-
2
-
-
77955411768
-
-
M. Brouard, C. Vallance, Eds. Royal Society of Chemistry, Cambridge, chap. 5
-
D. W. Chandler, S. Stolte, in Tutorials in Molecular Reaction Dynamics, M. Brouard, C. Vallance, Eds. (Royal Society of Chemistry, Cambridge, 2010), chap. 5.
-
(2010)
Tutorials in Molecular Reaction Dynamics
-
-
Chandler, D.W.1
Stolte, S.2
-
3
-
-
0000857160
-
-
S. Weinreb, A. H. Barrett, M. L. Meeks, J. C. Henry, Nature 200, 829 (1963).
-
(1963)
Nature
, vol.200
, pp. 829
-
-
Weinreb, S.1
Barrett, A.H.2
Meeks, M.L.3
Henry, J.C.4
-
5
-
-
0000469094
-
-
S. Stolte, Nature 353, 391 (1991).
-
(1991)
Nature
, vol.353
, pp. 391
-
-
Stolte, S.1
-
6
-
-
34547428373
-
-
D. Watanabe, H. Ohoyama, T. Matsumura, T. Kasai, Phys. Rev. Lett. 99, 043201 (2007).
-
(2007)
Phys. Rev. Lett.
, vol.99
, pp. 043201
-
-
Watanabe, D.1
Ohoyama, H.2
Matsumura, T.3
Kasai, T.4
-
7
-
-
0035860549
-
-
K. T. Lorenz et al., Science 293, 2063 (2001).
-
(2001)
Science
, vol.293
, pp. 2063
-
-
Lorenz, K.T.1
-
11
-
-
84862851260
-
-
S. Y. T. van de Meerakker, H. L. Bethlem, N. Vanhaecke, G. Meijer, Chem. Rev. 112, 4828 (2012).
-
(2012)
Chem. Rev.
, vol.112
, pp. 4828
-
-
Van De Meerakker, S.Y.T.1
Bethlem, H.L.2
Vanhaecke, N.3
Meijer, G.4
-
12
-
-
33748789342
-
-
J. J. Gilijamse, S. Hoekstra, S. Y. T. van de Meerakker, G. C. Groenenboom, G. Meijer, Science 313, 1617 (2006).
-
(2006)
Science
, vol.313
, pp. 1617
-
-
Gilijamse, J.J.1
Hoekstra, S.2
Van De Meerakker, S.Y.T.3
Groenenboom, G.C.4
Meijer, G.5
-
14
-
-
80054039419
-
-
P. Hartogh et al., Nature 478, 218 (2011).
-
(2011)
Nature
, vol.478
, pp. 218
-
-
Hartogh, P.1
-
22
-
-
84871013209
-
-
note
-
The labels X2P3/2, X2P1/2, v, and j indicate the electronic states, the vibrational state, and the rotational state of both the OH and the NO radical, respectively. The spectroscopic symmetry labels e and f refer to the total parity of the electronic wave function, exclusive of rotation. The total inversion parity is indicated by the additional labels + and -.
-
-
-
-
24
-
-
0000885312
-
-
M. T. Vonk, J. A. Bacon, C. F. Giese, W. R. Gentry, J. Chem. Phys. 106, 1353 (1997).
-
(1997)
J. Chem. Phys.
, vol.106
, pp. 1353
-
-
Vonk, M.T.1
Bacon, J.A.2
Giese, C.F.3
Gentry, W.R.4
-
25
-
-
0001326504
-
-
P. Sharkey, I. R. Sims, I. W. M. Smith, P. Bocherel, B. R. Rowe, J. Chem. Soc. Faraday Trans. 90, 3609 (1994).
-
(1994)
J. Chem. Soc. Faraday Trans.
, vol.90
, pp. 3609
-
-
Sharkey, P.1
Sims, I.R.2
Smith, I.W.M.3
Bocherel, P.4
Rowe, B.R.5
-
26
-
-
2142803437
-
-
Materials and methods are available as supplementary materials on
-
Materials and methods are available as supplementary materials on Science Online.
-
Science Online
-
-
-
27
-
-
61549137017
-
-
L. Scharfenberg, H. Haak, G. Meijer, S. Y. T. van de Meerakker, Phys. Rev. A 79, 023410 (2009).
-
(2009)
Phys. Rev. A
, vol.79
, pp. 023410
-
-
Scharfenberg, L.1
Haak, H.2
Meijer, G.3
Van De Meerakker, S.Y.T.4
-
28
-
-
84870994492
-
-
note
-
It was verified that all scattered molecules are detected with equal probability, and no density-to-flux correction was needed to relate the measured scattering signals to relative inelastic cross sections. See supplementary materials for more information.
-
-
-
-
31
-
-
0032375659
-
-
M. T. Nguyen, R. Sumathi, D. Sengupta, J. Peeters, Chem. Phys. 230, 1 (1998).
-
(1998)
Chem. Phys.
, vol.230
, pp. 1
-
-
Nguyen, M.T.1
Sumathi, R.2
Sengupta, D.3
Peeters, J.4
-
32
-
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84870978251
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note
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The OH-NO spin states with S = 0 and S = 1 are not distinguished in our model; the 4 x 4 matrices for each spin state are therefore identical.
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33
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84870999265
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note
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Although the quadrupole moment vanishes in the j = 1/2 state of NO, the quadrupole moment in the molecular frame contributes to the collisions producing NO states with j = 3/2 and 5/2 that yield important contributions to the measured cross sections.
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