Research ArticleCONDENSED MATTER PHYSICS

Cavity quantum-electrodynamical polaritonically enhanced electron-phonon coupling and its influence on superconductivity

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Science Advances  30 Nov 2018:
Vol. 4, no. 11, eaau6969
DOI: 10.1126/sciadv.aau6969

Abstract

So far, laser control of solids has been mainly discussed in the context of strong classical nonlinear light-matter coupling in a pump-probe framework. Here, we propose a quantum-electrodynamical setting to address the coupling of a low-dimensional quantum material to quantized electromagnetic fields in quantum cavities. Using a protoypical model system describing FeSe/SrTiO3 with electron-phonon long-range forward scattering, we study how the formation of phonon polaritons at the two-dimensional interface of the material modifies effective couplings and superconducting properties in a Migdal-Eliashberg simulation. We find that through highly polarizable dipolar phonons, large cavity-enhanced electron-phonon couplings are possible, but superconductivity is not enhanced for the forward-scattering pairing mechanism due to the interplay between coupling enhancement and mode softening. Our results demonstrate that quantum cavities enable the engineering of fundamental couplings in solids, paving the way for unprecedented control of material properties.

INTRODUCTION

Strong coupling and manipulation of matter with photons in quantum-electrodynamical (QED) environments are becoming a major research focus across many disciplines. Among the topics with large potential are the creation of exciton-polariton condensates (1), polaritonic chemistry (25) and transport (6), quantum nanoplasmonics (7), light-induced topology (810) and magnetism in 2D materials (11), and novel spectroscopies (12). In condensed matter, the search for control knobs to design properties of quantum materials is an ongoing broad research effort (13). One possible route is to use the nonequilibrium dynamics and coherent manipulation of quantum many-body systems with ultrashort laser pulses (1423). However, in these cases, “classical” light was typically used. Here, we propose a new route toward manipulating microscopic couplings in solids and inducing ordered phases especially at interfaces and in two-dimensional (2D) materials.

The discovery of enhanced superconductivity in monolayer FeSe on SrTiO3 (2426) and its possible relation to a cross-interfacial electron-phonon coupling (2729) has stimulated considerable interest with an ongoing open debate (3035). Irrespective of the outcome of this debate, the interfacial phonon mode under consideration is of particular interest for light-control purposes as it has a dipole moment implying bilinear phonon-photon coupling, while at the same time, the phonon also couples bilinearly to in-plane FeSe electrons, with a vertex that is strongly peaked for small momentum transfers known as forward scattering. This combination of features is due to the high degree of anisotropy owing to the interfacial structure. Here, we use a prototypical model system, related to FeSe/SrTiO3, for this extreme forward scattering to investigate how photon-phonon coupling in cavities can affect electron-phonon coupling and phonon-mediated superconductivity.

RESULTS

Setup: 2D material inside a cavity

In Fig. 1A, we show the setup for a 2D material inside a QED cavity environment with perfectly reflecting mirrors. The mirrors confine the photon modes inside the cavity and can lead to strong light-matter coupling even when only the vacuum of the electromagnetic field is considered (36, 37). Specifically, we propose a layered structure of a 2D material (e.g., monolayer FeSe) on a dielectric substrate with a large dielectric constant (e.g., SrTiO3) that further helps confine the cavity photon modes of interest.

Fig. 1 Setup of 2D material in optical cavity, phonon polariton frequency dispersions, and momentum-dependent electron-phonon coupling vertices for the polariton branches.

(A) We consider a setup with a 2D material on a dielectric substrate inside a small optical cavity with mirrors as shown. (B) Schematic phonon, photon, and upper and lower polariton dispersions versus 2D in-plane momentum q. The coupling of the phononic dipole current to the photonic vector potential leads to a splitting determined by the plasma frequency ωP. In the cavity, ωP is controlled by the cavity volume. (C) Momentum-dependent squared electron-boson vertex g2(q). For forward scattering, the squared bare electron-phonon vertex Embedded Image is peaked near q = 0. In the polaritonic case (ωP > 0), the upper polariton branch inherits some of the electron-phonon coupling at small q.

