Inspired by Aral and Gupta [2], they defined a generalization of q-Baskakov type operators using q-Beta integral and obtained some important approximation properties, which motivates us to introduce the q analogue of this kind of gamma operators.
So here the question is, if we don't know how many features there are, what those features are, then how do we define a nonparametric generalization of this basic model to allow for, essentially, an unbounded number of features.
A projective or affine Klingenberg plane (PK-, AK-plane) is defined as a generalization of ordinary affine and ordinary projective plane (see [3]).
Next, we define ε-BTP, a generalization of the BTP problem that allows for the possibility that VAFs are observed with errors and some VAFs are not observed.
Here we have defined a Dunkl generalization of these modified operators.
The signature of a subsystem is defined to be a generalization of its interface, including the subsystem's explicit ports, locally defined and inherited data stores, as well as scoped gotos/froms.
Gulati et al. [11] defined the generalized ( F, α, ρ, d ) -V-type I function-a generalizatiof of convexity.
On the other hand, note that the generalized weighted quasiarithmetic mean defined in (2.1) is a generalization of the extended means.
The theory used here to define the stress strain relations is a generalization of Biot's theory and has been developed by Santos et al.
If g V 1 denotes the cortical metric in an arbitrary parameterization, its components can be used to define the Laplace Beltrami operator as a generalization of the Laplacian differential operator.
