ライフサイエンスコーパス: ionization energy

1 s suggested by accurately measured adiabatic ionization energies.

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

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

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

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

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

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

8 The observed ionization energies and characters compare very well wit

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

10 The ionization energies and proton affinities correlate line

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

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

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

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

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

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

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

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

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

20 The ionization energies as a function of film thickness give

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

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

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

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

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

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

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

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

29 Ionization energy exhibited by PI, equivalent to 10.8 eV

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

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

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

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

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

35 Lower ionization energies have been exploited leading to organ

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

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

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

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

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

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

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

43 The lowest ionization energies measured by photoelectron spectrosco

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

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

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

47 0.1 eV and further indicated that the lower ionization energies of clusters permitted their detectio

48 The ionization energies of conformationally constrained, new

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

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

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

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

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

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

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

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

57 The first ionization energies of these indoles are natural indole

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

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

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

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

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

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

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

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

66 +/- 2.8 kcal mol(-1)) was combined with the ionization energy of hydrogen (313.6 kcal mol(-1)) to af

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

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

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

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

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

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

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

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

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

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

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

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

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

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

81 The ionization energy trends as a function of the substituti

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

83 The Mg ionization energy was extracted by the phenomenological

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

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