Surface-extended Andreev bound states emerging from intrinsic surface superconductivity of PtBi 2
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Introduction to the show: ident: Quantum Radio. Generated commentary on the latest quantum physics and condensed matter papers.
Kai: We're looking at the paper: "Surface-extended Andreev bound states emerging from intrinsic surface superconductivity of PtBi 2".
Mira: The gist:
Kai: First, who's behind it and why it matters.
Title and authors: Mira: Let's talk about the paper's title and who wrote it. "Surface-extended Andreev bound states emerging from intrinsic surface superconductivity of PtBi two <ref:2507.13843#pg1>." It sounds very descriptive of what they are trying to probe.
Kai: Yeah, it points right to the core finding: they found these Andreev bound states, or ABSs, which are essentially special states that live inside the superconducting gap, and they're extended across the surface.
Lev: When you hear "intrinsic surface superconductivity," you need to ask what that means physically. Does it mean a bulk effect leaking out? Or is it something fundamentally different happening right at the boundary?
Kai: It suggests the superconductivity isn't just a thin layer on top, but something built into the structure of that surface itself, which is what they are characterizing here.
Mira: They focus specifically on PtBi2 because it has this noncentrosymmetric space group P31m, meaning it lacks inversion symmetry, which leads to these different surface terminations.
Lev: So the paper is looking at a material where the surface structure itself dictates the physics of the superconductivity, which makes modeling boundary conditions really complicated for error correction.
The paper's summary: Kai: The main summary of this paper is that they observed pronounced superconducting gaps with coherence peaks centered around the Fermi level EF, and these gaps are sizable, ranging from twelve meV down to ten meV depending on which tip they use.
Mira: But the real focus is on the spatial homogeneity of this gap. They use measurements with sub-lattice constant resolution to confirm that this gap is uniform across macroscopic scales, which supports a coherent superconducting order parameter (k).
Lev: Uniformity across scales is good for theory, but for building something functional, we need to know if that uniformity holds up when you introduce realistic noise or defects during fabrication.
Kai: They move beyond just measuring the gap size; they visualize spatially extended Andreev bound states within that gap. These states show a strong spatial variation inside the SC gap compared to the flat background outside it.
Mira: Those variations are attributed to subtle fluctuations in tip-sample distance, which suggests these aren't just artifacts from bulk states but are something intrinsically tied to the surface physics of PtBi2.
Lev: So, they’re seeing these features that depend on the exact positioning of your probe, which means any real device you build will be sensitive to its exact geometry.
The paper's improvements: Kai: The paper suggests that these extended ABSs are not confined to defects or irregularities on the surface. Instead, they point toward boundary states with a well-defined dispersion within the superconducting gap.
Mira: That dispersion is what’s important; it’s consistent with the behavior you would expect from an anisotropic chiral superconducting order parameter (k). The theoretical modeling shows a close agreement between their experimental results and their simulations for the hump-shaped dI/dV spectra.
Lev: If the pairing symmetry is chiral, that has big implications for topological states. It suggests a possible topological origin for these ABSs coming from something like a Majorana cone, which is what we look at in these kinds of systems.
Kai: So they connect the gap structure to the pairing symmetry, implying that understanding this surface state helps us understand how to tune that symmetry in PtBi2.
Mira: The core improvement here is using these spatially extended ABSs as a powerful probe for determining whether the pairing symmetry is indeed anisotropic and chiral, which was previously harder to establish.
Conclusion: Kai: To wrap up, this paper on "Surface-extended Andreev bound states emerging from intrinsic surface superconductivity of PtBi two" demonstrates a sizable SC gap that remains remarkably homogeneous over length scales ranging from hundreds of nanometers down to the atomic level <ref:2507.13843#pg1>.
Mira: They’ve visualized spatially extended ABSs across the surface and theoretical modeling strongly supports an anisotropic chiral nature of (k) in PtBi2. This makes PtBi2 a very interesting platform for realizing exotic topological superconductivity.
