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15
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0022029557
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The basic electrospray source for mass spectrometry is described by: Whitehouse, C. M.; Dreyer, R. N.; Yamashita, M.; Fenn, J. B. Anal. Chem. 1985, 57, 675.
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16
-
-
16944367144
-
-
Approximate ranges for tube lens potentials are the following: low ≈30-44 V, medium ≈45-60 V, high ≈60-80 V
-
Approximate ranges for tube lens potentials are the following: low ≈30-44 V, medium ≈45-60 V, high ≈60-80 V.
-
-
-
-
17
-
-
16944363361
-
-
note
-
2 could be used.
-
-
-
-
20
-
-
0000992681
-
-
Thermochemical work by mass spectrometric techniques has been done for small organometallic ions. For several examples, see: Halle, L. F.; Armentrout, P. B.; Beauchamp, J. L. Organometallics 1982, 1, 963. Armentrout, P. B.; Halle, L. F.; Beauchamp, J. L. J. Am. Chem. Soc. 1981, 103, 6501. Armentrout, P. B.; Beauchamp, J. L. J. Am. Chem. Soc. 1981, 103, 784. For some more recent work on small complexes, see: Sunderlin, L. S.; Wang, D.; Squires, R. R. J. Am. Chem. Soc. 1993, 115, 12060. Sunderlin, L. S.; Squires, R. R. J. Am. Chem. Soc. 1993, 115, 337.
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Halle, L.F.1
Armentrout, P.B.2
Beauchamp, J.L.3
-
21
-
-
0000674497
-
-
Thermochemical work by mass spectrometric techniques has been done for small organometallic ions. For several examples, see: Halle, L. F.; Armentrout, P. B.; Beauchamp, J. L. Organometallics 1982, 1, 963. Armentrout, P. B.; Halle, L. F.; Beauchamp, J. L. J. Am. Chem. Soc. 1981, 103, 6501. Armentrout, P. B.; Beauchamp, J. L. J. Am. Chem. Soc. 1981, 103, 784. For some more recent work on small complexes, see: Sunderlin, L. S.; Wang, D.; Squires, R. R. J. Am. Chem. Soc. 1993, 115, 12060. Sunderlin, L. S.; Squires, R. R. J. Am. Chem. Soc. 1993, 115, 337.
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Armentrout, P.B.1
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22
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0000338419
-
-
Thermochemical work by mass spectrometric techniques has been done for small organometallic ions. For several examples, see: Halle, L. F.; Armentrout, P. B.; Beauchamp, J. L. Organometallics 1982, 1, 963. Armentrout, P. B.; Halle, L. F.; Beauchamp, J. L. J. Am. Chem. Soc. 1981, 103, 6501. Armentrout, P. B.; Beauchamp, J. L. J. Am. Chem. Soc. 1981, 103, 784. For some more recent work on small complexes, see: Sunderlin, L. S.; Wang, D.; Squires, R. R. J. Am. Chem. Soc. 1993, 115, 12060. Sunderlin, L. S.; Squires, R. R. J. Am. Chem. Soc. 1993, 115, 337.
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Armentrout, P.B.1
Beauchamp, J.L.2
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23
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0001389439
-
-
Thermochemical work by mass spectrometric techniques has been done for small organometallic ions. For several examples, see: Halle, L. F.; Armentrout, P. B.; Beauchamp, J. L. Organometallics 1982, 1, 963. Armentrout, P. B.; Halle, L. F.; Beauchamp, J. L. J. Am. Chem. Soc. 1981, 103, 6501. Armentrout, P. B.; Beauchamp, J. L. J. Am. Chem. Soc. 1981, 103, 784. For some more recent work on small complexes, see: Sunderlin, L. S.; Wang, D.; Squires, R. R. J. Am. Chem. Soc. 1993, 115, 12060. Sunderlin, L. S.; Squires, R. R. J. Am. Chem. Soc. 1993, 115, 337.