For the particular example of FeSe/SrTiO3, the effect of the cavity is to couple the electromagnetic field of the photons polarized along the z direction, perpendicular to the interfacial plane, to a cross-interfacial phonon mode. Here, we go beyond the often-used rotating-wave and dipole approximations for the light-matter interaction and use full minimal dipolar coupling including the JA and A2 terms (see section S2), which makes the theory manifestly gauge invariant and avoids unphysical divergences. The phonon has a dipole moment along the z direction that involves motion of the O and Ti ions in the topmost layer of SrTiO3, spatially very close to the FeSe monolayer. Specifically, one quasi-dispersionless optical Fuchs-Kliewer phonon at 92 meV (29) was identified as the most relevant phonon mode that strongly couples to the FeSe electrons both in angle-resolved photoemission (27) and high-resolution electron energy loss spectroscopies (29). The influence of screening on this mode is not settled yet, particularly when it comes to phonon linewidths (30, 31). However, the experimental evidence for its influence on electronic properties (27, 29) is definitely present, suggesting use of this mode to build a simplified model Hamiltonian to address the impact of reaching strong light-matter coupling on the superconducting behavior of the material. We specifically use a single-band model for the electrons in two spatial dimensions in a partially filled band with filling n = 0.07 per spin, as previously used to model the relevant electronic structure fitting angle-resolved photoemission data (28). A bilinear electron-phonon scattering is introduced by a coupling vertex Embedded Image that is strongly peaked near momentum Embedded Image with a coupling range q0. The coupling strength g0 is adjusted to keep a total dimensionless coupling strength λ ≈ 0.18 independent of q0, where λ is determined from the effective electronic mass renormalization m*/m = 1 + λ in the metallic normal state above the superconducting critical temperature in the absence of the cavity coupling. This conservative choice of λ is, for instance, below the value of 0.25 that was given in (29).

Through phonon-photon coupling, we study phonon-polariton formation in this setting. In Fig. 1B, we show schematically the resulting polariton branches that stem from a gauge-invariant coupling involving both JA and A2 terms, where J is the current of phononic dipoles associated to an infrared-active phonon mode, and A is the electromagnetic gauge field of the photons. The relevant effective coupling strength between photons and phonons is given by the phononic plasma frequency Embedded Image, with M as the reduced mass of the phonon (see section S2). For the 2D system in the cavity, the plasma frequency is controlled by the length of the vacuum inside the cavity in the z direction, Lz, and the 2D unit cell area ν0,2D = LxLy/NxNy, with Li and Ni as the length and number of unit cells of the system in i direction, respectively. The plasma frequency sets the splitting between the upper and lower polariton branches, reminiscent of the LO-TO splitting in bulk semiconductors. Obviously, this splitting is only relevant at very small momenta q, since the photon energies quickly become large compared to the phonon frequency as q increases because of the large magnitude of the speed of light.

The formation of phonon polaritons leads to a redistribution of the electron-phonon coupling vertex into the two polariton branches. In the following, we refer to this coupling between electrons and phonon polaritons as “electron-phonon coupling,” since the coupling originates from electron-phonon coupling in the free-space setting without cavity, and direct electron-photon coupling is not relevant in our setup. In Fig. 1C, we plot the squares of the coupling vertices between electrons and the respective polaritons as a function of q/kF, where kF is the Fermi momentum. A realistic value of the coupling range for FeSe/SrTiO3 was estimated as q0/kF ≈ 0.1, as needed to create replica bands in angle-resolved photoemission that duplicate primary band features without substantial momentum smearing (27, 28). In a microscopic model, this value depends on the distance h0 between the topmost TiO2 layer and the FeSe monolayer as well as the anisotropy of in-plane and perpendicular dielectric constants via Embedded Image, with realistic estimates ϵ/ϵ ≈ 100 and 1/(h0kF) ≈ 1. This coupling range is larger than the momentum at which photon and phonon branches cross and mix most strongly in the polariton formation process. This implies that the modification of electron-phonon coupling due to the cavity only happens at very small momenta typically smaller than q0/kF. Thus, to investigate how the degree of forward scattering influences the way in which cavity coupling is able to modify the electronic properties, we use different values for q0/kF below, envisioning that cavity effects are enhanced when q0/kF becomes smaller, which would, in practice, be achieved by making the dielectric-constant anisotropy ratio larger. In Table 1, we summarize the relevant parameter values of the bare material used in our simulations.

Table 1 Parameters of the bare material system without the cavity used for the simulations discussed in the main text.
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Cavity-enhanced electron-phonon interaction

The critical question to answer here is how the redistribution of the coupling vertex to the upper and lower polariton branches affects the electronic properties. We investigate this by a diagrammatic approach using Matsubara Green’s functions. We adopt the same approximations used in (28) and compute the self-consistent Migdal-Eliashberg diagram with dressed electronic Green’s function in Nambu space, allowing us to take into account superconducting order. The central quantity is the electronic self-energy Embedded Image, written in terms of the Pauli matrices Embedded Image, the effective mass renormalization Embedded Image, the band dispersion renormalization Embedded Image, and the anomalous self-energy Embedded Image, which vanishes in the normal state.

