Stark effect and dissociation of mesons in holographic conductor
arXiv:2308.00361 · doi:10.1007/JHEP11(2023)128
Abstract
We study the meson spectrum of the supersymmetric Yang-Mills theory with fundamental hypermultiplets for a finite electric field by using the D3/D7 model. The spectrum for scalar and vector mesons is computed by analyzing the (quasi-)normal modes for the fluctuations of the D7-brane embedding and gauge fields. In the presence of an electric field, two different phases in the background are realized: the meson and dissociation phases. In this paper, we analyze the meson spectrum of scalar and vector mesons for all ranges of the electric field and explore the effect of the electric field on the meson spectrum, that is, the Stark effect. In the meson spectrum, we observe the avoided crossing between different levels due to the coupling of fluctuations via the electric field.
31 pages, 12 figures. v2: match published version
References in corpus (17)
- Minkowski-space correlators in AdS/CFT correspondence: recipe and applications
- Metallic AdS/CFT
- Holographic Phase Transitions with Fundamental Matter
- Holographic spectral functions and diffusion constants for fundamental matter
- Hydrodynamics of Holographic Superconductors
- AdS/CFT with Flavour in Electric and Magnetic Kalb-Ramond Fields
- Flavoured Large N Gauge Theory in an External Magnetic Field
- Finite Temperature Large N Gauge Theory with Quarks in an External Magnetic Field
- Quarks in an External Electric Field in Finite Temperature Large N Gauge Theory
- Spectroscopy of fermionic operators in AdS/CFT
- Merger Transitions in Brane--Black-Hole Systems: Criticality, Scaling, and Self-Similarity
- Measurement and numerical calculation of Rubidium Rydberg Stark spectra
- Fermions and baryons as open-string states from brane junctions
- Electric Field Quench in AdS/CFT
- Holographic Spectral Functions in Metallic AdS/CFT
- Dynamical stability and filamentary instability in holographic conductors
- Mechanism for Negative Differential Conductivity in Holographic Conductors