“…If a monolayer is placed between the two Fig. 1 Some one-electron donors D (1-4) with their first gas-phase ionization potentials I D (6.25 eV for N,N,N 0 ,N 0 -tetramethyl-para-phenylenediamine (TMPD, 1), 71 6.83 eV for tetrathiafulvalene (TTF, 2), 72 7.6 eV for bis(ethylenedithio)tetrathiafulvalene (BEDT-TTF, 3), 73 9.38 eV for benzene (4)) 74,75 some one-electron acceptors A (5-8) with their gasphase electron affinities A A (1.9 eV for para-benzoquinone (BQ, 5), 76 2.6 to 2.8 eV for buckminsterfullerene (C 60 , 6), 77 2.8 eV for 7,7,8,8-tetracyanoquinodimethane (TCNQ, 7), 78 then corrected to 3.3 eV, 79 3.13 eV for 2,3-chloro-5,6-dicyano-para-benzoquinone (DDQ, 8)), 80 and some metals with their bulk work functions f (3.66 eV for Mg, 81 4.24 eV for Al(111), 82 5.31 eV for Au(111), 83 5.7 eV for Pt (111), 84 electrodes instead of a single molecule, then polarization energies must be discussed: putting charges on any one molecule will cost somewhat less energy, because partial charges will be induced in the neighboring molecules of the monolayer.…”