate oxides with enthusiastic developments and hopes for rapid applications, nowadays the interest has decreased, but the electron pairing mechanism remains a matter of debate. What has happened in these 40 years and what can be expected for the future?
- 1 November 2026
- Published by AIP Publishing in Low Temperature Physics
- Vol. 52 (11) , 1286-1295
1986 A landmark in the research of superconductivity: From elemental and simple crystalline systems to complex oxide ceramics (Topical review)
Celebrating 40 years of superconductivity in ceramic oxides, we review the history and milestones, beginning in 1986, the year of the discovery, until today. While the first years after the discovery were marked by almost daily news on cuprate oxides with enthusiastic developments and hopes for rapid applications, nowadays the interest has decreased, but the electron pairing mechanism remains a matter of debate. What has happened in these 40 years and what can be expected for the future?
- Open Access
- 30 October 2025
- Published by MDPI AG in Condensed Matter
- Vol. 10 (4) , 56
Nanoscale Lattice Heterostructure in High-Tc Superconductors
Low-temperature superconductivity has been known since 1957 to be described by BCS theory for effective single-band metals controlled by the density of states at the Fermi level, very far from band edges, the electron–phonon coupling constant l, and the energy of the boson in the pairing interaction w0, but BCS has failed to predict high-temperature superconductivity in different materials above about 23 K. High-temperature superconductivity above 35 K, since 1986, has been a matter of materials science, where manipulating the lattice complexity of high-temperature superconducting ceramic oxides (HTSCs) has driven materials scientists to grow new HTSC quantum materials up to 138 K in HgBa2Ca2Cu3O8 (Hg1223) at ambient pressure and near room temperature in pressurized hydrides. This perspective covers the major results of materials scientists over the last 39 years in terms of investigating the role of lattice inhomogeneity detected in these new quantum complex materials. We highlight the nanoscale heterogeneity in these complex materials and elucidate their special role played in the physics of HTSCs. Especially, it is highlighted that the geometry of lattice and charge complex heterogeneity at the nanoscale is essential and intrinsic in the mechanism of rising quantum coherence at high temperatures.
- 30 October 2025
- Published by MDPI AG in Condensed Matter
- Vol. 10 (4) , 56
Open AccessNanoscale Lattice Heterostructure in High-Tc Superconductors
Low-temperature superconductivity has been known since 1957 to be described by BCS theory for effective single-band metals controlled by the density of states at the Fermi level, very far from band edges, the electron–phonon coupling constant l, and the energy of the boson in the pairing interaction w0, but BCS has failed to predict high-temperature superconductivity in different materials above about 23 K. High-temperature superconductivity above 35 K, since 1986, has been a matter of materials science, where manipulating the lattice complexity of high-temperature superconducting ceramic oxides (HTSCs) has driven materials scientists to grow new HTSC quantum materials up to 138 K in HgBa2Ca2Cu3O8 (Hg1223) at ambient pressure and near room temperature in pressurized hydrides. This perspective covers the major results of materials scientists over the last 39 years in terms of investigating the role of lattice inhomogeneity detected in these new quantum complex materials. We highlight the nanoscale heterogeneity in these complex materials and elucidate their special role played in the physics of HTSCs. Especially, it is highlighted that the geometry of lattice and charge complex heterogeneity at the nanoscale is essential and intrinsic in the mechanism of rising quantum coherence at high temperatures.
- Open Access
- 19 December 2024
- Published by MDPI AG in Condensed Matter
- Vol. 9 (4) , 56
Multiband Superconductivity, Polarons, Jahn-Teller Polarons, Heterogeneity, and High-Temperature Superconductivity
Early on, oxides were ruled out from superconductivity, since they are typically large-band-gap insulators. Nevertheless, a rather small number of them were found to be superconducting, with transition temperatures up to 14 K and a remarkably low carrier density. This was the starting point of K. Alex Müller (KAM) becoming interested in superconductivity in oxides. Step by step, he advanced the research on oxides and finally discovered, together with J. Georg Bednorz, high-temperature superconductivity (HTSC) in the perovskite-type compound Ba-La-Cu-O. Even though he was inspired by specific and clear ideas in his search, he added new impact in the understanding of HTSC for many years after receipt of the Nobel prize for this discovery.
