Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Physica B Condensed Matter

On the fractional perturbation theory and optical transitions in bulk semiconductors: Emergence of negative damping and variable charged mass

Rami Ahmad El‐Nabulsi, Waranont Anukool

Published May 5, 2023• 7 citations
Publisher
DOI
10.1016/j.physb.2023.414942

Related papers

Microscopic theory of optical dephasing in semiconductors

S. W. Koch, T. Meier, F. Jahnke +1 more

Applied Physics A•Nov 1, 2000•24 citations

Many-body signatures of dimensional reduction in quasi-one-dimensional ZrS 3

Anonymous, Letizia Chiodo

The electronic and optical properties of quasi-one-dimensional transition-metal trichalcogenides remain largely unexplored beyond the mean-field approximation, and it is not clear how they evolve as the crystal is thinned. By performing first-principles many-body perturbation theory calculations, we determine the quasiparticle band structures and the polarization-resolved optical response of ZrS 3 in the bulk, bilayer, and monolayer limits, using a hierarchy of methods (hybrid DFT, G W , and the Bethe-Salpeter equation). We find that all three systems are indirect-gap semiconductors with a quasidirect character, the direct-indirect splitting being δ ≈ 0.10 – 0.13 eV and nearly independent of both the level of theory and the dimensionality. The mean-field gaps are almost insensitive to thickness, whereas the quasiparticle corrections increase the gap by ≈ 0.9 eV from bulk to monolayer. The effective exact-exchange fraction reproducing the G W gap scales as α ∼ ɛ ∞ − 1 , increasing from ≈ 0.19 to ≈ 0.33 , so that no single hybrid functional describes the full dimensional series. The optical onset blueshifts monotonically ( ≈ 2.4 → 2.8 → 3.0 eV ) and the near-edge absorption is strongly dichroic. A change in light polarization does not simply shift the excitonic resonance ( ≈ 0.09 eV ); it also reorganizes the underlying excitonic wave function, selecting distinct band channels and k -space regions. A real-space, participation-ratio analysis resolves moderately delocalized, Wannier-Mott-like excitons templated along the covalent chains. They are predominantly sulfur-derived (75%–88% of the density on sulfur for the chain-polarized bulk states), which identifies them as ( S 2 ) 2 − disulfide excitations rather than S → Zr charge-transfer states, while in the bilayer the electron delocalizes across both layers, the real-space imprint of interlayer screening. These results provide a consistent reference for the quasiparticle and excitonic energy scales of ZrS 3 from the bulk to the few-layer limit.

Physical review. B./Physical review. B•Oct 1, 2026•0 citations

Generation of quantum light with tunable Wigner negativity with a semiconductor quantum dot

Hubert Lam, Petr Steindl, Yann Portella +8 more

Wigner-negative states of light are key resources for quantum advantage in continuous-variable optical quantum computing. They can be produced probabilistically via frequency conversion and photon detection, or deterministically by exploiting the single-photon nonlinearity of a quantum emitter. Here, we generate such Wigner-negative states of light with a tunable negativity using a single semiconductor quantum dot in a cavity. Optical coherent control of the quantum-dot transition allows to generate a quantum superposition of zero and one photon. The generated quantum states are characterized point-by-point in the phase space through homodyne measurement. The emergence of Wigner-function negativity is observed as the excitation power is increased. After correcting for collection and propagation losses, we obtain fidelities to the ideal state and quantum purities above 95%, together with near-optimal quadrature squeezing. The ability to generate a wide variety of Wigner-negative states with mature semiconductor technology opens promising opportunities for continuous-variable optical quantum technologies.

quant-pharXiv:2610.36233•Oct 28, 2026•0 citations

Many-Body Theory of Coherent Optical Effects in Semiconductors

Rolf H. Binder, Yuan Z. Hu, A. Knorr +2 more

NATO ASI series. Series B : Physics•Jan 1, 1994•4 citations

Holographic entanglement negativity for a single subsystem in conformal field theories with a conserved charge

