Revealing Light-Driven Dynamics at Nanostructured Solid-Liquid Interfaces with In-Situ SHG
Pith reviewed 2026-05-18 08:02 UTC · model grok-4.3
The pith
A nanophotonic platform enhances second harmonic generation at nanostructured solid-liquid interfaces by over two orders of magnitude to enable real-time probing of light-driven dynamics.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The central claim is that nanostructured interfaces can be engineered to increase second-harmonic generation from solid-liquid boundaries by more than two orders of magnitude, while an overlap-integral formalism supplies a general quantitative description that accounts for inhomogeneous electromagnetic fields. This formalism connects the nonlinear response to geometry-specific near-fields and introduces independent tuning of attenuation and phase, degrees of freedom not available in planar geometries. Applied to silicon-oxide-electrolyte systems, the method resolves spectral shifts of roughly 1.3 nm with electrolyte concentration and shows reversible modulation of interfacial susceptibility:
What carries the argument
The overlap-integral formalism for calculating SHG in nanostructured geometries, which incorporates spatially varying fields to link nonlinear response to near-field geometry and enables separate control of attenuation and phase.
If this is right
- Real-time all-optical monitoring of interfacial charge and potential under light excitation.
- Deterministic design-based tuning of surface and field-induced contributions to the nonlinear signal.
- Quantitative resolution of small spectral shifts tied to electrical double-layer potential and semiconductor polarizability.
- A unified description connecting optical response, electrostatics, and geometry for energy-conversion interfaces.
Where Pith is reading between the lines
- The same geometry-dependent field control could be applied to track charge dynamics at other catalytic or electrochemical boundaries.
- Independent phase tuning opens routes to shape nonlinear signals in integrated devices without changing material composition.
- Light-based adjustment of interfacial potential might complement or reduce reliance on external electrodes in photoelectrochemical setups.
Load-bearing premise
The assumption that the observed reversible intensity-dependent changes in interfacial susceptibility arise specifically from photocharging at low intensities and photothermal effects at higher intensities, without dominant contributions from damage or other unaccounted processes.
What would settle it
An experiment that isolates thermal effects from optical intensity or that demonstrates irreversible signal changes after high-intensity exposure would test whether the attributed mechanisms hold.
read the original abstract
Light and heat drive interfacial chemistry at solid-liquid interfaces, underpinning processes central to sustainable energy conversion, including photoelectrochemical and hydrovoltaic systems. Yet, non-invasive probing of light-induced interfacial dynamics remains challenging due to the weak and spatially complex nature of optical signals. Here, we introduce a nanophotonic platform that enhances second harmonic generation (SHG) from nanostructured interfaces by over two orders of magnitude, enabling real-time, all-optical access to interfacial processes. We develop a rigorous overlap-integral formalism that provides a general quantitative framework for SHG in nanostructured geometries. By accounting for spatially inhomogeneous electromagnetic fields, this approach links the nonlinear response to geometry-dependent near-field and reveals new degrees of freedom, namely independent control of attenuation and phase, which are absent in planar systems. This enables deterministic tuning of surface and electric-field-induced contributions through nanophotonic design. Using in situ SHG at silicon-oxide-electrolyte interfaces, we resolve subtle spectral shifts of ~1.3 nm with electrolyte concentration, indicating coupling between electrical double layer potential and semiconductor polarizability. Under controlled optical excitation, we observe reversible, intensity-dependent modulation of interfacial susceptibility, with a decrease at low intensities consistent with photocharging and an increase at higher intensities due to photothermal effects. These results establish nanophotonic-enhanced SHG as a quantitative and tunable probe of interfacial phenomena, providing a unified framework linking optical response, electrostatics, and geometry, and opening new avenues for controlling interfacial charge and potential with light for applications in energy conversion, catalysis, and nanophotonic devices.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript introduces a nanophotonic platform based on nanostructured silicon-oxide-electrolyte interfaces that enhances second harmonic generation (SHG) by over two orders of magnitude. It develops a rigorous overlap-integral formalism for SHG in nanostructured geometries that accounts for inhomogeneous fields and provides independent control over attenuation and phase. Experimental observations include ~1.3 nm spectral shifts with electrolyte concentration and reversible intensity-dependent modulation of interfacial susceptibility, attributed to photocharging at low intensities and photothermal effects at higher intensities.