We first investigate the effect of the cavity on the effective electron-phonon coupling λ itself. This is of interest independent of superconductivity to be discussed below, as the electron-phonon coupling affects many other properties of materials, such as the conductivity, structural phase transitions, or superconductivity in standard Bardeen-Cooper-Schrieffer (BCS) superconductors. In particular, it plays a pivotal role for terahertz-driven nonequilibrium phases of materials. In Fig. 2, we show how cavity coupling modifies the temperature-dependent quasiparticle mass renormalization obtained from the normal self-energy for the different coupling ranges, realistic q0/kF = 0.105 (Fig. 2A), reduced q0/kF = 0.053 (Fig. 2B), and very small q0/kF = 0.021 (Fig. 2C). The first observation is that independent of the cavity, λ shows a strong temperature dependence, with a peak around Tc, decreasing both toward higher temperatures and toward lower temperatures deep inside the ordered phase. The former is readily understood as a usual temperature effect when at high temperature, the system becomes more and more classical and less correlated. The latter is understood by considering the fact that correlation effects are reduced deep in the ordered phase when quantum fluctuations lose their importance and a quasi-classical mean-field description can be adopted. λ is enhanced by the cavity at all temperatures. The cavity effects are more pronounced as ωP increases for fixed q0/kF and as q0/kF decreases for fixed ωP.

Fig. 2 Temperature-dependent electron-phonon coupling for different coupling ranges and plasma frequencies.

(A) Dimensionless electron-phonon coupling strength extracted from the normal self-energy at Embedded Image at the smallest Matsubara frequency, Embedded Image, as a function of temperature for a value of the coupling range in momentum space q0/kF = 0.105 representative of FeSe/SrTiO3, and different phononic plasma frequencies ωP as indicated. The case ωP = 0 represents the system without cavity. For increasing ωP, λ increases. Below the superconducting transition, which also shifts with ωP (see Fig. 3), λ decreases consistently for all values of ωP. (B) Temperature-dependent λ for smaller q0/kF = 0.053 and different ωP. As for the superconducting order parameter, the effects of the cavity coupling that is parameterized by ωP are more pronounced. (C) For even smaller q0/kF = 0.021, we obtain a strongly enhanced λ accompanied by the shift in the superconducting transition that shows up as a cusp in λ(T), which reaches a maximum at Tc.

Light-modified superconductivity

We now turn to the effect of the cavity on superconductivity. Naively, one might expect that an enhanced λ leads to enhanced superconducting critical temperature Tc. However, the relation is nontrivial as also the effective polariton frequency is relevant for Tc. We will see in the following that, unfortunately, for our system, the enhancement of λ is canceled by a reduction in the effective frequency.

Figure 3A shows the resulting temperature-dependent superconducting order gap Embedded Image evaluated at the smallest Matsubara frequency and at a Fermi momentum Embedded Image along the Brillouin zone diagonal for a coupling range q0/kF = 0.105 representative of FeSe/SrTiO3. Starting from a critical temperature Tc ≈ 63 K in the absence of the cavity (ωP = 0.0), we find a slight reduction of superconductivity as the cavity is introduced and its extension Lz in the z direction perpendicular to the 2D material is reduced, resulting in a nonzero Embedded Image. For perhaps unrealistically large values ωP = 5.0 (eV), a reduction of Tc on the order of 1 K is found in our simulations, which would likely require cavity sizes of a few lattice constants and might, in practice, be too small to achieve at the moment.

Fig. 3 Temperature-dependent superconducting gap for different coupling ranges and plasma frequencies.

(A) The superconducting gap at Embedded Image at the smallest Matsubara frequency, Embedded Image, as a function of temperature for a value of the coupling range in momentum space q0/kF = 0.105 representative of FeSe/SrTiO3, and different phononic plasma frequencies ωP (measured in electron volts for the FeSe example) as indicated. The case ωP = 0 represents the system without cavity. For the decreasing cavity volume, ωP increases, causing a decrease in Δ and the superconducting critical temperature Tc. (B) Temperature-dependent gap for smaller q0/kF = 0.053 and different ωP. The light-suppressed superconductivity is more pronounced. (C) For even smaller q0/kF = 0.021, strongly reduced Δ values are observed with increasing ωP.

