On two aspects of the Painleve analysis

We use the Calogero equation to illustrate the following two aspects of the Painleve analysis of nonlinear PDEs. First, if a nonlinear equation passes the Painleve test for integrability, the singular expansions of its solutions around characteristic hypersurfaces can be neither single-valued functions of independent variables nor single-valued functionals of data. Second, if the truncation of singular expansions of solutions is consistent, the truncation not necessarily leads to the simplest, or elementary, auto-Backlund transformation related to the Lax pair.


Introduction
The Painlevé analysis is a simple and reliable tool for testing the integrability of nonlinear ODEs and PDEs [1,2].Concerning PDEs, there is strong empirical evidence-though no proven theorem as yet-that every nonlinear equation possessing the Painlevé property in formulation for PDEs inevitably belongs either to the class of C-integrable equations (exactly linearizable equations, including Darboux integrable ones) or to the class of S-integrable equations (Lax integrable equations, including Liouville integrable bi-Hamiltonian ones).The Painlevé analysis of nonlinear PDEs is usually performed along the socalled Weiss-Kruskal algorithm, which combines the Weiss' singular expansions of solutions around movable hypersurfaces [3] and the Kruskal's simplifying representation for singularity manifolds [4], and which follows step by step the Ablowitz-Ramani-Segur algorithm for ODEs [5].
The very first step of the Weiss-Kruskal algorithm, however, has no counterpart in the Ablowitz-Ramani-Segur algorithm: starting the Painlevé analysis of a nonlinear PDE, one must determine which of analytic hypersurfaces are characteristic for the tested equation, in order to perform the whole subsequent analysis of solutions around non-characteristic hypersurfaces only.Ward [6] was first who stated and substantiated that the Painlevé property for PDEs must not fix any structure of solutions at characteristic hypersurfaces.Afterward, the essence of Ward's statement was mentioned as "a fact tacitly assumed by all Painlevé practitioners" [1].Lately, however, Weiss [7,8] declared that his result "runs counter to the observation of Ward" and that "expansions about characteristic manifolds are required to be single-valued" as functionals of data.
In the present paper, in Section 2, we show that the Ward's definition of the Painlevé property for PDEs still remains well-founded and that the objections of Weiss are caused by some terminological confusion.We do this via the singularity analysis of the Calogero equation [9,10]: This nonlinear PDE (1) is useful to illustrate one more aspect of the Painlevé analysis.In Section 3, we find two different Bäcklund transformations of the Calogero equation ( 1) into itself: one follows from the truncated singular expansion for u, the other one follows from the Lax pair of (1), and the former turns out to be a special case of the square of the latter.Consequently, the Painlevé analysis does not lead to the simplest, or elementary, auto-Bäcklund transformation of (1), a phenomenon similar to what was observed in [11].
Section 4 contains concluding remarks.

