Enhancement of optical nonlinearity and spontaneous emission in nano-engineered epsilon-near-zero materials

Author(s):  
Howard Lee ◽  
Sudip Gurung ◽  
Khant Minn ◽  
Aleksei Anopchenko ◽  
Subhajit Bej
2020 ◽  
Author(s):  
Justus Bohn ◽  
Ting-Shan Luk ◽  
Craig Tollerton ◽  
Sam Hutchins ◽  
Igal Brener ◽  
...  

Abstract Nonlinear optical devices and their implementation into modern nanophotonic architectures are constrained by their usually moderate nonlinear response. Recently, epsilon-near-zero (ENZ) materials have been found to have a strong optical nonlinearity, which can be enhanced through the use of cavities or nano-structuring. Here, we study the pump dependent properties of the plasmon resonance in the ENZ region in a thin layer of thin indium tin oxide (ITO). Exciting this mode using the Kretschmann-Raether configuration, we study reflection switching properties of a 60nm layer close to the resonant plasmon frequency. We demonstrate the thermal switching mechanism, which results in a shift in the plasmon resonance frequency of 20THz for a TM pump intensity of 75GW/cm2. For degenerate pump and probe frequencies, we highlight an additional coherent contribution, not previously isolated in ENZ nonlinear optics studies, which leads to an overall pump induced change in reflection from 1% to 45%.


2018 ◽  
Vol 12 (2) ◽  
pp. 79-83 ◽  
Author(s):  
M. Zahirul Alam ◽  
Sebastian A. Schulz ◽  
Jeremy Upham ◽  
Israel De Leon ◽  
Robert W. Boyd

2021 ◽  
Vol 4 (1) ◽  
Author(s):  
Futai Hu ◽  
Liu Li ◽  
Yuan Liu ◽  
Yuan Meng ◽  
Mali Gong ◽  
...  

AbstractPlasmonic cavities can provide deep subwavelength light confinement, opening up new avenues for enhancing the spontaneous emission process towards both classical and quantum optical applications. Conventionally, light cannot be directly emitted from the plasmonic metal itself. Here, we explore the large field confinement and slow-light effect near the epsilon-near-zero (ENZ) frequency of the light-emitting material itself, to greatly enhance the “forbidden” two-plasmon spontaneous emission (2PSE) process. Using degenerately-doped InSb as the plasmonic material and emitter simultaneously, we theoretically show that the 2PSE lifetime can be reduced from tens of milliseconds to several nanoseconds, comparable to the one-photon emission rate. Furthermore, we show that the optical nonlocality may largely govern the optical response of the ultrathin ENZ film. Efficient 2PSE from a doped semiconductor film may provide a pathway towards on-chip entangled light sources, with an emission wavelength and bandwidth widely tunable in the mid-infrared.


Author(s):  
Khant Minn ◽  
Aleksei Anopchenko ◽  
Ching-Wen Chang ◽  
Jinmin Kim ◽  
Yu-Jung Lu ◽  
...  

Author(s):  
Sisira Suresh ◽  
Orad Reshef ◽  
M. Zahirul Alam ◽  
Jeremy Upham ◽  
Mohammad Karimi ◽  
...  

Nanophotonics ◽  
2020 ◽  
Vol 9 (14) ◽  
pp. 4287-4293
Author(s):  
Heng Wang ◽  
Kang Du ◽  
Ruibin Liu ◽  
Xinhai Dai ◽  
Wending Zhang ◽  
...  

AbstractThe physical origin of epsilon-near-zero (ENZ) optical nonlinearity lies in the hot-electron dynamics, in which electron scattering plays an important role. With the damping factor defined by hot electron scattering time, the Drude model could be extended to modeling ENZ optical nonlinearity completely. We proposed a statistical electron scattering model that takes into account the effect of electron distribution in a nonparabolic band and conducted the investigation on indium tin oxide (ITO) with femtosecond-pump continuum-probe experiment. We found that ionized impurity scattering and acoustic phonon scattering are the two major scattering mechanisms, of which the latter had been neglected before. They dominate at low-energy and high-energy electrons, respectively, and are weakened or boosted for high electron temperature, respectively. The electron energy–dependent scattering time contributed from multiple scattering mechanisms shows the electron density–dependent damping factor. The comprehensive understanding of electron scattering in ITO will help to develop a complete model of ENZ optical nonlinearity.


ACS Photonics ◽  
2018 ◽  
Vol 5 (6) ◽  
pp. 2287-2294 ◽  
Author(s):  
Vincenzo Caligiuri ◽  
Milan Palei ◽  
Muhammad Imran ◽  
Liberato Manna ◽  
Roman Krahne

2019 ◽  
Vol 27 (5) ◽  
pp. 7426 ◽  
Author(s):  
Xueke Duan ◽  
Fan Zhang ◽  
Zhiyuan Qian ◽  
He Hao ◽  
Lingxiao Shan ◽  
...  

Nanomaterials ◽  
2021 ◽  
Vol 11 (12) ◽  
pp. 3424
Author(s):  
Wenjuan Shi ◽  
Hongjun Liu ◽  
Zhaolu Wang

The nonlinear optical response of common materials is limited by bandwidth and energy consumption, which impedes practical application in all-optical signal processing, light detection, harmonic generation, etc. Additionally, the nonlinear performance is typically sensitive to polarization. To circumvent this constraint, we propose that orthogonal nanoantennas coupled to Al-doped zinc oxide (AZO) epsilon-near-zero (ENZ) material show a broadband (~1000 nm bandwidth) large optical nonlinearity simultaneously for two orthogonal polarization states. The absolute maximum value of the nonlinear refractive index n2 is 7.65 cm2∙GW−1, which is 4 orders of magnitude larger than that of the bare AZO film and 7 orders of magnitude larger than that of silica. The coupled structure not only realizes polarization independence and strong nonlinearity, but also allows the sign of the nonlinear response to be flexibly tailored. It provides a promising platform for the realization of ultracompact, low-power, and highly nonlinear all-optical devices on the nanoscale.


Nanomaterials ◽  
2021 ◽  
Vol 11 (6) ◽  
pp. 1410
Author(s):  
M. Channab ◽  
C. F. Pirri ◽  
A. Angelini

In this work, we discuss the use of epsilon-near-zero (ENZ) metamaterials to efficiently couple light radiated by a dipolar source to an in-plane waveguide. We exploit both enhanced and directional emission provided by ENZ metamaterials to optimize the injection of light into the waveguide by tuning the metal fill factor. We show that a net increase in intensity injected into the waveguide with respect to the total power radiated by the isolated dipole can be achieved in experimentally feasible conditions. We think the proposed system may open up new opportunities for several optical applications and integrated technologies, especially for those limited by outcoupling efficiency and emission rate.


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