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This is the topmost object in the hierarchy, and there will be only one of these objects for a simulation. It contains settings controlling details of the calculation, such as the units used. The data files PGOPHER uses (.pgo) thus contain one mixture, with all other objects contained within it, and the name of the mixture will normally be the name of the file. The Mixture object contains one or more Species and Simulation objects and an optional Correlations object.
Note that many or the parameters were moved into the Simulation object in version 5.2.
| Units | Units for calculation of frequencies/energy - valid values
            are cm1 (cm-1), MHz, Kelvin
            and eV. The key change this makes is in
            calculating Boltzmann factors from temperature and for
            selected intensity units; the units are otherwise not
            significant. | 
        
| PrintLevel | Controls the amount of printout in the Log window. Possible values, in
            order of increasing amount of output are:
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| Precision | Precision of printout (decimal places after the point). | 
| BasisOrder | How to order the basis states making up a basis. Valid values are: boDefault, boDiagonal and boStateDiagonal. | 
| QuantumNumberFormat | Controls how quantum numbers are read and displayed.
            Possible values are:
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| FitCycles | Number of least squares fit cycles to do on each press of a "fit" button. | 
| FitDetails | 
          If true, display more
            information following a fit, currently a singular value
            decomposition of the parameters. | 
        
| AutoReplot | If false, automatic recalculation of the simulation is disabled in some circumstances. Use if the program is running slowly. | 
| AllowComplex | If set, calculations will be
            performed using complex wavefunctions if there are matrix
            elements that require it. Otherwise purely imaginary matrix
            elements are multiplied by -i to force them to be real. This often has
            no effect on the calculations, but there are circumstances
            where the calculation is wrong if the matrix elements are
            not allowed to be complex. Circumstances in which it is not
            significant include cases where the factor of -i is simply equivalent
            to a different phase choice for the basis states, or where
            the interaction involved is sufficiently small that second
            order perturbation theory gives a good result, as the energy
            shift essentially depends on the square modulus of the
            matrix element. | 
        
| NoLineList | Disable the use of recorded
            line lists during simulations. This disables some features,
            such as the ability to right click on a line to identify it,
            but allows larger calculations to be performed. For example,
            the maximum J in a
            simple asymmetric top calculation is increased from about
            200 to 500 with this setting. | 
        
| ShowEstUnc | 
          Show estimated uncertainties
            of line positions in the line list
              window and in line lists (use PrintLevel = LineList or Export
            a line list from the File menu). | 
        
| ShowDerivatives | Show derivatives with respect
            to parameters in line lists. | 
        
| SVDlimit | Number of contributions to show for each SVD
            vector; 0 for all. |