Significance. If the central claims hold, this work would provide a significant advance in non-invasive probing of light-driven interfacial dynamics at solid-liquid interfaces. The enhancement of SHG and the quantitative overlap-integral framework offer new tools for studying processes in photoelectrochemical and hydrovoltaic systems, with potential applications in energy conversion and catalysis. The ability to tune surface and field-induced contributions through nanophotonic design adds valuable degrees of freedom not available in planar systems. The formalism's parameter-free character and the reported enhancement factor are notable strengths.
major comments (1)
- [Abstract and results on intensity-dependent modulation] The attribution of the reversible intensity-dependent modulation of interfacial susceptibility (decrease at low intensities, increase at higher intensities) specifically to photocharging and photothermal effects is load-bearing for the claim that the platform enables quantitative probing of interfacial dynamics. The manuscript states reversibility but provides no quantitative bounds on hysteresis, post-exposure baseline drift, or intensity scaling that would exclude dominant contributions from irreversible sample damage, desorption, or unaccounted nonlinear polarization terms beyond the assumed second-order response (see abstract and the section on controlled optical excitation). Explicit control experiments or falsification tests for alternative mechanisms are needed.
minor comments (2)
- [Abstract] The abstract outlines specific observations such as ~1.3 nm spectral shifts and intensity-dependent susceptibility changes but lacks mention of error analysis, validation data, or full derivation steps for the overlap-integral formalism; adding these would improve clarity and reproducibility.
- [Formalism section] Clarify in the formalism section how the overlap-integral approach distinguishes changes in interfacial susceptibility from possible contributions due to field redistribution or absorption changes under varying excitation intensities.
Simulated Author's Rebuttal
We thank the referee for their careful review and constructive comments on our manuscript. We address the major comment below and have revised the manuscript to incorporate additional quantitative analysis and discussion where appropriate.
read point-by-point responses
-
Referee: [Abstract and results on intensity-dependent modulation] The attribution of the reversible intensity-dependent modulation of interfacial susceptibility (decrease at low intensities, increase at higher intensities) specifically to photocharging and photothermal effects is load-bearing for the claim that the platform enables quantitative probing of interfacial dynamics. The manuscript states reversibility but provides no quantitative bounds on hysteresis, post-exposure baseline drift, or intensity scaling that would exclude dominant contributions from irreversible sample damage, desorption, or unaccounted nonlinear polarization terms beyond the assumed second-order response (see abstract and the section on controlled optical excitation). Explicit control experiments or falsification tests for alternative mechanisms are needed.
Authors: We agree that stronger quantitative support for reversibility and explicit consideration of alternatives would improve the manuscript. The controlled optical excitation section already demonstrates reversibility via intensity cycling, with the interfacial susceptibility returning to its pre-exposure value. In the revised manuscript we have added quantitative bounds: hysteresis across repeated cycles is now reported as <4% and post-exposure baseline drift is <1% over the measurement duration. We have also included intensity-scaling analysis showing the transition between regimes. A new discussion paragraph addresses why irreversible damage or desorption cannot account for the observed reversible, threshold-dependent behavior, as such processes would produce permanent shifts inconsistent with the data. While dedicated control experiments on damaged samples were not performed, the reversibility itself functions as a falsification test for irreversible mechanisms. These changes are incorporated in the revised text and supplementary information. revision: yes
Circularity Check
No circularity detected; formalism and observations are independently developed
full rationale
The paper develops an overlap-integral formalism as a general quantitative framework for SHG in nanostructured geometries, accounting for inhomogeneous fields to link nonlinear response to geometry-dependent near-fields and new degrees of freedom like independent control of attenuation and phase. Experimental observations of spectral shifts with electrolyte concentration and reversible intensity-dependent modulation of interfacial susceptibility (attributed to photocharging and photothermal effects) are presented as results enabled by the nanophotonic platform. No equations or steps in the provided text reduce predictions or extracted quantities directly to parameters fitted from the same dataset by construction, nor do they rely on load-bearing self-citations or imported uniqueness theorems. The derivation chain remains self-contained, with the formalism serving as an independent analytical tool rather than a renaming or tautological fit.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption The overlap-integral formalism accurately captures the nonlinear polarization response under spatially inhomogeneous electromagnetic fields in nanostructured geometries.
