I21-Resonant Inelastic X-ray Scattering (RIXS)
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Marli R.
Cantarino
,
Rafael M. P.
Teixeira
,
Kevin R.
Pakuszewski
,
Wagner R.
Da Silva Neto
,
Juliana G.
De Abrantes
,
Mirian
Garcia-Fernandez
,
Pascoal G.
Pagliuso
,
Cris
Adriano
,
Claude
Monney
,
Thorsten
Schmitt
,
Eric C.
Andrade
,
Fernando A.
Garcia
Diamond Proposal Number(s):
[33194]
Open Access
Abstract: In doped Hund's metals, such as the iron-based superconductors, effects like charge doping and chemical pressure are often considered the dominant factors. Partial chemical substitution, however, inevitably introduces disorder. Here, we investigate spin excitations in Ba(Fe1−𝑥Cr𝑥)2As2 (CrBFA) by high-resolution resonant inelastic x-ray scattering for samples with 𝑥=0,0.035, and 0.085. In CrBFA, Cr acts as a hole dopant, but also introduces localized spins that compete with Fe-derived magnetic excitations. We found that the Fe-derived magnetic excitations are softened and damped, becoming overdamped for 𝑥=0.085. At this doping level, complementary angle-resolved photoemission spectroscopy measurements show increased electronic localization and a suppression of the nematic 𝑑𝑥𝑧/𝑑𝑦𝑧 band splitting present in the parent compound. We thus propose a localized spin model that explicitly incorporates substitutional disorder and Cr local moments, successfully reproducing our key observations. Our findings reveal a case where disorder dominates over charge doping in the case of a Hund's metal.
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Feb 2026
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I21-Resonant Inelastic X-ray Scattering (RIXS)
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Zubia
Hasan
,
Grace A.
Pan
,
Harrison
Labollita
,
Austin
Kaczmarek
,
Suk Hyun
Sung
,
Shekhar
Sharma
,
Purnima P.
Balakrishnan
,
Edward
Mercer
,
Vivek
Bhartiya
,
Alpha T.
N'Diaye
,
Zaher
Salman
,
Thomas
Prokscha
,
Andreas
Suter
,
Alexander J.
Grutter
,
Mirian
Garcia-Fernandez
,
Ke-Jin
Zhou
,
Jonathan
Pelliciari
,
Valentina
Bisogni
,
Ismail
El Baggari
,
Darrell G.
Schlom
,
Matthew R.
Barone
,
Charles M.
Brooks
,
Katja C.
Nowack
,
Antia S.
Botana
,
Brendan D.
Faeth
,
Alberto
De La Torre
,
Julia A.
Mundy
Diamond Proposal Number(s):
[34236]
Open Access
Abstract: Geometrically frustrated lattices can display a range of correlated phenomena, ranging from spin frustration and charge order to dispersionless flat bands due to quantum interference. One particularly compelling family of such materials is the half-valence spinel LiB2O4 materials. On the B-site frustrated pyrochlore sublattice, the interplay of correlated metallic behavior and charge frustration leads to a superconducting state in LiTi2O4 and heavy fermion behavior in LiV2O4. To date, however, LiTi2O4 has primarily been understood as a conventional BCS superconductor despite a lattice structure that could host more exotic ground states. Here, we present a multimodal investigation of LiTi2O4, combining ARPES, RIXS, proximate magnetic probes, and ab-initio many-body theoretical calculations. Our data reveals a novel mobile polaronic ground state with spectroscopic signatures that underlie co-dominant electron-phonon coupling and electron-electron correlations also found in the lightly doped cuprates. The cooperation between the two interaction scales distinguishes LiTi2O4 from other superconducting titanates, suggesting an unconventional origin to superconductivity in LiTi2O4. Our work deepens our understanding of the rare interplay of electron-electron correlations and electron-phonon coupling in unconventional superconducting systems. In particular, our work identifies the geometrically frustrated, mixed-valence spinel family as an under-explored platform for discovering unconventional, correlated ground states.
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Jan 2026
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I20-Scanning-X-ray spectroscopy (XAS/XES)
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Diamond Proposal Number(s):
[31940]
Abstract: Epitaxial YBa 2 Cu3O7−δ/MgO thin films fabricated with pulsed laser deposition are grown as idealised epitaxial systems with a minimal number of different elements for X-ray absorption spectroscopy studies of irradiation damage. These films are characterised in terms of their superconducting performance, crystallinity, surface morphology, and Cu local environment. This reveals a structural heterogeneity of [100] oriented material, referred to as “a-axis grains”, decorating the desired [001] oriented phase of the thin film, coinciding with suppressed superconducting performance.