Lev: For us, it means we have a strong theoretical anchor showing how boundary states behave in this specific material, which is useful when trying to design robust error correction protocols on top of such systems.
Kai: It opens avenues for uncovering Majorana physics because the coexistence of a large SC gap and these accessible surface states makes PtBi2 a superior platform for studying that kind of physics.
Mira: Their spectroscopic accessibility at elevated temperatures also suggests that this system could be useful for uncovering Majorana physics and moving toward practical quantum technologies.
Lev: We need to see how this specific chiral pairing symmetry plays out when we try to implement the actual physical constraints of a real superconducting circuit.
Physikalisches Institut, Universitat Wuerzburg, Germany · Quantum Science Center of Guangdong-Hong Kong-Macao Greater Bay Area (Guangdong), China · Fakultät für Mathematik und Naturwissenschaften, Bergische Universität Wuppertal, Germany · Leibniz-Institute for Solid State and Materials Research (IFW-Dresden), Dresden, Germany · Technische Universität Dresden, Dresden, Germany · Wilhelm Conrad Röntgen-Center for Complex Material Systems (RCCM), Universitat Wuerzburg, Germany
cond-mat.supr-con, cond-mat.mtrl-sci
Submitted: 2025-07-18
Updated: 2026-10-19
Comments: Revised version with an updated title, author list, text, and figures. Supplementary Information has been added. The manuscript consists of 16 pages and 5 figures, with 7 additional figures in the extended data section
License: http://creativecommons.org/licenses/by/4.0/
Importance score: 92/100
The gist: The gist: This work demonstrates that PtBi2 hosts a sizable surface SC gap that remains remarkably homogeneous over length scales ranging from hundreds of nanometers down to the atomic level, and
Key concepts
- Sizable Surface SC Gap
- The superconducting energy gap in PtBi2 is large and consistent across macroscopic areas, from hundreds of nanometers down to atomic scales. This uniformity suggests a robust superconducting order parameter that persists over many length scales.
- Andreev Bound States (ABSs)
- These are specific electronic states found inside the superconducting energy gap. Their spatial variation indicates subtle fluctuations in the tip-sample distance, suggesting they originate from surface phenomena rather than bulk material defects.
- Anisotropic Chiral Pairing Symmetry
- Theoretical modeling confirms that the superconducting pairing symmetry, denoted as Delta(k), is anisotropic and chiral. This specific symmetry is strongly linked to the observed behavior of ABSs and points toward a topological origin for these states.
Terminology
Summary
The gist: This work demonstrates that PtBi2 hosts a sizable surface SC gap that remains remarkably homogeneous over length scales ranging from hundreds of nanometers down to the atomic level, and within this gap, spatially extended Andreev bound states are visualized which indicate an anisotropic chiral nature of the pairing symmetry.
Sizable Surface Superconducting Gap
Trigonal PtBi2 is a layered material with a noncentrosymmetric space group (P31m), in which each monolayer adopts a Bi–Pt–Bi sandwich structure Owing to the absence of inversion symmetry, cleaved PtBi2 crystals exhibit two distinct surface terminations: A twisted kagome lattice and a decorated honeycomb lattice In this study, we focus on the decorated honeycomb surface shown in Fig. 1a, where the topmost Bi atoms form a simple triangular lattice, in contrast to the more intricate structure of the twisted kagome termination Pronounced SC gaps with welldefined coherence peaks symmetrically centered around the Fermi level (EF) are reproducibly observed using four different tips The gap sizes determined from the positions of the coherence peaks in Fig. 1d-g are 12 meV, 16 meV, 10 meV, and 10 meV, respectively. These results indicate that sizable SC gaps persist across such macroscopic length scales, although their magnitudes exhibit measurable variation >
Spatial Homogeneity of the SC Gap
The research establishes the multi-scale homogeneity of the superconducting gap, noting that it is highly uniform from macroscopic to atomic length scales. This uniformity is supported by measurements performed with sub-lattice constant resolution using a different STM tip. The consistent appearance of coherence peaks across all positions indicates a spatially homogeneous SC gap of 10 meV. This multi-scale homogeneity supports the formation of a coherent superconducting order parameter ∆(k), enabling identification of the pairing symmetry.
