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7
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22344454438
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3 is less exothermic by an amount equal to the electron affinity (EA) of the A species.
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8
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0035857240
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(f) Syrstad, E. A.; Truecek, F. Am. Soc. Mass. Spectrom. 2004, 16, 208-224. (This latter paper contains the most up-to-date discussion of the mechanism of Scheme 1b.)
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22344455455
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note
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Rydberg states of high principal quantum number are known to have long lifetimes and large radial extents.
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16
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Orlando, FL, June
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(a) Sawicka, A.; Skurski, P.; Hudgins, R. R.; Simons, J. J. Phys. Chem. B 2003, B107, 13505-13511. (We should note that, later, in ref 5, Uggerud also considered the possibility of direct electron attachment to SS bonds.)
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22344456185
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2 species interacting with the positive site(s).
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33
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22344435347
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note
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An analogous discussion could be made comparing the C=O π* orbital's attraction and that of a positive site elsewhere in a peptide or protein.
-
-
-
-
34
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5544310402
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Al-Khalili, A.; Thomas, R.; Ehlerding, A.; Heilberg, F.; Geppart, W. D.; Zhaunerchyk, V.; Uggerud, E.; Vedde, J.; Adlhart, C.; Semaniak, J.; Kaminska, M.; Zubarev, R. A.; Kjeldsen, F.; Andersson, P. U.; Österdahl, F.; Bednarska, V. A.; Paal, A. J. Chem. Phys. 2004, 121, 5700-5708.
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35
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22344446115
-
-
note
-
As will become clear soon, most of the energy available in the collisions that we are studying will come from converting the cation-anion Coulomb attraction energy to relative translational energy. The initial internal vibrational-rotational energy of the cation or anion will be a small fraction of the total energy and can therefore be ignored.
-
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39
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For example, see Desfrancois, C. Phys. Rev. A 1995, A51, 3667-3675.
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22344442505
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note
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1,2.
-
-
-
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42
-
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22344447681
-
-
note
-
Electron-cation and anion-cation collision cross sections are usually considerably greater than, for example, gas-kinetic cross sections, especially when the relative kinetic energies are low. It is the effect of the long-range Coulomb attractive potentials that makes these collision cross sections so large.
-
-
-
-
43
-
-
22344437025
-
-
note
-
+ sites are separated by more rigid units than methylene groups, so one could be more confident about knowing the distance between these two sites.
-
-
-
-
44
-
-
22344434622
-
-
note
-
The radial sizes of orbitals vary inversely as the square root of their electron binding energies. Because the Rydberg and σ* binding energies differ by a factor of 2, the radial sizes of the corresponding orbitals will be similar.
-
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45
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21744436851
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Zajfman, D.7
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46
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22344456318
-
-
note
-
We choose this electron energy because it is characteristic of the low-energy ECD experiments to which we are trying to relate.
-
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47
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48
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0035860864
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-1/2. Therefore, for electrons that have kinetic energy in the 0.1 -eV range, as we are considering here, the cross section is expected to be somewhat larger than that stated here.
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50
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0034630936
-
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These values are obtained by simply adding the unscreened Coulomb potentials of the two positive sites at the center of the S-S or C=O bond. We have shown (for example, see Skurski, P.; Simons, J.; Wang, X.-B.; Wang, L.-S. J. Am. Chem. Soc. 2000, 122, 4499-4507) that there is little, if any, dielectric screening produced by bonds within a molecule. The dielectric screening would be substantial if the molecule were surrounded by a bulk material that has a significant dielectric constant.
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|