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Morales F, Richter M, Ivanov M, Husakou A. Non-instantaneous third-order optical response of gases in low-frequency fields. OPTICS EXPRESS 2022; 30:23579-23586. [PMID: 36225034 DOI: 10.1364/oe.458765] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 03/28/2022] [Accepted: 05/13/2022] [Indexed: 06/16/2023]
Abstract
It is commonly assumed that for low-intensity short optical pulses far from resonance, the third-order optical nonlinear response is instantaneous. We solve the three-dimensional time-dependent Schrödinger equation for the hydrogen atom and show that this is not the case: the polarization is not simply proportional to the cube of the electric field even at low intensities. We analyze the fundamental-frequency and third-harmonic nonlinear susceptibilities of hydrogen, investigate their dependence on intensity, and find that the delays in the Kerr response rapidly approach the femtosecond time-scale at higher intensities, while the delays in the third harmonic generation remain much lower. We also propose an experimental scheme to detect and characterize the above effects.
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Li G, Palomba S, de Sterke CM. A theory of waveguide design for plasmonic nanolasers. NANOSCALE 2018; 10:21434-21440. [PMID: 30427024 DOI: 10.1039/c8nr04898c] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/09/2023]
Abstract
We propose a theory for the waveguide design and analysis for plasmonic nanolasers by reformulating the fundamental waveguide requirements. This theory does not rely on further optimizing previously used structures, but examines each possible design without prejudice. Our exploration of one-dimensional (i.e., layered) plasmonic nanowaveguide geometries and the subsequent extension to 2D structures not only provides a deep understanding of the characteristics of currently used designs, but also leads to superior structures with the potential to address long-standing challenges in plasmonic nanolasers. In addition, we discover analogies between the reformulated fundamental requirements for the waveguide for nanolasers and nanoscale four-wave mixing (FWM) devices. Therefore, after a slight modification, our theory can also be applied to the waveguide design for plasmonic FWM devices.
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Affiliation(s)
- Guangyuan Li
- Institute of Photonics and Optical Science (IPOS), School of Physics, The University of Sydney, NSW 2006, Australia
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Bahl A, Majety VP, Scrinzi A, Kolesik M. Nonlinear optical response in molecular nitrogen: from ab-initio calculations to optical pulse simulations. OPTICS LETTERS 2017; 42:2295-2298. [PMID: 28614335 DOI: 10.1364/ol.42.002295] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 04/14/2017] [Accepted: 05/04/2017] [Indexed: 06/07/2023]
Abstract
Using first-principle multi-electron calculations via the hybrid anti-symmetrized coupled channels method, we create a model to describe both the nonlinear polarization and ionization of the nitrogen molecule. Based on the metastable electronic state approach, it is designed for space-and-time-resolved simulations in nonlinear optics that require modeling of optical pulses that exhibit rich spectral dynamics and propagate over long distances. As a demonstration of the model's utility, we study low-order harmonic generation in mid-infrared optical filaments.
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Franco-Ortiz M, Corella-Madueño A, Rosas-Burgos RA, Adrian Reyes J, Avendaño CG. Saturation and stability of nonlinear photonic crystals. JOURNAL OF PHYSICS. CONDENSED MATTER : AN INSTITUTE OF PHYSICS JOURNAL 2017; 29:125701. [PMID: 28059777 DOI: 10.1088/1361-648x/aa5752] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/06/2023]
Abstract
We consider a one-dimensional photonic crystal made by an infinite set of nonlinear nematic films immersed in a linear dielectric medium. The thickness of each equidistant film is negligible and its refraction index depends continuously on the electric field intensity, giving rise to all the involved nonlinear terms, which joints from a starting linear index for negligible amplitudes to a final saturation index for extremely large field intensities. We show that the nonlinear exact solutions of this system form an intensity-dependent band structure which we calculate and analyze. Next, we ponder a finite version of this system; that is, we take a finite array of linear dielectric stacks of the same size separated by the same nonlinear extremely thin nematic slabs and find the reflection coefficients for this arrangement and obtain the dependence on the wave number and intensity of the incident wave. As a final step we analyze the stability of the analytical solutions of the nonlinear crystal by following the evolution of an additive amplitude to the analytical nonlinear solution we have found here. We discuss our results and state our conclusions.
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Affiliation(s)
- M Franco-Ortiz
- Posgrado en Nanotecnología, Universidad de Sonora, Apartado Postal 1626, Hermosillo, Sonora, Mexico. Departamento de Física, Universidad de Sonora, Apartado Postal 1626, Hermosillo, Sonora, Mexico
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Khurgin JB, Sun G, Chen WT, Tsai WY, Tsai DP. Ultrafast Thermal Nonlinearity. Sci Rep 2015; 5:17899. [PMID: 26644322 PMCID: PMC4672269 DOI: 10.1038/srep17899] [Citation(s) in RCA: 11] [Impact Index Per Article: 1.2] [Reference Citation Analysis] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 07/14/2015] [Accepted: 10/28/2015] [Indexed: 11/09/2022] Open
Abstract
Third order nonlinear optical phenomena explored in the last half century have been predicted to find wide range of applications in many walks of life, such as all-optical switching, routing, and others, yet this promise has not been fulfilled primarily because the strength of nonlinear effects is too low when they are to occur on the picosecond scale required in today's signal processing applications. The strongest of the third-order nonlinearities, engendered by thermal effects, is considered to be too slow for the above applications. In this work we show that when optical fields are concentrated into the volumes on the scale of few tens of nanometers, the speed of the thermo-optical effects approaches picosecond scale. Such a sub-diffraction limit concentration of field can be accomplished with the use of plasmonic effects in metal nanoparticles impregnating the thermo-optic dielectric (e.g. amorphous Si) and leads to phase shifts sufficient for all optical switching on ultrafast scale.