Sayid Mondal, Boudhayan Paul, Gautam Sengupta +1 more

Abstract We utilize a holographic construction to compute the entanglement negativity for bipartite mixed state configurations of a single subsystem in CFTd s with a conserved charge dual to bulk A d S d + 1 geometries. In this context, we obtain the holographic entanglement negativity for single subsystems with long rectangular strip geometries in CFTd s with a conserved charge dual to bulk non extremal and extremal Reissner–Nordström (RN)- A d S d + 1 black holes at the leading order in a perturbation theory. We demonstrate that the holographic entanglement negativity computed involves the elimination of thermal contributions at the leading order confirming earlier results in the literature. This also conforms to quantum information theory expectations and constitutes further consistency checks for the holographic construction.

arXiv:2102.05848•Journal of Physics A Mathematical and Theoretical•Sep 19, 2023•7 citations

Theory of coherent effects in semiconductors

Stefan W. Koch, C. Sieh, T. Meier +8 more

Journal of Luminescence•Nov 1, 1999•33 citations
The electronic and optical properties of quasi-one-dimensional transition-metal trichalcogenides remain largely unexplored beyond the mean-field approximation, and it is not clear how they evolve as the crystal is thinned. By performing first-principles many-body perturbation theory calculations, we determine the quasiparticle band structures and the polarization-resolved optical response of ZrS 3 in the bulk, bilayer, and monolayer limits, using a hierarchy of methods (hybrid DFT, G W , and the Bethe-Salpeter equation). We find that all three systems are indirect-gap semiconductors with a quasidirect character, the direct-indirect splitting being δ ≈ 0.10 – 0.13 eV and nearly independent of both the level of theory and the dimensionality. The mean-field gaps are almost insensitive to thickness, whereas the quasiparticle corrections increase the gap by ≈ 0.9 eV from bulk to monolayer. The effective exact-exchange fraction reproducing the G W gap scales as α ∼ ɛ ∞ − 1 , increasing from ≈ 0.19 to ≈ 0.33 , so that no single hybrid functional describes the full dimensional series. The optical onset blueshifts monotonically ( ≈ 2.4 → 2.8 → 3.0 eV ) and the near-edge absorption is strongly dichroic. A change in light polarization does not simply shift the excitonic resonance ( ≈ 0.09 eV ); it also reorganizes the underlying excitonic wave function, selecting distinct band channels and k -space regions. A real-space, participation-ratio analysis resolves moderately delocalized, Wannier-Mott-like excitons templated along the covalent chains. They are predominantly sulfur-derived (75%–88% of the density on sulfur for the chain-polarized bulk states), which identifies them as ( S 2 ) 2 − disulfide excitations rather than S → Zr charge-transfer states, while in the bilayer the electron delocalizes across both layers, the real-space imprint of interlayer screening. These results provide a consistent reference for the quasiparticle and excitonic energy scales of ZrS 3 from the bulk to the few-layer limit.
Wigner-negative states of light are key resources for quantum advantage in continuous-variable optical quantum computing. They can be produced probabilistically via frequency conversion and photon detection, or deterministically by exploiting the single-photon nonlinearity of a quantum emitter. Here, we generate such Wigner-negative states of light with a tunable negativity using a single semiconductor quantum dot in a cavity. Optical coherent control of the quantum-dot transition allows to generate a quantum superposition of zero and one photon. The generated quantum states are characterized point-by-point in the phase space through homodyne measurement. The emergence of Wigner-function negativity is observed as the excitation power is increased. After correcting for collection and propagation losses, we obtain fidelities to the ideal state and quantum purities above 95%, together with near-optimal quadrature squeezing. The ability to generate a wide variety of Wigner-negative states with mature semiconductor technology opens promising opportunities for continuous-variable optical quantum technologies.
Abstract We utilize a holographic construction to compute the entanglement negativity for bipartite mixed state configurations of a single subsystem in CFTd s with a conserved charge dual to bulk A d S d + 1 geometries. In this context, we obtain the holographic entanglement negativity for single subsystems with long rectangular strip geometries in CFTd s with a conserved charge dual to bulk non extremal and extremal Reissner–Nordström (RN)- A d S d + 1 black holes at the leading order in a perturbation theory. We demonstrate that the holographic entanglement negativity computed involves the elimination of thermal contributions at the leading order confirming earlier results in the literature. This also conforms to quantum information theory expectations and constitutes further consistency checks for the holographic construction.