To investigate the effect of the forward-scattering coupling range, we look at the change of the superconducting order in the case of q0/kF = 0.053 that is reduced by a factor of 2 from the realistic value described above (see Fig. 3B). In this case, the polaritonic redistribution of the coupling is expected to be more effective, as there is a better match between the coupling range and the polariton mixing. This is observed in the superconducting order enhancement. Where a value of ωP = 5.0 was needed in Fig. 3A to obtain a visible modification of Tc, here, a smaller value ωP = 2.5 is sufficient to enhance Tc by ≈1 K. Even larger ωP leads to enhancements of order 5%. Last, if we decrease the range by another factor of 2, q0/kF = 0.021, the modification is relatively strong with changes of more than 10%, shifting Tc by up to 10 K (Fig. 3C).

Analysis of the influence of the cavity on superconductivity

To gain physical intuition into why the enhancement of λ is insufficient to enhance superconductivity, we take a look at the approximate equation for Tc derived by Rademaker et al. (28) in the extreme forward-scattering and weak-coupling limitEmbedded Image(1)

From this expression, it becomes clear that the enhancement of λ has to be sufficiently strong compared to the suppression of Ω that happens concomitantly in our case. This should be contrasted with the standard expression for a momentum-independent coupling vertex in the BCS theory, Embedded Image The quasi-linearity in λ in Eq. 1 leads to relatively high Tc for moderate values of λ but, in the cavity, also has the negative effect that the enhancement of Tc scales only linearly rather than exponentially with λ.

DISCUSSION

Unfortunately, the enhancement of λ predicted here does not lead to an enhancement of the superconducting critical temperature Tc in our chosen setting. This effect is explained by the linear scaling of the critical temperature with λ for the case of extreme forward scattering in contrast to the exponential scaling for momentum-independent coupling. However, for more conventional pairing mechanisms not geared toward forward scattering, the observed enhancement of λ could naturally lead to enhanced Tc. Similarly, in dirty superconductors, momentum-conservation constraints are relaxed, which may lead to enhancement rather than suppression of Tc, as discussed in a slightly different context in (38).

Moreover, our theory and the analytical estimates of Tc are valid only in the Migdal-Eliashberg regime of weak coupling, unrenormalized polaritons, and adiabaticity. A polaritonic enhancement of λ could still lead to the enhancement of Tc even for the forward-scattering case at intermediate couplings, when feedback effects on the polaritons become important and when nonadiabatic effects come into play. Similarly, interplay between polaritonic pairing and other pairing mechanisms such as spin or orbital fluctuations is a subject for future study. It is possible that in these cases, our original motivation of this work, namely to enhance superconductivity in a cavity, might work out.

In summary, we propose to use QED cavity settings to control polaritonically mediated effects in low-dimensional materials. In reality, the size of the achieved effects will depend on the quality factor of the cavity, the degree to which our idealized boundary conditions are realized in practice, and on the required large coupling strengths that can actually be reached in real devices. However, our above results are ground-state modifications that are still qualitatively valid even in dissipative systems (5, 39). Moreover, for organic molecules in cavities, the ultrastrong-coupling regime was even achieved in bad cavities with small quality factors (40). Here, we predict changes of Tc in a few percent range for few-percent changes of the electron-phonon coupling λ. Known examples of LO-TO splitting in bulk semiconductors such as GaP suggest typical ratios of ωP/Ω of order 10% (41), an order of magnitude smaller than the ones used in this work. However, we caution that these are very different materials from the ones used here, and oxide dielectrics close to the ferroelectric phase transition, such as SrTiO3, were suggested to have giant LO-TO splittings exceeding 50% of the TO frequency (42) due to enhanced Born effective charges, placing them much closer to the values explored here. It remains to be answered how large realistic LO-TO splittings can become at interfaces. It will definitely be important to explore strategies for enhancing the plasma frequency by synthesizing samples using different substrates with strongly coupled polar phonons and exploring interface and heterostructure engineering to optimize the dielectric environment.

We note that a related idea of exciton-mediated superconducting pairing (43) in 2D heterostructures was introduced (44) and recently discussed in the context of transition-metal dichalcogenides (45). These proposals require exciton-polariton condensates to exist in the first place, which then affect pairing in doped nearby layers via coupling of quasi-free electrons to condensed exciton polaritons. By contrast, our present proposal does not rely on bosonic condensation but rather focuses on directly modifying the electron-phonon coupling through polariton formation in a cavity. For the example of FeSe/SrTiO3, our proposal could help shed light on the abovementioned debate about the role of the forward-scattering phonon for superconductivity. If the coupling of the phonon to electrons is unimportant, then the polaritonic effects will not play a role, which could serve as a test for the influence of the phonon on the electronic properties. Similarly, it was recently suggested to use classical lasers in a pump-probe setting to study the forward-scattering nature of the phonon (46). Ongoing work focuses on a realistic ab initio computation of cavity-enhanced couplings via dipolar phonons using the framework of QED density functional theory (47).

