Absolute cross-section measurements in XQQ instruments: Ar+ + N2 → Ar + N+2
暂无分享,去创建一个
[1] J. Vine,et al. Quantification of leukotriene B4 in synovial fluid by gas chromatography/tandem mass spectrometry. , 1988, Biomedical & environmental mass spectrometry.
[2] R. Boyd,et al. Reaction-induced mass discrimination in XQQ instruments. Absolute cross-sections for N2+˙ + SF6 → N2 + SFx+ (x=1-5) , 1988 .
[3] G. Parlant,et al. Theoretical state‐to‐state inelastic cross sections for collisions of Ar+(2P3/2, 2P1/2) with N2 , 1988 .
[4] R. Boyd,et al. Instrument‐independent tandem mass spectrometry database for XQQ instruments: The dynamical prerequisites , 1988 .
[5] R. Boyd,et al. A comparison of three experimental techniques for ion structure studies via collision‐induced reactions: The [C5H8]+˙ example , 1987 .
[6] R. Martinez. The NBS triple quadrupole tandem mass spectrometer , 1987 .
[7] G. Parlant,et al. Theoretical state‐to‐state charge transfer cross sections for collisions of Ar+ (2P3/2, 2P1/2) with N2 , 1987 .
[8] R. Martinez,et al. Validation of absolute target thickness calibrations in a QQQ instrument by measuring absolute total cross-sections of Ne+ (Ne, Ne) Ne+ , 1986 .
[9] J. Shao,et al. Absolute spin-orbit-state excitation cross sections for the reactions Ar+(2 P32) + Ar(1S0) and Ar+(2P32) + N2 (X, v = 0) , 1986 .
[10] M. Gross,et al. Structures of gas phase C5H8 radical cations: A collisional ionization study , 1986 .
[11] J. Shao,et al. A state‐to‐state study of the electron transfer reactions Ar+(2P3/2,1/2)+N2(X̃,v=0)→Ar(1S0) +N+2(X̃,v’) , 1986 .
[12] P. Dawson,et al. Dissociation of the benzene ion by low energy collisions , 1986 .
[13] C. Ng,et al. Fine structure effect on the charge transfer reaction of Ar+(2P3/2,1/2)+N2 (X̃ 1Σ+g, v=0) , 1986 .
[14] J. Beynon,et al. Collision-induced dissociations of ions from zero to 4 keV translational energy in a single apparatus , 1985 .
[15] C. Ng,et al. A state‐to‐state study of the symmetric charge transfer reaction Ar+(2P3/2,1/2)+Ar(1S0) , 1985 .
[16] R. Hyland,et al. Zero stability and calibration results for a group of capacitance diaphragm gages , 1985 .
[17] J. Sullivan. Development of variable capacitance pressure transducers for vacuum applications , 1985 .
[18] E. Gislason,et al. Theoretical state-to-state cross sections for the Ar++ N2 ⇌ Ar + N2+ system , 1985 .
[19] S. Leone,et al. Laser-induced fluorescence measurement of nascent vibrational and rotational product state distributions in the charge transfer of Ar++N2→Ar+N+2 (v=0,1) at 0.2 eV , 1984 .
[20] P. F. Knewstubb,et al. Integral cross-section measurement for rare gas ion/atom collisions , 1984 .
[21] M. Hamdan,et al. Energy dependence of the reactions of Ar+·(2P12) and Ar+·(2P32) with N2 , 1984 .
[22] J. Futrell,et al. A crossed beam study of the charge‐transfer reaction of Ar+ with N2 at low and intermediate energies , 1984 .
[23] P. Dawson,et al. A round robin on the reproducibility of standard operating conditions for the acquisition of library MS/MS spectra using triple quadrupoles , 1984 .
[24] R. Cooks,et al. Gas-phase thermochemical information from triple quadrupole mass spectrometers: Relative proton affinities of amines , 1983 .
[25] P. Dawson. A study of the collision-induced dissociation of C2H5OH2+ using various target gases , 1983 .
[26] D. J. Douglas,et al. Studies of the mechanism of collision induced dissociation at low energies using a triple quadrupole , 1983 .
[27] D. J. Douglas,et al. The role of kinetic energy in triple quadrupole collision induced dissociation (CID) experiments , 1983 .
[28] P. Dawson,et al. Comparison of low-energy collisionally induced dissociation of n-butyl benzene ions with photodissociation , 1982 .
[29] P. Dawson. The collision-induced dissociation of protonated water clusters studied using a triple quadrupole , 1982 .
