Growth and Transport Properties of InAsSb Nanoflags

arXiv:2602.11060 · cond-mat.mtrl-sci, cond-mat.mes-hall · Submitted 2026-02-11 · Read on arXiv

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Introduction to the show: ident: Quantum Radio. Generated commentary on the latest quantum physics and condensed matter papers.

Kai: I'm Kai, and with me are Mira and Lev, guest researcher.

Mira: Today's paper: "Growth and Transport Properties of InAsSb Nanoflags".

Kai: The gist: The present work reports, for the first time, the growth of high-quality free-standing InAsSb nanoflags and their electronic properties.

Mira: First, who's behind it and why it matters.

Paper summary: Kai: So, looking back at the "Growth and Transport Properties of InAsSb Nanoflags" paper by Serra and his team, what does this actually mean for the broader field beyond just the material properties they measured?

Mira: It means they’ve shown that you can engineer ternary compounds like InAsSb to get a material with a larger Landé g-factor while keeping mobility competitive with InAs and InSb >

Lev: If you can achieve that higher g-factor in a structure that is still somewhat scalable, it opens up new avenues for exploring topological superconductivity in hybrid S-Sm systems because of the spin physics involved >

Kai: And the fact they found surface Fermi level pinning, similar to InAs, suggests this material might be much easier to couple into superconducting circuits than some other candidates >

Mira: And the fact that they found surface Fermi level pinning, similar to InAs, suggests this material might be much easier to couple into superconducting circuits than some other candidates >

Kai: It’s about proving that InAsSb isn't just a theoretical curiosity but a tangible platform for quantum applications while retaining many of the desirable traits from InSb >

Lev: If you can achieve that higher g-factor in a structure that is still somewhat scalable, it opens up new avenues for exploring topological superconductivity in hybrid S-Sm systems because of the spin physics involved >

Mira: They also managed to get InAs0 point 77Sb0 point 23 nanoflags that are quite long, around two thousand plus or minus one hundred eighty nanometers long, and they confirmed these structures have a Landé g-factor larger than pure InAs or InSb >

Kai: So you're saying this ternary alloy stuff doesn't just mess with the material; it actually improves a fundamental property like the g-factor while keeping mobility decent?

Mira: Exactly. And they also found evidence of surface Fermi level pinning, which is a known behavior in InAs systems, so it suggests these nanoflags might couple to superconductors more easily >

Lev: That similarity to InAs behavior is important because it makes this material look like it could be much easier to couple into superconducting circuits than some other candidates >

Conclusion: Kai: So we've been digging into these new InAsSb nanoflags, and now we're getting to where the authors wrap up their main points on this paper, "Growth and Transport Properties of InAsSb Nanoflags."

Mira: Right. Essentially, they’re showing how you can actually grow these high-quality, free-standing structures for the first time with various alloy compositions >

Kai: And what's the big takeaway from that growth work? What did they end up growing?

Mira: They managed to get InAs0 point 77Sb0 point 23 nanoflags that are quite long, around two thousand plus or minus one hundred eighty nanometers long, and they confirmed these structures have a Landé g-factor larger than pure InAs or InSb >

Kai: So you're saying this ternary alloy stuff doesn't just mess with the material; it actually improves a fundamental property like the g-factor while keeping mobility decent?

Mira: Exactly. And they also found evidence of surface Fermi level pinning, which is a known behavior in InAs systems, so it suggests these nanoflags might couple to superconductors more easily >

Kai: That's interesting because usually when you mix things up like that, you expect the mobility to drop way off a cliff. How did they manage that? What numbers are we looking at here?

Mira: They showed the mobility is still comparable to some of the best InAs and InSb nanoflags they've seen. The estimated g-factor is around fifty-eight point seven plus or minus four point zero, which lines up pretty well with what's seen in other related shallow quantum wells >

Kai: Fifty-eight point seven for a g-factor in a nanoflag structure—that’s substantial. Lev, from an error correction standpoint, if we were trying to build something on this, does that level of g-factor give us any real advantage?

Lev: Well, the higher g-factor definitely gives you more control over spin physics when you start looking at topological states in hybrid systems. It’s a better starting point for those kinds of experiments than what you’re getting with standard InAs >

Kai: So they've shown the material *can* be made and that it has these desirable electronic features, but what's the next step? What's left to do with these nanoflags?

Mira: They point out that while ternary compounds are harder to grow than simple binaries, you gain control over things like the lattice constant and band gap just by changing the composition >

Kai: And they end by suggesting these specific nanoflags are a good platform for studying topological superconductivity in S-Sm systems. So, the authors think this is a promising way forward?

Mira: They see it as a strong candidate to host exotic bound states because of that large g-factor and the surface conduction effects they observed >

Kai: Right. It’s moving from just measuring properties to actually proposing what these structures could do in future quantum circuits.

NEST, Istituto Nanoscienze-CNR and Scuola Normale Superiore

cond-mat.mtrl-sci, cond-mat.mes-hall

Submitted: 2026-02-11

Updated: 2026-02-11

Journal ref: Nanoscale, 2026, 18, 5741

DOI: 10.1039/d5nr05226b

License: http://creativecommons.org/licenses/by/4.0/

Importance score: 73/100

The gist: The gist: The present work reports, for the first time, the growth of high-quality free-standing InAsSb nanoflags and their electronic properties.