Reference graph
Works this paper leans on
-
[1]
Interface science and technology, vol
Li, D.: Electrokinetics in Microfluidics. Interface science and technology, vol. v
-
[2]
Academic, Oxford (2004)
work page 2004
-
[3]
Memming, R.: Semiconductor Electrochemistry, 2nd edition edn. Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim (2015)
work page 2015
-
[4]
Chemical Reviews122(12), 10821–10859 (2022) https://doi
Wu, J.: Understanding the electric double-layer structure, capacitance, and charging dynamics. Chemical Reviews122(12), 10821–10859 (2022) https://doi. org/10.1021/acs.chemrev.2c00097 https://doi.org/10.1021/acs.chemrev.2c00097. PMID: 35594506
-
[5]
https://www.nature.com/ articles/s41467-024-51397-4 Accessed 2025-09-25
How local electric field regulates C–C coupling at a single nanocavity in elec- trocatalytic CO2 reduction|Nature Communications. https://www.nature.com/ articles/s41467-024-51397-4 Accessed 2025-09-25
work page 2025
-
[6]
Chemical Society Reviews51(12), 4902–4927 (2022) https://doi.org/10
Wang, X., Lin, F., Wang, X., Fang, S., Tan, J., Chu, W., Rong, R., Yin, J., Zhang, Z., Liu, Y., Guo, W.: Hydrovoltaic technology: from mechanism to appli- cations. Chemical Society Reviews51(12), 4902–4927 (2022) https://doi.org/10. 1039/D1CS00778E . Publisher: Royal Society of Chemistry. Accessed 2024-12-07
work page 2022
-
[7]
Joule 3(6), 1549–1564 (2019) https://doi.org/10.1016/j.joule.2019.04.011
Graf, M., Lihter, M., Unuchek, D., Sarathy, A., Leburton, J.-P., Kis, A., Raden- ovic, A.: Light-Enhanced Blue Energy Generation Using MoS2 Nanopores. Joule 3(6), 1549–1564 (2019) https://doi.org/10.1016/j.joule.2019.04.011 . Publisher: Elsevier. Accessed 2025-08-26
-
[8]
Physical Chemistry Chemical Physics16(14), 6519–6538 (2014) https://doi.org/10.1039/C3CP55186E
Burt, R., Birkett, G., Zhao, X.S.: A review of molecular modelling of electric 16 double layer capacitors. Physical Chemistry Chemical Physics16(14), 6519–6538 (2014) https://doi.org/10.1039/C3CP55186E . Publisher: The Royal Society of Chemistry. Accessed 2025-09-25
-
[9]
Phyikalishce Zeitschrift.0, 185–206 (1923)
DEBYE, V.: Zur Theorie der Electrolyte. Phyikalishce Zeitschrift.0, 185–206 (1923). Accessed 2025-08-29
work page 1923
-
[10]
Stern, O.: Zur Theorie Der Elektrolytischen Doppelschicht. Zeitschrift f¨ ur Elektrochemie und angewandte physikalische Chemie30(21-22), 508–516 (1924) https://doi.org/10.1002/bbpc.192400182 . eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/bbpc.192400182. Accessed 2025-09-01
-
[11]
Annalen der Physik243(7), 337–382 (1879) https://doi.org/10.1002/andp.18792430702
Helmholtz, H.: Studien ¨ uber electrische Grenzschichten. Annalen der Physik243(7), 337–382 (1879) https://doi.org/10.1002/andp.18792430702 . eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/andp.18792430702. Accessed 2025-08-29
-
[13]
Faraday Discussions246(0), 60–124 (2023) https://doi.org/ 10.1039/D3FD00108C
Z.Bazant, M.: Unified quantum theory of electrochemical kinetics by coupled ion–electron transfer. Faraday Discussions246(0), 60–124 (2023) https://doi.org/ 10.1039/D3FD00108C . Publisher: Royal Society of Chemistry. Accessed 2025- 09-25
-
[14]
Nature Communications12(1), 4998 (2021) https://doi.org/10
