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

arXiv:1506.06889 · Physical Review A

Mode coupling and photon antibunching in a bimodal cavity containing a dipole quantum emitter

Yulong Liu, Guan-Zhong Wang, Yu-xi Liu, Franco Nori

Published Jan 28, 2016• 37 citations
arXivHTMLPDF

Abstract

We study the effect of mode coupling on a single-photon device in which a dipole quantum emitter (DQE) is embedded in a bimodal whispering-gallery-mode cavity. A scatterer is used to induce mode coupling between counterclockwise and clockwise propagating light fields, which interact with the DQE. We find that the antibunching increases when an additional cavity field is coupled to the DQE interacting with a cavity field. In contrast to models for the interaction between a DQE and a (one-mode or two-mode) cavity field, we find that a strong photon antibunching can occur, even for a weaker DQE-field coupling strength and large dephasing of the DQE, when mode coupling is introduced. We also find that mode coupling can make the device robust against either (1) the frequency mismatch between cavity modes and the DQE or (2) the coupling strength mismatch between the DQE and each mode in the two-mode cavity. Moreover, we find that these mismatches can be used to generate better antibunching. Our study shows that mode coupling in a bimodal cavity is very important for the realization of a good single-photon device.

DOI
10.1103/physreva.93.013856

Related papers

Improving photon antibunching with two dipole-coupled atoms in whispering-gallery-mode microresonators

Ye Qu, Shu-Ting Shen, Jiahua Li +1 more

In the two-atom or multiatom system, the atoms can interact with each other through exchange of virtual photon. This kind of energy exchange is often referred as the dipole-dipole interaction (DDI). Here we consider this DDI system consisting of a pair of two-level atoms strongly coupled with a bimodal whispering-gallery-mode (WGM) microresonator which is driven by an external laser field. Our aim is to explore the photon correlation characteristics of the proposed architecture using realistic experimental parameter values. We compare in detail the quality of photon antibunching (i.e., the smallness of the second-order correlation function) from three involved configurations in cavity quantum electrodynamics (QED): (i) only one two-level atom, (ii) two far apart two-level atoms without DDI, and (iii) two DDI (dipole-coupled) two-level atoms are respectively coupled to the driven WGM microresonator through the evanescent field. We clearly show that the DDI between both atoms can distinctly enhance the photon antibunching even in the weak-coupling regime in configuration (iii) with feature-rich line shapes. We also find that the photon antibunching can be modulated by properly adjusting the atom-cavity coupling strength. In addition, we display that this strong photon antibunching is robust against the cooperative atomic decay. Our DDI-based cavity QED scheme may provide an alternative way to the construction of integrated on-chip single-photon sources.

Physical Review A•Feb 7, 2020•14 citations

Quality of photon antibunching in two cavity-waveguide arrangements on a chip

Jiahua Li, Ying Wu

A quantum emitter coupled to an optical bimodal cavity in the solid-state implementation has recently proven to be an excellent platform for coherent generation of nonclassical light on a chip. However, the impacts of the structural couplings between the photonic modes via different arrangements of optical cavity and waveguide are rarely considered. Here, we explore in detail the characteristics of the photon antibunching in bimodal cavity quantum electrodynamics (QED) via taking into account two different cavity-waveguide arrangements: (i) an inline geometry and (ii) a side-coupled geometry. In our scheme, both cavity modes are simultaneously coupled to a two-level emitter but are not directly coupled to each other, owing to their orthogonal polarizations. It is clearly shown that the quality of the photon antibunching in the bimodal cavity QED, namely, the smallness of the second-order intensity correlation function at zero time, is closely related to the cavity-waveguide arrangements. The optimal photon antibunching can be achieved in the side-coupled geometry and the antibunching quality is about two orders of magnitude lower than that in the inline geometry. This enhancement of the photon antibunching is ascribed to the combination of two kinds of quantum interference effects in the waveguide-cavity QED system. We also find that the side-coupled architecture can make the device robust against the frequency mismatch between the two cavity modes, as compared to the inline geometry. In addition, we find that this mismatch can be used to generate better antibunching. The realization of our proposal with existing cavity-waveguide QED architectures is also discussed.1 MoreReceived 15 September 2018DOI:https://doi.org/10.1103/PhysRevA.98.053801©2018 American Physical SocietyPhysics Subject Headings (PhySH)Research AreasCavity quantum electrodynamicsQuantum description of light-matter interactionQuantum interference effectsTechniquesCavity resonatorsAtomic, Molecular & Optical

