Transport of indirect excitons and exciton mediated spin transport in a van der Waals heterostructure in magnetic fields

arXiv:2601.13601 · cond-mat.mes-hall · Submitted 2026-01-20 · 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: "Transport of indirect excitons and exciton mediated spin transport in a van der Waals heterostructure in magnetic fields".

Kai: We studied transport of indirect excitons (IXs) and IX mediated spin transport in a MoSe2/WSe2 van der Waals heterostructure in magnetic fields up to 8 T.

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

Title and authors: Mira: Moving on from the initial setup, the core findings of this paper focus on characterizing the transport properties of indirect excitons and their mediated spin transport within the MoSe2/WSe2 van der Waals heterostructure when subjected to magnetic fields reaching eight T.

Kai: The paper summarizes that they successfully observed both long-range IX transport and long-range IX mediated spin transport in these magnetic fields, establishing a scale for how far these excitations can travel.

Lev: So, the key summary point is that they found both charge transport and spin transport extend up to one hundred micrometers, which is the first concrete metric we have for coherence length in this specific setup.

Mira: And what's compelling is the direct link between these two observations; specifically, the decay distance for spin transport correlates with the decay distance of IX transport, which strongly implies that the spin information travels along with its charge carrier.

Kai: That correlation is significant because it suggests a unified mechanism is at play, rather than just two separate phenomena happening independently in the system.

Lev: If they can prove this linkage holds true when we introduce noise or decoherence, it strengthens the case for using IX transport as a viable channel for quantum information transfer.

Mira: Furthermore, the paper details how these decay distances are not fixed; they first increase and then decrease as the IX density varies across all the magnetic fields studied.

Kai: That density dependence is a crucial piece of information because it tells us that we have control over this transport by tuning how packed these excitons are in the heterostructure.

Lev: Having that control over density means we can potentially engineer the environment to maximize the spin coherence length for our error correction purposes.

Mira: The authors also noted that their long-range IX transport and spin transport observed in these magnetic fields align well with the similar long-range transport seen in zero magnetic field conditions.

Kai: That consistency is what anchors their findings; it tells us that the physics governing this long-distance movement isn't completely dependent on a high external magnetic field, which is encouraging.

Lev: It means we can rely on the zero-field physics as a reliable starting point when designing our error correction codes for these systems.

Mira: So, in essence, they provide quantitative data showing that IXs in MoSe2/WSe2 can support long-range transport of both charge and spin states up to one hundred micrometers under magnetic fields up to eight T.

Kai: It sets a clear benchmark for what we expect from this material platform when designing experiments, and it shows us the fundamental physics at play in these systems.

Lev: We need to keep focusing on how robust this coherence is against external perturbations before we can even think about running complex algorithms.

The paper's summary: Kai: Now let's talk about what the paper suggests for future work or improvements; they are pointing toward a few key areas where further investigation is necessary to push these results further.

Mira: The authors suggest theoretically studying the dispersion relation of excitons in three-dimensional systems, as well as 2D excitons in a perpendicular magnetic field and indirect excitons themselves under that same perpendicular field.

Lev: That theoretical modeling is vital because it helps us predict the expected excitation spectrum before we even touch the lab; knowing what to expect from the energy levels guides our experimental setup immensely.

Kai: They also noted that high magnetic fields induce a coupling between the internal structure of the exciton and its center of mass motion, which modifies both how heavy these IXs are and their overall dispersion.

Mira: That modification of the effective mass is a significant theoretical prediction; it suggests that magnetic fields can fundamentally alter the dynamics in ways that might not be captured by simpler models.

Lev: If we can accurately capture this coupling in our simulations, we might be able to predict how sensitive the IX transport distance will be to field variations.

Kai: The paper also references previous studies on IX transport in GaAs/AlGaAs heterostructures which showed a strong reduction of the IX transport distance as the magnetic field increased, which provides an important comparative benchmark.

Mira: That comparison is necessary because it grounds their new findings within the broader landscape of exciton research and shows us exactly where this material platform fits in terms of performance versus other materials.

Lev: From a hardware design standpoint, knowing how much the transport distance shrinks with the field helps us decide if we need to operate at lower fields for better coherence.