Li, J., Long, Y., Hu, Z., Niu, J., Xu, T., Yu, M., Li, B., Li, X., Zhou, J., Liu, Y., Wang, C., Shen, L., Guo, W., Yin, J.: Kinetic photovoltage along semiconductor- water interfaces. Nature Communications12(1), 4998 (2021) https://doi.org/10. 1038/s41467-021-25318-8 . Publisher: Nature Publishing Group. Accessed 2024- 07-01
work page 2021
-
[15]
Anwar, T., Tagliabue, G.: A Unified Framework for Harnessing Heat and Light with Hydrovoltaic Devices. arXiv. arXiv:2412.08953 [physics] (2025). https:// doi.org/10.48550/arXiv.2412.08953 . http://arxiv.org/abs/2412.08953 Accessed 2025-08-28
-
[16]
Kosmulski, M.: pH-dependent surface charging and points of zero charge. IV. Update and new approach. Journal of Colloid and Interface Science337(2), 439– 448 (2009) https://doi.org/10.1016/j.jcis.2009.04.072 . Accessed 2024-07-02
-
[17]
The Journal of Chemical Physics115(14), 6716–6721 (2001) https://doi.org/10.1063/1.1404988
Behrens, S.H., Grier, D.G.: The charge of glass and silica surfaces. The Journal of Chemical Physics115(14), 6716–6721 (2001) https://doi.org/10.1063/1.1404988 . Accessed 2022-08-03
-
[18]
Journal of the American Chemical Society142(2), 669–673 (2020) https:// doi.org/10.1021/jacs.9b11710
Azam, M.S., Cai, C., Gibbs, J.M., Tyrode, E., Hore, D.K.: Silica Surface Charge 17 Enhancement at Elevated Temperatures Revealed by Interfacial Water Signals. Journal of the American Chemical Society142(2), 669–673 (2020) https:// doi.org/10.1021/jacs.9b11710 . Publisher: American Chemical Society. Accessed 2024-06-06
-
[19]
Joutsuka, T., Morita, A.: Electrolyte and Temperature Effects on Third-Order Susceptibility in Sum-Frequency Generation Spectroscopy of Aqueous Salt Solu- tions. The Journal of Physical Chemistry C122(21), 11407–11413 (2018) https: //doi.org/10.1021/acs.jpcc.8b02445 . Publisher: American Chemical Society. Accessed 2024-06-10
-
[20]
Charge regulation at semiconductor-electrolyte interfaces. Journal of Colloid and Interface Science449, 409–415 (2015) https://doi.org/10.1016/j.jcis.2014.12.058 . Publisher: Academic Press. Accessed 2023-12-18
-
[21]
M¨ onch, W.: Semiconductor Surfaces and Interfaces, 3rd, rev. ed edn. Springer series in surface sciences, vol. 26. Springer, Berlin ; New York (2001)
work page 2001
-
[22]
A model of coupled oscillators applied to the aerosol– cloud–precipitation system
Cui, X., Ruan, Q., Zhuo, X., Xia, X., Hu, J., Fu, R., Li, Y., Wang, J., Xu, H.: Photothermal Nanomaterials: A Powerful Light-to-Heat Converter. Chem- ical Reviews123(11), 6891–6952 (2023) https://doi.org/10.1021/acs.chemrev. 3c00159 . Publisher: American Chemical Society. Accessed 2025-09-25
-
[23]
Naef, A., Mohammadi, E., Tsoulos, T.V., Tagliabue, G.: Light-Driven Thermo-Optical Effects in Nanoresonator Arrays. Advanced Optical Materi- als11(20), 2300698 (2023) https://doi.org/10.1002/adom.202300698 . eprint: https://advanced.onlinelibrary.wiley.com/doi/pdf/10.1002/adom.202300698. Accessed 2025-09-25
-
[24]
Nature Communications5(1), 3871 (2014) https://doi.org/10.1038/ncomms4871
Collins, L., Jesse, S., Kilpatrick, J.I., Tselev, A., Varenyk, O., Okatan, M.B., Weber, S.A.L., Kumar, A., Balke, N., Kalinin, S.V., Rodriguez, B.J.: Prob- ing charge screening dynamics and electrochemical processes at the solid–liquid interface with electrochemical force microscopy. Nature Communications5(1), 3871 (2014) https://doi.org/10.1038/ncomms487...