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Affiliation(s)
- Jacob B Khurgin
- Department of Electrical and Computer Engineering, Johns Hopkins University, Baltimore, Maryland 21218
| | - Greg Sun
- Department of Engineering, University of Massachusetts Boston, Boston, Massachusetts 02125
| | - Wei Ting Chen
- Department of Physics, National Taiwan University, Taipei 10617, Taiwan
| | - Wei-Yi Tsai
- Department of Physics, National Taiwan University, Taipei 10617, Taiwan
| | - Din Ping Tsai
- Department of Physics, National Taiwan University, Taipei 10617, Taiwan.,Research Center for Applied Sciences, Academia Sinica, Taipei 11529, Taiwan
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Schnebelin C, Cassagne C, de Araújo CB, Boudebs G. Measurements of the third- and fifth-order optical nonlinearities of water at 532 and 1064 nm using the D4σ method. OPTICS LETTERS 2014; 39:5046-5049. [PMID: 25166070 DOI: 10.1364/ol.39.005046] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.2] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/03/2023]
Abstract
The nonlinear response of liquid water was investigated at 1064 and 532 nm using a Nd:YAG laser delivering pulses of 17 ps and its second harmonic. The experiments were performed using the D4σ method combined with the Z-scan technique. Nonlinear refractive indices of third- and fifth-order were determined, as well as the three-photon absorption coefficient, for both wavelengths. A good agreement was found between theory and experiment.
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Tarazkar M, Romanov DA, Levis RJ. Higher-order nonlinearity of refractive index: The case of argon. J Chem Phys 2014; 140:214316. [DOI: 10.1063/1.4880716] [Citation(s) in RCA: 24] [Impact Index Per Article: 2.4] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/14/2022] Open
Affiliation(s)
- Maryam Tarazkar
- Department of Chemistry, Temple University, Philadelphia, Pennsylvania 19122, USA
- Center for Advanced Photonics Research, Temple University, Philadelphia, Pennsylvania 19122, USA
| | - Dmitri A. Romanov
- Center for Advanced Photonics Research, Temple University, Philadelphia, Pennsylvania 19122, USA
- Department of Physics, Temple University, Philadelphia, Pennsylvania 19122, USA
| | - Robert J. Levis
- Department of Chemistry, Temple University, Philadelphia, Pennsylvania 19122, USA
- Center for Advanced Photonics Research, Temple University, Philadelphia, Pennsylvania 19122, USA
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Kolesik M, Moloney JV. Modeling and simulation techniques in extreme nonlinear optics of gaseous and condensed media. REPORTS ON PROGRESS IN PHYSICS. PHYSICAL SOCIETY (GREAT BRITAIN) 2014; 77:016401. [PMID: 24366913 DOI: 10.1088/0034-4885/77/1/016401] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.2] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/03/2023]
Abstract
Computer simulation techniques for extreme nonlinear optics are reviewed with emphasis on the high light-intensity regimes in which both bound and freed electronic states contribute to the medium response and thus affect the optical pulse dynamics. The first part concentrates on the optical pulse propagation modeling, and provides a classification of various approaches to optical-field evolution equations. Light-matter interaction models are reviewed in the second part, which concentrates on methods that can be integrated with time- and space-resolved simulations encompassing realistic experimental scenarios.
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Affiliation(s)
- M Kolesik
- College of Optical Sciences, University of Arizona, Tucson, AZ 85721, USA. Department of Physics, Constantine the Philosopher University, Nitra, Slovakia
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Khurgin JB, Sun G. Plasmonic enhancement of the third order nonlinear optical phenomena: figures of merit. OPTICS EXPRESS 2013; 21:27460-27480. [PMID: 24216967 DOI: 10.1364/oe.21.027460] [Citation(s) in RCA: 10] [Impact Index Per Article: 0.9] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/02/2023]
Abstract
Recent years have seen increased interest in the plasmonic enhancement of nonlinear optical effects, yet there remains an uncertainty as to the limits of this enhancement. We present a simple and physically transparent theory for the plasmonic enhancement of third order nonlinear optical processes and show that while a huge enhancement of the effective nonlinear index can be attained, the most relevant figure of merit, the phase shift per one absorption length, remains very low. This suggests that while nonlinear plasmonic materials are not suitable for applications requiring high efficiency, for example in all-optical switching and wavelength conversion, they can be very useful for applications where overall high efficiency is not critical, such as in sensing.
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Wahlstrand JK, Cheng YH, Milchberg HM. High field optical nonlinearity and the Kramers-Kronig relations. PHYSICAL REVIEW LETTERS 2012; 109:113904. [PMID: 23005631 DOI: 10.1103/physrevlett.109.113904] [Citation(s) in RCA: 4] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 02/20/2012] [Indexed: 06/01/2023]
Abstract
The nonlinear optical response to high fields is absolutely measured for the noble gas atoms He, Ne, Ar, Kr, and Xe. We find that the response is quadratic in the laser field magnitude up to the ionization threshold of each gas. Its size and quadratic dependence are well predicted by a Kramers-Kronig analysis employing known ionization probabilities, and the results are consistent with calculations using the time-dependent Schrödinger equation.
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Affiliation(s)
- J K Wahlstrand
- Institute for Research in Electronics and Applied Physics, University of Maryland, College Park, Maryland 20742, USA
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