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Sunderlin, L.S.1
Wang, D.2
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0001758449
-
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Thermochemical work by mass spectrometric techniques has been done for small organometallic ions. For several examples, see: Halle, L. F.; Armentrout, P. B.; Beauchamp, J. L. Organometallics 1982, 1, 963. Armentrout, P. B.; Halle, L. F.; Beauchamp, J. L. J. Am. Chem. Soc. 1981, 103, 6501. Armentrout, P. B.; Beauchamp, J. L. J. Am. Chem. Soc. 1981, 103, 784. For some more recent work on small complexes, see: Sunderlin, L. S.; Wang, D.; Squires, R. R. J. Am. Chem. Soc. 1993, 115, 12060. Sunderlin, L. S.; Squires, R. R. J. Am. Chem. Soc. 1993, 115, 337.
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Sunderlin, L.S.1
Squires, R.R.2
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25
-
-
16944364829
-
-
note
-
-5 torr (usually argon), as measured by a cold cathode gauge. The interaction region was 18.5 cm long. Typically, thresholds were measured at four different pressures and extrapolated to zero pressure. Even at the highest pressures used, the amount of fragmentation of the parent ions remained below 15%.
-
-
-
-
26
-
-
0001102844
-
-
0 = 1.28 eV (298 K value). The absolute value of the energy scale was determined by stepping the potential of the collision cell, and then fitting the derivative of the resulting retardation curve to a Gaussian function. The maximum of the Gaussian was taken as the absolute zero of the energy scale. It coincided with the potential of the first octopole.
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Anderson, S.G.1
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0001235939
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Dalleska, N. F.; Honma, K.; Armentrout, P. B. J. Am. Chem. Soc. 1993, 775, 12125.
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0004133516
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Gaussian 94 (Revision A.1); M. J. Frisch, G. W. Trucks, H. B. Schlegel, P. M. W. Gill, B. G. Johnson, M. A. Robb, J. R. Cheeseman, T. A. Keith, G. A. Petersson, J. A. Montgomery, K. Raghavachari, M. A. Al-Laham, V. G. Zakrzewski, J. V. Ortiz, J. B. Foresman, J. Cioslowski, B. J. Stefanov, A. Nanyakkara, M. Challacombe, C. Y. Peng, P. Y. Ayala, W. Chen, M. W. Wong, J. L. Andres, E. S. Replogle, R. Gomperts, R. L. Martin, D. J. Fox, J. S. Binkley, D. J. DeFrees, J. Baker, J. P. Stewart, M. HeadGordon, C. Gonzalez, and J. A. Pople; Gaussian, Inc.: Pittsburgh, PA, 1995.
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84986468432
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84986525876
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Jonas, V.; Frenking, G.; Reetz, M. T. J. Comp. Chem. 1992, 13, 919. Jonas, V.; Frenking, G.; Reetz, M. T. J. Comp. Chem. 1992, 13, 935. Veldkamp, A.; Frenking, G. J. Comp. Chem. 1992, 13, 1184.
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Jonas, V.; Frenking, G.; Reetz, M. T. J. Comp. Chem. 1992, 13, 919. Jonas, V.; Frenking, G.; Reetz, M. T. J. Comp. Chem. 1992, 13, 935. Veldkamp, A.; Frenking, G. J. Comp. Chem. 1992, 13, 1184.
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Veldkamp, A.1
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16944365034
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This methodology is described in: Loh, S. K.; Hales, D. A.; Lian, L.; Armentrout, P. B. J. Chem. Phys. 1989, 90, 5467.
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0013498851
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3) (M = Al, Sc) were reoptimized at the CAS(4,4)/LANL1DZ level. Frequencies at this level were then computed and used to guide the estimates for the current system.
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Rappé, A.K.1
Upton, T.H.2
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38
-
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16944365186
-
-
note
-
-1) produced deconvoluted thresholds that differed by much less than the stated ±0.1 eV error bounds.
-
-
-
-
39
-
-
0003466962
-
-
John Wiley: New York
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The internal rotor energy levels were computed from the reduced moments of inertia for rotation of the Cp ligand, the trimethylphosphine unit as a whole, and the individual methyl groups, using the computed equilibrium geometry of 6. See: Berry, R. S.; Rice, S. A.; Ross, J. Physical Chemistry, 1st ed.; John Wiley: New York, 1980; p 771. Two methyl rotors, and rotation of the phosphine unit, are lost at the transition state, which accounts for the marked effect on the computed threshold energy.
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Berry, R.S.1
Rice, S.A.2
Ross, J.3
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