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Rovibrational contributions, nuclear

Fig. 3. Orientationally averaged total stopping cross section St for protons impinging on H2O as a function of proton velocity along with the experimental results of Reynolds et ah (filled circles) [28]. 5 e, and represent the electronic, nuclear, and rovibrational contributions to the stopping, respectively. Fig. 3. Orientationally averaged total stopping cross section St for protons impinging on H2O as a function of proton velocity along with the experimental results of Reynolds et ah (filled circles) [28]. 5 e, and represent the electronic, nuclear, and rovibrational contributions to the stopping, respectively.
Fig. 9. Stopping cross section per atom for proton projectiles colliding with atomic and molecular hydrogen targets as a function of the acceptance angle 0 for projectiles energies of 0.5, 1.5, 5.0, 10.0, and 25.0 keV. Note the nuclear plus rovibrational contributions when large scattering angles are taken into account. Fig. 9. Stopping cross section per atom for proton projectiles colliding with atomic and molecular hydrogen targets as a function of the acceptance angle 0 for projectiles energies of 0.5, 1.5, 5.0, 10.0, and 25.0 keV. Note the nuclear plus rovibrational contributions when large scattering angles are taken into account.
Calculated Rovibrational Contributions, Temperature Corrections, and Nuclear Magnetic Shielding Constants at 300 K [<7(300 K)] in Comparison with Corresponding Shielding Constants Derived from Experimental Spin-Rotation Constants" ... [Pg.401]


See other pages where Rovibrational contributions, nuclear is mentioned: [Pg.302]    [Pg.403]    [Pg.405]    [Pg.55]    [Pg.243]    [Pg.245]    [Pg.253]    [Pg.36]    [Pg.303]    [Pg.204]    [Pg.282]    [Pg.6]    [Pg.69]   


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