[30] Ken'ichiro Tanaka,et al. State selected ion–molecule reactions by a TESICO technique. IV. Relative importance of the two spin‐orbit states of Ar+ in the charge transfer reactions with N2 and CO , 1982 .
[31] W. Lindinger,et al. Energy dependencies of the reactions of Ar+ with H2, N2, CO, O2, CO2, N2O, and COS , 1982 .
[32] D. J. Douglas,et al. The use of triple quadrupoles for sequential mass spectrometry: 2—A detailed case study , 1982 .
[33] P. Dawson,et al. The effective containment of parent ions and daughter ions in triple quadrupoles used for collisional dissociation , 1982 .
[34] R. Cooks,et al. Relative gas-phase acidities from triple quadrupole mass spectrometers , 1982 .
[35] D. J. Douglas. Mechanism of the collision-induced dissociation of polyatomic ions studied by triple quadrupole mass spectrometry , 1982 .
[36] N. Kobayashi,et al. Fine-Structure Transitions in Ar + ( 2 P j )+Ar( 1 S 0 ) Collisions in the Energy Range 60 eV–1500 eV , 1981 .
[37] T. Matsuo,et al. Study of Low Energy Charge Transfer Reactions of Metastable Ar Ions with Ar, Kr and Xe Atoms by Time-of-Flight Technique , 1981 .
[38] H. Villinger,et al. Charge transfer of Ar + + N 2 ⇄ N 2 + + Ar at near thermal energies , 1981 .
[39] N. Adams,et al. Charge-transfer reaction Ar + + N 2 ⇄N + 2 + Ar at thermal energies , 1981 .
[40] R. Browning,et al. Symmetric charge transfer in argon, krypton and xenon: the effect of spin-orbit coupling studied using photoelectron-photoion coincidence spectroscopy , 1981 .
[41] T. Märk,et al. Molecular ion formation in decaying plasmas produced in pure argon and krypton , 1981 .
[42] T. Matsuo,et al. Study of Low Energy Charge Transfer Reactions of Metastable Argon Ions with Argon Atoms by Time-of-Flight Technique , 1980 .
[43] W. E. Falconer,et al. Fine-structure transitions during charge transfer in argon , 1980 .
[44] P. Dawson. Ion Optical Properties of Quadrupole Mass Filters , 1980 .
[45] P. Dawson. Energetics of ions in quadrupole fields , 1976 .
[46] K. Kadota,et al. Neutralization Method for Detection of Metastable Ions and Its Application to the Production of Metastable Rare Gas Ions by Electron Impact , 1975 .
[47] W. E. Falconer,et al. Crossed‐molecular‐beam study of the kinematics and dynamics of charge‐transfer collisions , 1974 .
[48] N. Hishinuma. Relative Charge Transfer Efficiencies of 2 P 3/2 and 2 P 1/2 Rare-Gas Ions in Their Own Gases , 1972 .
[49] K. Birkinshaw,et al. Inelastic collisions between atomic ions and diatomic molecules , 1971 .
[50] T. F. Moran,et al. Application of the Statistical Phase‐Space Theory to the Reactions of Rare‐Gas Ions with Nitrogen Molecules , 1971 .
[51] J. Paulson,et al. Study of ion—neutral reactions with a time-of-flight double mass spectrometer☆ , 1970 .
[52] F. Fehsenfeld,et al. Temperature Dependences of the Rate Coefficients for the Reactions of Ar+ with O2, H2, and D2 , 1970 .
[53] I. Kanomata,et al. Low Energy Ion-Neutral Reactions. I. 22Ne++20Ne, and Ar++N2 , 1969 .
[54] P. P. Ong,et al. Drift measurements of ion-molecule reactions , 1969 .
[55] F. Fehsenfeld,et al. Thermal‐Energy Ion—Neutral Reaction Rates. VI. Some Ar+ Charge‐Transfer Reactions , 1966 .
[56] R. Lehrle,et al. Ion-molecule reactions in the gas phase. Change transfer studied at translational energies up to 2000 eV , 1966 .
[57] R. Amme,et al. Ion‐Beam Excitation Effects on the Single Charge Transfer between Argon and Nitrogen , 1965 .
[58] H. D. Hagstrum. Detection of Metastable Atoms and Ions , 1960 .
[59] W. F. Sheridan,et al. Experimental Determinations of Charge Transfer Cross Sections and Secondary Electron Emission by Ion Bombardment , 1957 .