Quantum calculus
Quantum calculus, sometimes called calculus without limits, is equivalent to traditional infinitesimal calculus without the notion of limits. The two types of calculus in quantum calculus are q-calculus and h-calculus. The goal of both types is to find "analogs" of mathematical objects, where, after taking a certain limit, the original object is returned. In q-calculus, the limit as q tends to 1 is taken of the q-analog. Likewise, in h-calculus, the limit as h tends to 0 is taken of the h-analog. The parameters and can be related by the formula.
Differentiation
The q-differential and h-differential are defined as:and
respectively. The q-derivative and h-derivative are then defined as
and
respectively. By taking the limit as of the q-derivative or as of the h-derivative, one can obtain the derivative:
Integration
q-integral
A function F is a q-antiderivative of f if DqF = f. The q-antiderivative is denoted by and an expression for F can be found from:, which is called the Jackson integral of f. For, the series converges to a function F on an interval xα| is bounded on the interval for some.The q-integral is a Riemann–Stieltjes integral with respect to a step function having infinitely many points of increase at the points qj..The jump at the point qj is qj. Calling this step function gq gives dgq = dqt.
h-integral
A function F is an h-antiderivative of f if DhF = f. The h-integral is denoted by. If a and b differ by an integer multiple of h then the definite integral is given by a Riemann sum of f on the interval, partitioned into sub-intervals of equal width h. The motivation of h-integral comes from the Riemann sum of f. Following the idea of the motivation of classical integrals, some of the properties of classical integrals hold in h-integral. This notion has broad applications in numerical analysis, and especially finite difference calculus.Example
In infinitesimal calculus, the derivative of the function is . The corresponding expressions in q-calculus and h-calculus are:where is the q-bracket
and
respectively. The expression is then the q-analog and is the h-analog of the power rule for positive integral powers. The q-Taylor expansion allows for the definition of q-analogs of all of the usual functions, such as the sine function, whose q-derivative is the q-analog of cosine.