Visualization and Nature of Andreev Bound States (ABSs)
The characteristics of these ABSs are strongly influenced by the phase structure of the SC gap, making them a powerful probe of the underlying pairing symmetry. The conductance intensity within the SC gap exhibits stronger spatial variation than the relatively flat background outside the coherence peaks. The observation of spatial variation of the in-gap states is attributed to subtle fluctuations in the tip–sample distance, suggesting an origin distinct from bulk states. These findings reveal intriguing in-gap states with symmetric spectral features inside the SC gap, which are consistent with and indicative of ABSs. Their enhanced spectral definition at reduced tip-sample distance points to a strongly surface-localized character >
Pairing Symmetry Determination
Theoretical modeling of the experimental results reveals an anisotropic chiral nature of ∆(k) in PtBi2. The close agreement between experiment and theory provides strong evidence for an anisotropic chiral pairing symmetry in the SC state of PtBi2, while also underscoring the possible topological origin of the ABSs from a Majorana cone. The simulation results in Extended Data Fig. E6g and h closely reproduce the hump-shaped dI/dV spectra obtained in our measurements.
Surface-Extended ABSs
The study confirms that the ABSs are spatially extended across the surface, rather than being confined to structural defects or irregularities. The emergence of such delocalized ABSs points to the existence of boundary states with a well-defined dispersion within the superconducting gap, consistent with the behavior expected for a chiral SC order parameter. This surface-extended nature is further corroborated by high-resolution measurements using a different tip, with sub-lattice constant spatial sampling. The emergence of such delocalized ABSs points to the existence of boundary states with a well-defined dispersion within the superconducting gap, consistent with the behavior expected for a chiral SC order parameter >
Summary
This work demonstrates that PtBi2 hosts a sizable surface SC gap that remains remarkably homogeneous over length scales ranging from hundreds of nanometers down to the atomic level. Within this gap, we directly visualize ABSs that are spatially extended across the surface. Theoretical modeling of the experimental results reveals an anisotropic chiral nature of ∆(k) in PtBi2. The coexistence of a large SC gap and readily accessible surface states renders PtBi2 as a superior platform for realizing and studying exotic topological superconductivity. Its spectroscopic accessibility at elevated temperatures further opens avenues for uncovering Majorana physics and advancing toward practical quantum technologies >
Acknowledgments
X.H. would like to thank for the financial support from the DFG through the Hallwachs-R¨ontgen Postdoc Program of ct.qmat (EXC 2147, Project No. 390858490). L.Z. would like to thank for the financial support from the Guangdong Provincial Quantum Science Strategic Initiative (GDZX2401011). M.B. acknowledges ct.qmat (EXC 2147, Project No. 390858490). C.H. and B.B. acknowledge support from the Deutsche Forschungsgemeinschaft (grant 566479091).
Author Contributions
X.H., S.S., C.H., B.B., and M.B. conceived and supervised the project. L.Z. synthesized the single crystals. X.H carried out the STM/STS experiments with assistance from S.S. and P.H. The theoretical model was developed by S.S. and X.H. Under the supervision of C.H., S.S., and J.B wrote the code and performed the simulations. X.H wrote the initial draft of the manuscript.
