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1
-
-
85033841148
-
-
note
-
2H, D, or deuterium. Hydrogen or hydrogenic is used when no isotopic specification is intended.
-
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5
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0001337564
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Sinniah, K.1
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10
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C. C. Cheng, S. R. Lucas, H. Gutleben, W. J. Choyke, and J. T. Yates, Jr., J. Am. Chem. Soc. 114, 1249 (1992); Surf. Sci. 273, L441 (1992).
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Cheng, C.C.1
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11
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13
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0011652482
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W. R. Gentry, in Atomic and Molecular Beam Methods, edited by G. Scoles (Oxford University Press, Oxford, 1988), Vol. 1, p. 54.
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Gentry, W.R.1
-
14
-
-
85033837221
-
-
note
-
This precursor pulse composition is an effective compromise over a neat HI expansion and an expansion of HI in high dilution in a light carrier gas. The former case would provide the highest H atom yield/pulse, while the later case would provide both high terminal jet velocity, which is necessary to exclude cofragmenl I atoms from striking the crystal, and the dominant presence of a collision partner for H atoms of similar mass, thereby best equalizing angular and energy relaxation probabilities.
-
-
-
-
15
-
-
0003413619
-
-
2/HI mole fraction of a "new" lecture bottle and one that was stored at room temperature for about one year
-
2/HI mole fraction of a "new" lecture bottle and one that was stored at room temperature for about one year.
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Downs, A.J.1
Adams, C.J.2
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16
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85033855260
-
-
note
-
All uncertainties derived from statistical methods represent one standard deviation.
-
-
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18
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0003158036
-
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edited by G. Scoles Oxford University Press, Oxford
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D. R. Miller, in Atomic and Molecular Beam Methods, edited by G. Scoles (Oxford University Press, Oxford, 1988), p. 14.
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Miller, D.R.1
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19
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0026414417
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21
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5244317082
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Z. H. Lu, K. Griffiths, P. R. Norton, and T. K. Sham, Phys. Rev. Lett. 68, 1343 (1992); D. T. Jiang, G. W. Anderson, K. Griffiths, T. K. Sham, and P. R. Norton, Phys. Rev. B 48, 4952 (1993); and references therein.
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0000096491
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and references therein
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0000654363
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25
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0020813101
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0001999815
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29
-
-
85033839032
-
-
note
-
Asymmetry parameters β reported for the photolysis of HI in Ref. 25 are multiplied by a factor of 2 throughout this manuscript, conforming to the expression of I(Θ) given in Ref. 26.
-
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31
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0001503553
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A. Garcia-Vela, R. B. Gerber, and J. J. Valentini, J. Chem. Phys. 97, 3297 (1992); A. Garcia-Vela and R. B. Gerber, ibid. 98, 427 (1993).
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A. Garcia-Vela, R. B. Gerber, and J. J. Valentini, J. Chem. Phys. 97, 3297 (1992); A. Garcia-Vela and R. B. Gerber, ibid. 98, 427 (1993).
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Moore, W.J.1
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37
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85033861161
-
-
note
-
0 would be the valve throughput minus that (unknown) fraction which is not reflected from the pump on the first-pass interaction of the pulse.
-
-
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38
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0003420784
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Physical Electronics Industries, Inc., Edina, MN
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42
-
-
85033866260
-
-
note
-
39While the D atom exposure for the as-prepared surface is in the saturation regime, thereby implying preparation of a 1.0 ML monodeuteride adlayer (see Sec. III A), the observation of a 10%-15% hydrogen coverage increase with hyperthermal H atom exposure may suggest that the monolayer on the as-prepared surface is not complete. A decrease in the assumed as-prepared coverage of 10%-15% would result in a nominally 10%-15% decrease in the calculated value of the absolute D atom depletion probability; this level of uncertainty is insignificant given the statistical uncertainty associated with the D atom depletion probability.
-
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46
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