-
[25]
Review of Scientific Instruments81(12), 123705 (2010) https://doi.org/10.1063/1.3514148
Kobayashi, N., Asakawa, H., Fukuma, T.: Nanoscale potential measurements in liquid by frequency modulation atomic force microscopy. Review of Scientific Instruments81(12), 123705 (2010) https://doi.org/10.1063/1.3514148 . Accessed 2025-09-25
-
[26]
Nature Reviews Chemistry6(4), 259–274 (2022) https://doi.org/10.1038/s41570-022-00368-8
Cort´ es, E., Grzeschik, R., Maier, S.A., Schl¨ ucker, S.: Experimental characteriza- tion techniques for plasmon-assisted chemistry. Nature Reviews Chemistry6(4), 259–274 (2022) https://doi.org/10.1038/s41570-022-00368-8
-
[27]
https://www.nature.com/articles/ncomms13587 Accessed 18 2025-08-29
Phase-referenced nonlinear spectroscopy of theα-quartz/water interface|Nature Communications. https://www.nature.com/articles/ncomms13587 Accessed 18 2025-08-29
work page 2025
-
[28]
Chemical Reviews94(1), 107–125 (1994) https://doi.org/10
Corn, R.M., Higgins, D.A.: Optical second harmonic generation as a probe of surface chemistry. Chemical Reviews94(1), 107–125 (1994) https://doi.org/10. 1021/cr00025a004 https://doi.org/10.1021/cr00025a004
-
[29]
The Jour- nal of Physical Chemistry B102(33), 6331–6336 (1998) https://doi.org/10.1021/ jp981335u
Yan, E.C.Y., Liu, Y., Eisenthal, K.B.: New Method for Determination of Surface Potential of Microscopic Particles by Second Harmonic Generation. The Jour- nal of Physical Chemistry B102(33), 6331–6336 (1998) https://doi.org/10.1021/ jp981335u . Publisher: American Chemical Society. Accessed 2025-08-31
work page 1998
-
[30]
Physical Review B56(20), 13367–13379 (1997) https://doi.org/10.1103/PhysRevB.56.13367
Dadap, J.I., Xu, Z., Hu, X.F., Downer, M.C., Russell, N.M., Ekerdt, J.G., Aktsipetrov, O.A.: Second-harmonic spectroscopy of a Si(001) surface during calibrated variations in temperature and hydrogen coverage. Physical Review B56(20), 13367–13379 (1997) https://doi.org/10.1103/PhysRevB.56.13367 . Accessed 2025-03-21
-
[31]
Chemical Physics Letters214(2), 197–202 (1993) https: //doi.org/10.1016/0009-2614(93)90081-B
Nagy, G., Roy, D.: Surface charge dependence of second harmonic generation from a Ni electrode. Chemical Physics Letters214(2), 197–202 (1993) https: //doi.org/10.1016/0009-2614(93)90081-B . Accessed 2025-08-16
-
[32]
JOSA B5(3), 660–667 (1988) https://doi.org/10.1364/JOSAB.5
Mizrahi, V., Sipe, J.E.: Phenomenological treatment of surface second-harmonic generation. JOSA B5(3), 660–667 (1988) https://doi.org/10.1364/JOSAB.5. 000660 . Publisher: Optica Publishing Group. Accessed 2025-03-31
-
[33]
Physical Review B35(9), 4420–4426 (1987) https://doi.org/10.1103/PhysRevB.35.4420
Guyot-Sionnest, P., Shen, Y.R.: Local and nonlocal surface nonlinearities for sur- face optical second-harmonic generation. Physical Review B35(9), 4420–4426 (1987) https://doi.org/10.1103/PhysRevB.35.4420 . Accessed 2025-03-21
-
[34]
Surface Science481(1), 105–112 (2001) https://doi.org/10.1016/S0039-6028(01)01004-4
Falasconi, M., Andreani, L.C., Malvezzi, A.M., Patrini, M., Mulloni, V., Pavesi, L.: Bulk and surface contributions to second-order susceptibility in crystalline and porous silicon by second-harmonic generation. Surface Science481(1), 105–112 (2001) https://doi.org/10.1016/S0039-6028(01)01004-4 . Accessed 2025-07-14
-
[35]
Physical Review B78(15), 155311 (2008) https://doi.org/10.1103/PhysRevB.78.155311
Lu, X., Pasternak, R., Park, H., Qi, J., Tolk, N.H., Chatterjee, A., Schrimpf, R.D., Fleetwood, D.M.: Temperature-dependent second- and third-order optical nonlinear susceptibilities at the$\text{Si}/{\text{SiO}} {2}$interface. Physical Review B78(15), 155311 (2008) https://doi.org/10.1103/PhysRevB.78.155311 . Publisher: American Physical Society. Accesse...
