1 Introduction
Ordinary linear differential equations allow easy access to the singularities of their solutions: every point which is a singularity of some solution of the differential equation must be a zero of the coefficient of the highest order derivative appearing in the equation, or a singularity of one of the other coefficients. For example, is a solution of the equation , and the singularity at is reflected by the root of the polynomial in front of the term in the equation. Unfortunately, the converse is not true: there may be roots of the leading coefficient which do not indicate solutions that are singular there. For example, all the solutions of the equation are constant multiples of , and none of these functions is singular at .
For a differential equation with polynomial coefficients and , the roots of are called the singularities of the equation. Those roots of such that the equation has no solution that is singular at are called apparent. In other words, a root of is apparent if the differential equation admits linearly independent formal power series solutions in . Deciding whether a singularity is apparent is therefore the same as checking whether the equation admits a fundamental system of formal power series solutions at this point. This can be done by inspecting the socalled indicial polynomial of the equation at : if there exists a power series solution of the form , then is a root of this polynomial.
When some singularity of an ODE is apparent, then it is always possible to construct a second ODE whose solution space contains all the solutions of the first ODE, and which does not have as a singularity. This process is called desingularization. The idea is easily explained. The key observation is that a point is a singularity if and only if the indicial polynomial at is different from or the ODE does not admit linearly independent formal power series solutions in . As the indicial polynomial at an apparent singularity has only nonnegative integer roots, we can bring it into the required form by adding a finite number of new factors. Adding a factor to the indicial polynomial amounts to adding a solution of the form to the solution space, and this is an easy thing to do using wellknown arithmetic of differential operators. See [1, 4, 7, 12, 13] for an expanded version of this argument and [1, 2] for analogous algorithms for recurrence equations.
The purpose of the present paper is to generalize the two facts sketched above to the multivariate setting. Instead of an ODE, we consider systems of PDEs known as Dfinite systems. For such systems, we define the notion of a singularity in terms of the polynomials appearing in them (Definition 3.1). We show in Theorem 3.4 that a point is a singularity of the system unless it admits a basis of power series solutions in which the starting terms are as small as possible with respect to some term order. Then a singularity is apparent if the system admits a full basis of power series solutions, the starting terms of which are not as small as possible. We then prove in Theorem 4.6 that apparent singularities can be removed like in the univariate case by adding suitable additional solutions to the system at hand. The resulting system will be contained in the Weyl closure [23] of the original ideal, but unlike Tsai [23] we cannot guarantee that it is equal to the Weyl closure. Based on Theorem 3.4 and Theorem 4.6, we show how to remove a given apparent singularity (Algorithms 5.10 and 5.19), and how to detect whether a given point is an apparent singularity (Algorithm 5.13). At last, we present an algorithm for computing formal power series solutions of a Dfinite system at apparent singularities.
2 Preliminaries
In this section, we recall some notions and conclusions concerning linear partial differential operators, Gröbner bases, formal power series, solution spaces and Wronskians for Dfinite systems. We also specify notation to be used in the rest of this paper.
2.1 Rings of differential operators
Throughout the paper, we assume that is a field of characteristic zero and is a positive integer. For instance, can be the field of complex numbers. Let be the ring of usual commutative polynomials over . The quotient field of is denoted by . Then we have the ring of differential operators with rational function coefficients , in which addition is coefficientwise and multiplication is defined by associativity via the commutation rules

;