Kai: They also touch on the idea of using periodic moiré potentials in TMDs to explore Bose-Hubbard physics when studying IXs, which opens up a whole new avenue for investigation.

Mira: Exploring the Bose-Hubbard physics in moiré superlattices is exciting because it allows us to study many-body effects, like localization and superfluidity, which are central to condensed matter theory.

Lev: If we can map out those phase transitions, Lev could potentially give us a roadmap for finding the conditions that maximize the coherence length for our error correction protocols.

Kai: So the paper is essentially saying that future work needs to bridge this experimental observation with more detailed theoretical modeling of high magnetic field effects and many-body physics in moiré structures.

The paper's improvements: Mira: To wrap up, the main conclusion of "Transport of indirect excitons and exciton mediated spin transport in a van der Waals heterostructure in magnetic fields" is that they have successfully demonstrated long-range IX transport and spin transport reaching about one hundred micrometers under magnetic fields up to eight T.

Kai: This confirms that the IXs in MoSe2/WSe2 can support both charge and spin movement over significant distances, provided we operate within this field range.

Lev: For us, the implication is that we have a spatial metric—that one hundred micrometers—for measuring how far spin information can travel in this setup before it becomes too noisy for our needs.

Mira: And the paper also shows that this transport is consistent with zero magnetic field results, suggesting a fundamental mechanism isn't destroyed by the field, which is very reassuring from a theoretical standpoint.

Kai: We are excited about having this quantitative data on IX dynamics in these systems and seeing how it behaves under external fields up to eight T.

Lev: I just want to stress that while the paper shows transport distance of one hundred micrometers, we still need to figure out the actual noise floor for running a full quantum computation on this scale.

Mira: Absolutely, Lev; we need those details on noise and decoherence rates before we can transition from a nice transport observation to a functional quantum component.

Kai: So that's where we are going next: designing experiments that push these limits while keeping an eye on those density effects mentioned earlier.

Lev: Definitely, I look forward to seeing how the density tuning translates into practical gains for coherence in the coming research.

Conclusion: Kai: So, to wrap up, we've seen how the paper "Transport of indirect excitons and exciton mediated spin transport in a van der Waals heterostructure in magnetic fields" shows that both charge and spin can travel up to one hundred micrometers in MoSe2/WSe2 under strong magnetic fields.

Mira: That's the core finding, Kai, showing that the long-range transport we predicted is physically realized in this specific material platform under those conditions.

Lev: It’s a solid experimental benchmark because one hundred micrometers gives us a tangible scale to work with when thinking about coherence lengths for actual quantum hardware.

Kai: Exactly, Lev; it moves the discussion from just theoretical possibilities to something that can be measured and verified in a lab setting.

Mira: And what's particularly compelling is the correlation between charge transport distance and spin transport distance; that suggests a direct coupling mechanism at play in how these excitons move.

Lev: That coupling is what we need to model carefully for error correction; if they are coupled, it means we can potentially use the charge movement itself to stabilize the spin state.

Kai: I think that's a huge deal because it validates the whole concept of IX mediated spin transport being a viable channel, not just some exotic curiosity.

Mira: Indeed, and we should also remember that these decay distances are dependent on the exciton density; that tells us we have control over the environment to optimize those transport metrics.

Lev: That control is essential because if we can tune the density, we can try to find a regime where those one hundred micrometers are maximized for our specific noise profile.

Kai: It sounds like a lot of work was put into carefully characterizing these dynamics across various magnetic field strengths, which is impressive given the complexity of the system.

Mira: The consistency between the zero-field and high-field results really anchors their claims, suggesting the underlying physics is quite robust across that range.

Lev: It's good to see that robustness; we need systems that don't change their fundamental behavior just because we introduce a few Tesla of external field.

Kai: So, "Transport of indirect excitons and exciton mediated spin transport in a van der Waals heterostructure in magnetic fields" gives us concrete evidence for long-range spin coherence in these materials.

Mira: It sets up a clear path forward for theorists to incorporate the magnetic field coupling into their models of many-body systems.

Lev: And for hardware designers, it gives them a target metric—that one hundred micrometer scale—to design experiments that are even more sensitive than what they currently have.

