of the thesis]
[Comments on this module]
of the thesis]
[Comments on this module]
By comparison of measurements and calculations the missing parameters of the covalent potential curve and the value of H12 can be estimated. Moreover, the suitability of the applied stationary-phase approximation and Landau-Zener theory can be rated at its true value because the ionic potential curve is well known.
a shows the polar differential cross section, defined by
, for the chemi-ionization process of sodium on iodine and calculated by the lowest-order stationary-phase approximation
With the potential parameters and H12 of Table 1 and taking into account a weight factor 1/8, the calculation leads to absolute values of the differential cross section .
|Figure: A08-m5bii1-F1: Polar differential cross section for chemi-ionization (CM
system) at Ei=13.1 eV,
calculated in semi-classical approximation with the potential
parameters of Table A08-m5bi-T1 and the coupling parameters H12=
0.065 eV and Hrot=0 eV.
(a) Differential cross section with complete interference structure, calculated with the lowest-order stationary-phase approximation. The region of the classical rainbow angle cl,rb has been omitted.
(b) Differential cross section calculated with the stationary-phase approximation and uniform rainbow approximation showing separated the long-wavelength interference structures due to a + c ( 065,full curve), b + c ( 65250, full curve) and d + e ( 02300, dashed curve) interferences.
(c) Full bars indicate the measured maxima of the interference structure on the differential cross section due to net-attractive scattering. Dashed bars indicate the maxima due to net-repulsive scattering. The complete measured cross section curve at Er =13.1 eV is given in Fig.
Fig. A08-m5bii1-F1b shows the differential cross section with simplified interference structure. The major part has been calculated by the lowest-order stationary-phase approximation . The rainbow region has been calculated in the uniform approximation . An additional simplification in Fig. A08-m5bii1-F1b is the separate reproduction of the attractive and repulsive scattering contribution as though they could be distinguished.
Because the origin of the oscillatory features of Fig. A08-m5bii1-F1a can be seen easily from Fig. A08-m5bii1-F1b and the latter figure is more easily related to the deflection function and the potential curves, Fig. A08-m5bii1-F1b is more suitable to fit the interference structure of the calculated and measured differential cross section by adjustment of the potential parameters. Moreover, convolution of the differential cross section of Fig. A08-m5bii1-F1 a and Fig. A08-m5bii1-F1 b even with the smallest angular resolution of the detector of 0.3º fwhm will lead to equal results.
|Figure A08-m5bii1-F2: Relative polar differential cross section for chemi-ionization (CM system). The cross sections, measured at a colliding energy of 13.1 and 18.2 eV, have been set in scales with shifted zero points|
|Figure A08-m5bii1-F3: Rainbow structure versus initial colliding energy (CM system). The dashed curves show the calculated positions of the maxima of rainbow and supernumeraries|
The cross sections exhibit Stueckelberg oscillations due to interference of the ionic and covalent repulsive-scattering contributions just beyond the rainbow angle. The corresponding branches of the deflection curve are d and e, where the e-branch is calculated from the known ionic potential.
The Stueckelberg oscillations in the experimental cross sections shown in Fig. A08-m5bii1_F2 for < 65 eV degree are due to the interference of the differential cross-section contributions related to the a and c branches of the deflection curves. The measured maxima of the 13.1 eV curve have been indicated in Fig. A08-m5bii1-F1c together with the calculated structure.
For Stueckelberg oscillations just beyond the rainbow angle, the measured wavelength as a function of the kinetic energy can be fitted perfectly with the calculations.
However, on the range 40 65 obviously the distances between the calculated maxima are too small. The relative wavelength discrepancy is the largest at .
For decreasing scattering angles the measured and calculated oscillation wavelengths increase while the deviation decreases from twenty percent at to zero percent at and ends up in an opposite deviation meaning a calculated wavelength too large compared to the measurements. However, the latter deviation is not precarious because it can be improved by a careful adjustment of the onset of the covalent repulsive potential as can be seen from Fig. A08-m5bi-F4 of the potential and Fig. A08-m5bi-F2 of the deflection function.
More serious is the deviation on the 40 65 range because this part of the differential cross section deals only with scattering from the known ionic potential and the flat part of the covalent potential curve. It is very remarkable that the deviation on this range is the same as the deviation of measured and calculated maxima just on the other side of the minimum in the differential cross section (the range of the high-number supernumeraries). The completely resolved differential cross section curve with Ei=18.2 eV gives the same trend with equal deviations of measured and calculated wavelengths around = 65 eV degree.
