ライフサイエンスコーパス: ionization energy

1 hat yield stable cationic fragments (smaller ionization energy).

2 d a localized deep defect state with a large ionization energy.

3 sent very electron-rich compounds with a low ionization energy.

4 s suggested by accurately measured adiabatic ionization energies.

5 compared using both activation and carbon 1s ionization energies.

6 the hpp ligands largely accounts for the low ionization energies.

7 and tryptophan, this approach yields aqueous ionization energies (4.46 and 4.58 eV, respectively) in

8 Adiabatic ionization energies (AIEs) of 1-c-C5H7OO (8.70 +/- 0.05

9 nitio methodology to determine the adiabatic ionization energies (AIEs) of specific gas-phase cytosin

10 ach carbon on the PAH, and (4) average local ionization energy (ALIE) at atom or bond sites.

11 combination of DFT-calculated average local ionization energies (ALIEs), thermodynamics of the produ

12 The observed ionization energies and characters compare very well wit

13 oxidation of various systems using adiabatic ionization energies and electron affinities calculated f

14 fied in the gas phase based on the adiabatic ionization energies and isotopic substitution studies.

15 The ionization energies and proton affinities correlate line

16 A comparison of the ionization energies and proton affinities, together with

17 Substrate magnetization-dependent ionization energies and work function values were deconv

18 elocalized shallow defect state with a small ionization energy and a localized deep defect state with

19 selectivity data by incorporating the clock ionization energy and C-C bond elongation during cation

20 chemical calculations are presented for the ionization energy and cation stability of several alkeny

21 ely photoionized and identified based on the ionization energy and distinct mass-to-charge ratios in

22 , which permit measurement of the molecule's ionization energy and fragmentation onsets.

23 The decrease in ionization energy and increase in electron affinity in t

24 Both the ionization energy and optical band gap are found to foll

25 s from the competition between trends in the ionization energy and the ion-substrate coupling, down t

26 s, and the corresponding changes in vertical ionization energy and vertical electron affinity of the

27 eatures; namely, stoichiometry, ionic radii, ionization energies, and oxidation states for each of th

28 the large difference between Ag(+) and Cu(+) ionization energies ( approximately 1.5 eV), which shoul

29 When uridine and 2'-deoxythymidine ionization energies are evaluated, the results agree wit

30 In aqueous solution, the base and phosphate ionization energies are more similar, and only differ by

31 in 2 dimensions and mass spectra at variable ionization energies are shown to give unparalleled power

32 eV) and calculated (CCSD(T)/pVQZ) adiabatic ionization energies are the same; (2) the origin band ro

33 The ionization energies as a function of film thickness give

34 e NW surface, based on their reduced optical ionization energy as compared with that in bulk.

35 Further, the interplay between first ionization energy, atomic mass, and ionic Lewis acidity

36 s amine-containing fragments with calculated ionization energies below 7.9 eV is attributed mostly to

37 k (1400 < T5 < 1700 K, 3 < P5 < 16 bar) with ionization energies between 10 and 13 eV.

38 Electronic properties such as lower ionization energies built into the single-molecule build

39 y structure dependent, consistent with local ionization energy calculations.

40 A total of 30 ionization energies can be accurately described by an ad

41 ransfer such as the reorganization energies, ionization energies, charge-injection barriers, polariza

42 Both the low ionization energy Co6Te8(PEt3)6 and high electron affini

43 calculating electron trajectory, excitation/ionization energy deposition, elastic scattering energy

44 en the physical properties of a ligand, e.g. ionization energy, dipole moment, and polarizability, an

45 Nucleus-independent chemical shifts (NICS), ionization energies, electron affinities, and PCET energ

46 s centered about the hydrogen donor/acceptor ionization energy epsilon(+/-).

47 Ionization energy exhibited by PI, equivalent to 10.8 eV

48 The carbon 1s ionization energies for all of the carbon atoms in 10 fl

49 The temporal evolution of ionization energies for the excited pipi* state along th

50 frameworks and apply it to obtain the first ionization energy for six prototype materials including

51 ment, are minimized by lowering the electron ionization energy from the usual 70 to 10 eV.

52 resonance energies, proton affinities, core ionization energies, frontier molecular orbitals, atomic

53 Lower ionization energies have been exploited leading to organ

54 ction reaction efficiencies and the vertical ionization energies (IE) of the hydrogen-atom donors, bu

55 nization efficiencies was greatest when high ionization energy (IE) solvent compositions (IEs above 1

56 A'-site cation structure influences the WF, ionization energy (IE), and electron affinity (EA) of n

57 ly the few rare earths with the lowest third ionization energies (IEs) of all elements (<23 eV).

58 previously obtained by fitting experimental ionization energies in isoelectronic series.

59 the quantum confinement in the photoemission ionization energy in air and optical band gap of carbon

60 Substantial lowering of ionization energies is found which is anticipated to hav

61 Thus, soft-ionization energies leading to organic compounds being i

62 dopant with low formation energy and thermal ionization energy leading to p-type conductivity.