- 19 December 2024
- Published by MDPI AG in Condensed Matter
- Vol. 9 (4) , 56
Open AccessMultiband Superconductivity, Polarons, Jahn-Teller Polarons, Heterogeneity, and High-Temperature Superconductivity
Early on, oxides were ruled out from superconductivity, since they are typically large-band-gap insulators. Nevertheless, a rather small number of them were found to be superconducting, with transition temperatures up to 14 K and a remarkably low carrier density. This was the starting point of K. Alex Müller (KAM) becoming interested in superconductivity in oxides. Step by step, he advanced the research on oxides and finally discovered, together with J. Georg Bednorz, high-temperature superconductivity (HTSC) in the perovskite-type compound Ba-La-Cu-O. Even though he was inspired by specific and clear ideas in his search, he added new impact in the understanding of HTSC for many years after receipt of the Nobel prize for this discovery.
- Open Access
- 4 December 2024
- Published by MDPI AG in Nanomaterials
- Vol. 14 (23) , 1944
Transition to Metallic and Superconducting States Induced by Thermal or Electrical Deoxidation of the Dislocation Network in the Surface Region of SrTiO3
The question as to why deoxidized SrTiO3−δ becomes metallic and superconducting at extremely low levels of oxygen vacancy concentration has been a mystery for many decades. Here, we show that the real amount of effused oxygen during thermal reduction, which is needed to induce superconducting properties, is in the range of only 1014/cm3 and thus even lower than the critical carrier concentrations assumed previously (1017–1019/cm3). By performing detailed investigations of the optical and electrical properties down to the nanoscale, we reveal that filaments are forming during reduction along a network of dislocations in the surface layer. Hence, a reduced epi-polished SrTiO3−δ crystal has to be regarded as a nano-composite consisting of a perfect dielectric matrix with negligible carrier density, which is short-circuited by metallic filaments with a local carrier density in the range of 1020/cm3. We present that electro-degradation leads to a more pronounced evolution of filamentary bundles and thus can generate a superconducting state with higher TC than thermal reduction. These findings indicate that traditional homogeneous models of superconductivity in self-doped SrTiO3−δ need to be revised, and we propose an alternative explanation taking into account the coexistence of metallic dislocation cores with polar insulating regions allowing for polaronic coupling.
- 4 December 2024
- Published by MDPI AG in Nanomaterials
- Vol. 14 (23) , 1944
Open AccessTransition to Metallic and Superconducting States Induced by Thermal or Electrical Deoxidation of the Dislocation Network in the Surface Region of SrTiO3
The question as to why deoxidized SrTiO3−δ becomes metallic and superconducting at extremely low levels of oxygen vacancy concentration has been a mystery for many decades. Here, we show that the real amount of effused oxygen during thermal reduction, which is needed to induce superconducting properties, is in the range of only 1014/cm3 and thus even lower than the critical carrier concentrations assumed previously (1017–1019/cm3). By performing detailed investigations of the optical and electrical properties down to the nanoscale, we reveal that filaments are forming during reduction along a network of dislocations in the surface layer. Hence, a reduced epi-polished SrTiO3−δ crystal has to be regarded as a nano-composite consisting of a perfect dielectric matrix with negligible carrier density, which is short-circuited by metallic filaments with a local carrier density in the range of 1020/cm3. We present that electro-degradation leads to a more pronounced evolution of filamentary bundles and thus can generate a superconducting state with higher TC than thermal reduction. These findings indicate that traditional homogeneous models of superconductivity in self-doped SrTiO3−δ need to be revised, and we propose an alternative explanation taking into account the coexistence of metallic dislocation cores with polar insulating regions allowing for polaronic coupling.
- Open Access
- 14 November 2024
- Published by MDPI AG in Preprints.org
Multi-Band Superconductivity, Polarons, Jahn-Teller Polarons, Heterogeneity and High-Temperature Superconductivity
Early on oxides were ruled out from superconductivity, since these are typically large band gap insulators. Nevertheless a rather small number of them were found to be superconducting with transition temperatures up to 14 K and a remarkable low carrier density. This was the starting point of K. Alex Müller (KAM) to get interested in superconductivity in oxides. Step by step he advanced in the research in oxides and finally discovered together with J. Georg Bednorz high-temperature superconductivity (HTSC) in the perovskite type compound Ba-La-Cu-O. Even though inspired from specific and clear ideas in his search, he added new impact in the understanding of HTSC for many years after receipt of the Nobel prize for this discovery.
