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1 nthesis recombined in reverse order of their ionization potential.
2 ng for heterogeneity in electron density and ionization potential.
3 n, zero electron affinity and an unsurpassed ionization potential.
4 ical as well as on the electron affinity and ionization potential.
5 undergo an inversion as a function of alkyne ionization potential.
6 cal band gap of 1.75 eV combined with a high ionization potential.
7  reported to very significantly decrease its ionization potential.
8 gth of its triple bond, nonpolarity and high ionization potential.
9 tions of rate constants with FMO energies or ionization potentials.
10 ct energetic shifts for ligands of differing ionization potentials.
11 tting to experimental heats of formation and ionization potentials.
12  species to determine adiabatic and vertical ionization potentials.
13  reveal how electron temperature varies with ionization potential and accommodates density effects.
14 sorption is likely due to both a decrease in ionization potential and an increase in bond length and
15               Additionally, optical data and ionization potential and electron affinity data were uti
16           By contrast, little change in both ionization potential and electron affinity is found in t
17           A good agreement is found with the ionization potential and isotope shifts, while disagreem
18  consistent with the periodic trends of both ionization potential and lattice energies of the species
19 2) pressure were optimized, with the optimum ionization potential and N(2) pressure found to be 3206
20 ags was separately used to lower the peptide ionization potential and permit direct ionization by 7.8
21  is found to be highly dependent on both the ionization potential and the C-H bond strength of the su
22 step, because this site has a relatively low ionization potential and this causes the radical cation
23 ly(p-phenylene ethynylene)s (PPEs) with high ionization potentials and associated high excited-state
24 significant gap between the M- and L-shells' ionization potentials and can be accelerated by strong,
25 erfluorination is calculated to increase the ionization potentials and electron affinities by approxi
26 s emphasized that one needs to use adiabatic ionization potentials and electron affinities instead of
27 plied to atoms and molecules for calculating ionization potentials and electron affinities, but fails
28 energies in good agreement with experimental ionization potentials and electron affinities.
29 rated to exist as air-stable solids with low ionization potentials and large dipole moments.
30 -tuning their electronic properties, such as ionization potentials and mechanistic pathways for react
31 ation generation (DeltaDeltaH(f) degrees and ionization potentials) and for probing the structures of
32                          Operating position, ionization potential, and N(2) pressure were optimized,
33  fragments (nN+), presence of S-P fragments, ionization potential, and presence of C-N fragments.
34  performance as a function of concentration, ionization potential, and sample complexity.
35                   We yield the band gap, the ionization potential, and the electron affinity in good
36 erties such as bond and excitation energies, ionization potentials, and electron affinities.
37 s include the bond dissociation energies and ionization potentials, and the reactions include those w
38 In addition, their dissociation energies and ionization potentials are reduced from those in correspo
39 tal properties of the additive metals (e.g., ionization potential) as physicochemical parameters, new
40 o the target molecule, the difference in the ionization potentials between helium and the molecule re
41      Modifications to guanine that lower its ionization potential convert it to a better trap for the
42               An accurate description of the ionization potential depression of ions in plasmas due t
43  electrochemically do not correlate with the ionization potentials determined by photoelectron spectr
44 nt of inertia, total energy, polarizability, ionization potential, dipole moment, subpolarity), compu
45 ectroscopy (UPS), and those with the highest ionization potentials displayed high sensitivity for the
46  fully bypass QM calculations and derive the ionization potential, electron affinity, and conceptual
47 ated oligomeric segment has its own discrete ionization potential, electron affinity, and optical ban
48                                 However, the ionization potential, electron affinity, chemical hardne
49            Standard enthalpies of formation, ionization potentials, electron affinities, and band gap
50 al-benzene distances, dissociation energies, ionization potentials, electron affinities, and spin mul
51 mproving the accuracy in heats of formation, ionization potentials, electron affinities, and total at
52     These measurements, combined with double-ionization-potential equation-of-motion coupled-cluster
53 rmation and adiabatic electron affinities or ionization potentials for N3, N3-, N5+, and N5- from tot
54 can be accelerated by up to 27 GeV in a high-ionization-potential gas (argon), boosting their initial
55 rgy metastable atoms (e.g., He(M)) with high ionization potentials (IE = 19.80 eV) did not show boost
56 the guanine base is the site with the lowest ionization potential in oligonucleotides and DNA and is
57  the data are presented as a function of the ionization potential IP.
