物理化学学报 >> 2025, Vol. 41 >> Issue (5): 100041.doi: 10.1016/j.actphy.2024.100041
收稿日期:2024-10-25
修回日期:2024-11-18
录用日期:2024-11-19
发布日期:2025-04-18
通讯作者:
Email: gongm@fudan.edu.cn (龚鸣)
基金资助:
Xueting Cao, Shuangshuang Cha, Ming Gong*(
)
Received:2024-10-25
Revised:2024-11-18
Accepted:2024-11-19
Published:2025-04-18
Contact:
Email: gongm@fudan.edu.cn (Ming Gong)
Supported by:摘要:
界面双电层是电催化反应的核心区域。催化剂表面原子、反应物、中间体、产物、溶剂分子和离子等组分,共同构成了复杂的动态反应网络。这种特殊的组成和结构赋予界面双电层以特殊的性质,深刻地影响了电催化反应的路径与结果。本文将以电催化反应中的双电层为主要研究对象,围绕双电层理论模型及其历史沿革、双电层的实验表征方法和双电层对电催化反应的影响这三个方面,以若干电催化反应前沿研究为例,阐述双电层与电催化反应之间的关联,并介绍一些特定情形下电催化双电层研究的研究方法和研究逻辑。
曹雪婷, 察爽爽, 龚鸣. 电催化反应中的界面双电层:理论、表征与应用[J]. 物理化学学报, 2025, 41(5), 100041. doi: 10.1016/j.actphy.2024.100041
Xueting Cao, Shuangshuang Cha, Ming Gong. Interfacial Electrical Double Layer in Electrocatalytic Reactions: Fundamentals, Characterizations and Applications[J]. Acta Phys. -Chim. Sin. 2025, 41(5), 100041. doi: 10.1016/j.actphy.2024.100041
表1
"
| Symbols | Connotations |
| A | the interactions between adsorbates in the Frumkin adsorption isotherm |
| b | difference between the Gibbs free energy change for the formation of the down-state water at the electrode surface and the up-state water |
| β | symmetry factor |
| ca | concentration of adsorbates in the bulk phase of the solution |
| c0 | concentration of species i in the bulk phase of the solution |
| concentration of the reduced species Re in the bulk phase of the solution in the interfacial single-electron transfer reaction | |
| concentration of the oxidized species Ox in the interfacial single-electron transfer reaction | |
| concentration of the oxidized species Ox in the bulk phase of the solution in the interfacial single-electron transfer reaction | |
| csurface | concentration of species on electrode surface |
| C | double layer (differential) capacitance |
| Ccharge | capacitance formed when ions are adsorbed on the electrode surface |
| Cdipole | capacitance formed when water dipoles are adsorbed by the electrode |
| Ceqcm | correction constant for EQCM resonator |
| CM | the contribution of electrode side to the interfacial capacitance |
| CH | the contribution of Helmholtz layer to the interfacial capacitance |
| CG | the contribution of diffusion layer to the interfacial capacitance |
| χ(2) | second-order optical susceptibility |
| χ(3) | third-order optical susceptibility |
| The effective second-order optical susceptibility | |
| d | Differential notation (as distinguished from italicized d for the plate separation distance) |
| d | the plate separation distance in the parallel plate capacitor model |
| E | electric field intensity |
| e0 | the charge carried by one single electron |
| ε | the dielectric constant in a certain medium |
| ε0 | vacuum dielectric constant |
| F | Faraday constant |
| f | f= F/RT |
| Δf | the change in vibrational frequency measured by EQCM |
| ΔGn | Gibbs free energy change for primitive reaction steps associated with n proton-electron pairs |
| the change of surface dipole potential | |
| gM | the electrode potential on the metal electrode surface within the double layer |
| gS | the electrode potential on the solution side within the double layer |
| The surface potential contributed by oriented water molecules | |
| I2ω | the emitted light intensity of SHG |
| i | imaginary unit, species designation (such as species i) |
| i | current density |
| i0 | exchange current density |
| icath | cathodic current density |
| iS | the current of the substrate in SECM |
| iT | the (Faradaic) current passing through the tip in SECM |
| k0 | standard reaction rate constant |
| kb | backward reaction rate constant |
| kf | forward reaction rate constant |
| κ-1 | the characteristic thickness of the EDL in the GC model |
| KA→B | the integral capacitance from A to B |
| γ | interfacial tension |
| kB | Boltzmann constant |
| Δm | the change of the electrode mass |
| Mads | the molar mass of adsorbed species |
| dipole moment | |
| the electrochemical potential of the electrons on the reference electrode | |
| the electrochemical potential of the electrons on the (other) metal electrode | |
| Δμ | Stark tunability |
| n | Variable indicating ‘number’, e.g., number of radical reactions, number of water molecules in hydrated ions, etc. |
| Ne, trans | electron transfer coefficient per unit mole of reaction |
| Nt | the background signal in a radiotracer measurement |
| Nt’ | the signal under the voltage without specific adsorption in a radiotracer measurement |
| Nt’’ | the signal under the voltage with specific adsorption in a radiotracer measurement |
| Nwater | number of water molecules on the electrode surface |
| ϕ | the phase of emitted light of SHG |
| φ | inner potential, the electrode potential under certain conditions |
| Δφ | the potential difference within the electrical double layer, i.e., the electrode | solution interface potential difference |
| φt | the potential of the working electrode at time t |
| φdc | the potential of the working electrode under direct current |
| φx | the potential at a distance x from the electrode surface, with the bulk solution potential defined as 0 |
| ψ | outer potential |
| Δψ | the outer potential difference of the electrical double layer |
| ω | frequency |
