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. Author manuscript; available in PMC: 2015 Mar 1.
Published in final edited form as: Chem Sci. 2013 Dec 10;5(3):1008–1014. doi: 10.1039/C3SC53181C

Table 2.

Computational, electrochemical, and optical data for IDTs 7a–7d and diones 8a–8d

Computationala Electrochemicalb Opticalc
Compd EHOMO ELUMO Egap Ered1 Ered2 Eox EHOMO ELUMO Egap λmax EGap
7a −5.35 −3.17 2.18 −0.92 −1.69d 0.93 −5.57 −3.72 1.85 561 2.07
7b −5.30 −3.34 1.96 −0.80 −1.62d 0.92 −5.56 −3.84 1.72 624 1.88
7c −5.41 −3.22 2.18 −0.94 −1.59d 0.93d −5.57d −3.70 1.88 592 1.96
7d −5.29 −3.46 1.84 −0.61 −1.24d 0.98d −5.62d −4.03 1.59 632 1.83
8ae −6.12 −3.40 2.72 −0.91 −1.49 −3.73 566 1.75
8bf −5.99 −3.47 2.51 598 1.66
8ce −6.22 −3.41 2.81 −0.87 −1.27 −3.77 551 1.89
8df −5.94 −3.51 2.43 609 1.56
a

Calculations were performed at the B3LYP/6-31G** level of theory; energies are in eV.

b

CVs were recorded using 1–5 mM of analyte in 0.1 M Bu4NOTf/CH2Cl2 at a scan rate of 50 mV s−1 with a glassy carbon working electrode, a Pt coil counter electrode, and a Ag wire pseudo-reference. Values reported as the half-wave potential (vs SCE) using the Fc/Fc+ couple (0.46 V) as an internal standard. HOMO and LUMO energy levels in eV were approximated using SCE = −4.68 eV vs vacuum (see ref 18) and E1/2 values for reversible processes or Ep values for irreversible processes.

c

Spectra were obtained in DMSO; wavelengths are in nm. The optical HOMO/LUMO gap was determined as the intersection of the x-axis and a tangent line passing through the inflection point of the lowest-energy absorption; energies are in eV.

d

Reported as V at peak current, not half-wave potential.

e

Due to poor solubility in CH2Cl2, o-dichlorobenzene (ODCB) was used as solvent for electrochemical measurements.

f

Cyclic voltammetry measurements could not be obtained due to poor solubility of the compound.