Replication Data for: Temporal loss boundary engineered photonic cavity (doi:10.21979/N9/EXZCGV)

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Document Description

Citation

Title:

Replication Data for: Temporal loss boundary engineered photonic cavity

Identification Number:

doi:10.21979/N9/EXZCGV

Distributor:

DR-NTU (Data)

Date of Distribution:

2022-03-23

Version:

1

Bibliographic Citation:

Longqing, Cong; Han, Jiaguang; Zhang, Weili; Singh, Ranjan, 2022, "Replication Data for: Temporal loss boundary engineered photonic cavity", https://doi.org/10.21979/N9/EXZCGV, DR-NTU (Data), V1

Study Description

Citation

Title:

Replication Data for: Temporal loss boundary engineered photonic cavity

Identification Number:

doi:10.21979/N9/EXZCGV

Authoring Entity:

Longqing, Cong (Southern University of Science and Technology, Shenzhen, 518055, China)

Han, Jiaguang (Tianjin University, Tianjin, 300072, China)

Zhang, Weili (Oklahoma State University, Stillwater, OK, 74078, USA)

Singh, Ranjan (Nanyang Technological University)

Software used in Production:

Origin

Software used in Production:

CST Microwave

Grant Number:

MOE2016-T3-1-006

Grant Number:

NRF-CRP23-2019-0005

Distributor:

DR-NTU (Data)

Access Authority:

Singh Ranjan

Depositor:

Srivastava, Yogesh Kumar

Date of Deposit:

2022-03-23

Holdings Information:

https://doi.org/10.21979/N9/EXZCGV

Study Scope

Keywords:

Physics, Physics, transient loss boundary

Abstract:

Losses are ubiquitous and unavoidable in nature inhibiting the performance of most optical processes. Manipulating losses to adjust the dissipation of photons is analogous to braking a running car that is as important as populating photons via a gain medium. Here, we introduce the transient loss boundary into a photon populated cavity that functions as a ‘photon brake’ and probe photon dynamics by engineering the ‘brake timing’ and ‘brake strength’. Coupled cavity photons can be distinguished by stripping one photonic mode through controlling the loss boundary, which enables the transition from a coupled to an uncoupled state. We interpret the transient boundary as a perturbation by considering both real and imaginary parts of permittivity, and the dynamic process is modeled with a temporal two-dipole oscillator: one with the natural resonant polarization and the other with a frequency-shift polarization. The model unravels the underlying mechanism of concomitant coherent spectral oscillations and generation of tone-tuning cavity photons in the braking process. By synthesizing the temporal loss boundary into a photon populated cavity, a plethora of interesting phenomena and applications are envisioned such as the observation of quantum squeezed states, low-loss nonreciprocal waveguides and ultrafast beam scanning devices.

Kind of Data:

Experimental and simulation dataData

Methodology and Processing

Sources Statement

Data Access

Other Study Description Materials

Related Publications

Citation

Identification Number:

10.1038/s41467-021-27014-z

Bibliographic Citation:

Cong, L., Han, J., Zhang, W., & Singh, R. (2021). Temporal loss boundary engineered photonic cavity. Nature Communications, 12(1), 6940.

Citation

Identification Number:

10356/155838

Bibliographic Citation:

Cong, L., Han, J., Zhang, W. & Singh, R. (2021). Temporal loss boundary engineered photonic cavity. Nature Communications, 12(1), 6940-.

Other Study-Related Materials

Label:

Temporal Loss Boundary Engineered Photonic Cavity.opj

Text:

Data corresponding to all the figures. Experimental and simulation data

Notes:

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