Highly Efficient Single-Exciton Strong Coupling with Plasmons by Lowering Critical Interaction Strength at an Exceptional Point.

The single-exciton strong coupling with the localized plasmon mode (LPM) at room temperature is highly desirable for exploiting quantum technology. However, its realization has been a very low probability event due to the harsh critical conditions, severely compromising its application. Here, we present a highly efficient approach for achieving such a strong coupling by reducing the critical interaction strength at the exceptional point based upon the damping inhibition and matching of the coupled system, instead of enhancing the coupling strength to overcome the system's large damping. Experimentally, we compress the LPM's damping linewidth from about 45 nm to about 14 nm using a leaky Fabry-Perot cavity, a good match to the excitonic linewidth of about 10 nm. This method dramatically relaxes the harsh requirement in mode volume by more than an order of magnitude and allows a maximum direction angle of the exciton dipole relative to the mode field of up to around 71.9°, significantly improving the success rate of achieving the single-exciton strong coupling with LPMs from about 1% to about 80%.

[1]  Huanjun Chen,et al.  Room-Temperature Strong Coupling Between a Single Quantum Dot and a Single Plasmonic Nanoparticle. , 2022, Nano letters.

[2]  Rongbin Su,et al.  Quantum exceptional chamber induced by large nondipole effect of a quantum dot coupled to a nano-plasmonic resonator , 2021 .

[3]  S. Gwo,et al.  Tuning of Two-Dimensional Plasmon-Exciton Coupling in Full Parameter Space: A Polaritonic Non-Hermitian System. , 2021, Nano letters.

[4]  Jia Zhu,et al.  Stable, high-performance sodium-based plasmonic devices in the near infrared , 2020, Nature.

[5]  R. Ma,et al.  Revealing the missing dimension at an exceptional point , 2020 .

[6]  Matthias Heinrich,et al.  Observation of PT-symmetric quantum interference , 2019, Nature Photonics.

[7]  M. Raschke,et al.  Tip-enhanced strong coupling spectroscopy, imaging, and control of a single quantum emitter , 2019, Science Advances.

[8]  Yogesh N. Joglekar,et al.  Quantum state tomography across the exceptional point in a single dissipative qubit , 2019, Nature Physics.

[9]  M. Miri,et al.  Exceptional points in optics and photonics , 2019, Science.

[10]  Xing Rong,et al.  Observation of parity-time symmetry breaking in a single-spin system , 2018, Science.

[11]  M. Pelton,et al.  Strong coupling and induced transparency at room temperature with single quantum dots and gap plasmons , 2018, Nature Communications.

[12]  B. Hecht,et al.  Near-field strong coupling of single quantum dots , 2018, Science Advances.

[13]  L. Liz‐Marzán,et al.  Femtosecond laser reshaping yields gold nanorods with ultranarrow surface plasmon resonances , 2017, Science.

[14]  Yuri S. Kivshar,et al.  Fano resonances in photonics , 2017, Nature Photonics.

[15]  H. Doeleman,et al.  Antenna-cavity hybrids: matching polar opposites for Purcell enhancements at any linewidth , 2016, 1605.04181.

[16]  Jeremy J. Baumberg,et al.  Single-molecule strong coupling at room temperature in plasmonic nanocavities , 2016, Nature.

[17]  G. Haran,et al.  Vacuum Rabi splitting in a plasmonic cavity at the single quantum emitter limit , 2015, Nature Communications.

[18]  Q. Gong,et al.  Single-Band 2-nm-Line-Width Plasmon Resonance in a Strongly Coupled Au Nanorod. , 2015, Nano letters.

[19]  W. Barnes,et al.  Strong coupling between surface plasmon polaritons and emitters: a review , 2014, Reports on progress in physics. Physical Society.

[20]  Darrick E. Chang,et al.  Quantum nonlinear optics — photon by photon , 2014, Nature Photonics.

[21]  J. D. Thompson,et al.  Nanophotonic quantum phase switch with a single atom , 2014, Nature.

[22]  Nicolas Large,et al.  Near-field mediated plexcitonic coupling and giant Rabi splitting in individual metallic dimers. , 2013, Nano letters.

[23]  Oliver Benson,et al.  Assembly of hybrid photonic architectures from nanophotonic constituents , 2011, Nature.

[24]  F J García de Abajo,et al.  Quantum plexcitonics: strongly interacting plasmons and excitons. , 2011, Nano letters.

[25]  Rosalba Saija,et al.  Nanopolaritons: vacuum Rabi splitting with a single quantum dot in the center of a dimer nanoantenna. , 2010, ACS nano.

[26]  P. Mulvaney,et al.  Surface plasmon mediated strong exciton-photon coupling in semiconductor nanocrystals. , 2009, Nano letters.

[27]  H. J. Kimble,et al.  The quantum internet , 2008, Nature.

[28]  Dirk Englund,et al.  Controlling cavity reflectivity with a single quantum dot , 2007, Nature.

[29]  T. Paterek,et al.  An experimental test of non-local realism , 2007, Nature.

[30]  M. Atatüre,et al.  Quantum nature of a strongly coupled single quantum dot–cavity system , 2006, Nature.

[31]  Warwick P. Bowen,et al.  Observation of strong coupling between one atom and a monolithic microresonator , 2006, Nature.

[32]  Stephan W Koch,et al.  Vacuum Rabi splitting in semiconductors , 2006 .

[33]  G. Rupper,et al.  Vacuum Rabi splitting with a single quantum dot in a photonic crystal nanocavity , 2004, Nature.

[34]  V. Kulakovskii,et al.  Strong coupling in a single quantum dot–semiconductor microcavity system , 2004, Nature.

[35]  A. D. Boozer,et al.  Supplementary Information for Experimental Realization of a One-Atom Laser in the Regime of Strong Coupling , 2003 .

[36]  K. Vahala Optical microcavities , 2003, Nature.

[37]  Robert C. Hilborn,et al.  Einstein coefficients, cross sections, f values, dipole moments, and all that , 1982, physics/0202029.