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Jan 2026
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I05-ARPES
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Diamond Proposal Number(s):
[36633]
Open Access
Abstract: The 4Hb polytype of TaS2 is a natural heterostructure of H and T-type layers. Intriguing recent evidence points towards a possibly chiral superconducting ground state, unlike the superconductivity found in other polytypes where the T layers are absent, requiring understanding of the possible contributions of electrons from the T layers. Here we use micro-focused angle resolved photoemission spectroscopy to reveal that the T termination of the 4Hb structure is metallic, but a subsurface T layer - seen below an H termination and thus more representative of the bulk case - is gapped. The results imply a complete charge transfer of 1 electron per 13 Ta from the T to adjacent H layers in the bulk, but an incomplete charge transfer at the T termination, yielding a metallic Fermi surface with a planar-chiral character. A similar metallic state is found in an anomalous region with likely T-H-H’ stacking at the surface. Our results exclude cluster Mott localisation in either the bulk or surface of 4Hb-TaS2 and point to a scenario of superconductivity arising from Josephson-like tunneling between the H layers.
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Jan 2026
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I09-Surface and Interface Structural Analysis
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H. J.
Elmers
,
O.
Tkach
,
Y.
Lytvynenko
,
H.
Agarwal
,
D.
Biswas
,
J.
Liu
,
A.-A.
Haghighirad
,
M.
Merz
,
S.
Pakhira
,
G.
Garbarino
,
T.-L.
Lee
,
J.
Demsar
,
G.
Schönhense
,
M.
Le Tacon
,
O.
Fedchenko
Diamond Proposal Number(s):
[37580]
Abstract: This study uses angle-resolved photoemission spectroscopy to examine the low-temperature electronic structure of Cs(V0.95Nb0.05)3Sb5, demonstrating that partially substituting V atoms with isoelectronic Nb atoms results in an increase of the bandwidth and enhanced gap opening at the Dirac-like crossings due to the resulting chemical pressure. This increases the magnetic circular dichroism signal in the angular distribution compared to CsV3Sb5, enabling detailed analysis of magnetic circular dichroism in several bands near the Fermi level. These results substantiate the predicted coupling of orbital magnetic moments to three van Hove singularities near the Fermi level at 𝑀 points. Previous studies have observed that Nb doping lowers the charge density transition temperature and increases the critical temperature for superconductivity. This article demonstrates that Nb doping concomitantly increases the magnetic circular dichroism signal attributed to orbital moments.
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Dec 2025
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I05-ARPES
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I.
Biało
,
Qisi
Wang
,
J.
Küspert
,
X.
Hong
,
L.
Martinelli
,
O.
Gerguri
,
Y.
Chan
,
K.
Von Arx
,
O. K.
Forslund
,
W. R.
Pudełko
,
C.
Lin
,
N. C.
Plumb
,
Y.
Sassa
,
D.
Betto
,
N. B.
Brookes
,
M.
Rosmus
,
N.
Olszowska
,
Ma. D.
Watson
,
T. K.
Kim
,
C.
Cacho
,
M.
Horio
,
M.
Ishikado
,
H. M.
Rønnow
,
J.
Chang
Diamond Proposal Number(s):
[32147]
Open Access
Abstract: Strong electron correlations drive Mott insulator transitions. Yet, there exists no framework to classify Mott insulators by their degree of correlation. Cuprate superconductors, with their tunable doping and rich phase diagrams, offer a unique platform to investigate the evolution of these interactions. However, spectroscopic access to a clean half-filled Mott-insulating state is lacking in compounds with the highest superconducting onset temperature. To fill this gap, we introduce a pristine, half-filled thallium-based cuprate system, Tl2Ba5Cu4Ox. Using high-resolution resonant inelastic x-ray scattering, we probe long-lived magnon excitations and uncover a pronounced kink in the magnon dispersion, marked by a simultaneous change in group velocity and lifetime broadening. Modeling the dispersion within a Hubbard-Heisenberg approach, we extract the interaction strength and compare it with other cuprate systems. Our results establish a cuprate universal relation between electron-electron interaction and magnon zone-boundary dispersion. Superconductivity seems to be optimal at intermediate correlation strength, suggesting an optimal balance between localization and itinerancy.