| qCA | the charge density of specific adsorbed ions |
| qd | the total diffuse charge density in solution |
| qM | the charge density of the (metal) electrode |
| ΔQ | the change of quantity of electric charge during electrocatalytic reactions |
| R | ideal gas constant |
| R | the roughness of the electrode |
| t | time |
| T | absolute temperature |
| θa | coverage (referring to the fraction of the surface that is covered) |
| θ | the phase difference between χ(3) and χ(2) |
| U | Maximum value of dipole-dipole interaction energy |
| V | the voltage drop per unit area of M | S EDL interface |
| Vapp | applied potential |
| vscan | the potential scan rate in cyclic voltammetry |
| x | the vertical distance of the target site from the electrode surface |
| X | the constant related to lateral interactions, 0 < X < 1 |
| y | an artificially defined physical quantity to represent the electrical and lateral interactions in interactions within EDL |
| Z | an artificially defined physical quantity to represent the distribution of water in the up and down states on the electrode surface |
| z | the number of charges per ion |
表2
"
| Characterization Techniques | Abbreviation | Basic Principles | Vertical Resolution | Horizontal Resolution | Time Resolution | Information | On the Electrode Side | IHP/Adsorption Layer | OHP & Diffusion Layer | Category |
| Electrocapillary | – | Measurement of interfacial tension as a function of applied voltage | Macroscopic nature | Macroscopic nature | Measurement of the differential capacitance and the potential of zero charge of an EDL | Electrochemical Method | ||||
| Cyclic Voltammetry | CV | Potential scanning cyclically to obtain the current-potential relationship | Macroscopic nature | Macroscopic nature | Electrochemical behaviors of the system | Electrochemical Method | ||||
| Alternating Current Voltammetry | ACV | Relationship between the variation of AC amplitude and phase with DC polarization potential at a given electrical signal frequency | Macroscopic nature | Macroscopic nature | Distinguishing between Faraday and charging currents and separating to obtain information on different electrochemical processes | Electrochemical Method | ||||
| Electrochemical Impedance Spectroscopy | EIS | Variation of AC impedance of an electrochemical system as a function of the frequency of an applied electrical signal under a certain condition of DC polarization | Macroscopic nature | Macroscopic nature | Frequency dependent, up to milliseconds | Solution resistance from reference electrode to working electrode, double layer capacitance, charge transfer resistance, detection of diffusion processes from the body to the electrode surface and in the electrolyte | Electrochemical Method | |||
| Electrochemical Quartz Crystal Microbalance | EQCM | The oscillation frequency of quartz crystal lenses is affected by changes in electrode mass, thus correlating electrochemical information with changes in electrode mass | Relationships between mass, current and charge as a function of potential in the surface layer of solid electrodes, tracking mass transfer and charge transfer processes | Derivative Electrochemical Method | ||||||
| Radiotracer Measurements | - | Detection of β particles from isotope decay in the electrolyte by means of a scintillation counter, where the signal from the decay of the radioactive substrate is not recorded if it is adsorbed on the electrode | Surface radiation intensity or surface concentration, corresponding to the number of molecules adsorbed on the electrode surface Limitations lie in finding target molecules with radioactive isotopes | √ | Spectroscopy | |||||
| in situ/operando Infrared Reflection Absorption Spectroscopy | IRRAS | The infrared light passes through a thin layer of electrolyte to illuminate the interface, while elective absorption occurs and multiple reflections and attenuation result in an outgoing light that contains information about the interface | 100 nm | 5 μm | In the order of milliseconds and microseconds | Chemical nature and adsorption structure of adsorbed species Orientation of molecules on surfaces and the effect of double layer electric fields on intramolecular bonding Functional groups, molecular symmetry, and catalyst-molecule interactions | (very weak) | √ | IR Spectroscopy | |
| Attenuated Total Reflectance Infrared Spectroscopy | ATR-IR | Infrared light irradiates the sample to be measured, penetrates into the interface to a certain depth and undergoes selective absorption, and is reflected and attenuated several times to obtain the outgoing light which contains the interface information | 100 nm | 5 μm | √ | √ (no resolution) | √ | IR Spectroscopy | ||
| Surface Enhanced Infrared Absorption Spectroscopy | SEIRAS | When a molecule is adsorbed on the surface of a noble metal, transition metal or semiconductor substrate, its infrared absorption signal is dramatically amplified by several orders of magnitude | 10 nm | 5 μm | √ | √ | √ | IR Spectroscopy | ||