Note added in revision

Upon revision of the manuscript, we became aware of two related works that discuss related ideas of modifying superconducting properties by electron-photon interactions in cavities (38, 48).

MATERIALS AND METHODS

We used a cavity QED setting with plane-wave mode expansion inside a cavity, with fixed-node boundary conditions for confined cavity photon modes along the z direction and periodic boundary conditions in the extended 2D plane (see section S1). Specifically, we use the Migdal-Eliashberg approximation to the electronic self-energy to a coupled electron-polariton model Hamiltonian involving electron-phonon forward scattering and dipolar phonon-photon coupling.

The electron-polariton Hamiltonian has the formEmbedded Imagewith Embedded Image (Embedded Image) as the electron creation (annihilation) operators at wave vector Embedded Image and spin σ and Embedded Image as the electronic band dispersion measured relative to the chemical potential μ, which was adjusted to fix a band filling of 0.07 per spin. Furthermore, N is the number of k points in the 2D Brillouin zone, and Embedded Image is the polariton-momentum Embedded Image-dependent electron-polariton coupling to branch λ = ±Embedded Image(2)Embedded Image(3)with bosonic polariton creation (annihilation) operators Embedded Image (Embedded Image) for the polaritons with energiesEmbedded Image(4)

The unitary transformation from phonons and photons to polaritons is parameterized byEmbedded Image(5)

Here, the underlying bare energies are given by the electronic hopping t = 0.075 eV (28) and the phonon frequency Ω = 92 meV (29), and the bare photon dispersion is Embedded Image with speed of light c, and we used a variable effective phononic plasma frequency ωP throughout the main text. Further details can be found in sections S2 and S3.

The Migdal-Eliashberg electronic self-energy on the Matsubara frequency axis is given byEmbedded Imagewith self-consistent electronic Nambu Green’s function Ĝ, decomposed into Pauli matrices Embedded Image, unrenomalized polaritonic Green’s function D(0), and fermionic Matsubara frequencies ωn = (2n + 1)π/β and bosonic Matsubara frequencies ωn = 2nπ/β, n ∈ ℤ, and inverse temperature β = (kBT)−1. This amounts to the approximation that the bare phonon mode already contains the energy-shift renormalization due to electron-phonon coupling as the bare phonon frequency is taken from experimental data, and further renormalizations of the phonon polaritons due to electron-polariton coupling are small. The self-consistent computation of Embedded Image was initialized with a seed for the anomalous superconducting self-energy of 0.007 eV and a convergence criterion of 10−6 eV. Further details can be found in section S4.

SUPPLEMENTARY MATERIALS

Supplementary material for this article is available at http://advances.sciencemag.org/cgi/content/full/4/11/eaau6969/DC1

Section S1. Relevant photon modes in cavity

Section S2. Phonon-photon Hamiltonian

Section S3. Electron-polariton Hamiltonian

Section S4. Migdal-Eliashberg simulations

This is an open-access article distributed under the terms of the Creative Commons Attribution-NonCommercial license, which permits use, distribution, and reproduction in any medium, so long as the resultant use is not for commercial advantage and provided the original work is properly cited.

REFERENCES AND NOTES

Acknowledgments: Discussions with H. Appel, S. Johnston, S. Latini, A. J. Millis, and L. Rademaker are gratefully acknowledged. Funding: M.A.S. acknowledges financial support from the DFG through the Emmy Noether Programme (SE 2558/2-1). A.R. acknowledges financial support from the European Research Council (ERC-2015-AdG-694097), Grupos Consolidados (IT578-13), and the European Union’s H2020 program under GA no. 676580 (NOMAD). Author contributions: M.A.S. performed the calculations. M.A.S. and M.R. developed the model, with critical feedback from A.R. The idea of cavity-enhanced electron-phonon coupling was conceived by all authors while developing the implications of cavity QED density functional theory to materials. All authors discussed the results and wrote the manuscript. Competing interests: The authors declare that they have no competing interests. Data and materials availability: All data needed to evaluate the conclusions in the paper are present in the paper and/or the Supplementary Materials. All data generated and analyzed during this study are available from the corresponding author upon reasonable request.
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