Physical Review A•Nov 1, 2018•18 citations

Antibunching effect of photons in a two-level emitter-cavity system

Xinyun Liang, Zhenglu Duan, Qin Guo +3 more

A two-level quantum emitter interacting with a cavity field is an important model for investigating the photon blockade (PB) effect. Most work on this topic relies on the assumption that the emitter transition frequency is resonant with the fundamental mode frequency of the cavity. In this work we relax this constraint and reexamine the PB effect in a more general emitter-cavity system with arbitrary emitter and cavity detunings from a driving field. The results show that when the signs of the emitter and cavity detunings are the same, a PB occurs only in the strong-coupling regime, but for opposite signs of the emitter and cavity detunings, strong photon antibunching is observed in both the weak- and strong-coupling regimes, and better antibunching is achieved compared with the case when the signs are the same. More interestingly, we find that this PB arises from quantum interference for both weak and strong nonlinearities. These results deepen our understanding of the underlying mechanism of PBs and may contribute to the construction of single-photon sources with higher purity and better flexibility using two-level emitter-cavity systems.

arXiv:1811.06690•Physical Review A•Dec 19, 2019•48 citations

Multiphoton blockade and antibunching in an optical cavity coupled with dipole-dipole-interacting Λ -type atoms

Z Haider, Shahid Qamar, Muhammad Irfan

We study multiphoton blockade effects in a single-mode cavity interacting with two three-level atoms in $\mathrm{\ensuremath{\Lambda}}$ configuration having position-dependent atom-field coupling. We consider the effects of dipole-dipole interaction (DDI) between the three-level atoms and show how the presence of DDI strongly influences the multiphoton blockade. For symmetric coupling of the atoms with the field, the DDI induces an asymmetry in the emission spectra as a function of pump field detuning. At positive detuning, the single-photon blockade gets stronger as a function of DDI strength, leading to photon antibunching. However, it becomes weaker at negative detuning and can also completely vanish. We show that this vanishing single-photon blockade is associated with a strong two-photon blockade, leading to two-photon bunching. Therefore, by just tuning the frequency of the pump field, we can achieve two very distinct features. We also study the effects of DDI when the atoms are asymmetrically coupled with the field and show that the proposed system exhibits two-photon bunching. We believe our results are important for the experimental realization of such systems where DDI may be present.

arXiv:2304.02047•Physical Review A•Apr 4, 2023•12 citations

Optimal photon antibunching in a quantum-dot–bimodal-cavity system

Wen Zhang, Zhongyuan Yu, Yumin Liu +1 more

We theoretically investigate the photon statistics in a cavity quantum electrodynamics system of a single quantum dot coupled to a bimodal nanocavity. It is shown in a recent work [A. Majumdar, M. Bajcsy, A. Rundquist, and J. Vu\ifmmode \check{c}\else \v{c}\fi{}kovi\ifmmode \acute{c}\else \'{c}\fi{}, Phys. Rev. Lett. 108, 183601 (2012)] that the system can generate strongly sub-Poissonian light when one of the cavity modes is driven coherently and resonantly. We study the two-mode coherent driving regime of the coupled system. The effect of additional cavity mode driving on statistical characteristics of photon emission is presented by evaluating the zero-delay second-order correlation function ${g}^{2}$(0). The antibunching character can be optimized by regulating the ratio between driving strengths of two cavity modes to achieve optimal combination of superbunched and coherent light. As a result ${g}^{2}$(0) can be reduced up to several orders of magnitude [${g}^{2}$(0)$\phantom{\rule{0.16em}{0ex}}\ensuremath{\sim}\phantom{\rule{0.16em}{0ex}}$10${}^{\ensuremath{-}7}$] with proper system parameters, compared with the one-mode driving system [${g}^{2}$(0)$\phantom{\rule{0.16em}{0ex}}\ensuremath{\sim}\phantom{\rule{0.16em}{0ex}}$0.1].

