Abstract
In situ analysis of electrochemical interfaces modified with molecular adsorbates using fluorescence microscopy is outlined. The fluorescence intensity from the fluorophore-modified adsorbate is strongly quenched when the separation of the fluorophore from the metal electrode surface is decreased below 200 nm. The theory describing this important characteristic is outlined with emphasis on the lifetime and far-field intensity of the fluorophore as a function of the separation from the metal. A number of examples are given in which fluorescence microscopy is used to study surfaces modified with the self-assembled monolayers (SAMs) composed of either alkylthiols, peptides, or DNA. The ability to interrogate both the lateral and axial distributions of the adsorbed monolayers within the micron scale optical resolutions is highlighted. The influence of the electrode potential (or charge) on the fluorescence images is shown for the reductive or oxidative removal of the adsorbate. The preparation of modified electrode surfaces is also reviewed, illustrating the influence of surface crystallography on the resulting surface modification or thiol exchange processes. Preliminary results of a DNA SAM studied using 2-photon fluorescence lifetime imaging microscopy are presented, demonstrating the measurement of lifetime distributions and its correspondence with the theory. In situ spectroelectrochemical fluorescence microscopy is thus shown to be useful in studying the electrochemical interface in terms of its homogeneity of modification, the structure in the axial direction away from the electrode surface and the influence of charge (or potential) on the dynamics of the interface.
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Acknowledgements
The authors would like to express their gratitude to the Advanced Materials and Processing Engineering Laboratory (AMPEL), the Mechanical and Electronic Shops in the Department of Chemistry (UBC), and Laboratory for Advanced Spectroscopy and Imaging Research (LASIR) for continued support of the development of this methodology. We would also like to acknowledge the assistance by Dr. S. Kamal in using and adapting the two-photon FLIM microscope for use with the spectroelectrochemical cell. The HS-C10-BODIPY and HS-Aib4-BODIPY molecules were gratefully provided by Prof. M. Workentin (Western University) and Prof. F. Maran (University of Padova), respectively. We would also like to thank Prof C. Buess-Herman and Dr. T. Doneux of the Université Libre de Bruxelles for very helpful discussions and collaboration on method development. Funding for this work was provided by NSERC (Canada) through the Discovery Grant and RTI programs. JCM benefited from a scholarship by CONACYT (Mexico) for his graduate studies.
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Appendix
Glassblowing instruction for making the spectroelectrochemical cells. The process developed in the UBC chemistry glass shop to create the cells involves a borofloat window of the appropriate diameter and the tubing to match. The addition of ports and the location of the ports are added as requested. Most of the cells manufactured have 4 ports around the main or top joint, with a further 3–4 on the cell body. The ports on the cell body were straight through or ring seals with stems and stopcocks to direct material to the window at the bottom of the cell.
The first step is the manufacture of the cell bodies with the main or top joint (standard taper 14/23 socket). These have been made primarily from 38-mm borosilicate tubing as this diameter matches the 1.5″ windows. Cells have been made from (1″) 25.5 mm to (2″) 50 mm with (1.5″) 38 mm proving to be the most resilient. The glass joints are sealed to the tubing with an effort to maintain a shoulder for the positioning of future ports. The main body of the cell will then be pulled to a point leaving tubing to the length requested. This step is usually repeated several times to maintain a “stock” of cell bodies in preparation for sealing the windows onto the bottom of the tubing.
The bottom of the main bodies of the cells are cut using a wet saw and then washed with tap water to remove any excess grit. The cell bodies are then ready for polishing using diamond pads. Beginning with 200 grit, the bottom of the cell is polished and then rinsed with tap water. Next diamond pads with 400 grit, 500 grit, 800 grit, and finally 1500 grit were used. This is done in an effort to allow the window to seal to the cell body using less heat.
Sealing the windows onto the cell body is done with the use of a glass lathe, with the cell body in a holder using the 14/23 joint at the head stock and a 30-mm carbon rod held in the tail stock. A window is placed between the cell body and the carbon rod. The window is then sandwiched between the carbon and glass cell body and set to slowly rotate with a hand torch gently heating the bottom of the cell body and window. The torch tip used on the national hand torch is size one, which allows for a very sharp, tight fire. The fire needs to be quickly adjustable from a gassy soft fire to a strong sharp oxygen rich fire as the window and cell body warm up and are ready to be sealed.
Using a carbon paddle to ensure that the window remains in contact with the cell body, the hand torch fire is sharpened and sealing the window is started. Once a light tacking of the window occurs with the cell body, the carbon rod is withdrawn a short distance from the window face. If the carbon rod remains too long on the window, the window will be distorted and conform to the carbon rod.
Fusing the window to the cell body can begin with special regard for the wash of the torch flame. Any incidental heat can and will melt the window which can be heard flexing from the heat at this point in the procedure. The polishing done to the bottom of the cell body facilitates a quick seal between the window and cell body.
Once the window is attached, the cell is placed in a hot oven to anneal. This is usually the time that stress can cause the window to shatter; every effort needs to be taken to protect the new seal from sharp changes in temperature. These seals can be so sensitive that the barometric pressure affects the likelihood of survival; this is a speculative explanation for windows failing to survive the experience of being sealed onto the cell.
Once the windows have been annealed to 565 °C, they are very resilient to temperature changes. This allows the ports to be sealed on the cell usually beginning from the top ports around the main joint and then down the cell body to the window. The only special care that needs to be taken is to protect the window from blunt force.
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Casanova-Moreno, J., Yu, Z.L., Massey-Allard, J., Ditchburn, B., Young, J.F., Bizzotto, D. (2017). In Situ Spectroelectrochemical Fluorescence Microscopy for Visualizing Interfacial Structure and Dynamics in Self-assembled Monolayers. In: Miomandre, F., Audebert, P. (eds) Luminescence in Electrochemistry. Springer, Cham. https://doi.org/10.1007/978-3-319-49137-0_2
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