| in situ/operando Raman Spectroscopy | Raman | Scattered light undergoes an energy exchange within the illuminated object, and the difference in photon energy between the scattered light and the incident light reflects information about the vibrational energy levels of the molecules | 500 nm | 2-3 μm | Generally in the order of milliseconds with CCD; in the order of 10 nanoseconds with pump light | Structure and orientation of molecules on the surface, the effect of the electric field of the double electric layer on intramolecular bonding; qualitative and quantitative information about the electrode composition in the near-surface region, i.e., bonding on the catalyst surface; changes in the surface with potential, state of charge, and/or time | √ | √ (no resolution) | √ | Raman Spectroscopy |
| Surface enhanced Raman Spectroscopy | SERS | When a molecule is adsorbed on the surface of a noble metal, transition metal or semiconductor substrate, the Raman scattering signal is dramatically amplified by several orders of magnitude | 1 nm | √ | √ | √ | Raman Spectroscopy | |||
| Sum Frequency Generation Vibrational Spectroscopy | SFG-VS | Simultaneous irradiation of an electrochemical interface with non-central symmetry (satisfying symmetry breaking) by an infrared beam and a visible beam produces a sum-frequency signal | Measurement of surface potential, molecular structure, symmetry and orientation of interfacial reactants/solvents/intermediates, and surface number density | √ | √ | No solution phase information | Nonlinear Optical Characterization | |||
| Second Harmonic Generation | SHG | Two incident photons of the same frequency pass through the electrode-electrolyte interface to produce a doubled-frequency photon, and the resulting intensity of the incident light reflects the electric field information at the interface | Measurement of surface potential, determination of zero-charge potential, molecular structure and orientation of interfacial reactants/solvents/intermediates | √ | √ | No solution phase information | Nonlinear Optical Characterization | |||
| in situ X-ray Diffraction | XRD | Using an in situ electrochemical cell, X-rays diffract with the working electrode phase and contain information on the bulk phase of the crystalline electrode under reaction conditions | > 1 mm | 1–3 μm | Fast enough to capture the typical dynamic processes of active substances in operando experiments | Qualitative and quantitative information on the (average) composition of bulk phase electrodes Changes in the crystal structure of bulk phase electrodes with potential, state of charge and/or time | √ (bulk) | × | × | X-Ray Diffraction Spectroscopy |
| in situ X-ray absorption near edge structure | XANES | Incident X-rays excite the inner electrons to unoccupied energy levels and the X-rays are strongly absorbed, reflecting information about the oxidation state and electronic structure of the element under test | Penetrate the bulk phase | Average oxidation states and electronic configurations of specific elements in electrode materials for amorphous electrodes | √ (bulk) | Characterization of hydrogen bond strength of water molecules in IHP | × | X-Ray Absorption Spectroscopy | ||
| in situ Extended X-ray Absorption Fine Structure | EXAFS | Incident X-ray excitation to the continuum state of the inner electrons interferes with neighboring atoms, reflecting information such as bond distances and coordination numbers | Penetrate the bulk phase | 5 Å range of short-range covalent structures | Interface constituent element analysis, interatomic distances, coordination information, available for amorphous electrodes | √ (bulk) | × (analyzed indirectly in conjunction with other techniques) | × | X-Ray Absorption Spectroscopy | |
| Ambient Pressure X-ray Photoelectron Spectroscopy | APXPS | Improvements to the vacuum system, X-ray source and feeding technique have enabled the XPS to be tested at near atmospheric pressure, measuring the photoelectron beam formed by the incident X-rays striking the inner electrons | 1–12 nm | 30 μm | Qualitative and semi-quantitative elemental analysis, depth imaging, oxidation states; molecular structure identification at interfaces | √ | √ | √ | Photoelectron Spectroscopy | |
| Ambient Pressure Resonance Auger Electron Spectroscopy | APRAES | The incident X-ray-excited inner electron leaps back into the inner vacancy and the energy released excites the valence electron, the Rochelle electron | 1–6 nm | 0.02–50 μm | Surface elemental composition, adsorbate coverage, interfacial electronic structure | √ | √ | √ | Photoelectron Spectroscopy | |
| Electrochemical Scanning Tunneling Microscopy | EC-STM | The tunnelling current is sensitive to the probe-sample distance and the electronic properties of the sample, reflecting interfacial information | 0.1–1 nm | 1–10 nm | In the order of milliseconds | Adsorption of species structure, electrode surface morphology, electronic structure and active sites, information on both liquid and solid phase sides can be obtained | √ | √ | Scanning Probe Microscopy | |
| Scanning Electrochemical Microscopy | SECM | Faraday currents generated by electrochemical reactions at the interface, which are strongly correlated with the probe-sample distance, reflect interfacial information | 10 nm | 20–50 nm | Quantification of local concentrations of interfacial species, adsorbed species coverage, local pH, surface reactivity | √ | Scanning Probe Microscopy |
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