Physical Review A•Apr 21, 2014•93 citations

Photon antibunching and nonlinear effects for a quantum dot coupled to a semiconductor cavity

Frank Bello, David M. Whittaker

The models presented simulate pumping techniques that can be used on modern semiconductor devices which are capable of coupling a quantum dot and cavity mode in order to determine a more efficient method of producing a single-photon emitter while taking into consideration typical parameters which are achievable given today's standards of coupling strength. Cavity quantum electrodynamics are incorporated in the calculations as we compare various pumping schemes for the system that either use on-resonant laser excitation or nonresonant excitation due to a wetting layer. In particular, we look to study how antibunching effects change for each method as the cavity finesse is increased toward the strong coupling regime. Experimentally these studies are equivalent to nonlinear pump-probe measurements, where a strong pump, either resonant or nonresonant, is used to excite the coupled system, and the resulting state is characterized using a weak, resonant probe beam.

arXiv:0808.3280•Physical Review B•Sep 28, 2010•4 citations
We study the effect of mode coupling on a single-photon device in which a dipole quantum emitter (DQE) is embedded in a bimodal whispering-gallery-mode cavity. A scatterer is used to induce mode coupling between counterclockwise and clockwise propagating light fields, which interact with the DQE. We find that the antibunching increases when an additional cavity field is coupled to the DQE interacting with a cavity field. In contrast to models for the interaction between a DQE and a (one-mode or two-mode) cavity field, we find that a strong photon antibunching can occur, even for a weaker DQE-field coupling strength and large dephasing of the DQE, when mode coupling is introduced. We also find that mode coupling can make the device robust against either (1) the frequency mismatch between cavity modes and the DQE or (2) the coupling strength mismatch between the DQE and each mode in the two-mode cavity. Moreover, we find that these mismatches can be used to generate better antibunching. Our study shows that mode coupling in a bimodal cavity is very important for the realization of a good single-photon device.
In the two-atom or multiatom system, the atoms can interact with each other through exchange of virtual photon. This kind of energy exchange is often referred as the dipole-dipole interaction (DDI). Here we consider this DDI system consisting of a pair of two-level atoms strongly coupled with a bimodal whispering-gallery-mode (WGM) microresonator which is driven by an external laser field. Our aim is to explore the photon correlation characteristics of the proposed architecture using realistic experimental parameter values. We compare in detail the quality of photon antibunching (i.e., the smallness of the second-order correlation function) from three involved configurations in cavity quantum electrodynamics (QED): (i) only one two-level atom, (ii) two far apart two-level atoms without DDI, and (iii) two DDI (dipole-coupled) two-level atoms are respectively coupled to the driven WGM microresonator through the evanescent field. We clearly show that the DDI between both atoms can distinctly enhance the photon antibunching even in the weak-coupling regime in configuration (iii) with feature-rich line shapes. We also find that the photon antibunching can be modulated by properly adjusting the atom-cavity coupling strength. In addition, we display that this strong photon antibunching is robust against the cooperative atomic decay. Our DDI-based cavity QED scheme may provide an alternative way to the construction of integrated on-chip single-photon sources.
A quantum emitter coupled to an optical bimodal cavity in the solid-state implementation has recently proven to be an excellent platform for coherent generation of nonclassical light on a chip. However, the impacts of the structural couplings between the photonic modes via different arrangements of optical cavity and waveguide are rarely considered. Here, we explore in detail the characteristics of the photon antibunching in bimodal cavity quantum electrodynamics (QED) via taking into account two different cavity-waveguide arrangements: (i) an inline geometry and (ii) a side-coupled geometry. In our scheme, both cavity modes are simultaneously coupled to a two-level emitter but are not directly coupled to each other, owing to their orthogonal polarizations. It is clearly shown that the quality of the photon antibunching in the bimodal cavity QED, namely, the smallness of the second-order intensity correlation function at zero time, is closely related to the cavity-waveguide arrangements. The optimal photon antibunching can be achieved in the side-coupled geometry and the antibunching quality is about two orders of magnitude lower than that in the inline geometry. This enhancement of the photon antibunching is ascribed to the combination of two kinds of quantum interference effects in the waveguide-cavity QED system. We also find that the side-coupled architecture can make the device robust against the frequency mismatch between the two cavity modes, as compared to the inline geometry. In addition, we find that this mismatch can be used to generate better antibunching. The realization of our proposal with existing cavity-waveguide QED architectures is also discussed.1 MoreReceived 15 September 2018DOI:https://doi.org/10.1103/PhysRevA.98.053801©2018 American Physical SocietyPhysics Subject Headings (PhySH)Research AreasCavity quantum electrodynamicsQuantum description of light-matter interactionQuantum interference effectsTechniquesCavity resonatorsAtomic, Molecular & Optical