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Dec 2025
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I11-High Resolution Powder Diffraction
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Abstract: This thesis reports the synthesis and characterisation of various layered mixed transition metal chalcogenide and pnictide materials. The commonality between the studied systems is that they exhibit exotic magnetic phenomena, such as high- and low-Tc superconductivity and long-range magnetic order of the 3d transition metal moments.
Chapter 3 details the effect of Ni substitution in ACo2Ch2 phases, where A = K, Rb, Cs, and Ch = S, Se. All of the Co-based phases show ferromagnetism, with the sole exception of antiferromagnetic CsCo2Se2, suggesting that larger interlayer separation favours antiferromagnetic order. On the other hand, all ANi2Ch2 phases show paramagnetism with a low-Tc superconducting transition below 2 K. Upon substitution of Ni for Co, a solid solution forms, which is evident from Synchrotron PXRD, and magnetometry measurements reveal a region of antiferromagnetic ordering, before the onset of paramagnetism at high substitution levels. These drastic changes in magnetism arise from the addition of an electron to the 3d band of the metallic ACo2Ch2 phases. The antiferromagnetic members of the KCo2−xNixCh2 (Ch = S, Se) series were studied by neutron powder diffraction, revealing A-type antiferromagnetism in x = 0.5 and 1 members, while the long-range magnetic order was not detected in x = 1.5 member. The refined magnetic model is highly anisotropic and is characterised by ferromagnetic coupling between Co/Ni ions within the (Co/Ni)2Se2 sheets and an antiferromagnetic interaction between the adjacent (Co/Ni)2Se2 sheets along the stacking axis. The mechanisms responsible for the different types of magnetic coupling are direct ferromagnetic interactions between transition metal ions within the plane, while the RKKY mechanism is responsible for the between-the-plane antiferromagnetic coupling, as the distance between the planes is too large (~5 Å) for any kind of direct interaction. PND of the CsCo2−xNixSe2 solid solution also showed A-type antiferromagnetism in its x = 1 member, and an intriguing structural distortion was found from Synchrotron PXRD for a small region of compositions between 1.1 ≤ x ≤ 1.4. The tetragonal symmetry of the parent phase is lowered to orthorhombic in these compositions.
Chapters 4 and 5 detail the effect of chemical disorder and pressure, respectively, on the 1144 family of iron-based superconductors. CaKFe4As4 is subject to chemical doping with small amounts of Ca to introduce chemical disorder on one of its sublattices, however, the phase behaves as a line phase and its structural features do not allow any disorder on any of the sublattices. On the other hand, SrRbFe4As4 is subject to elevated pressures in a high-pressure Synchrotron PXRD experiment. It is found that no lattice collapse, driven by formation of As-As bonds, occurs between 0-26 GPa, as was reported in the case in related compounds.
Chapter 6 details the high-pressure synthesis of LaNixBi2, a low-Tc superconductor with a very small superconducting volume fraction. It is found that superconductivity likely has an extrinsic origin, as even a highly pure LaNixBi2 shows minimal superconducting volume fraction and its superconducting features, including Tc and Hc1 are coincidental with that of Ni-Bi secondary phases.
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Dec 2025
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I09-Surface and Interface Structural Analysis
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Abstract: Superconducting microwave circuits are a promising physical implementation of quantum computing. A significant challenge with the development of superconducting qubits is the materials source of loss leading to qubit decoherence. Much of this loss is dielectric loss or quasiparticle dissipation at superconductor surfaces and interfaces. In order to understand the loss mechanisms microscopically, it is necessary to have an accurate picture of the atomic structure and microstructure. In this work, we explore the structure of three interfaces. First, we present non- destructive X-ray characterization of the NbH surface precipitation in Nb thin films. Unwanted hydride precipitation in niobium-based superconducting circuits is a side effect of hydrofluoric acid etching of the Nb surface oxide. The precipitate microstructure is challenging to probe because of the high mobility of hydrogen in niobium. Using X-rays diffraction, we show evidence supporting phase-field simulations that the nucleation of NbH occurs at free surfaces. Using darkfield X-ray nanoprobe microscopy, we identify a complex microstructure suggesting a martensitic nucleation that transitions to a dendritic growth. Next, we present X-ray standing wave excited X-ray photoelectron spectroscopy of the annealed, Nb(110) ordered oxide surface layer. We discover the existence of an oxygen interstitial rich subsurface layer and identify the origin of two distinct oxygen chemical states at the surface: one coming from this subsurface layer, and the other from the surface NbO termination. Last, we present the heteroepitaxy of single crystal Al2O3 with a TiN. We identify TiN as an ideal substrate for the epitaxial growth of Al2O3 in a capacitor geometry based on the high degree of crystallinity and sharp interfaces with minimal diffusion and
3
we measure the two-level-state loss of the Al2O3 junction dielectric layer. We present this interface as an alternative to the commonly used amorphous alumina in Josephson Junctions.
