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1 ach to the Mn(v) horizontal lineO (dpi-ppi)* frontier orbital.
2 nity of PVPP towards phenols is related with frontier orbitals.
3 mall energy differences between all adjacent frontier orbitals.
4 g and thereby obtaining information on their frontier orbitals.
5 ificantly different relative energies of the frontier orbitals.
6  groups of the donor (those derived from the frontier orbitals 2e and 6a(1) of the isolated methoxy g
7 I) d(pi) orbital and one of the two thiolate frontier orbitals, a condition that is absent in the Fe(
8                                   Charge and frontier orbital analyses suggest that charge transfer m
9              The optical spectra, along with frontier orbital analysis, show that the assumption that
10                                  Analysis of frontier orbitals and geometries, B3LYP/6-31G(d)//B3LYP/
11 rized using electrostatic potential maps and frontier orbital calculations.
12                                          The frontier orbitals consistently and simply indicate high
13 and, conventional reactivity indices such as frontier orbital density take only the electronic state
14 the electronic gap and a modification of the frontier orbitals directly associated with the formation
15 dealized C3 symmetry) with doubly degenerate frontier orbitals, (e)(3) = [|mL +/- 2>](3) = [x(2) - y(
16 structure highlights the controlling role of frontier orbital effects underpinning the catalytic perf
17  on individual MD snapshots show significant frontier orbital electronic population on the bridge in
18 onic decoupling to investigate geometric and frontier orbital electronic properties of almost undistu
19          We show for the first time that the frontier orbital energetics (conduction band minimum (CB
20                           Despite similar Ti frontier orbital energies demonstrated by these spectra,
21  energy of the deep blue dopant and the high frontier orbital energies of hosts needed to transport c
22                Moreover, calculations on the frontier orbital energies of PhobPMe isomers and their b
23  data, in terms of the absolute and relative frontier orbital energies of their constituent [porphina
24 1,2,5]thiadiazole) (E-BBTD-E)} that regulate frontier orbital energy levels and progressively increas
25 te that modulation of semiconducting polymer frontier orbital energy levels can drive spectral shifts
26  the devices is related to the offset of the frontier orbital energy levels of the donor and acceptor
27 tching is that it induces a downshift of the frontier orbital energy levels of the station it is on (
28     This reflects both the dependence of the frontier orbitals for the semiconducting nanotubes on th
29 important finding in our simulations is that frontier orbitals HOMO and LUMO undergo substantial stab
30 ant than the symmetries of the substituent's frontier orbitals in determining the mode of bond locali
31 -orbit coupling in lifting the degeneracy of frontier orbitals in highly symmetric thallium cluster a
32 ith the carbonyl compounds, and (4) negative frontier orbital interaction values DeltaDeltaE(PhC(O)H)
33 ity index, Omega, based on electrostatic and frontier orbital interactions gives a good correlation w
34 imensional aromaticity as a result of strong frontier orbital interactions.
35 y of femtosecond X-ray spectroscopy to probe frontier-orbital interactions with atom specificity.
36 of solvation on the relative energies of the frontier orbitals is equally important and may even reve
37 tures and discernible activity trends at the frontier orbital level: (1) increasing the number of flu
38 h the pi* orbital of the ligand, making both frontier orbitals localized at the organic linker.
39 ensity functional theory methods, the ligand frontier orbital lying closer to the Fermi energy of the
40                  A simplified version of the frontier orbital model for a noncovalent dimer is used t
41                             The DFT-computed frontier orbital of the relevant protein segments sugges
42 markable effects on the energy levels of the frontier orbitals of Au25(SR)18(-) nanoclusters.
43  provide the tools to visualize not only the frontier orbitals of chemical reaction partners and prod
44 suggest that the effect of borylation on the frontier orbitals of each donor helps to explain differe
45 mented by analyzing the electron density and frontier orbitals of key reaction intermediates.
46 al data and an analysis of the DFT-predicted frontier orbitals of likely intermediates, were used to
47                                          The frontier orbitals of the (nacnac)Cr(II) fragment direct
48                Calculation of the charge and frontier orbitals of the aromatic donor (HOMO) and the N
49    Further spin density distribution and the frontier orbitals of the computed species suggest that t
50 ering dynamics perturbed the energies of the frontier orbitals of these structures, as determined thr
51 culations have revealed the concentration of frontier orbitals on the fullerene cage and a narrow dis
52                            Inspection of the frontier orbital ordering of 1 shows a relatively small
53 e show that mesomeric effects delocalize the frontier orbitals over the substituents recovering stron
54 ction were also probed by Fukui function and frontier-orbital overlap analysis in combination with pr
55                                            A frontier orbital perspective, looking at the interaction
56 orbital description, which provides a set of frontier orbitals populated by Fe 3d electrons.
57                   A detailed analysis of the frontier orbitals provided by the electronic structure c
58                                            A frontier orbital scheme provides molecular insight into
59                           An analysis of the frontier orbitals suggests this superexchange pathway to
60 ed wide enough to include one of the cluster frontier orbitals, the current blockade is lifted and ch
61                           It is found that a frontier orbital which is a mixing state between the e(g
62 e electron affinity and maintain delocalized frontier orbitals while significantly decreasing the tra
63 energy conformation maximizes overlap of the frontier orbitals while simultaneously minimizing interm
64  N(2) to two Zr centers, availability of the frontier orbitals with appropriate symmetry, and inflexi
65 sitions for the agents tested and overlap of frontier orbitals within the nucleophilic loci of the NC

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