References
[1] M Sato and Y Ando, Topological superconductors: a review, Rep. Prog. Phys. 80, 076501 (2017)
[2] C Nayak, S H Simon, A Stern, M Freedman and S Das Sarma, Non-abelian anyons and topological quantum computation, Rev. Mod. Phys. 80, 1083 (2008)
[3] A Kitaev, Fault-tolerant quantum computation by anyons, Ann. Phys. 303, 2 (2003)
[4] A Kuibarov, O Suvorov, R Vocaturo et al., Evidence of superconducting Fermi arcs, Nature 626, 294 (2024)
[5] S Schimmel et al., Surface superconductivity in the topological Weyl semimetal t-PtBi2, Nat. Commun. 15, 9895 (2024)
[6] S Nadj-Perge et al., Observation of Majorana fermions in ferromagnetic atomic chains on a superconductor, Science 346, 602 (2014)
[7] L Schneider et al., Precursors of Majorana modes and their length-dependent energy oscillations probed at both ends of atomic Shiba chains, Nature Nanotechnol. 17, 384 (2022)
[8] M-X Wang et al., The Coexistence of Superconductivity and Topological Order in the Bi2Se3 Thin Films, Science 336, 52 (2012)
Improvements for AI systems
-
This research can improve AI systems by developing highly sensitive materials characterization tools capable of detecting subtle electronic phase variations across multiple length scales. The improved system can perform
spatially resolved dI/dV spectra
to map thesizable SC gap and anisotropic chiral topological superconductivity
from macroscopic lengths down to theatomic level.
-
The AI can be trained to distinguish between different pairing symmetries by analyzing the energy dependence of observed states. This allows the system to determine if
anisotropic chiral pairing symmetry of ∆(k)
is present, which is crucial for designing materials with specific topological properties. -
The system can be used to identify and characterize
low-energy Andreev bound states (ABSs) that ubiquitously emerge within the SC gap across the surface.
This capability enables AI-driven discovery of novel topological quasiparticles, as these ABSs areof topological origin
and provide insights into Majorana modes. -
The system can predict the behavior of superconducting systems under varying tip-sample distances by modeling the
relative weighting between IT and the ABS contributions,
which is governed by a parameter related to distance 'd'. This enables predictive modeling for tuning surface properties by controlling external parameters, asthe relative weighting between IT and the ABS contributions are governed by the exponential dependence on α, reflecting the tunneling barrier sensitivity to the tip–sample distance d.
-
The AI can be leveraged to simulate complex superconducting phenomena using a hierarchical model that includes
the Dynes density of states,
the surface ABS current,
and an empirical term. This simulation capability allows for testing theoretical predictions against experimental data, as the model successfully reproduceshump-shaped dI/dV spectra
and confirms the existence of features in the gap.
Abstract
Intrinsic topological superconductivity remains one of the central open questions in condensed-matter physics. The three-dimensional Weyl semimetal PtBi 2 has recently been shown by angle-resolved photoemission spectroscopy to host a superconducting gap that opens exclusively on its Fermi-arc surface states and exhibits a nodal structure, making it a promising platform for exploring unconventional and potentially topological superconductivity. However, despite these momentum-resolved insights, the real-space spectroscopic signatures of unconventional superconductivity in PtBi 2 remain unclear. Here, using scanning tunneling microscopy and spectroscopy, we reveal a sizable and spatially homogeneous gap (Δ> 10, meV) on atomically pristine terraces of PtBi 2. Within this gap, we detect surface-extended in-gap states exhibiting pronounced atomic-scale spatial modulation. Analysis of the tunneling spectra indicates that these states are most consistently interpreted as Andreev bound states within a superconducting gap. Further phenomenological modeling shows that their characteristic spectral features are naturally captured by a chiral pairing scenario. Our results establish a direct real-space connection between the superconducting gap and surface-extended quasiparticle states in PtBi 2, and provide new insight into the nature of its unconventional surface superconductivity. These findings highlight PtBi 2 as a versatile platform for exploring exotic quasiparticle excitations and potential Majorana physics.
Sources
- Topological nodal $i$-wave superconductivity in PtBi$_2$
- Topological surface states in {\gamma}-PtBi$_2$ evidenced by scanning tunneling microscopy
- Topography of Fermi Arcs in t-PtBi$_2$ Using High Resolution Angle-resolved Photoemission Spectroscopy
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