Janet basis
In mathematics, a Janet basis is a normal form for systems of linear homogeneous partial differential equations (PDEs) that removes the inherent arbitrariness of any such system.  It was introduced in 1920 by Maurice Janet.  It was first called the Janet basis by Fritz Schwarz in 1998.

The left hand sides of such systems of equations may be considered as differential polynomials of a ring, and Janet's normal form as a special basis of the ideal that they generate. By abuse of language, this terminology will be applied both to the original system and the ideal of differential polynomials generated by the left hand sides. A Janet basis is the predecessor of a Gröbner basis introduced by Bruno Buchberger for polynomial ideals. In order to generate a Janet basis for any given system of linear pde's a ranking of its derivatives must be provided; then the corresponding Janet basis is unique. If a system of linear pde's is given in terms of a Janet basis its differential dimension may easily be determined; it is a measure for the degree of indeterminacy of its general solution. In order to generate a Loewy decomposition of a system of linear pde's its Janet basis must be determined first.

Generating a Janet basis 

Any system of linear homogeneous pde's is highly non-unique, e.g. an arbitrary linear combination of its elements may be added to the system without changing its solution set. A priori it is not known whether it has any nontrivial solutions. More generally, the degree of arbitrariness of its general solution is not known, i.e. how many undetermined constants or functions it may contain. These questions were the starting point of Janet's work; he considered systems of linear pde's in any number of dependent and independent variables and generated a normal form for them. Here mainly linear pde's in the plane with the coordinates  and  will be considered; the number of unknown functions is one or two. Most results described here may be generalized in an obvious way to any number of variables or functions.
In order to generate a unique representation for a given system of linear pde's, at first a ranking of its derivatives must be defined.

Definition
A ranking of derivatives is a total ordering such that for any two derivatives ,  and
, and any derivation operator  the relations  and
 are valid.

A derivative  is called higher than  if . The highest
derivative in an equation is called its leading derivative. For the derivatives up to order two of a single function  depending on  and  with  two possible order are
 the  order  and the  order .

Here the usual notation  is used. If the number of functions is higher than one, these orderings have to be generalized appropriately, e.g. the orderings  or  may be applied.
The first basic operation to be applied in generating a Janet basis is the reduction of an equation  w.r.t. another one . In colloquial terms this means the following: Whenever a derivative of  may be
obtained from the leading derivative of  by suitable differentiation, this differentiation is performed and the
result is subtracted from . Reduction w.r.t. a system of pde's means reduction w.r.t. all elements of the system. A system of linear pde's is called autoreduced if all possible reductions have been performed.

The second basic operation for generating a Janet basis is the inclusion  of integrability conditions. They are obtained
as follows: If two equations  and  are such that by suitable differentiations two new equations
may be obtained with like leading derivatives, by cross-multiplication with its leading coefficients and subtraction of the resulting equations a new equation is obtained, it is called an integrability condition. If by reduction w.r.t. the remaining equations of the system it does not vanish it is included as a new equation to the system.

It may be shown that repeating these operations always terminates after a finite number of steps with a unique answer which is called the Janet basis for the input system. Janet has organized them in terms of the following algorithm.

Janet's Algorithm Given a system of linear differential polynomials  , the Janet basis corresponding to  is returned.

 S1: (Autoreduction) Assign 

 S2: (Completion) Assign 

 S3: (Integrability conditions) Find all pairs of leading terms  of  and  of  such that differentiation w.r.t. a nonmultiplier  and multipliers   leads to

and determine the integrability conditions

 S4: (Reduction of integrability conditions). For all  assign 

 S5: (Termination?) If all  are zero return , otherwise make the assignment , reorder  properly and goto S1

Here  is a subalgorithm that returns its argument with all possible reductions performed,  adds certain equations to the system in order to facilitate determining the integrability conditions. To this
end the variables are divides into multipliers and non-multipliers; details may be found in the above references. Upon successful termination a Janet basis for the input system will be returned.

Example 1 Let the system  be given with ordering  and .  Step S1 returns the autoreduced system

 

Steps S3 and S4 generate the integrability condition  and reduces it to , i.e. the Janet basis for the originally given system is  with the trivial solution .

The next example involves two unknown functions  and , both depending on  and .

Example 2 Consider the system

in  ordering. The system is already autoreduced, i.e. step S1 returns it unchanged. Step S3 generates the two integrability conditions

Upon reduction in step S4 they are

In step S5 they are included into the system and the algorithms starts again with step S1 with the extended system. After a few more iterations finally the Janet basis

is obtained. It yields the general solution  with two undetermined constants  and .

Application of Janet bases 

The most important application of a Janet basis is its use for deciding the degree of indeterminacy of a system of linear homogeneous partial differential equations. The answer in the above Example 1 is that the system under consideration allows only the trivial solution. In the second Example 2 a two-dimensional solution space is obtained. In general, the answer may be more involved, there may be infinitely many free constants in the general solution; they may be obtained from the Loewy decomposition of the respective Janet basis. Furthermore, the Janet basis of a module allows to read off a Janet basis for the syzygy module.

Janet's algorithm has been implemented in Maple.

External links 

 www.alltypes.de – Implementation of Janet's basis