58           Here, we show that PAHs with lower ionization potential (IP) are more easily removed by pyr
59   The O-H bond dissociation energy (BDE) and ionization potential (IP) key parameters were computed i
60            Fluoro substitution increases the ionization potential (IP) of indole, thereby suppressing
61 ng on the oxidation state of State I and the ionization potential (IP) of the organics; that is, only
62         A plot of electron affinity (EA) and ionization potential (IP) versus energy band gap (E(G))
63 ar mass compounds showing appropriate redox (ionization potential (IP), electron affinity (EA)), elec
64 ed from the natural log of rate constants vs ionization potentials (IP) indicates that fluoroalkenes
65                                              Ionization potentials (IP) ranged from 5.15 to 5.21 eV;
66   Experiments demonstrate that peptides with ionization potentials (IPs) above 7.87 eV can be single-
67 ) by using Wilkinson's catalyst versus their ionization potentials (IPs) and versus their lowest unoc
68 f aqueous ionization energies with gas-phase ionization potentials (IPs) indicates that hydration alt
69      The comparison of computed and measured ionization potentials makes it possible to investigate t
70                                          The ionization potential of B(9) is measured to be 8.45+/-0.
71  (Me)CG sequences may be caused by a lowered ionization potential of guanine bases paired with (Me)C
72                       As a result of the low ionization potential of neutral arginine, the actual hyd
73 erg series, we obtain an upper limit for the ionization potential of nobelium.
74            Correlations are made between the ionization potential of the acceptor molecules and the l
75 adiation with photon energy greater than the ionization potential of the adsorbed molecules, photoele
76  K) are decelerated with the decrease of the ionization potential of the alkali metal.
77 ion tag for the entire peptide, lowering the ionization potential of the complex below the 7.87-eV ph
78  k(cat) can be expressed as functions of the ionization potential of the donor (I(D)) and the electro
79             The dependence of Phi(TT) on the ionization potential of the flanking purine is more pron
80  level energies were used to re-evaluate the ionization potential of the indium atom to be [Formula:
81 ncrease in the O-H BDE and a decrease of the ionization potential of the phenol.
82                             We find that the ionization potential of the solvent-anion system is ofte
83  the proton affinity, fluoride affinity, and ionization potential of VX and the simulants.
84 ld also be sensitive and selective since the ionization potential of VX is small.
85        The basicity and, to a lesser extent, ionization potential of Z(-) were found to correlate wit
86 (3)O)3 is shown to have low first and second ionization potentials of 2.49 and 4.64 eV, respectively,
87  films of synthesized materials revealed the ionization potentials of 5.31-5.47 eV.
88  them it is necessary that the difference in ionization potentials of contiguous guanine and adenine
89 estimated lattice energies and the adiabatic ionization potentials of the anions and electron affinit
90 is linearly correlated with the one-electron ionization potentials of the corresponding heterocyclic
91 ing primarily from the shallow valence-shell ionization potentials of the iodide anions.
92                                          The ionization potentials of the polymer thin films were det
93 ations, we observe a large dependence of the ionization potentials of the polymers estimated by elect
94 ce bandedge (5.0 eV) was misaligned with the ionization potentials of the widely used transport layer
95  semiconductor NCs with the vastly different ionization potentials of their Ag(+) and Cu(+) dopants.
96          Solid-state electron affinities and ionization potentials of these siloles were measured usi
97       The density functional theory-computed ionization potentials of unsaturated diamondoid dimers c
98 nantly involves photoexcitation of the lower ionization potential species (donor) followed by electro
99 a matrix consisting of a compound with a low ionization potential such as benzo[ghi]perylene in the f
100 predicted free energies of base stacking and ionization potentials, suggesting a possible origin via
101 ore weakly correlated with sequence-specific ionization potential than G oxidation produced by ribofl
102 igher energy HOMO orbital and lower computed ionization potential than the only other significantly p
103  energy significantly lower than the guanine ionization potential, the one-photon ionization quantum
104 e predicted electron affinity, the predicted ionization potential, the optical gap, and the dispersib
105 es indicate that in addition to lowering the ionization potential, the presence of the aromatic tag i
106                            With their higher ionization potentials, the helium ions He(2+) and He(+)
107 nforcement of an ansatz that generalizes the ionization potential theorem to the removal of an electr
108 m states of the Ni9Te6 cluster, lowering its ionization potential to 3.39 eV thus creating a superalk
109 olar cells relative to P3HT due to increased ionization potentials was observed.
110 ch reproduce the experimental geometries and ionization potentials well.
111           Their electrochemically determined ionization potentials were only moderately dependent on
112  backbone--due to an increase in the polymer ionization potential--while the short-circuit current de
113 near correlation of the calculated effective ionization potentials with the experimental oxidation po
114  facilitates correlation of these complexes' ionization potentials with their respective activity tow
115 rination leads to an increase in the polymer ionization potential without a significant change in opt

 
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