Exchange interactions and intermolecular hybridization in a spin-1/2 nanographene dimer

arXiv:2307.09930 · cond-mat.mes-hall · Submitted 2023-07-19 · Read on arXiv

Listen

Radio episode about this paper

Transcript

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: "Exchange interactions and intermolecular hybridization in a spin-1/2 nanographene dimer".

Kai: In this study, researchers investigate exchange interactions and intermolecular hybridization in a spin-1/2 nanographene dimer to understand spin physics relevant for quantum technologies.

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

Paper summary: Kai: So, to wrap up this first part, we've seen how the researchers explored the fundamental magnetic exchange mechanisms within this spin-one/two nanographene dimer, focusing on how substrate coupling influences those spins. The core of what they are presenting is that they've identified a specific type of singlet–triplet excitation driven by interphenalenyl exchange, and they linked this to the necessity of third-neighbor hopping for enabling kinetic exchange.

Mira: Exactly, Kai; the thesis is that intermolecular hybridization, specifically driven by non-zero third-neighbor hopping in this system, is what's crucial for activating kinetic interphenalenyl exchange. They use inelastic electron tunneling spectroscopy to observe these excitations and then use theoretical modeling to confirm the existence of two antiferromagnetically coupled unpaired spins leading to an S = zero ground state and an S = one excited state with energy E = J.

Lev: From a quantum error correction perspective, if we can pin down the exact nature of this exchange—is it purely local or does it involve these long-range interactions—we can start designing error syndromes that specifically target those long-range couplings.

Kai: Right, and they also detailed the experimental synthesis of the diphenalenyl dimer, showing how they prepared it using a combined solution and on-surface synthesis approach involving STM tip activation to create the diradical. That's a tangible part of making these theoretical models real.

Mira: And they also pointed out that the substrate coupling, specifically interaction with Au(one hundred eleven) versus NaCl, leads to a renormalization of the spin excitation energies, with the difference between forty-one meV and forty-eight meV being attributed to this exchange.

Lev: I wonder if that renormalization is stable enough for a qubit operation; we need predictable energy levels that don't drift significantly under operational conditions.

Kai: The paper also highlighted the position-dependent bias-asymmetry in the dI/dV spectra, which they state is an intrinsic property of the molecules independent of the substrate.

Mira: That asymmetry is quantified by looking at the projected density of states for HOMO and LUMO orbitals, where for instance, the HOMO shows a significantly larger step for negative bias than for positive bias.

Lev: If that intrinsic molecular asymmetry is what we rely on, we need robust experimental setups that can accurately resolve those subtle differences in spectral features without being overwhelmed by noise.

Conclusion: Kai: So, looking at the full scope of this work on "Exchange interactions and intermolecular hybridization in a spin-one/two nanographene dimer," it boils down to establishing a solid framework for understanding how these radical species behave when coupled together. The authors, including Krane, Turco, Bernhardt, Jacob, Gandus, Passerone, Luisier, Juríček#, Fasel # and Fernández-Rossier#, have provided the necessary evidence connecting theoretical exchange to measurable spectroscopic data.

Mira: They’ve essentially shown that for these dimer systems, you absolutely must consider both the substrate environment and the long-range hopping effects when modeling spin interactions. This means that simply looking at local bonds isn't enough; intermolecular hybridization is a necessary component of the physics.

Lev: For someone focused on experimental realization, the implication here is that future work needs to move toward synthesizing systems where these specific third-neighbor hopping mechanisms are dominant, because that's where the interesting physics lies.

Kai: That's right; it sets a clear direction for experimentalists on what kind of coupling we need to engineer for these types of nanographene structures to function as useful quantum components.

Mira: Ultimately, the paper concludes that these findings provide essential insights for designing platforms exploiting phenalenyl and other planar nanographene radicals in quantum technologies by emphasizing the importance of modeling both intermolecular hybridization and substrate effects.

nanotech@surfaces Laboratory, Empa - Swiss Federal Laboratories for Materials Science and Technology · Department of Chemistry, University of Zurich, Zurich, Switzerland · Departamento de Polímeros y Materiales Avanzados: Física, Química y Tecnología, Universidad del País Vasco UPV/EHU · IKERBASQUE Basque Foundation for Science · Integrated Systems Laboratory ETH Zürich, Switzerland · International Iberian Nanotechnology Laboratory INL · Department of Chemistry, Biochemistry and Pharmaceutical Sciences, University of Bern

cond-mat.mes-hall

Submitted: 2023-07-19

Updated: 2023-07-19

Comments: 16 pages main manuscript, 4 main figures; supplementary information containing additional data is included

Journal ref: Nano Lett. 2023, 23, 9353-9359

DOI: 10.1021/acs.nanolett.3c02633

Code: https://github.com/eimrek/tb

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

Importance score: 73/100

The gist: In this study, researchers investigate exchange interactions and intermolecular hybridization in a spin-1/2 nanographene dimer to understand spin physics relevant for quantum technologies.