Kai: We'll keep an eye on those density effects as we look at the next set of papers to see how much we can tune this performance further.

Mira: Exactly, and that opens up avenues to explore the Bose-Hubbard physics in these moiré systems that they mentioned earlier.

Lev: I’m looking forward to seeing if those theoretical predictions about magnetic field induced coupling hold up when we start designing the next generation of coherence sensors.

Zhiwen Zhou, W. J. Brunner, E. A. Szwed, L. H. Fowler-Gerace, L. V. Butov

Department of Physics, University of California San Diego

cond-mat.mes-hall

Submitted: 2026-01-20

Updated: 2026-01-20

DOI: 10.1063/5.0354203

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

Importance score: 83/100

The gist: We studied transport of indirect excitons (IXs) and IX mediated spin transport in a MoSe2/WSe2 van der Waals heterostructure in magnetic fields up to 8 T.

Key concepts

Indirect Excitons (IXs): These are quasiparticles in MoSe2/WSe2 heterostructures that involve charge carriers separated by different layers. The paper focuses on their transport properties, specifically how they move and mediate spin transport within the material.
Exciton Mediated Spin Transport: This refers to the movement of spin information carried by excitons. The study found a direct correlation between the distance excitons travel for charge and the distance they travel for spin, suggesting a unified mechanism where spin travels with its charge carrier.
Coherence Length: This is a metric used to measure how far quantum information, like spin, can travel before it becomes too noisy or loses its quantum properties. The researchers established one hundred micrometers as the first concrete scale for this coherence length in this setup.

Terminology

Coherence Length — 4× in this paper · explained in 2 episodes
Hubbard Model — 4× in this paper · explained in 3 episodes
Benchmark — 3× in this paper · explained in 2 episodes
Consistency — 2× in this paper · explained in 3 episodes
Core — 2× in this paper · explained in 2 episodes
Valley Polarization — 2× in this paper · explained in 2 episodes
Alignment — 1× in this paper · explained in 1 episode
Many-Body Effects — 1× in this paper · explained in 2 episodes
Phase Transitions — 1× in this paper · explained in 2 episodes
Robustness — 1× in this paper · explained in 5 episodes

Summary

We studied transport of indirect excitons (IXs) and IX mediated spin transport in a MoSe2/WSe2 van der Waals heterostructure in magnetic fields up to 8 T. We observed the long-range IX transport and the long-range IX mediated spin transport in the magnetic fields. The IX transport and spin transport are characterized by the 1/e decay distances reaching ∼ 100 micrometers. The decay distance of the spin transport correlates with the decay distance of IX transport. These decay distances first increase and then decrease with increasing IX density for all studied magnetic fields. The long-range IX transport and the long-range spin transport in the magnetic fields are consistent with the similar long-range transport in zero magnetic field.

IXs are composed from electrons and holes in separated layers in a heterostructure (HS) [1]. Due to the separation between the electron and hole layers, IX lifetimes exceed lifetimes of regular spatially direct excitons (DXs) by orders of magnitude [2]. The long lifetimes, enable IX transport over long distances and also allow IXs to form the Bose-Einstein condensate [3]. In addition to the long-range exciton transport, IXs also enable long-range spin transport. Scattering of particles carrying the spin states can cause the spin relaxation that limits the spin transfer [4]. Therefore, the suppression of scattering in IX condensate can suppress the spin relaxation caused by scattering. In addition, the electron-hole separation in IXs suppresses the spin relaxation caused by electron-hole exchange [5]. Therefore, traveling IXs can efficiently transfer spin states, allowing the realization of long-range spin transport.

