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Luminescent acetylthiol derivative tripodal osmium(II) and iridium(III) complexes: Spectroscopy in solution and on surfaces

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Luminescent acetylthiol derivative tripodal Osmium(II) and Iridium(III) complexes. Spectroscopy in solution and on surfaces

Srinidhi Ramachandra1, Federico Polo2, Fabio Edafe 3, Klaus C.

Schuermann2, Christian A. Nijhuis4, Peter Belser3 William F. Reus4, George M. Whitesides4, Luisa De Cola* 1,2

1Laboratory of Supramolecular Chemistry and Technology, University of Twente, P.O. box 217, 7500 AE Enschede, The Netherlands

2Westfälische Wilhelms-Universität Münster, Physikalisches Institut, Mendelstraße 7, 48149 Münster, Germany

3Department of Chemistry, University of Fribourg, chemin du musée 9, 1700 Fribourg, Switzerland

4Department of Chemistry and Chemical Biology, Harvard University, 12 Oxford street, Cambridge, MA 02138, USA

Supplementary Information

Experimental procedure for measuring and analyzing J(V) data:

A wire soldered to the syringe needle made electrical contact between the EGaIn and a Keithley 6430 sub-femtoamp electrometer. Using a tungsten needle, we grounded the Au substrate. We collected each J(V) trace by applying a sweep of voltages (1 trace = 0 V Æ 2 V Æ -2 V Æ 0 V in steps of 0.1 V) and measuring current with the electrometer. To obtain current density, J, we measured the diameter of the footprint of the conical tip of EGaIn on the surface of the SAM, calculated the area of the footprint by assuming a circular cross section, and divided the measured current by the calculated area. We imaged the junction using a CCD camera fitted with a 450x magnifying lens and situated in the plane of the Au surface (to afford a side view).

We measured a total of 264 J(V) traces by forming a total of 11 individual contacts between EGaIn and the SAM. These measurements were distributed over two separate, SAM- covered, Au substrates. Each trace yielded two values of current density for each applied voltage (one value for the forward arm of the trace, another for the reverse); thus, a total of 528 values of

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J were collected for each of the 41 discrete values of V. For each applied voltage, we

constructed a histogram (see figure S1), having 10 bins/decade, of log(|J|), where J has units of A/cm2. We found that, for each applied voltage, the values of log(|J|) were normally distributed (i.e. |J| was log-normally distributed). Using the nonlinear least-squares, trust-region fitting algorithm in MATLAB 7.8.0, we fit the distribution of log(|J|) with a Gaussian and determined the mean (μ) and standard deviation (σ) of log(|J|). The log-mean and log-standard deviation of

|J| are given by μlog = 10μ and σlog = 10σ, respectively. Thus, 68% of the distribution of |J| at a given voltage lies between 10μσ and 10μ + σ, or equivalently, between μlog / σlog and μlog u σlog. The average trace in figure 9 is a plot of μlog vs. voltage; the lower error bars of this trace representμlog /σlog and the upper error bars represent μlog uσlog.

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Figure S1. Fitted histograms of log(|J|), where J has units of A/cm2. The histograms (gray) of log(|J|) for applied voltages of -2.0 V (top) and 2.0 V (bottom) are fitted with Gaussians (black).

The Gaussian fit gives the log-mean (μlog = 10μ) and log-standard deviation (σlog = 10σ) at a given applied voltage. Values for μlog and σlog at each voltage are used to construct the average trace in figure 9.

Comparison of solution vs. SAM cyclic voltammograms

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Figure S2. Comparison of cyclic voltammograms of Os-SAc in solution (black) and Os-SAC SAM (blue).

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