| Up | Next | Prev | PrevTail | Tail | 
  An operator can be declared to be linear in its first argument over powers of its
second argument. If an operator f is so declared, f of any sum is broken up
into sums of fs, and any factors that are not powers of the variable are taken
outside. This means that f must have (at least) two arguments. In addition,
the second argument must be an identifier (or more generally a kernel), not an
expression.
Example:
If F were declared linear, then
                                                                     
                                                                     
f(a*x^5+b*x+c,x) -> 5 f(x ,x)*a + f(x,x)*b + f(1,x)*c
 More precisely, not only will the variable and its powers remain within the scope of the
f operator, but so will any variable and its powers that had been declared to depend on
the prescribed variable; and so would any expression that contains that variable or a
dependent variable on any level, e.g. cos(sin(x)).
To declare operators f and g to be linear operators, use:
                                                                     
                                                                     
linear f,g;
The analysis is done of the first argument with respect to the second; any other arguments are ignored. It uses the following rules of evaluation:
| f(0) | \(\longrightarrow \) | 0 | |
| f(-y,x) | \(\longrightarrow \) | -f(y,x) | |
| f(y+z,x) | \(\longrightarrow \) | f(y,x)+f(z,x) | |
| f(y*z,x) | \(\longrightarrow \) | z*f(y,x) | if z does not depend on x | 
| f(y/z,x) | \(\longrightarrow \) | f(y,x)/z | if z does not depend on x | 
To summarize, y “depends” on the indeterminate x in the above if either of the following
hold:
     
y is  an  expression  that  contains  x at  any  level  as  a  variable,  e.g.,
     cos(sin(x))
     y has been declared dependent on x by use
     of the declaration depend.The use of such linear operators can be seen in the paper [FH74] which contains a complete listing of a program for definite integration of some expressions that arise in fourth order quantum electrodynamics.
| Up | Next | Prev | PrevTail | Front |