,
where is the usual derivative of with respect to , . This ring is an Ore algebra [21, 9] and denoted by for brevity.
Another ring is , which is a subring of . We call it the ring of differential operators with polynomial coefficients or the Weyl algebra [22, Section 1.1].
A left ideal in is called Dfinite if the quotient
is a finite dimensional vector space over
. The dimension of as a vector space over is called the rank of and denoted by .For a subset of , the left ideal generated by is denoted by . For instance, let . Then is Dfinite because the quotient is a vector space of dimension over . Thus, .
2.2 Gröbner bases
Gröbner bases in are well known [15] and implementations for them are available for example in the Maple package Mgfun [8] and in the Mathematica package HolonomicFunctions.m [18]. We briefly summarize some facts about Gröbner bases.
We denote by the commutative monoid generated by . An element of is called a term. For a vector , the symbol stands for the term . The order of is defined to be . For a nonzero operator , the order of is defined to be the highest order of the terms that appear in effectively.
Let ^{1}^{1}1In examples, we use the graded lexicographic ordering with . be a graded monomial ordering [10, Definition 1, page 55] on . Since there is a onetoone correspondence between terms in and elements in , the ordering on induces an ordering on with if . Our main results on apparent singularities are based on the fact that there are at most finitely many terms lower than a given term. So we fix a graded ordering on in the rest of the paper.
For a nonzero element , the head term of , denoted by , is the highest term appearing in . The coefficient of is called the head coefficient of and is denoted by . For a subset of nonzero elements in , and stand for the sets of head terms and head coefficients of the elements in , respectively.
For a Gröbner basis in , a term is said to be parametric if it is not divisible by any term in . The set of exponents of all parametric terms is referred to as the set of parametric exponents of and denoted by . If is Dfinite, then its rank is also called the rank of and denoted by , which is equal to .
2.3 Formal power series
Let be the ring of formal power series with respect to . For and , there is a natural action of on , which is denoted by . For , it is straightforward to verify that
(1) 
For , the product is denoted by , and by . A formal power series can always be written in the form
where . Such a form is convenient for differentiation.
Taking the constant term of a formal power series gives rise to a ring homomorphism, which is denoted by . A direct calculation yields
(2) 
Thus, we can determine whether a formal power series is zero by differentiating and taking constant terms, as stated in the next lemma.
Lemma 2.1.
Let . Then if and only if, for all ,
The following result appears in [11] for . But the proof applies literally also for arbitrary values of . Please see [25, Lemma 4.3.3] for a detailed verification.
Lemma 2.2.
Let and be polynomials in with
If has a power series expansion for each , then the constant term of is nonzero.
The fixed ordering on also induces an ordering on the monoid generated by in the following manner: if . A nonzero element can be written as
where is nonzero. We call the initial exponent of .
2.4 Solutions and Wronskians
Basic facts about solutions of linear partial differential polynomials are presented in [16, Chapter IV, Section 5]. We recall them in terms of Dfinite ideals. The first proposition is a special case of Proposition 2 in [16, page 152].
Proposition 2.3.
For a left ideal with rank , there exists a differential field containing such that the solution space of has dimension over , where stands for the subfield of the constants in .
Such differential fields can also be constructed by the PicardVessiot approach (see, [20, Appendix D] or [6]). In the rest of this paper, we assume that is a differential field described in the above proposition. For a Dfinite ideal , the solution space of in is denoted by . Likewise, for a finiterank Gröbner basis , the solution space of is simply denoted by .
The next proposition is an analog of differential Nullstellensatz for Dfinite ideals. It is an easy consequence of Corollary 1 in [16, page 152].
Proposition 2.4.
Let be a dimensional linear subspace over . Then there exists a unique left ideal of rank such that
Furthermore, an operator belongs to if and only if annihilates every element of .
Linear dependence over constants can be determined by Wronskianlike determinants [16, Chapter II, Theorem 1], which implies that a finite number of elements in are linearly independent over if and only if they are linearly independent over any field of constants that contains .
Wronskianlike determinants are expressed by elements of via wedge notation in [19]. For and , the exterior product
is defined as a multilinear function from to that maps to:
It follows from Theorem 1 in [16, Chapter II] that , …, are linearly independent over if there exist such that
Let be a reduced and finiterank Gröbner basis in the Wronskian operator of is defined to be
The following proposition is Lemma 4 in [19] in slightly different notation.
Proposition 2.5.
Let , and .

The elements are linearly independent over if and only if is nonzero.

Let be the head term of an element of , and let be linearly independent over . Set and
in which the elements of are placed on the righthand side of a product. Then
The two propositions listed above will be used to reconstruct a Gröbner basis from its solutions.
3 Ordinary points and singularities
Let be in the form where and …, are distinct. We say that is primitive if
For brevity, a Gröbner basis in is said to be primitive if it is finite, reduced and its elements are primitive ones in . Every nontrivial left ideal in has a primitive Gröbner basis. The goal of this section is to characterize ordinary points of a primitive Gröbner basis of finite rank in terms of formal power series solutions.
3.1 Ordinary points
Our definitions of singularities and ordinary points are motivated by the material after [22, Lemma 1.4.21].
Definition 3.1.
Assume that is a primitive Gröbner basis of finite rank. A point is called an ordinary point of if, for every , . Otherwise, it is called a singularity of .
The above definitions are compatible with those in the univariate case [1, 7]. Note that the origin is an ordinary point of if and only if each element of has a nonzero constant term.
Example 3.2.
Consider the Gröbner basis in
We find that and . So has no singularity.
Example 3.3.
Consider the Gröbner basis [19, Example 3] in
In this case, and and . The singularities of are
which are two lines in . In particular, the origin is a singularity.
3.2 Characterization of ordinary points
From now on, we focus on formal power series solutions of a primitive Gröbner basis around the origin, as a point in can always be translated to the origin, and we may assume that is algebraically closed when necessary.
Theorem 3.4.
Let be a primitive Gröbner basis of finite rank. Then the origin is an ordinary point of if and only if has many linearly independent formal power series solutions whose initial exponents are exactly those in .
Proof.
Let , and , . Then we can write
Necessity. Assume that the origin is an ordinary point of . Then none of the ’s vanishes at the origin. We show how to construct formal power series solutions of by an approach described in [24].
We associate to each tuple an arbitrary constant . For a nonparametric term , let be its normal form with respect to . Although belongs to , there exists a power product of such that . Write
with . Set
(3) 
Note that can be chosen to be any power product of such that belongs to . Let
We claim that is a formal power series solution of , that is,
(4) 
(5) 
for all and . We proceed by Noetherian induction on the term order .
Starting with , we can write
(6) 
where . It follows that
By (3),
which can be rewritten as
Since is a ring homomorphism, we have
We see that by (6).
Assume that is a term higher than and, for all with and all ,
Reducing modulo , we have
where and are two power products of , and belongs to for all and . Moreover, belongs to . Applying the above equality to , we get
Applying to the above equality yields
By the induction hypothesis, for all with and for all . Thus,
Writing with , we see that the above equality implies
It follows from (3) that
Since is nonzero, is equal to zero. This proves (5). Therefore, our claim (4) holds. Since there are many parametric terms, the Dfinite system has many linearly independent formal power series solutions with initial exponents in .
Sufficiency. Let . Assume that are linearly independently formal power series solutions of whose the initial exponents are , …, , respectively. Without loss of generality, we assume further that, for all ,
where stands for Kronecker’s symbol.
Let . By the above assumption, the constant term of is nonzero. So the formal power series is invertible in .
The proof for the necessity of the above theorem also holds for an arbitrary left (not necessarily Dfinite) ideal , provided that the origin is an ordinary point of . In addition, the above theorem also holds when the fixed ordering is not graded. But the results in the next section hinge on the assumption that is graded.
4 Apparent singularities
The goal of this section is to define apparent singularities of a primitive Gröbner basis of finite rank, and to characterize them.
Definition 4.1.
Let be a primitive Gröbner basis of rank .