- 14 November 2024
- Published by MDPI AG in Preprints.org
Open AccessMulti-Band Superconductivity, Polarons, Jahn-Teller Polarons, Heterogeneity and High-Temperature Superconductivity
Early on oxides were ruled out from superconductivity, since these are typically large band gap insulators. Nevertheless a rather small number of them were found to be superconducting with transition temperatures up to 14 K and a remarkable low carrier density. This was the starting point of K. Alex Müller (KAM) to get interested in superconductivity in oxides. Step by step he advanced in the research in oxides and finally discovered together with J. Georg Bednorz high-temperature superconductivity (HTSC) in the perovskite type compound Ba-La-Cu-O. Even though inspired from specific and clear ideas in his search, he added new impact in the understanding of HTSC for many years after receipt of the Nobel prize for this discovery.
- Open Access
- 8 May 2024
- Published by MDPI AG in Condensed Matter
- Vol. 9 (2) , 24
Meeting and Working with K. Alex Müller: Personal Memories
- 8 May 2024
- Published by MDPI AG in Condensed Matter
- Vol. 9 (2) , 24
Open AccessMeeting and Working with K. Alex Müller: Personal Memories
- Open AccessOxygen isotope effect on the superfluid density within the $d-$wave and $s-$wave pairing channels of YBa$_2$Cu$_4$O$_8$We report on measurements of the oxygen isotope ($^{16}$O/$^{18}$O) effect (OIE) on the transition temperature $T_{\rm c}$ and the zero-temperature in-plane magnetic penetration depth $λ_{\rm ab}(0)$ in the stoichiometric cuprate superconductor YBa$_2$Cu$_4$O$_8$ by means of muon-spin rotation/relaxation. An analysis of the temperature evolution of $λ^{-2}_{\rm ab}$ in terms of coexisting $s+d-$wave order parameters reveals that the OIE on the superfluid density $ρ_{\rm s}(0)\proptoλ^{-2}_{\rm ab}(0)$ stems predominantly from the $d-$wave component while the contribution of the $s-$wave one is almost zero. The OIE on the transition temperature $T_{\rm c}$ is found to be rather small: $δT_{\rm c}/T_{\rm c}= -0.32(7)$%, compared to the total OIE on the superfluid density $ρ_{\rm s}(0)$: $δρ_{\rm s}(0)/ρ_{\rm s}(0)= -2.8(1.0)$%. The partial OIE's on the corresponding $d-$wave and $s-$wave components of $ρ_{\rm s}(0)$ are $δρ_{\rm s,d}(0)/ρ_{\rm s}(0)= -3.0(1.2)$%, and $δρ_{\rm s,s}(0)/ρ_{\rm s}(0)= 0.2(1.2)$%, respectively. Our results demonstrate that polaron formation in the CuO$_2$ planes is the origin of the observed OIE in the $d-$wave channel. In the much weaker $s-$wave channel, fermionic quasiparticles are present, which do not contribute to the OIE on $ρ_{\rm s}(0)$. Our results support the original idea of K. Alex Müller on the polaronic nature of the supercarries in high-temperature cuprate superconductors.Open AccessOxygen isotope effect on the superfluid density within the $d-$wave and $s-$wave pairing channels of YBa$_2$Cu$_4$O$_8$We report on measurements of the oxygen isotope ($^{16}$O/$^{18}$O) effect (OIE) on the transition temperature $T_{\rm c}$ and the zero-temperature in-plane magnetic penetration depth $λ_{\rm ab}(0)$ in the stoichiometric cuprate superconductor YBa$_2$Cu$_4$O$_8$ by means of muon-spin rotation/relaxation. An analysis of the temperature evolution of $λ^{-2}_{\rm ab}$ in terms of coexisting $s+d-$wave order parameters reveals that the OIE on the superfluid density $ρ_{\rm s}(0)\proptoλ^{-2}_{\rm ab}(0)$ stems predominantly from the $d-$wave component while the contribution of the $s-$wave one is almost zero. The OIE on the transition temperature $T_{\rm c}$ is found to be rather small: $δT_{\rm c}/T_{\rm c}= -0.32(7)$%, compared to the total OIE on the superfluid density $ρ_{\rm s}(0)$: $δρ_{\rm s}(0)/ρ_{\rm s}(0)= -2.8(1.0)$%. The partial OIE's on the corresponding $d-$wave and $s-$wave components of $ρ_{\rm s}(0)$ are $δρ_{\rm s,d}(0)/ρ_{\rm s}(0)= -3.0(1.2)$%, and $δρ_{\rm s,s}(0)/ρ_{\rm s}(0)= 0.2(1.2)$%, respectively. Our results demonstrate that polaron formation in the CuO$_2$ planes is the origin of the observed OIE in the $d-$wave channel. In the much weaker $s-$wave channel, fermionic quasiparticles are present, which do not contribute to the OIE on $ρ_{\rm s}(0)$. Our results support the original idea of K. Alex Müller on the polaronic nature of the supercarries in high-temperature cuprate superconductors.