Key concepts

Landé g-factor
This property describes how strongly the electron's spin interacts with its motion in a material. A larger g-factor means the spin-orbit interaction is stronger, which is crucial for spintronic and topological applications. The InAsSb nanoflags found have a significantly larger g-factor than standard InAs or InSb.
Mobility
Mobility measures how easily charge carriers (electrons) can move through the material when an electric field is applied. High mobility indicates efficient charge transport, which is vital for high-performance electronic devices. The measured mobility of these nanoflags was found to be comparable to the best InAs and InSb nanoflags.
Surface Fermi Level Pinning
This phenomenon occurs at the surface of a semiconductor where the energy level that determines electrical conduction becomes fixed or 'pinned.' This pinning behavior in InAs0.77Sb0.23 nanoflags is similar to that seen in InAs, which is important for controlling how electrons behave near the material's boundary.
Ternary Compounds
These are semiconductor materials made from three different elements, like InAsSb (Indium Arsenide Antimonide). Growing ternary compounds is generally more difficult than growing binary compounds. However, they offer unique advantages because their properties—like the band gap and effective mass—can be precisely tuned by changing the ratio of the constituent elements.

Terminology

Summary

The gist: The present work reports, for the first time, the growth of high-quality free-standing InAsSb nanoflags and their electronic properties.

Material Properties and Growth

Different growth conditions have been explored, and zinc-blende InAsSb nanoflags of various composition have been obtained Different growth conditions have been explored, and zinc-blende InAsSb nanoflags of various composition have been obtained>. In particular, InAs0.77Sb0.23 nanoflags are on average (2000±180) nm long, (640±50) nm wide, and (130±30) nm thick We show that these nanoflags have a Landé g-factor larger than InAs and InSb and a mobility comparable to those of the best performing InAs and InSb nanoflags. The estimated Landé g-factor of these InAsSb NFs is g∗ = 58.7 ± 4.0, which is in good agreement with the recently reported value of g∗ ∼ 55 for an InAsSb shallow QW.

Experimental Synthesis and Characterization

The synthesis of the InAs-InAsSb heterostructures has been carried out by Au-assisted vapor-liquid-solid (VLS) growth in a chemical beam epitaxy (CBE) system on InAs(111)B substrates. The morphology of the grown samples has been studied through field-emission scanning electron microscopy (SEM), employing a Zeiss Merlin SEM with an accelerating voltage of 5 kV and probe current between 90 pA and 100 pA, detecting secondary electrons. To characterize the heterostructure crystal structure and chemical composition, the InAsSb NFs have been mechanically transferred on a Cu grid and studied by transmission electron microscopy (TEM) in a JEOL JEM-F200 operated at 200 kV, equipped with an EDX spectrometer.

Electronic Transport Measurements

Low temperature transport measurements have been performed at 2.7 K, at B = 0, B = 0.25 T, and B = −0.25 T. The data was measured with an AC current bias of 100 nA and performing back-gate voltage sweeps, back and forth, between ±40 V. From the measurements at B = 0, we calculated the longitudinal conductance Gxx as follows: Gxx = Rxx / (R2xx + R2xy) ≈ 1/Rxx. The field-effect mobility obtained from the linear fit to the conductance curve is µFE = LWCox · ∂Gxx / ∂Vbg. We found the oxide capacitance to be Cox = εSiO2 / ε0 tox, and this value is in good agreement with previous work. The field-effect mobility obtained from the linear fit to the conductance curve is µFE = 2.2 · 104 cm 2/(Vs) (at 2.7 K).

Magneto-transport Analysis

Hall effect measurements were taken, for different Vbg values, by measuring source-drain current Isd, longitudinal four-probe voltage drop Vxx, and Hall voltage Vxy with lock-in amplifiers with an AC current bias of 100 nA. The charge carrier density n is calculated as n = Isd / e · ∂Vxy / ∂B −1. The Hall mobility is calculated as µH = L W · ⟨Vxx⟩ · ∂Vxy / ∂B. At 0.44 K, Hall mobility has a peak of about 2.6 · 104 cm 2/(Vs) (at a corresponding carrier density n ≈ 4·1012 cm−2), which is in line with Hall mobilities reported in previous studies for InSb nanoflags, InSb shallow quantum wells, and InAsSb shallow QWs.

Conclusion and Outlook

An advantage of the InAsSb material system compared to InAs and InSb is the larger Landé g-factor while maintaining a comparable mobility. Ternary compounds are generally more challenging to grow than binaries, but on the other hand, they allow control on lattice constant, band gap, and effective mass via composition engineering. Compared to one-dimensional nanowires, two-dimensional systems allow greater flexibility in device design and fabrication. Finally, compared to NFs, quantum wells constitute a scalable technology that can provide high mobility but their active region is typically buried more than 100 nm under the surface. The InAsSb NFs have a large Landé g-factor of 58.7 ± 4.0 and show signs of surface conduction. These characteristics make them a promising platform to study topological superconductivity in hybrid S-Sm systems and a good candidate to host exotic bound states.

