-
1
-
-
0028141903
-
-
Aquilanti, V.; Ascenzi, D.; Cappelletti, D.; Pirani, F. Nature 1994, 371, 399.
-
(1994)
Nature
, vol.371
, pp. 399
-
-
Aquilanti, V.1
Ascenzi, D.2
Cappelletti, D.3
Pirani, F.4
-
2
-
-
33751155506
-
-
Aquilanti, V.; Ascenzi, D.; Cappelletti, D.; Pirani, F. J. Phys. Chem. 1995, 99, 13620.
-
(1995)
J. Phys. Chem.
, vol.99
, pp. 13620
-
-
Aquilanti, V.1
Ascenzi, D.2
Cappelletti, D.3
Pirani, F.4
-
3
-
-
3943076370
-
-
Aquilanti, V.; Ascenzi, D.; Cappelletti, D.; Franceschini, S.; Pirani, F. Phys. ReV. Lett. 1995, 74, 2929.
-
(1995)
Phys. ReV. Lett.
, vol.74
, pp. 2929
-
-
Aquilanti, V.1
Ascenzi, D.2
Cappelletti, D.3
Franceschini, S.4
Pirani, F.5
-
4
-
-
0000061114
-
-
Anthony, E. B.; Schade, W.; Bastian, M. J.; Bierbaum, V. M.; Leone, S. R. J. Chem. Phys. 1997, 106, 5413.
-
(1997)
J. Chem. Phys.
, vol.106
, pp. 5413
-
-
Anthony, E.B.1
Schade, W.2
Bastian, M.J.3
Bierbaum, V.M.4
Leone, S.R.5
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7
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84866772445
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Note that values of the degree of alignment reported in Table 2 of ref 2 must be considered as the average of several measurements performed under slightly different experimental conditions, while the weights W(J,mJ) reported in Table 1 of the same paper refer to one sample set of data and are not sufficient to fully reconstruct results in Table 2.
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Note that values of the degree of alignment reported in Table 2 of ref 2 must be considered as the average of several measurements performed under slightly different experimental conditions, while the weights W(J,mJ) reported in Table 1 of the same paper refer to one sample set of data and are not sufficient to fully reconstruct results in Table 2.
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8
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84866749912
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Aquilanti, V.; Ascenzi, D.; Cappelletti, D.; De Castro, M.; Pirani, F. J. Chem. Phys. 1998, 109, 3839.
-
(1998)
J. Chem. Phys.
, vol.109
, pp. 3839
-
-
Aquilanti, V.1
Ascenzi, D.2
Cappelletti, D.3
De Castro, M.4
Pirani, F.5
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9
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0000442993
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An example of the important role of this coupling is given in
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An example of the important role of this coupling is given in: Happer, W.; Miron, E.; Schaefer, S.; Schreiber, D.; van Wijngaarden, W. A.; Zeng, X. Phys. ReV. A 1984, 29, 3092.
-
(1984)
Phys. ReV. A
, vol.29
, pp. 3092
-
-
Happer, W.1
Miron, E.2
Schaefer, S.3
Schreiber, D.4
Van Wijngaarden, W.A.5
Zeng, X.6
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10
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84908642308
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The recoupling of polarized K with S to give J, which occurs also between successive collisions in the expansion, would lead to a natural depolarization effect in the case of unpolarized spin In such conditions the maximum alignment observable for K ) 1 should be even lower with respect to that obtained according to PH.
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The recoupling of polarized K with S to give J, which occurs also between successive collisions in the expansion, would lead to a natural depolarization effect in the case of unpolarized spin (see: Altkorn, R.; Zare, R. N.; Greene, C. H. Mol. Phys. 1985, 55, 1). In such conditions the maximum alignment observable for K ) 1 should be even lower with respect to that obtained according to PH.
-
(1985)
Mol. Phys.
, vol.55
, pp. 1
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Altkorn, R.1
Zare, R.N.2
Greene, C.H.3
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11
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0031561416
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In this paper anisotropy effects for the N2-Xe system on the value of the cross section and on the position of "glory" extrema have been measured. The observed effects are of the same magnitude as in a pioneering work on the scattering of NO, state selected by a hexapolar field and oriented by means of a magnetic field
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Aquilanti, V.; Ascenzi, D.; Cappelletti, D.; Fedeli, R.; Pirani, F. J. Phys. Chem. A 1997, 101, 7648. In this paper anisotropy effects for the N2-Xe system on the value of the cross section and on the position of "glory" extrema have been measured. The observed effects are of the same magnitude as in a pioneering work on the scattering of NO, state selected by a hexapolar field and oriented by means of a magnetic field
-
(1997)
J. Phys. Chem. A
, vol.101
, pp. 7648
-
-
Aquilanti, V.1
Ascenzi, D.2
Cappelletti, D.3
Fedeli, R.4
Pirani, F.5
-
13
-
-
36749109960
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-
Sinha, M. P.; Caldwell, C. D.; Zare, R. N. J. Chem. Phys. 1975, 61, 491.