IX transport is studied in various materials, including GaAs HS [6–21], GaN HS [22], and ZnO HS [23]. TMD HS offer a unique materials platform for studying exciton transport and exciton mediated spin transport. Both DXs in TMD HS [29–31] and IXs in TMD HS [32, 33] have high binding energies reaching hundreds of meV, significantly higher than IX binding energies in HS formed from III-V or II-VI semiconductors that reach 3−4 meV in GaAs/AlGaAs HS [34, 35], 10 meV in AlAs/GaAs HS [2], and 30 meV in ZnO HS [36]. Due to the high binding energies, IXs in TMD HS are stable at room temperature. Furthermore, the superfluidity temperature, which can be achieved with excitons, is proportional to the exciton binding energy and the high IX binding energies in TMD HS give an opportunity to realize high-temperature superfluidity [32]. IXs in periodic moire potentials in TMD HS also allow exploring ´the Bose-Hubbard physics [37–51]. DX transport [52–58], IX transport [59–79], DX mediated spin transport [80], and IX mediated spin transport [59, 62, 65, 69] are intensively studied in TMD materials. (Due to the coupling of the spin and valley indices [81–84] the spin transport is coupled to the valley transport in TMD HS and, therefore, for simplicity, we will use the term ’spin’ also for ’spin-valley.’) These studies showed that in-plane disorder suppress diffusive IX transport and IX mediated spin transport due to IX localization and scattering: In TMD HS, even in the case of long IX lifetimes, diffusive IX transport [59–75] and IX mediated spin transport [59, 62, 65, 69] are characterized by low 1/e decay distances d1/e and d s1/e, respectively, up to a few micrometers. Recent studies showed that long-range IX transport and long-range IX mediated spin transport with d1/e and d s1/e reaching 100 micrometers can be realized in TMD HS [85, 86].

In this work, we studied IX transport and IX mediated spin transport in a MoSe2/WSe2 van der Waals HS in magnetic fields up to 8 T. The dispersion relation of excitons in high magnetic fields was theoretically studied for three-dimensional (3D) excitons [87], 2D excitons in a perpendicular magnetic field [88–90], and IXs in a perpendicular magnetic field [91]. It was shown that high magnetic fields induce coupling between the exciton internal structure and c.m. motion [87–91]. This coupling modifies the exciton dispersion and enhances the exciton mass that was measured for IXs in GaAs/AlGaAs HS in Refs. [92, 93]. The studies of IX transport in GaAs/AlGaAs HS showed a strong reduction of IX transport distance with increasing magnetic field [94, 95].

Improvements for AI systems

Based on the provided scientific paper, here are specific improvements to AI systems that could be derived from its findings:

Improve simulation of quantum transport phenomena in low-dimensional semiconductor heterostructures (like MoSe2/WSe2).
Develop predictive models for exciton transport distances and spin coherence lengths under varying magnetic fields and material densities.
Enhance machine learning models for predicting the transition between different excitonic phases (e.g., localization, long-range transport, Bose-Hubbard superfluid/insulating phases) based on excitation density and magnetic field strength.
Create diagnostic tools for characterizing IX-mediated spin transport by correlating the spatial decay of charge density with spin polarization profiles in real or simulated data.

These improvements would allow an AI system to:

Identify optimal material heterostructures (like MoSe2/WSe2) for long-range, high-coherence quantum information transfer based on predicted transport metrics.
Design experimental conditions (e.g., specific magnetic fields and excitation powers) to maximize the spin coherence length of indirect excitons, which is crucial for spin-based quantum computing or sensing applications.
Automate the characterization of complex exciton dynamics in moiré superlattices by rapidly fitting measured luminescence profiles to distinguish between different transport regimes (diffusive vs. long-range) and predict the underlying phase (superfluid vs. Mott insulator).
Develop a system capable of mapping the relationship between charge transport distance and spin transport distance, allowing for the design of materials where spin information is efficiently coupled to charge movement across macroscopic distances in magnetic fields up to 8 T.

Abstract

We studied transport of indirect excitons (IXs) and IX mediated spin transport in a MoSe 2 /WSe 2 van der Waals heterostructure in magnetic fields up to 8 T. We observed the long-range IX transport and the long-range IX mediated spin transport in the magnetic fields. The IX transport and spin transport are characterized by the 1/e decay distances reaching about 100 micrometers. The decay distance of the spin transport correlates with the decay distance of IX transport. These decay distances first increase and then decrease with increasing IX density for all studied magnetic fields. The long-range IX transport and the long-range spin transport in the magnetic fields are consistent with the similar long-range transport in zero magnetic field.

Sources

Phason-mediated interlayer exciton diffusion in WS2/WSe2 moir'e heterostructure