Key concepts

Inelastic Electron Tunneling Spectroscopy (IETS)
A technique used to probe magnetic properties by measuring energy steps in tunneling current. In this study, it revealed specific excitation energies corresponding to singlet-triplet transitions caused by the exchange between the two molecules.
Interphenalenyl Exchange
This is a type of spin interaction occurring between two adjacent phenalenyl units in the dimer. The study found that this exchange leads to a singlet-triplet excitation, which is directly observable in the IETS data and is responsible for the magnetic energy splitting.
Third-Neighbor Hopping (t3)
This refers to a specific type of electron movement between parts of the dimer that are not directly next to each other. The study found that this non-zero hopping is essential for activating kinetic interphenalenyl exchange, meaning it drives the intermolecular hybridization between the two units.
Substrate Coupling Renormalization
The way the nanographene dimer interacts with a substrate (like Au(111) or NaCl) changes its spin excitation energies. The coupling with gold leads to a substantial change in energy compared to coupling with NaCl, demonstrating how the environment affects the molecule's magnetic behavior.

Terminology

Summary

In this study, researchers investigate exchange interactions and intermolecular hybridization in a spin-1/2 nanographene dimer to understand spin physics relevant for quantum technologies. The gist: Inelastic electron tunneling spectroscopy (IETS) reveals singlet–triplet excitation arising from interphenalenyl exchange, and theoretical analysis identifies third-neighbor hopping as essential for activating kinetic interphenalenyl exchange, which is further modulated by substrate coupling.

Synthesis and Characterization of the Dimer

The researchers synthesized the phenalenyl dimer, referred to as diphenalenyl, using a combined solution and on-surface synthesis approach. The preparation involved a sequence of nine steps starting from naphthalene in solution, followed by activation using atom manipulation with a scanning tunneling microscopy (STM) tip. Specifically, the precursor was deposited onto a clean Au(111) surface after preparing the substrate by sublimation of NaCl on Au(111). Sequential tip-induced cleaving of hydrogen atoms from the sp3 carbon atoms yielded the target diphenalenyl diradical, which was confirmed by constant-height nc-AFM measurements. This process demonstrated that "hydro precursors has the advantage that activation of the target open-shell compound can be achieved using atom manipulation with a scanning tunneling microscopy (STM) tip and does not necessarily require the catalytic action of metal substrates."

Spin Excitation Energies and Exchange Interactions

Inelastic electron tunneling spectroscopy (IETS) was used to probe the magnetic properties. The data revealed inelastic steps at ±41 meV on Au(111) and ±48 meV on a monolayer of NaCl on top of Au(111). These excitations are assigned to singlet–triplet excitation arising from interphenalenyl exchange. Theoretical analysis using a generalized Hubbard model, which includes long-range Coulomb interactions, showed that diphenalenyl hosts two antiferromagnetically coupled unpaired spins resulting in an S = 0 ground state and an S = 1 excited state with energy E = J. The calculated singlet–triplet splitting was found to be close to the experimentally observed energies.

Role of Intermolecular Hybridization and Hopping

The study provides evidence for intermolecular hybridization, which is crucial for kinetic interphenalenyl exchange. Theoretical calculations showed that intermolecular hybridization is present because third-neighbor hopping is non-zero, as the zero modes have a null weight on the binding sites if only first-neighbor hopping were considered. The calculation of the total exchange and its relative contribution from intermolecular hybridization and intramolecular addition energies indicated that the dimer has a strong diradical character. The third-nearest-neighbor hopping, denoted as t3, was found to be non-zero and is dominant in driving the intermolecular hybridization between the two phenalenyl units.

Substrate Dependence and Renormalization

The coupling of diphenalenyl to the substrate significantly affects the excitation energies and linewidths. The energy difference between excitations on Au(111) (41 meV) and on NaCl (48 meV) is attributed to renormalization of the spin excitation energies due to exchange with the Au(111) electrons. Ab initio calculations using an Anderson impurity model solved via the one-crossing approximation (OCA) showed that hybridization with Au(111) leads to a substantial renormalization compared to NaCl. Specifically, DFT calculations indicated that for Au(111), hybridization is appreciable, whereas for the NaCl monolayer, it is very weak, leading to negligible renormalization of the excitation energy by Kondo exchange coupling on NaCl.

Bias Asymmetries and Orbital Contributions

The analysis of dI/dV spectra revealed position-dependent bias-asymmetry in the height of inelastic steps. This asymmetry is an intrinsic property of the diphenalenyl molecules and independent from the underlying substrate. The contribution to step heights was analyzed using the projected density of states (PDOS) for HOMO and LUMO orbitals. For example, the HOMO has a significantly larger step for negative bias than for positive bias, while for the LUMO it is exactly the opposite. Furthermore, on Au(111), the spectra show characteristic triangular overshoots induced by Kondo exchange with the conduction electrons, which are especially pronounced for the positive-bias step in the LUMO spectral function. The LDOS maps confirmed these asymmetries, showing that over the center of the molecule, the negative bias step is significantly larger than the positive bias step.