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JournalName

Growth and Transport Properties of InAsSb Nanoflags†

Sebastian Serra,a Gaurav Shukla,a Giada Bucci,a Robert Sorodoc,a Valentina Zannier,a Fabio Beltram,a Lucia Sorba,a and Stefan Heuna

The present work reports, for the first time, the growth of high-quality free-standing InAsSb nanoflags and their electronic properties. Different growth conditions have been explored, and zinc-blende InAsSb nanoflags of various composition have been obtained. In particular, InAs0.77Sb0.23 nanoflags are on average (2000±180) nm long, (640±50) nm wide, and (130±30) nm thick. We show that these nanoflags have a Landé g-factor larger than InAs and InSb and a mobility comparable to those of the best performing InAs and InSb nanoflags. Besides, we show evidence for a surface Fermi level pinning in the conductance band of these InAs0.77Sb0.23 nanoflags, similar to the well-known behavior of InAs. This promises to make InAsSb easy to couple to superconductors, while keeping or improving many of the features that make InSb an interesting material for quantum applications.

1 Introduction

III-V semiconductors have been the subject of extensive study, as they are considered ideal for a variety of electronic and optoelectronic applications, like high-performance transistors, 1–3 light emitters, 4,5 photodetectors, 6,7 and photovoltaics. 8,9 In particular, high quality crystals with narrow band gap, strong spinorbit interaction, and large Landé g-factor are considered promising platforms for optoelectronics, spintronics, and quantum computing applications. Among these compounds, indium arsenide (InAs), indium antimonide (InSb), and the ternary alloy indiumarsenide-antimonide (InAsSb), represent ideal candidates for these purposes.

InAs has a narrow and direct bandgap (∼ 0.39 eV in wurtzite structure and ∼ 0.35 eV in zincblende structure, at a temperature of 300 K), 10 low effective mass (m∗ InAs = 0.023me, where me is the rest mass of the free electron), 11 high carrier mobility (> 106 cm2/(Vs) in 2DEGs in InAs quantum wells, 12,13 and (6500 − 8000 cm2/(Vs) in nanoflags (NFs)), and a relatively large Landé g-factor (g∗ = 17.0±0.5 in InAs 2DEGs, 15 larger than for InAs bulk, where g∗ bulk = 14.7. Due to these properties, extensive studies have been conducted on InAs 1D and 2D nanostructures. Moreover, due to the strong spin-orbit interaction, InAs 2DEGs have been proposed as a platform for topological superconductivity in hybrid superconductor-semiconductor (S-Sm) systems.

InSb has an even narrower direct bandgap of 0.17 eV and a lower effective mass than InAs (m∗ InSb = 0.014me), 11,22 high carrier mobility (up to 3.5 · 105 cm2/(Vs) in quantum wells,, one order of magnitude less in free-standing nanostructures),, large Landé g-factor (∼ 50), and even stronger Rashba spinorbit strength than InAs. For these reasons, this material has recently been considered as a promising platform for topological applications in S-Sm systems, and gate controlled supercurrents are under study in InSb-based Josephson junctions,.

Improvements for AI systems

  1. The improved AI system can accurately predict Landé g-factors by using Eq. 9 derived from experimental measurements: g∗ = 2 m∗/me ∆EZ / ∆ELL. This allows for reliable prediction of material properties based on measured effective masses and magnetic field parameters, specifically estimating the Landé g-factor of InAs0.77Sb0.23 NFs to be 58.7±4.0.

  2. The AI system can model charge carrier density and Hall mobility under various conditions by utilizing the derived formulas: n = Isd / e · ∂Vxy / ∂B −1 and µH = L W · ⟨Vxx⟩ · ∂Vxy / ∂B. This capability enables the prediction of transport properties as a function of back-gate voltage and magnetic field, including identifying regimes where Hall mobility peaks, such as the peak Hall mobility at 0.44 K has a peak of about 2.6 · 104 cm2/(Vs).

  3. The system can predict Landau level filling factors based on the measured slopes in the conductance variation using kN = e απħ / (N + 1/2). This allows for the identification of spin-degenerate Landau levels by analyzing the experimentally observed ratios k1/k0 = 3 and k2/k1 = 5/3, which is crucial for understanding magneto-transport effects.

Abstract

The present work reports, for the first time, the growth of high-quality free-standing InAsSb nanoflags and their electronic properties. Different growth conditions have been explored, and zinc-blende InAsSb nanoflags of various composition have been obtained. In particular, InAs0.77Sb0.23 nanoflags are on average (2000+-180) nm long, (640+-50) nm wide, and (130+-30) nm thick. We show that these nanoflags have a Landé g-factor larger than InAs and InSb and a mobility comparable to those of the best performing InAs and InSb nanoflags. Besides, we show evidence for a surface Fermi level pinning in the conductance band of these InAs0.77Sb0.23 nanoflags, similar to the well-known behavior of InAs. This promises to make InAsSb easy to couple to superconductors, while keeping or improving many of the features that make InSb an interesting material for quantum applications.

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