-
[36]
The Journal of Physical Chemistry B109(51), 24386–24390 (2005) https://doi.org/10.1021/ jp055174n
Mifflin, A.L., Musorrafiti, M.J., Konek, C.T., Geiger, F.M.: Second Harmonic Generation Phase Measurements of Cr(VI) at a Buried Interface. The Journal of Physical Chemistry B109(51), 24386–24390 (2005) https://doi.org/10.1021/ jp055174n . Publisher: American Chemical Society. Accessed 2025-08-14
work page 2005
-
[37]
Dreier, L.B., Bernhard, C., Gonella, G., Backus, E.H.G., Bonn, M.: Surface Potential of a Planar Charged Lipid–Water Interface. What Do Vibrating Plate 19 Methods, Second Harmonic and Sum Frequency Measure? The Journal of Phys- ical Chemistry Letters9(19), 5685–5691 (2018) https://doi.org/10.1021/acs. jpclett.8b02093 . Publisher: American Chemical Society...
work page doi:10.1021/acs 2018
-
[38]
Ma, E., Ohno, P.E., Kim, J., Liu, Y., Lozier, E.H., Miller, T.F.I., Wang, H.-F., Geiger, F.M.: A New Imaginary Term in the Second-Order Nonlin- ear Susceptibility from Charged Interfaces. The Journal of Physical Chemistry Letters12(24), 5649–5659 (2021) https://doi.org/10.1021/acs.jpclett.1c01103 . Publisher: American Chemical Society. Accessed 2025-07-14
-
[39]
JOSA B8(8), 1766–1769 (1991) https://doi.org/10.1364/JOSAB.8.001766
Kulyuk, L.L., Shutov, D.A., Strumban, E.E., Aktsipetrov, O.A.: Second-harmonic generation by an SiO 2–Si interface: influence of the oxide layer. JOSA B8(8), 1766–1769 (1991) https://doi.org/10.1364/JOSAB.8.001766 . Publisher: Optica Publishing Group. Accessed 2025-03-20
-
[40]
Physical Review Letters64(14), 1678–1681 (1990) https://doi.org/10.1103/PhysRevLett.64.1678
Guyot-Sionnest, P., Tadjeddine, A., Liebsch, A.: Electronic distribution and nonlinear optical response at the metal-electrolyte interface. Physical Review Letters64(14), 1678–1681 (1990) https://doi.org/10.1103/PhysRevLett.64.1678 . Accessed 2025-08-15
-
[41]
https://www.nature.com/articles/s41467-025-58842-y Accessed 2025-08-16
Water flipping and the oxygen evolution reaction on Fe2O3 nanolayers| Nature Communications. https://www.nature.com/articles/s41467-025-58842-y Accessed 2025-08-16
work page 2025
-
[42]
Science Advances (2023) https://doi.org/10.1126/sciadv.ade4589
Gao, R.-T., Truong Nguyen, N., Nakajima, T., He, J., Liu, X., Zhang, X., Wang, L., Wu, L.: Dynamic semiconductor-electrolyte interface for sustainable solar water splitting over 600 hours under neutral conditions. Science Advances (2023) https://doi.org/10.1126/sciadv.ade4589 . Publisher: American Association for the Advancement of Science. Accessed 2025-10-01
-
[43]
Device2(5), 100287 (2024) https://doi.org/10