63 This was achieved by sublimation of a low ionization energy matrix compound, 1,5-diaminonapthalene

64 The lowest ionization energies measured by photoelectron spectrosco

65 atmospheric aerosols are analyzed and their ionization energies measured with uncertainties of +/-60

66 ee energies of hydration to describe aqueous ionization energies of 2'-deoxythymidine 5'-phosphate (5

67 Adiabatic ionization energies of 7.36 +/- 0.04 and 7.24 +/- 0.04 e

68 0.1 eV and further indicated that the lower ionization energies of clusters permitted their detectio

69 The ionization energies of conformationally constrained, new

70 ative approach for characterizing either the ionization energies of gases or the secondary-electron-e

71 Ionization energies of imipramine, desipramine, amitript

72 Since the photon energy is close to the ionization energies of most organic compounds, fragmenta

73 rained cyclic molecules to reduce the lowest ionization energies of sulfur, selenium, and tellurium c

74 ed on the errors of s- and d-electron second ionization energies of the 3d atoms, that effectively ci

75 In contrast to an earlier report, the ionization energies of the amino acids do not appear to

76 aks on the energy scale is determined by the ionization energies of the analyte molecules.

77 al results provides indirectly the adiabatic ionization energies of the free phosphine ligands, P(CH(

78 tity and is poorly correlated with the third ionization energies of the isolated metals but is well c

79 e substituents have a large influence on the ionization energies of the nitroethylene derivatives.

80 The first ionization energies of these BN heterocycles are in the

81 The first ionization energies of these indoles are natural indole

82 tocols, we accurately determine the vertical ionization energies of valence electrons of both the sol

83 CH(3)OO has been measured, and an adiabatic ionization energy of (10.33 +/- 0.05) eV was determined

84 An ionization energy of 11.61 +/- 0.07 eV between the neutr

85 culations, suggest a state-to-state vertical ionization energy of 11.70 +/- 0.05 eV between the C(3)(

86 e increase of n-type conductivity with donor ionization energy of 20 meV and resistivity of 10(-4) Om

87 reement with the theoretical vertical double ionization energy of 24.41 eV.

88 B fiber was chosen for the extraction and an ionization energy of 30 eV permitted to optimize the ana

89 t3)6 has a closed electronic shell and a low ionization energy of 4.74 eV, and the successive replace

90 ctivity was switched to p-type with acceptor ionization energy of 42 meV by altering hydrogen incorpo

91 issociation limit with the Cp(2)Mn adiabatic ionization energy of 6.12 +/- 0.07 eV.

92 The lowest experimental double ionization energy of [Formula: see text] has been found

93 hotoluminescence spectroscopy revealed an Mg ionization energy of about 100 meV, which agrees quite w

94 s spatially throughout the plasma, up to the ionization energy of argon atoms 15.76 eV.

95 tronic structure calculations determined the ionization energy of Br(2)Y to be ~8.3 +/- 0.1 eV and fu

96 Combined with the ionization energy of BzCr(CO)3, 7.30 +/- 0.05 eV, the th

97 The ionization energy of CpMn(CO)(3) was measured from the t

98 nlikely because the (experimental) adiabatic ionization energy of DMDS is almost 3 eV greater than th

99 display the changes in the work function and ionization energy of GO, supporting the functionalizatio

100 +/- 2.8 kcal mol(-1)) was combined with the ionization energy of hydrogen (313.6 kcal mol(-1)) to af

101 The determined adiabatic ionization energy of m-C8H8 is (7.27 +/- 0.01) eV.

102 e in the range from 8 to 16 eV, based on the ionization energy of nitrogen and the measurements of tu

103 emission temperatures (4,000-15,000 K); the ionization energy of O2 is more than twice its bond diss

104 on affinity of H(+) and the lowered vertical ionization energy of OH(-).

105 cesium atom (which has the lowest gas-phase ionization energy of the elements) or of any other known

106 roscopy, we directly determine the adiabatic ionization energy of the first triplet state of phenyliu

107 ation can be tuned to an energy close to the ionization energy of the sample molecules, thus minimizi

108 r semiconductor electrodes, we find that the ionization energy of the surface dopant can serve as a g

109 a)s is produced by the minimum average local ionization energy on the molecular surface.

110 hich has been determined to have a gas-phase ionization energy (onset, 3.51 electron volts) lower tha

111 ate)4 paddlewheel structures show record low ionization energies (onsets at 3.4 to 3.5 eV) and very n

112 clusters to become electron donors with low ionization energies or electron acceptors with high elec

113 ation of sulphur hexafluoride, SF(6), in the ionization energy range from threshold up to 48.4 eV has

114 These ionization energies reflect substantial (0.53-0.75 eV) o

115 Mass spectra at various ionization energies reveal the qualitative relative abun

116 xyguanosine 5'-monophosphate at a much lower ionization energy than the other three mononucleotides.

117 The results show that the shift to lower ionization energy that is expected with this substitutio

118 Combined with the adiabatic ionization energy, the three successive Mn-CO bond energ

119 The absorbed threshold ionization energy (TIE) and the threshold radiation dose

120 ions show the correlation from the gas-phase ionization energies to the solution redox potentials and

121 The ionization energy trends as a function of the substituti

122 asingly common technique to measure vertical ionization energies (VIEs) of aqueous solutes, but the i

123 n DNA depend on accurate values for vertical ionization energies (VIEs), reorganization energies, and

124 The Mg ionization energy was extracted by the phenomenological

125 y surface hopping calculations, and the core ionization energies were calculated for geometries sampl

126 For selected compounds, ionization energies were determined by gas-phase photoel

127 -dCMP- and 5'-dTMP-, a comparison of aqueous ionization energies with gas-phase ionization potentials