Some evidence of repulsive interference at small scattering angles has been indicated also in Fig. A08-m5bii1-F1c. This structure gives a check on the estimated repulsive part of the covalent potential. Because Fig. A08-m5bii1-F1 b clearly shows that at small angles the repulsive oscillation is the straight continuation of the attractive oscillation it is not very surprising that the calculated wavelength is somewhat too large compared to the measurements. The same applies to the 18.2 eV curve.
The general shape of the polar differential cross section is the cross section averaged over the quantal oscillations. This shape will nearly correspond to the classical differential cross section except at the classical rainbow angle, and thus is given by the relevant values of b, and the Landau-Zener transition probability Pb .
|Figure A08-m5bii1-F4: Smoothed differential cross sections for five different collision energies. (a), (b), (c), (d), (e): Full curves show the measured relative differential cross section, averaged over the interference structures. Absolute differential cross sections, calculated semi-classically and also averaged over the interference structure, have been given by the dashed curves. Use has been made of H12=0.05 eV. (f): At Ei=29.7 eV the curves show the calculated differential cross section for H12=0.04, 0.05 and 0.07 eV|
The general shape of the differential cross section has been measured and calculated at collision energies of 13.1, 20.7, 29.7, 38.7 and 55.0 eV, as shown in Figs. A08-m5bii1-F4a, b, c, d, e. The calculated values have been given on absolute scales, the measurements are only relative and have been given for the different energies on arbitrary, non-related scales.
The angular positions of special features agree very well: namely the maximum of the peak at due to covalent scattering, the minimum at due to scattering with maximal impact parameter and the maximum of the primary rainbow.
A permanent local disagreement is observed at the minimum of the differential cross section at , showing that the calculated cross section is too small continuously. The deviation increases at increasing energy. At least the major part cannot be caused by convolution effects on the measurements.
It has been shown that scattering from well-known parts of the internuclear potentials gives rise sometimes to a discrepancy of the calculated and measured interference structure. In spite of that, we have determined the repulsive parameters of the covalent potential curve from the repulsive interference structure.
However, the reliability is enlarged by the very good agreement of the kinetic-energy behaviour of the wavelength , while the disagreement of the interference wavelength on the range 0 150 shows an energy-dependent discrepancy. Perhaps the collisions with large impact parameters cause this discrepancy. The comparable calculated and measured interference structures due to collisions with smaller impact parameters consist of the primary rainbows and low-number supernumeraries that are in very good agreement.
In the preceding we have seen that there are only a few serious deviations of measurements and calculations that cannot be ascribed to measuring faults or doubts as to the correctness of the potentials used. Summarizing, these discrepancies are:
The deviations must be viewed in the light of the used approximations, i.e. in the light of the restrictions of the theoretical methods we used ,the most important of which are:
Comparing figures A08-m4bi1-F1 and A08-m5bii1-F2, we see that the deviations between measurements and calculations occur only near = 65 eV degree, for covalent as well as ionic scattering. The deviations are energy dependent and deal with the oscillation wavelengths and relative intensities. It is very remarkable that the approximations C, D, E, F and G mostly violate the real differential cross sections at the region around = 65.
Those approximations don't change the oscillatory structure but only the relative intensities. Some estimates of corrections to the approximations have been made, especially in view of the influence on the differential cross section at .
A correction to approximation D reduces Pb by passing an incomplete transition region. Because then in our energy range the product Pb(1 - Pb) decreases too, the differential cross section even decreases in the region of interest.
However, a correction to E indeed predicts a somewhat larger value of the differential cross section close to = 65, but there still exists the feature of for .
It is very difficult to introduce a correction to approximation F in the impact-parameter method. It will lead to a collection of deflection curves with the greatest differences of the relative shapes near . Indeed, a summation over the deflection curves never gives a zero value of the differential cross section due to collisions with large impact parameters. However, this averaging effect does not cause an important rise of the cross section on the whole region around = 65.
The remaining corrections to the intensity at are C and G dealing with the Landau-Zener coupling and rotation coupling. It is not expected that the Landau-Zener transition formula gives such wrong results, although this formula has been derived using the approximations that Uion and Ucov are linear in the region of the crossing and H12 is an essentially constant coupling element.
We have greater expectations for the rotation coupling to explain the intensity deviation. Rotational coupling will be treated in more detail in module A08-m5bii2 Quantitative interpretation .
If the rotation coupling is taken into account as well, the only one of the approximations A-G that can give a wrong result for the oscillatory wavelength of the differential cross section at is the lowest-order stationary-phase approximation. Delos and Thorson have given four statements that justify the application of this approximation on two-state collisions. One of them should not be satisfied in our case, namely the requirement of a collisional energy large compared to the potential-energy differences of the two states. This statement requires about equal classical trajectories along the two states. The deflection curves of Fig. A08-m5bi-F2 show that this requirement is not fulfilled.