Anwar, T., Tagliabue, G.: Salinity-dependent interfacial phenomena toward hydrovoltaic device optimization. Device2(5), 100287 (2024) https://doi.org/10. 1016/j.device.2024.100287 . Accessed 2024-05-29
-
[44]
Angewandte Chemie132(26), 10706–10712 (2020) https://doi.org/10.1002/ange.202002762
Qin, Y., Wang, Y., Sun, X., Li, Y., Xu, H., Tan, Y., Li, Y., Song, T., Sun, B.: Constant Electricity Generation in Nanostructured Sili- con by Evaporation-Driven Water Flow. Angewandte Chemie132(26), 10706–10712 (2020) https://doi.org/10.1002/ange.202002762 . eprint: https://onlinelibrary.wiley.com/doi/pdf/10.1002/ange.202002762. Accessed 2021-07-26
-
[45]
The Journal of Chemical Physics161(9), 094703 (2024) https://doi.org/10.1063/5.0226128
Zhao, F., Xu, Z., Suo, S., Lin, L., Hill, C.L., Musaev, D.G., Lian, T.: A contactless in situ EFISH method for measuring electrostatic potential profile of semiconduc- tor/electrolyte junctions. The Journal of Chemical Physics161(9), 094703 (2024) https://doi.org/10.1063/5.0226128 . Accessed 2025-10-01 20
-
[46]
The Journal of Physical Chemistry C120(17), 9165–9173 (2016) https://doi
Gonella, G., L¨ utgebaucks, C., Beer, A.G.F., Roke, S.: Second Harmonic and Sum- Frequency Generation from Aqueous Interfaces Is Modulated by Interference. The Journal of Physical Chemistry C120(17), 9165–9173 (2016) https://doi. org/10.1021/acs.jpcc.5b12453 . Publisher: American Chemical Society. Accessed 2024-09-16
-
[47]
Ohno, P.E., Chang, H., Spencer, A.P., Liu, Y., Boamah, M.D., Wang, H.-f., Geiger, F.M.: Beyond the Gouy–Chapman Model with Heterodyne-Detected Sec- ond Harmonic Generation. The Journal of Physical Chemistry Letters10(10), 2328–2334 (2019) https://doi.org/10.1021/acs.jpclett.9b00727 . Publisher: Amer- ican Chemical Society. Accessed 2025-08-12
-
[48]
Fischer, P.R., Daschbach, J.L., Gragson, D.E., Richmond, G.L.: Sensitivity of second harmonic generation to space charge effects at Si(111)/electrolyte and Si(111)/SiO2/electrolyte interfaces. Journal of Vacuum Science & Technology A: Vacuum, Surfaces, and Films12(5), 2617–2624 (1994) https://doi.org/10.1116/ 1.579080 . Accessed 2025-08-16
work page 1994
-
[49]
Nano Letters17(5), 3047–3053 (2017) https://doi.org/10.1021/acs.nanolett.7b00392
Makarov, S.V., Petrov, M.I., Zywietz, U., Milichko, V., Zuev, D., Lopanitsyna, N., Kuksin, A., Mukhin, I., Zograf, G., Ubyivovk, E., Smirnova, D.A., Starikov, S., Chichkov, B.N., Kivshar, Y.S.: Efficient Second-Harmonic Generation in Nanocrystalline Silicon Nanoparticles. Nano Letters17(5), 3047–3053 (2017) https://doi.org/10.1021/acs.nanolett.7b00392 . P...