A two-level quantum emitter interacting with a cavity field is an important model for investigating the photon blockade (PB) effect. Most work on this topic relies on the assumption that the emitter transition frequency is resonant with the fundamental mode frequency of the cavity. In this work we relax this constraint and reexamine the PB effect in a more general emitter-cavity system with arbitrary emitter and cavity detunings from a driving field. The results show that when the signs of the emitter and cavity detunings are the same, a PB occurs only in the strong-coupling regime, but for opposite signs of the emitter and cavity detunings, strong photon antibunching is observed in both the weak- and strong-coupling regimes, and better antibunching is achieved compared with the case when the signs are the same. More interestingly, we find that this PB arises from quantum interference for both weak and strong nonlinearities. These results deepen our understanding of the underlying mechanism of PBs and may contribute to the construction of single-photon sources with higher purity and better flexibility using two-level emitter-cavity systems.
We study multiphoton blockade effects in a single-mode cavity interacting with two three-level atoms in $\mathrm{\ensuremath{\Lambda}}$ configuration having position-dependent atom-field coupling. We consider the effects of dipole-dipole interaction (DDI) between the three-level atoms and show how the presence of DDI strongly influences the multiphoton blockade. For symmetric coupling of the atoms with the field, the DDI induces an asymmetry in the emission spectra as a function of pump field detuning. At positive detuning, the single-photon blockade gets stronger as a function of DDI strength, leading to photon antibunching. However, it becomes weaker at negative detuning and can also completely vanish. We show that this vanishing single-photon blockade is associated with a strong two-photon blockade, leading to two-photon bunching. Therefore, by just tuning the frequency of the pump field, we can achieve two very distinct features. We also study the effects of DDI when the atoms are asymmetrically coupled with the field and show that the proposed system exhibits two-photon bunching. We believe our results are important for the experimental realization of such systems where DDI may be present.
We theoretically investigate the photon statistics in a cavity quantum electrodynamics system of a single quantum dot coupled to a bimodal nanocavity. It is shown in a recent work [A. Majumdar, M. Bajcsy, A. Rundquist, and J. Vu\ifmmode \check{c}\else \v{c}\fi{}kovi\ifmmode \acute{c}\else \'{c}\fi{}, Phys. Rev. Lett. 108, 183601 (2012)] that the system can generate strongly sub-Poissonian light when one of the cavity modes is driven coherently and resonantly. We study the two-mode coherent driving regime of the coupled system. The effect of additional cavity mode driving on statistical characteristics of photon emission is presented by evaluating the zero-delay second-order correlation function g2{g}^{2}g2(0). The antibunching character can be optimized by regulating the ratio between driving strengths of two cavity modes to achieve optimal combination of superbunched and coherent light. As a result g2{g}^{2}g2(0) can be reduced up to several orders of magnitude [g2{g}^{2}g2(0)$\phantom{\rule{0.16em}{0ex}}\ensuremath{\sim}\phantom{\rule{0.16em}{0ex}}101010{}^{\ensuremath{-}7}]withpropersystemparameters,comparedwiththeone−modedrivingsystem[] with proper system parameters, compared with the one-mode driving system []withpropersystemparameters,comparedwiththeone−modedrivingsystem[{g}^{2}(0)(0)(0)\phantom{\rule{0.16em}{0ex}}\ensuremath{\sim}\phantom{\rule{0.16em}{0ex}}$0.1].
The models presented simulate pumping techniques that can be used on modern semiconductor devices which are capable of coupling a quantum dot and cavity mode in order to determine a more efficient method of producing a single-photon emitter while taking into consideration typical parameters which are achievable given today's standards of coupling strength. Cavity quantum electrodynamics are incorporated in the calculations as we compare various pumping schemes for the system that either use on-resonant laser excitation or nonresonant excitation due to a wetting layer. In particular, we look to study how antibunching effects change for each method as the cavity finesse is increased toward the strong coupling regime. Experimentally these studies are equivalent to nonlinear pump-probe measurements, where a strong pump, either resonant or nonresonant, is used to excite the coupled system, and the resulting state is characterized using a weak, resonant probe beam.