Assume that the origin is a singularity of . We call the origin an apparent singularity of if has linearly independent formal power series solutions over .

Assume that is a primitive Gröbner basis of finite rank. We call a left multiple of if
The above definition is compatible with the univariate case [1, Definition 5].
Example 4.2.
The solution space of the Gröbner basis
in is generated by . In this case,
Therefore, the origin is a singularity of . As has two linearly independent formal power series solutions, the origin is an apparent singularity of .
Let be another Gröbner basis such that
We find that is a left multiple of with rank .
Example 4.3.
The solution space of the Gröbner basis
in is generated by . In this case,
Therefore, the origin is an apparent singularity of .
Set
Let be another Gröbner basis with
We find that . By Definition 4.1 (ii), is a left multiple of with .
For a subset of , we denote by the set of initial exponents of nonzero elements in and call it the set of initial exponents of at the origin. Then is the dimension of , because any set of formal power series with distinct initial exponents are linearly independent over . For a primitive Gröbner basis , the origin is an ordinary point of if and only if by Theorem 3.4, it is an apparent singularity if and only if but by Definition 4.1.
Before characterizing apparent singularities, we prove two lemmas. The results in the first lemma are likely known, but we were not able to find proper references containing them.
Lemma 4.4.
Let and be finite ideals in . Then



.
Proof.
Let be a vector space over any field, and let and be two subspaces of . Set
and
It is straightforward to verify that the following sequence is exact^{2}^{2}2We thank Professor Yang Han for bring this exact sequence to our attention, which shortens our original proof..
It follows that is linearly isomorphic to In particular,
Setting , and , we prove the first assertion. The second assertion follows from the first one and Proposition 2.3.
For the last assertion, it is evident that . On the other hand,
Hence, . ∎
As a matter of notation, we define for . The second lemma illustrates a connection between parametric exponents and initial ones.
Lemma 4.5.
Let be a primitive Gröbner basis. Assume that has a basis in and for some . Then . Consequently, the origin is an ordinary point of .
Proof.
Assume that form a basis of and their initial exponents are distinct. Then . Let . And set
Then is a nonzero element in . For every with , let , which belongs to . Then because is nonzero and the ordering is graded. Since annihilates , it vanishes on . It follows from Proposition 2.4 that belongs to the extended ideal , in which is still a Gröbner basis. Thus, can be reduced to zero by . Accordingly, is not a parametric derivative of . In other words, is a subset of . Hence, because and . The origin is an ordinary point by Theorem 3.4. ∎
Theorem 4.6.
Let be a primitive Gröbner basis of rank . Assume that the origin is a singularity of . Then the origin is an apparent singularity of if and only if it is an ordinary point of some left multiple of .
Proof.
Sufficiency. Assume that the origin is an apparent singularity of .
Set For every , we denote by the left ideal generated by …, in . Note that the solution space of is spanned by . Set
Then the two left ideals and have no solution in common except the trivial one because . It follows from Lemma 4.4 (iii) that
In particular, has dimension over , because and have dimensions and , respectively. So . Let be a primitive Gröbner basis of
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