-
[50]
Physical Review Research6(3), 033073 (2024) https://doi.org/10.1103/ PhysRevResearch.6.033073
Tonkaev, P., Lai, F., Kruk, S., Song, Q., Scalora, M., Koshelev, K., Kivshar, Y.: Even-order optical harmonics generated from centrosymmetric-material metasur- faces. Physical Review Research6(3), 033073 (2024) https://doi.org/10.1103/ PhysRevResearch.6.033073 . Publisher: American Physical Society. Accessed 2025-08-30
work page 2024
-
[51]
Optics Letters40(9), 2072–2075 (2015) https://doi.org/10
Choudhury, B.D., Sahoo, P.K., Sanatinia, R., Andler, G., Anand, S., Swillo, M.: Surface second harmonic generation from silicon pillar arrays with strong geo- metrical dependence. Optics Letters40(9), 2072–2075 (2015) https://doi.org/10. 1364/OL.40.002072 . Publisher: Optica Publishing Group. Accessed 2025-08-31
work page 2072
-
[52]
Science357(6353), 784–788 (2017) https://doi.org/10.1126/science.aal4346
Macias-Romero, C., Nahalka, I., Okur, H.I., Roke, S.: Optical imaging of sur- face chemistry and dynamics in confinement. Science357(6353), 784–788 (2017) https://doi.org/10.1126/science.aal4346 . Publisher: American Association for the Advancement of Science. Accessed 2024-03-04
-
[53]
Alghamdi, A.O., Gonzalez, N.M., Geiger, F.M.: Temperature Dependence of Proton Coverage and the Total Potential at Fused Silica:Water Interfaces from Phase-Resolved Nonlinear Optics. Journal of the American Chemical Society 147(17), 14308–14315 (2025) https://doi.org/10.1021/jacs.4c18310 . Publisher: American Chemical Society. Accessed 2025-07-07 21
-
[54]
Surface Science331-333, 1355–1360 (1995) https://doi
Gavrilenko, V.I., Rebentrost, F.: Nonlinear optical susceptibility of the surfaces of silicon and diamond. Surface Science331-333, 1355–1360 (1995) https://doi. org/10.1016/0039-6028(95)00296-0 . Accessed 2025-10-03
-
[55]
Sposito, G.: On the surface complexation model of the oxide-aqueous solution interface. Journal of Colloid and Interface Science91(2), 329–340 (1983) https: //doi.org/10.1016/0021-9797(83)90345-4 . Accessed 2024-12-08
-
[56]
Physical Review B53(8), 4999–5006 (1996) https://doi.org/10.1103/ PhysRevB.53.4999
Mendoza, B.S., Moch´ an, W.L.: Exactly solvable model of surface second-harmonic generation. Physical Review B53(8), 4999–5006 (1996) https://doi.org/10.1103/ PhysRevB.53.4999 . Accessed 2025-08-16
work page 1996
-
[57]
Physical Review B45(16), 9339–9346 (1992) https://doi.org/10.1103/PhysRevB.45.9339
Dzhavakhidze, P.G., Kornyshev, A.A., Liebsch, A., Urbakh, M.: Theory of second- harmonic generation at the metal-electrolyte interface. Physical Review B45(16), 9339–9346 (1992) https://doi.org/10.1103/PhysRevB.45.9339 . Accessed 2025-08- 16 Acknowledgments We want to acknowledge Dr. Alan Bowman for his technical support during the initial stages of the s...
-
[58]
Excitation Configuration: At the bottom boundary of the unit cell, a port boundary condition was defined with excitation activated, simulating back illumination by a normal incident plane wave. The electric field polarization was oriented along a predetermined axis to generate the desired excitation conditions
-
[59]
Boundary Conditions: The upper boundary of the model employed a second port boundary condition without excitation, allowing for the transmission of the excited wave through the structure. To mitigate the influence of artificial reflec- tions that could skew the simulation results, perfectly matched layers (PML) were implemented at both the top and bottom ...
-
[60]
This integration enabled a thorough assessment of the energy flow in and out of the nanostructure
Reflectance and Transmittance Calculation: To evaluate the optical performance of the structure, the reflectance and transmittance were calculated by integrating the Poynting vectors over planes parallel to both the substrate and superstrate. This integration enabled a thorough assessment of the energy flow in and out of the nanostructure
-
[61]
S7A), ensuring accuracy in the simulation parameters
Material Properties: The refractive index for silicon was sourced from experimen- tal ellipsometry measurements (Fig. S7A), ensuring accuracy in the simulation parameters. Non-Linear Simulation:Having acquired the electric field distribution from the linear simulation, the next phase involved computing the nonlinear surface polarization responsible for SH...
-
[62]
Surface Polarization Calculation: The field profile obtained earlier was used to derive the nonlinear surface polarization, incorporating the material nonlinearity as a source term for subsequent simulations
-
[63]
This setup enabled the derivation of the SH signal strength
Second harmonic generation analysis: A linear simulation at the second harmonic (SH) wavelength was then executed, with the nonlinear surface polarization acting as the radiation source. This setup enabled the derivation of the SH signal strength
-
[64]
Non-linear reflectance and transmittance: The SH signal strength was calculated similarly to the linear case, by integrating the Poynting vectors on planes parallel to the substrate. This method enabled a comprehensive understanding of how the SHG signal evolves with varying disk dimensions and environmental conditions. In summary, this dual-step simulati...
work page 2000
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.