- Open Access
- 20 January 2022
- Published by MDPI AG in Condensed Matter
- Vol. 7 (1) , 10
Superconductivity and the Jahn–Teller Polaron
In this article, we review the essential properties of high-temperature superconducting cuprates, which are unconventional isotope effects, heterogeneity, and lattice responses. Since their discovery was based on ideas stemming from Jahn–Teller polarons, their special role, together with the Jahn–Teller effect itself, is discussed in greater detail. We conclude that the underlying physics of cuprates cannot stem from purely electronic mechanisms, but that the intricate interaction between lattice and charge is at its origin.
- 20 January 2022
- Published by MDPI AG in Condensed Matter
- Vol. 7 (1) , 10
Open AccessSuperconductivity and the Jahn–Teller Polaron
In this article, we review the essential properties of high-temperature superconducting cuprates, which are unconventional isotope effects, heterogeneity, and lattice responses. Since their discovery was based on ideas stemming from Jahn–Teller polarons, their special role, together with the Jahn–Teller effect itself, is discussed in greater detail. We conclude that the underlying physics of cuprates cannot stem from purely electronic mechanisms, but that the intricate interaction between lattice and charge is at its origin.
- Open Access
- 31 December 2020
- Published by MDPI AG in Condensed Matter
- Vol. 6 (1) , 2
From SrTiO3 to Cuprates and Back to SrTiO3: A Way Along Alex Müller’s Scientific Career
K.A. Müller took a long route in science leaving many traces and imprints, which have been and are still today initiations for further research activities. We “walk” along this outstanding path but are certainly not able to provide a complete picture of it, since the way was not always straight, often marked by unintended detours, which had novel impact on the international research society.
- 31 December 2020
- Published by MDPI AG in Condensed Matter
- Vol. 6 (1) , 2
Open AccessFrom SrTiO3 to Cuprates and Back to SrTiO3: A Way Along Alex Müller’s Scientific Career
K.A. Müller took a long route in science leaving many traces and imprints, which have been and are still today initiations for further research activities. We “walk” along this outstanding path but are certainly not able to provide a complete picture of it, since the way was not always straight, often marked by unintended detours, which had novel impact on the international research society.
- Open Access
- 3 August 2020
- Published by MDPI AG in Condensed Matter
- Vol. 5 (3) , 50
Suppression of the s-Wave Order Parameter Near the Surface of the Infinite-Layer Electron-Doped Cuprate Superconductor Sr0.9La0.1CuO2
The temperature dependencies of the in-plane () and out-of-plane () components of the magnetic field penetration depth were investigated near the surface and in the bulk of the electron-doped superconductor SrLaCuO by means of magnetization measurements. The measured and were analyzed in terms of a two-gap model with mixed -wave symmetry of the order parameter. is well described by an almost pure anisotropic d-wave symmetry component (%), mainly reflecting the surface properties of the sample. In contrast, exhibits a mixed -wave order parameter with a substantial s-wave component of more than 50%. The comparison of measured near the surface with that determined in the bulk by means of the muon-spin rotation/relaxation technique demonstrates that the suppression of the s-wave component of the order parameter near the surface is associated with a reduction of the superfluid density by more than a factor of two.- 3 August 2020
- Published by MDPI AG in Condensed Matter
- Vol. 5 (3) , 50
Open AccessSuppression of the s-Wave Order Parameter Near the Surface of the Infinite-Layer Electron-Doped Cuprate Superconductor Sr0.9La0.1CuO2
The temperature dependencies of the in-plane () and out-of-plane () components of the magnetic field penetration depth were investigated near the surface and in the bulk of the electron-doped superconductor SrLaCuO by means of magnetization measurements. The measured and were analyzed in terms of a two-gap model with mixed -wave symmetry of the order parameter. is well described by an almost pure anisotropic d-wave symmetry component (%), mainly reflecting the surface properties of the sample. In contrast, exhibits a mixed -wave order parameter with a substantial s-wave component of more than 50%. The comparison of measured near the surface with that determined in the bulk by means of the muon-spin rotation/relaxation technique demonstrates that the suppression of the s-wave component of the order parameter near the surface is associated with a reduction of the superfluid density by more than a factor of two.