Chinese Journal of Catalysis ›› 2022, Vol. 43 ›› Issue (11): 2757-2771.DOI: 10.1016/S1872-2067(22)64157-3
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Hai-Sheng Su, Xiaoxia Chang, Bingjun Xu*()
Received:
2022-06-01
Accepted:
2022-07-28
Online:
2022-11-18
Published:
2022-10-20
Contact:
Bingjun Xu
About author:
Bingjun Xu is the Ge li and Ning Zhao Chair Professor at College of Chemistry and Molecular Engineering of the Peking University. Dr. Xu received his Ph.D. in Physical Chemistry from Harvard University in 2011, and then worked as a postdoctoral researcher at Caltech. Dr. Xu started his independent research career in the Department of Chemical & Biomolecular Engineering at University of Delaware in 2013 as an Assistant Professor, and was promoted to a Centennial Development Associate Professor in 2019. Dr. Xu joined the Peking University in 2020. The current research interest of the Xu lab spans heterogeneous catalysis, electrocatalysis and in-situ/operando spectroscopy. Dr. Xu is an awardee of US NSF Early Career Award (2017), US Air Force Office of Scientific Research Young Investigator Award (2016), ACS Petroleum Research Fund Doctoral New Investigator Award (2015), the I&EC Class 2018 Influential Researchers (2018), and was elected as an Early Career Fellow in the Industrial & Engineering Chemistry Division of ACS (2022). He has published more than 100 peer reviewed articles.
Supported by:
Hai-Sheng Su, Xiaoxia Chang, Bingjun Xu. Surface-enhanced vibrational spectroscopies in electrocatalysis: Fundamentals, challenges, and perspectives[J]. Chinese Journal of Catalysis, 2022, 43(11): 2757-2771.
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URL: https://www.cjcatal.com/EN/10.1016/S1872-2067(22)64157-3
Fig. 1. Schematic of surface plasmonic resonance (a) and the electromagnetic enhancement of SERS (b). (c) Transmission electron microscopy image of typical Au@SiO2 nanoparticles with 55 nm-Au core and 2 nm-SiO2 shell. Reprinted with permission from Ref. [28]. Copyright 2020, American Chemical Society.
Fig. 2. Schematics of SERS nanostructures to monitor in situ electrocatalytic reactions. (a) SERS core-shell; (b) SHINs-satellite; (c) SHINs on flat electrodes.
Fig. 3. Schematics of two typical electrochemical spectral cells for SERS experiments. (a) A home-built cell. Reprinted with permission from Ref. [51]. Copyright 2013, Nature America, Inc. (b) A commercial cell. Reprinted with permission from Ref. [28]. Copyright 2020, American Chemical Society.
Fig. 5. Schematics of electrochemical cells for in situ ATR-SEIRAS experiments. (a) A typical cell. Reprinted with permission from Ref. [55]. Copyright 2019, American Chemical Society. (b) A side-facing cell. Reprinted with permission from Ref. [64]. Copyright 2022, Springer Nature. (c) A side-facing sell with stirring. Reprinted with permission from Ref. [65]. Copyright, 2020 American Chemical Society. (d) A modified cell for both in situ SEIRAS and SERS measurements. Reprinted with permission from Ref. [64]. Copyright 2022, Springer Nature.
Characteristic | SERS | SEIRAS |
---|---|---|
Vibrational mode | Changing polarizability | Changing dipole moment |
Optical cross-section | Raman scattering ~10-30 cm2 sr-1 | IR absorption ~10-20 cm2 sr-1 |
Spectral range | ~10-4000 cm-1 | ~1000-4000 cm-1 for conventional Si prisms (600-4000 cm-1 with thin micromachined Si wafers) |
Absorption of H2O | Weak | Strong |
Surface enhancement | Proportional to E4, routinely larger than 106 | Proportional to E2, usually 10-103 |
Irradiation source | Monochromatic laser, typically visible or near-IR laser | Continuum wavelength, typically in mid-IR region |
Photo damage | Relatively high | Relatively low |
Table 1 Comparison of surface-enhanced Raman and infrared absorption spectroscopies. E represents the enhancement of electromagnetic field.
Characteristic | SERS | SEIRAS |
---|---|---|
Vibrational mode | Changing polarizability | Changing dipole moment |
Optical cross-section | Raman scattering ~10-30 cm2 sr-1 | IR absorption ~10-20 cm2 sr-1 |
Spectral range | ~10-4000 cm-1 | ~1000-4000 cm-1 for conventional Si prisms (600-4000 cm-1 with thin micromachined Si wafers) |
Absorption of H2O | Weak | Strong |
Surface enhancement | Proportional to E4, routinely larger than 106 | Proportional to E2, usually 10-103 |
Irradiation source | Monochromatic laser, typically visible or near-IR laser | Continuum wavelength, typically in mid-IR region |
Photo damage | Relatively high | Relatively low |
Fig. 6. (a) In situ SEIRAS and SERS spectra on oxide-derived Cu film. (b) Plots of CO peak frequency as a function of potential. The Stark tuning rates were labeled. (c) In situ SEIRA spectra on oxide-derived Cu film at -0.7 VRHE with and without stirring. (d) Normalized peak area of COatop peaks (blue) and the current density (black) during the SEIRAS test in (c). Reprinted with permission from Ref. [74]. Copyright 2022, Springer Nature.
Fig. 7. CO adsorption isotherms on polycrystalline dendritic Cu particles. Reprinted with permission from Ref. [149]. Copyright 2022, John Wiley & Sons, Inc.
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