Interaction of exciton polaritons with the surface potential of thin semiconductor films:s-polarization geometry

1994 ◽  
Vol 50 (8) ◽  
pp. 5404-5411 ◽  
Author(s):  
B. Flores-Desirena ◽  
F. Pérez-Rodríguez ◽  
P. Halevi
Keyword(s):  
Surface Potential ◽  
Exciton Polaritons ◽  
Thin Semiconductor

scholarly journals Collective Mie Exciton-Polaritons in an Atomically Thin Semiconductor

2020 ◽  
Vol 124 (35) ◽  
pp. 19196-19203
Author(s):  
Shaojun Wang ◽  
T.V. Raziman ◽  
Shunsuke Murai ◽  
Gabriel W. Castellanos ◽  
Ping Bai ◽  
...  
Keyword(s):  
Exciton Polaritons ◽  
Thin Semiconductor

scholarly journals Optical valley Hall effect for highly valley-coherent exciton-polaritons in an atomically thin semiconductor

2019 ◽  
Vol 14 (8) ◽  
pp. 770-775 ◽  
Author(s):  
Nils Lundt ◽  
Łukasz Dusanowski ◽  
Evgeny Sedov ◽  
Petr Stepanov ◽  
Mikhail M. Glazov ◽  
...  
Keyword(s):  
Hall Effect ◽  
Exciton Polaritons ◽  
Thin Semiconductor ◽  
Valley Hall Effect

The effects of surface absorbed monolayer microdiffraction patterns

1988 ◽  
Vol 46 ◽  
pp. 680-681
Author(s):  
M. Pan ◽  
J.M. Cowley
Keyword(s):  
Surface Potential ◽  
Electron Probe ◽  
Potential Distribution ◽  
Crystal Surface ◽  
Normal Direction ◽  
Surface Image ◽  
Extended Surface ◽  
Gas Molecules ◽  
Surface Nature ◽  
Electron Microdiffraction

Electron microdiffraction patterns, obtained when a small electron probe with diameter of 10-15 Å is directed to run parallel to and outside a flat crystal surface, are sensitive to the surface nature of the crystals. Dynamical diffraction calculations have shown that most of the experimental observations for a flat (100) face of a MgO crystal, such as the streaking of the central spot in the surface normal direction and (100)-type forbidden reflections etc., could be explained satisfactorily by assuming a modified image potential field outside the crystal surface. However the origin of this extended surface potential remains uncertain. A theoretical analysis by Howie et al suggests that the surface image potential should have a form different from above-mentioned image potential and also be smaller by several orders of magnitude. Nevertheless the surface potential distribution may in practice be modified in various ways, such as by the adsorption of a monolayer of gas molecules.

Polariton – polariton scattering and the nonequilibrium condensation of exciton polaritons in semiconductor microcavities

2003 ◽  
Vol 173 (9) ◽  
pp. 995
Author(s):  
V.D. Kulakovskii ◽  
D.N. Krizhanovskii ◽  
A.I. Tartakovskii ◽  
Nikolai A. Gippius ◽  
Sergei G. Tikhodeev
Keyword(s):  
Exciton Polaritons ◽  
Semiconductor Microcavities ◽  
Nonequilibrium Condensation

Modeling on Effects of Charging Time and Recombination on Surface Potential Decay Crossover of LDPE

2016 ◽  
Vol 136 (2) ◽  
pp. 86-92 ◽  
Author(s):  
Daomin Min ◽  
Shengtao Li ◽  
Guochang Li ◽  
George Chen
Keyword(s):  
Surface Potential ◽  
Charging Time ◽  
Potential Decay

Direct Measurement of Charge Reversal on Lipid Bilayers using Heterodyne-Detected Second Harmonic Generation Spectroscopy

2019 ◽  
Author(s):  
HanByul Chang ◽  
Paul Ohno ◽  
Yangdongling Liu ◽  
Franz Geiger
Keyword(s):  
Lipid Bilayers ◽  
Surface Potential ◽  
Second Harmonic ◽  
Fluid Phase ◽  
Cationic Polyelectrolyte ◽  
Charge Reversal ◽  
Buried Interfaces ◽  
Phase Transition Temperatures ◽  
Complementary Techniques ◽  
Order Susceptibility

We report the detection of charge reversal induced by the adsorption of a cationic polyelectrolyte, poly(allylamine) hydrochloride (PAH), to buried supported lipid bilayers (SLBs), used as idealized model biological membranes. We observe changes in the surface potential in isolation from other contributors to the total SHG response by extracting the phase-shifted potential-dependent third-order susceptibility from the overall SHG signal. We demonstrate the utility of this technique in detecting both the sign of the surface potential and the point of charge reversal at buried interfaces without any prior information or complementary techniques<i>.</i>Furthermore, isolation of the second-order susceptibility contribution from the overall SHG response allows us to directly monitor changes in the Stern Layer. Finally, we characterize the Stern and Diffuse Layers over single-component SLBs formed from three different zwitterionic lipids of different gel-to-fluid phase transition temperatures (T<sub>m</sub>s). We determine whether the surface potential changes with the physical phase state (gel, transitioning, or fluid) of the SLB and incorporate 20 percent of negatively charged lipids to the zwitterionic SLB to investigate how the surface potential changes with surface charge.

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