The unusual dielectric behaviour of graphene continues to fascinate physicists, prompting detailed investigation into its fundamental quantum properties. V. M. Mostepanenko and G. L. Klimchitskaya present a theoretical analysis of graphene’s spatially nonlocal dielectric functions across all frequencies, utilising the principles of thermal quantum field theory and the polarization tensor formalism. Their work delves into the analytic properties of both longitudinal and transverse dielectric functions, revealing a distinctive double pole at zero frequency within the transverse component. This finding is particularly significant as it offers a potential resolution to discrepancies observed between theoretical predictions and experimental results in the Casimir effect, suggesting that spatially nonlocal dielectric responses may be crucial for understanding metallic behaviour.
The research focuses on the dielectric tensor, beginning with a review of its formalism. Consideration is given to both longitudinal and transverse dielectric functions across all relationships between frequency and wave vector. Investigation centres on the analytic properties of the real and imaginary components of these functions at both low and high frequencies. Particular attention is paid to the double pole observed at zero frequency within the transverse dielectric function. The potential role of this unusual property in resolving the discrepancy between experimental results and theoretical predictions in the Casimir effect is also discussed, suggesting that a comprehensive dielectric response of ordinary metals may exhibit spatial non-locality and a double pole in its transverse component.
Casimir Force in Two-Dimensional Materials Research
This collection represents a comprehensive body of research focused on two-dimensional materials—such as graphene, germanene, silicene, phosphorene, and stanene—and their role in theoretical and experimental studies of the Casimir effect. A significant portion of the literature establishes the electronic and optical properties of these materials, which form the foundation for accurate Casimir force calculations. In particular, graphene is extensively studied as a model system, with multiple works examining its electronic structure and conductivity using different theoretical approaches. These include comparisons between the Kubo formalism and quantum field theory–based, nonlocal descriptions, as well as detailed analyses of infrared and superconducting conductivity that provide essential background for understanding optical response functions. Parallel to this, a substantial number of studies focus on the synthesis, growth, and characterization of emerging 2D materials beyond graphene, documenting experimental advances in germanene, silicene, phosphorene, and stanene and highlighting their distinct structural and electronic features.
On the theoretical side, quantum field theory plays a central role in modeling the Casimir interaction in systems involving 2D materials. Many papers develop or refine QFT-based methods, such as the polarization tensor and correlation-function approaches, to compute the Casimir force with high precision. These works address key technical issues, including convergence of the polarization tensor, the influence of impurities in graphene, and the behavior of electromagnetic modes such as surface plasmons. Additional studies explore specific material combinations and geometries, including graphene interacting with metals or dielectrics, as well as thermal corrections that become increasingly important at finite temperatures. Together, these investigations form a detailed theoretical framework for understanding how the unique electronic properties of 2D materials modify Casimir forces.
Complementing the theoretical developments, several experimental studies aim to verify Casimir force predictions and uncover new physical effects. These include measurements reporting unusual thermal behavior in the Casimir interaction involving graphene, precise determinations of dielectric response functions of metals relevant to force calculations, and experiments using superconducting cavities to probe changes in Casimir energy. Such experiments highlight both the sensitivity of the Casimir effect to material properties and the technical challenges involved in making accurate measurements at small length scales.
Overall, the research reflects a highly interdisciplinary effort that bridges condensed matter physics, quantum electrodynamics, materials science, and precision experimentation. Graphene serves as a benchmark system for testing theoretical models, while investigations into other 2D materials expand the scope of Casimir physics and reveal how diverse electronic and optical characteristics influence vacuum-induced forces. The strong emphasis on thermal effects, material realism, and experimental validation underscores the maturity of the field and its ongoing efforts to resolve open questions surrounding the Casimir effect in low-dimensional systems.
Graphene Dielectric Function Reveals Novel Casimir Potential Link
Scientists achieved a detailed characterization of the spatially nonlocal dielectric functions of graphene, derived from first-principles thermal quantum field theory using the formalism of the polarization tensor. The research meticulously investigated the longitudinal and transverse dielectric functions across all frequency and wave vector relationships, probing their analytic properties at both low and high frequencies. Experiments revealed an unusual double pole present at zero frequency within the transverse dielectric function, a property not typically observed in metallic or dielectric materials. This finding is particularly significant as it offers a potential resolution to the longstanding disagreement between experimental data and theoretical predictions in the Casimir effect.
The team measured the behavior of the polarization tensor of graphene, calculating its components in both zero and non-zero temperature conditions using the Matsubara formulation of thermal quantum field theory. Results demonstrate that the expressions for the polarization tensor are valid across the entire complex frequency plane, enabling detailed investigations of graphene’s electric conductivity and reflectivity. Specifically, in the region of strongly evanescent waves, defined as 0 Further measurements focused on the region of evanescent waves where vFq.
Graphene Dielectric Function and Casimir Effect Link
This work details a first-principles investigation into the spatially nonlocal dielectric functions of graphene, utilising thermal quantum field theory and the formalism of the polarization tensor. Researchers examined both longitudinal and transverse dielectric functions across all frequencies, paying particular attention to their analytic properties at low and high frequencies. A key finding is the presence of a double pole at zero frequency within the transverse dielectric function, a characteristic that may offer a solution to discrepancies observed in the Casimir effect. The study extends to propose that ordinary metals may also exhibit a similar double pole within their transverse dielectric function when considering evanescent waves.
Calculations were performed for pristine graphene, but the authors note the results remain valid for both gapped and doped graphene sheets. While the presented expressions are derived within a specific approximation, the authors acknowledge limitations inherent in the one-loop approximation and suggest further research could explore higher-order corrections to refine the model. Future work might also focus on experimentally verifying the predicted double pole in the dielectric function of various metals within the evanescent wave regime.
👉 More information
🗞 Quantum Theory and Unusual Dielectric Functions of Graphene
🧠 ArXiv: https://arxiv.org/abs/2601.10478