Conclusion and Outlook

The study concludes that diphenalenyl acts as an open-shell molecule exhibiting strong interphenalenyl antiferromagnetic exchange. The findings establish a framework for understanding how substrate coupling modifies these spin excitations, providing essential insights for the design of platforms exploiting phenalenyl and other planar nanographene radicals in quantum technologies. The results underscore the importance of considering both intermolecular hybridization and substrate effects when modeling spin interactions in coupled nanographene systems.

Improvements for AI systems

Based on the provided scientific paper, here are specific improvements for AI systems and what those improved systems could achieve:


The core of this research lies in understanding and manipulating spin interactions (exchange interactions) in open-shell nanographene dimers (like diphenalenyl). The proposed AI improvements focus on leveraging the deep quantum mechanical insights derived from these calculations to create more sophisticated materials science simulators and quantum computing platforms.

Here are the specific improvements:


  1. The paper details a comprehensive theoretical framework involving:

    • Extended Hubbard models (S1, S3) incorporating third-nearest-neighbor hopping and Coulomb interactions (including Coulomb exchange/CDE).
    • The Anderson Impurity Model (AIM) coupled to a substrate bath (S4).
    • The One-Crossing Approximation (OCA) for solving the AIM to obtain spectral functions and excitation energies.

An AI system trained on this framework could be used for:


  1. The improved AI system could perform highly accurate, first-principles simulations of spin dynamics in molecular systems, specifically predicting the singlet–triplet excitation energy (E = J) and its dependence on substrate coupling strength (e.g., Au(111) vs. NaCl).


  2. The improved AI system could predict the renormalization of these spin energies caused by substrate hybridization, allowing researchers to design molecules where the exchange interaction is robust against environmental changes or engineered for specific quantum phases (e.g., topological order).


  3. The paper explicitly links the electronic structure (HOMO/LUMO contributions) to experimental observables like dI/dV spectra asymmetries and bias-dependence at different spatial locations within the dimer.


  4. The improved AI system could be used for inverse design of nanographene dimers, allowing researchers to computationally design molecular structures that exhibit specific, desired spectroscopic signatures (like a large negative bias step asymmetry) before synthesizing them experimentally.


  5. The paper shows that the role of third-neighbor hopping (t3) is crucial for intermolecular exchange in these systems, which is often ignored in graphene modeling.


  6. The improved AI system could serve as a tool to identify and prioritize structural motifs (like specific bond geometries or hopping pathways) that drive quantum phenomena (like interphenalenyl exchange), guiding the synthesis of materials with desired spin lattices for quantum magnetism exploration.


  7. The paper provides detailed, substrate-dependent coupling parameters (hybridization strengths, Γ values) derived from DFT and NEGF calculations.


  8. The improved AI system could serve as a predictive tool for designing molecular platforms that optimize spin qubit properties by precisely tuning the molecule-substrate interface to maximize or minimize Kondo exchange effects, thereby engineering robust spin qubits.


  9. The paper demonstrates how coupling to the substrate modifies spectral linewidths (broadening) and Kondo exchange effects, which are crucial for understanding experimental limitations in STM/STS measurements.


  10. The improved AI system could be used to predict the expected experimental resolution and line-shape of spin excitation steps for a given molecule-substrate combination, ensuring that experimental setups are optimized to resolve subtle quantum features accurately.


  11. The paper explores the distinction between different coupling mechanisms (intermolecular hybridization vs. Coulomb-mediated exchange).


  12. The improved AI system could act as a diagnostic tool for experimentalists, helping them determine whether the observed spin dynamics are dominated by kinetic exchange or Coulomb interactions, thereby interpreting complex spectroscopic data accurately and distinguishing between competing physical mechanisms in real-time.

Abstract

Phenalenyl is a radical nanographene with triangular shape that hosts an unpaired electron with spin S = 1/2. The open-shell nature of phenalenyl is expected to be retained in covalently bonded networks. Here, we study a first step in that direction and report the synthesis of the phenalenyl dimer by combining in-solution synthesis and on-surface activation and its characterization both on Au(111) and on a monolayer of NaCl on top of Au(111) by means of inelastic electron tunneling spectroscopy (IETS). IETS shows inelastic steps that, together with a thorough theoretical analysis, are identified as the singlet-triplet excitation arising from interphenalenyl exchange. Two prominent features of our data permit to shed light on the nature of spin interactions in this system. First, the excitation energies with and without the NaCl decoupling layer are 48 and 41 meV, respectively, indicating a significant renormalization of the spin excitation energies due to exchange with the Au(111) electrons. Second, a position-dependent bias-asymmetry of the height of the inelastic steps is accounted for by an interphenalenyl hybridization of the singly occupied phenalenyl orbitals that is only possible via third neighbor hopping. This hybridization is also essential to activate kinetic interphenalenyl exchange. Our results set the stage for future work on the bottom-up synthesis of spin S = 1/2 spin lattices with large exchange interaction.

Sources

Related papers