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Dec 2025
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I06-Nanoscience (XPEEM)
I10-Beamline for Advanced Dichroism - scattering
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Di
Tian
,
Haotian
Zheng
,
Zewei
Huang
,
Sijie
Wu
,
Pengcheng
Li
,
Cong
Li
,
Jianbing
Zhang
,
Xinyu
Shu
,
Jinling
Zhou
,
Yang
Liu
,
Yanhong
Gu
,
Meng
Wang
,
Di
Yi
,
Tianxiang
Nan
,
Zhen
Chen
,
Qing
He
,
Huaqiang
Wu
,
Shuyun
Zhou
,
Weidong
Luo
,
Pu
Yu
Open Access
Abstract: Layered oxide materials, with their two-dimensional crystalline architectures and tunable interlayer interaction, serve as a fertile field for harnessing emergent quantum phenomena. Among these materials, metallic delafossites (e.g., PdCoO2) have emerged as a prominent system with extraordinary two-dimensional electronic properties, though their intrinsic lack of ferromagnetism has remained a fundamental constraint. Here, we report the creation of robust, bulk high-temperature ferromagnetism (𝑇𝑐>420 K) in inherently nonmagnetic PdCoO2 through controlled hydrogenation while preserving the delafossite structure. This process induces layer-selective electron doping into CoO2 layers, stabilizing Ising-type ferromagnetism with pronounced perpendicular magnetic anisotropy while preserving the material’s exceptional metallicity. Remarkably, the system self-assembles into a superlattice of alternating metallic Pd and insulating ferromagnetic hydrogenated CoO2 layers, enabling an unconventional anomalous Hall effect mediated by interlayer spin-charge coupling. These findings demonstrate that bulk ferromagnetism can be achieved in delafossite oxides while preserving their structural integrity, positioning hydrogenated delafossites as a versatile platform for exploring correlated quantum effects and designing multifunctional devices.
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Nov 2025
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I05-ARPES
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Y.
Alexanian
,
A.
De La Torre
,
S.
Mckeown Walker
,
M.
Straub
,
G.
Gatti
,
A.
Hunter
,
S.
Mandloi
,
E.
Cappelli
,
S.
Riccò
,
F. Y.
Bruno
,
M.
Radovic
,
N. C.
Plumb
,
M.
Shi
,
J.
Osiecki
,
C.
Polley
,
T. K.
Kim
,
P.
Dudin
,
M.
Hoesch
,
R. S.
Perry
,
A.
Tamai
,
F.
Baumberger
Diamond Proposal Number(s):
[10348, 12404, 17381]
Open Access
Abstract: The fate of the Fermi surface in bulk electron-doped Sr2IrO4 remains elusive, as does the origin and extension of its pseudogap phase. Here, we use high-resolution angle-resolved photoelectron spectroscopy (ARPES) to investigate the electronic structure of Sr2−xLaxIrO4 up to x = 0.2, a factor of two higher than in previous work. We find that the antinodal pseudogap persists up to the highest doping level, and thus beyond the sharp increase in Hall carrier density to ≃ 1 + x recently observed above x* ≃ 0.161. This suggests that doped iridates host a unique phase of matter in which a large Hall density coexists with an anisotropic pseudogap, breaking up the Fermi surface into disconnected arcs. The temperature boundary of the pseudogap is T* ≃ 200 K for x = 0.2, comparable to cuprates and to the energy scale of short range antiferromagnetic correlations in cuprates and iridates.
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Oct 2025
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