-
(1975)
J. Chem. Phys.
, vol.61
, pp. 491
-
-
Sinha, M.P.1
Caldwell, C.D.2
Zare, R.N.3
-
14
-
-
0000906475
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Visser, A. G.; Bekooy, J. P.; van der Meij, L. K.; de Vreugd, C.; Korving, J. Chem. Phys. 1977, 20, 391.
-
(1977)
J. Chem. Phys.
, vol.20
, pp. 391
-
-
Visser, A.G.1
Bekooy, J.P.2
Van Der Meij, L.K.3
De Vreugd, C.4
Korving5
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15
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-
0000910220
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Hefter, U.; Ziegler, G.; Mattheus, A.; Fischer, A.; Bergmann, K. J. Chem. Phys. 1986, 85, 286.
-
(1986)
J. Chem. Phys.
, vol.85
, pp. 286
-
-
Hefter, U.1
Ziegler, G.2
Mattheus, A.3
Fischer, A.4
Bergmann, K.5
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16
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84866763362
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Pullman, D. P.; Friedrich, B.; Herschbach, D. R. J. Chem. Phys. 1990, 93, 322.
-
(1990)
J. Chem. Phys.
, vol.93
, pp. 322
-
-
Pullman, D.P.1
Friedrich, B.2
Herschbach, D.R.3
-
17
-
-
33751500080
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-
Friedrich, B.; Pullman, D. P.; Herschbach, D. R. J. Phys. Chem. 1991, 95, 8118.
-
(1991)
J. Phys. Chem.
, vol.95
, pp. 8118
-
-
Friedrich, B.1
Pullman, D.P.2
Herschbach, D.R.3
-
19
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-
0001499799
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-
Saleh, H. J.; McCaffery, A. J. J. Chem. Soc., Faraday Trans. 1993, 89, 3217.
-
(1993)
J. Chem. Soc., Faraday Trans.
, vol.89
, pp. 3217
-
-
Saleh, H.J.1
McCaffery, A.J.2
-
20
-
-
0000253382
-
-
Pullman, D. P.; Friedrich, B.; Herschbach, D. R. J. Phys. Chem. 1995, 99, 7407.
-
(1995)
J. Phys. Chem.
, vol.99
, pp. 7407
-
-
Pullman, D.P.1
Friedrich, B.2
Herschbach, D.R.3
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21
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84866749913
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Simple models based on classical mechanics cannot be exhaustive in the comprehensive of a phenomenon where the rotational relaxation plays such a dominant role
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Simple models based on classical mechanics cannot be exhaustive in the comprehensive of a phenomenon where the rotational relaxation plays such a dominant role.
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22
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36549093372
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Beneventi, L.; Casavecchia, P.; Volpi, G. G. J. Chem. Phys. 1986, 85, 7011.
-
(1986)
J. Chem. Phys.
, vol.85
, pp. 7011
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-
Beneventi, L.1
Casavecchia, P.2
Volpi, G.G.3
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23
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84952278747
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In ref 8 close-coupling quantum-mechanical calculations have been reported supporting the experimentally observed effects for O2-Kr and O2- Xe systems. The same code is used here for the O2-He system in press
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In ref 8 close-coupling quantum-mechanical calculations have been reported supporting the experimentally observed effects for O2-Kr and O2- Xe systems. The same code is used here for the O2-He system. See: Aquilanti, V.; Ascenzi, D.; de Castro Vítores, M.; Pirani, F.; Cappelletti, D. J. Chem. Phys., in press.
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J. Chem. Phys.
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Aquilanti, V.1
Ascenzi, D.2
De Castro Vítores, M.3
Pirani, F.4
Cappelletti, D.5
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24
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84866750079
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The O2 molecules in the beam source exhibit a broad distribution of rotational levels (significantly populated up to K ) 21). The level K ) 5 is among the most populated ones
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The O2 molecules in the beam source exhibit a broad distribution of rotational levels (significantly populated up to K ) 21). The level K ) 5 is among the most populated ones.
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25
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4243839875
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See for instance: Kuebler, N. A.; Robin, M. B.; Yang, J. J.; Gedanken, A.; Herrick, D. R. Phys. ReV. A 1988, 38, 737.
-
(1988)
Phys. ReV. A
, vol.38
, pp. 737
-
-
Kuebler, N.A.1
Robin, M.B.2
Yang, J.J.3
Gedanken, A.4
Herrick, D.R.5
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