“…Present standard are least-squares (χ 2 ) fits started in [108] and steadily extended to include more and more data, for recent examples see, e.g., [100,109]. The least-squares (χ 2 ) fits and subsequent analysis of extrapolation errors as well as correlations are a standard technique and well documented at several places [92,110,111]. The tasks is to optimise a set of model parameters p = (p 1 , ..., p N p ) such that a representative set of observables {Ô i , i = 1...N d } is optimally reproduced.…”
Section: Brief Review Of χ 2 Analysismentioning
confidence: 99%
“…the rescaled version of a parameter p is p rescal = (p − p SV−bas )/∆p SV−min . This implies that the interval of rescaled force parameters [−1, +1] represents the range of reasonable parameters for which the reproduction of data remains nearly as good as for the minimum (χ 2 growing at most by one unit [110,111,92]). …”
Section: Trend Analysis For the Key Observables Of 266 Hsmentioning
This is a short review of methods and results of calculations of fission barriers and fission halflives of even-even superheavy nuclei. An approvable agreement of the following approaches is shown and discussed: The macroscopic-microscopic approach based on the stratagem of the shell correction to the liquid drop model and a vantage point of microscopic energy density functionals of Skyrme and Gogny type selfconsistently calculated within Hartree-Fock-Bogoliubov method. Mass parameters are calculated in the Hartree-Fock-Bogoliubov cranking approximation. A short part of the paper is devoted to the nuclear fission dynamics. We also discuss the predictive power of Skyrme functionals applied to key properties of the fission path of 266 Hs. It applies the standard techniques of error estimates in the framework of a χ 2 analysis.
“…Present standard are least-squares (χ 2 ) fits started in [108] and steadily extended to include more and more data, for recent examples see, e.g., [100,109]. The least-squares (χ 2 ) fits and subsequent analysis of extrapolation errors as well as correlations are a standard technique and well documented at several places [92,110,111]. The tasks is to optimise a set of model parameters p = (p 1 , ..., p N p ) such that a representative set of observables {Ô i , i = 1...N d } is optimally reproduced.…”
Section: Brief Review Of χ 2 Analysismentioning
confidence: 99%
“…the rescaled version of a parameter p is p rescal = (p − p SV−bas )/∆p SV−min . This implies that the interval of rescaled force parameters [−1, +1] represents the range of reasonable parameters for which the reproduction of data remains nearly as good as for the minimum (χ 2 growing at most by one unit [110,111,92]). …”
Section: Trend Analysis For the Key Observables Of 266 Hsmentioning
This is a short review of methods and results of calculations of fission barriers and fission halflives of even-even superheavy nuclei. An approvable agreement of the following approaches is shown and discussed: The macroscopic-microscopic approach based on the stratagem of the shell correction to the liquid drop model and a vantage point of microscopic energy density functionals of Skyrme and Gogny type selfconsistently calculated within Hartree-Fock-Bogoliubov method. Mass parameters are calculated in the Hartree-Fock-Bogoliubov cranking approximation. A short part of the paper is devoted to the nuclear fission dynamics. We also discuss the predictive power of Skyrme functionals applied to key properties of the fission path of 266 Hs. It applies the standard techniques of error estimates in the framework of a χ 2 analysis.
“…The major and minor principal axes components of the diffusivity tensor k• and k2, k• -> k 2, respectively, can be calculated using [Brandt, 1976] k with the regular axes estimates kxx and kyy. We suggest that the minor principal axes estimates k 2 and k* 2 are the most reliable estimates of the eddy diffusivity that can be extracted from drifter data.…”
“…In the continuous approximation, such sequence of quantum unitary operations leads to the output state |ψ (θ) in (30). Such quantum mechanical wave-vector is such that its Fisher information function F (θ) [39] is independent of the parameter θ (it is a constant quantity),…”
Section: B Grover's Information Geometric Dynamicsmentioning
We present an information geometric characterization of Grover's quantum search algorithm. First, we quantify the notion of quantum distinguishability between parametric density operators by means of the Wigner-Yanase quantum information metric. We then show that the quantum searching problem can be recast in an information geometric framework where Grover's dynamics is characterized by a geodesic on the manifold of the parametric density operators of pure quantum states constructed from the continuous approximation of the parametric quantum output state in Grover's algorithm. We also discuss possible deviations from Grover's algorithm within this quantum information geometric setting.
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