Breaking Solitons and the Painlevé Property
Let us take the fourth-order three-dimensional nonlinear PDE (1) and assume for a while that we know nothing about its integrability and solutions.Does this equation (1) pass the Painlevé test for integrability?The answer will be "yes", if we adopt the Ward's definition [6] of the Painlevé property for PDEs.But the answer will be "no", if we change the definition as proposed by Weiss [7,8].
It is an easy task to perform the Painlevé analysis of (1) along the Weiss-Kruskal algorithm.A hypersurface φ(x, y, t) = 0 is non-characteristic for the PDE (1) if φ 3 x φ y = 0 (see, e.g., [12] for the definition and meaning of noncharacteristic hypersurfaces).The Kruskal's ansatz φ = x + ψ(y, t) with ψ y = 0 both simplifies calculations and excludes characteristic hypersurfaces from consideration.The assumption that the dominant behavior of solutions is algebraic around φ = 0, that is u = u 0 (y, t)φ p + • • • , leads to the only branch to be tested: p = −1 with u 0 = −2.(Branches with p = 0, 1, 2, 3, also admitted by (1), need no analysis: they are governed by the Cauchy-Kovalevskaya theorem [12] because the Kovalevskaya form of the PDE (1) is analytic everywhere.)Then we substitute u = −2φ −1 + • • •+ u r (y, t)φ r−1 + • • • into (1), find that u r is not determined if r = −1, 1, 4, 6 (r = −1 corresponds to the arbitrariness of ψ), and conclude that the tested branch is generic.Finally, we substitute u = ∞ i=0 u i (y, t)φ i−1 into (1), find recursion relations for u i , and check compatibility conditions at the resonances, where the arbitrary functions u 1 , u 4 and u 6 appear.All the compatibility conditions turn out to be identities.Consequently, the PDE (1) has passed the Weiss-Kruskal algorithm well.Since this algorithm is sensitive to algebraic and non-dominant logarithmic singularities only, we can only conjecture that the tested equation possesses the Painlevé property in the sense that all solutions of (1) are single-valued around all non-characteristic hypersurfaces.And we should expect (1) to be integrable.
The PDE (1) is integrable indeed [9,10].It arises as the compatibility con-dition for the over-determined, linear in Φ, system where the spectral parameter α is any function α(y, t) satisfying the equation All solutions of ( 4), except α = constant, are multi-valued functions: for any non-constant initial value α(y, 0), the nonlinear wave α = α(y, t) inevitably breaks (overturns, overlaps) at some finite t [13].Therefore solutions of (1), obtainable by the inverse scattering transform with any non-constant α, are multi-valued functions as well.For example, the one-soliton solution of (1), where λ(y, t), µ(y, t) and β(y, t) are any functions satisfying the equations λ t + 4λ 2 λ y = 0 (λ 2 = −α) and µ t + 4λ 2 µ y = 2λβ y , becomes a multi-valued function when α breaks [14].The N -soliton solution of (1), determined by N solutions α 1 , . . ., α N of (4), breaks whenever any of α 1 , . . ., α N breaks [14].At first sight, such a complicated branching of solutions of (1) seems to be incompatible with the Painlevé property.Nevertheless, there is no contradiction between the fact that solutions of (1) are multi-valued functions and the fact that solutions of (1) are single-valued around all non-characteristic hypersurfaces: solutions can branch and do branch at characteristic hypersurfaces only.Indeed, it was noticed and stressed in [14] that solutions of (1) break (i.e.u y → ∞ at finite values of u) for all values of x simultaneously, the fact meaning that the corresponding singularity manifolds φ = 0 are characteristic for (1), φ x = 0. Consequently, the breaking solitons do not break the Painlevé property in the Ward's formulation [6] because they never break at non-characteristic hypersurfaces.
Let us proceed to the Weiss' objections [7,8] against the Ward's formulation of the Painlevé property for PDEs.The Weiss' counter-example is "the expansion about the characteristic manifold where k = constant.This expansion, however, does not represent solutions around characteristic hypersurfaces: characteristic hypersurfaces for this equation are determined by the condition φ x = 0, not by φ x = 1.Actually, this Taylor expansion represents solutions around any non-characteristic hypersurface φ = 0 in the important case when the Cauchy-Kovalevskaya theorem [12] does not work: in this case we have u x = 0 at φ = 0, whereas the Kovalevskaya form of the equation is singular at u x = 0. We can only agree with Weiss that the consideration of such special Taylor expansions is an essential part of the Painlevé analysis, but the Weiss' words "the expansion about the characteristic manifold " turn out to be too misleading because no actual expansions around characteristic hypersurfaces can be found in the papers [7,8].Now let us return to the Calogero equation (1) and see what really happens at the characteristic hypersurfaces φ(x, y, t) = 0 with φ x φ y = 0. When, for example, φ x = 0 and φ y = 0, we take φ = y + ψ(t) and u = u 0 (x, t)φ p + • • • , p = constant, and find from (1) that any value of p is admissible.Therefore the expansions will not be single-valued functionals of φ for non-integer p.For example, if p = − 1 2 , we get the expansion with the coefficients u i determined by the recursion relations where n = 0, 1, 2, . .., and u i = 0 at i < 0. The structure of ( 7) differs from the habitual structure of recursion relations for non-characteristic hypersurfaces very considerably.There are no resonances in ( 7), but the expansion (6) contains infinitely many arbitrary functions of t in addition to ψ(t): they arise pair by pair as "constants" of integration of ( 7) because ( 7) is a second-order ODE in u n for every n.Namely, , where σ i (t) and τ i (t) are arbitrary functions, i = 0, 1, 2, . ... We see that the expansion ( 6) is multi-valued both as a function of x, y, t (via coefficients u i and non-integer degrees of φ) and as a functional of φ.Consequently, if we accept the Weiss' formulation [7,8] of the Painlevé property, the integrable Calogero equation (1) will not pass the Painlevé test for integrability.Evidently, the Weiss' formulation asks too much of the tested equation.

Two auto-Bäcklund transformations
Let us try to find a Bäcklund transformation of the Calogero equation (1) into itself.Two different methods will lead us to two different transformations.Then we will find a relation between the two results.
First we employ the method of truncated singular expansions of Weiss [15] and the new expansion function χ = (φ −1 φ x − 1 2 φ −1 x φ xx ) −1 of Conte [16] which simplifies computations very considerably (note also that the Kruskal's ansatz is not used for φ in what follows).We substitute u = g(x, y, t)χ −1 + f (x, y, t) into the Calogero equation ( 1) and find that g = −2 and that φ and f must satisfy the following system of four equations: where x φ y , and d = −φ −1 x φ t .Substituting (8) into ( 9), we get s x + 2f xx = 0 which leads to s + 2f x = 2α, where the function α(y, t) appears as a "constant" of integration.Then (8) changes into d − 4αc + 2f y = 0, ( 10) is satisfied identically, and α t = 4αα y follows from (11) (that is why we use the same letter α as for the spectral parameter).Consequently, the system ( 8)-( 11) is equivalent to the system of two equations where α(y, t) is any solution of (4).The truncated expansion is a Miura transformation of the system (12) into the equation ( 1).One more Miura transformation of ( 12) into (1), namely, where v satisfies (1), follows from ( 13) automatically [15,16].This chain of two Miura transformations ( 13) and ( 14) generates an auto-Bäcklund transformation for (1).Indeed, eliminating φ and f from ( 13) and ( 14) by means of ( 12) and differentiations, we get the following system: where w = u − v, z = u + v, and α(y, t) is any solution of (4).Direct but tedious computations prove that the system (15)-( 16) is compatible in v if u satisfies (1), and that the system is compatible in u if v satisfies (1) (i.e. one gets (1) for u when eliminates v from ( 15)-( 16) by differentiations, and vice versa).Therefore, according to the definition [17], the system (15)-( 16) is a Bäcklund transformation of the PDE (1) into itself.It looks strange, however, that the x-part (15) of the obtained Bäcklund transformation is a second-order ODE, whereas the equation ( 2) of the associated linear problem for the PDE (1) is the same as for the potential KdV equation u t = u xxx −3u 2 x .Let us apply the method of Chen [18] to the linear problem (2)-( 3) and find that the PDE (1) does admit one more auto-Bäcklund transformation with the same first-order x-part as for the potential KdV equation.We rewrite (2) as u x = (Φ x /Φ) x + (Φ x /Φ) 2 + α, introduce the new variable ω such that ω x = (Φ x /Φ) 2 + α, and get in this way u = ω ± ε, where ε = (ω x − α) 1/2 .Then (3) gives us the following fourth-order PDE for ω: It is very essential that ( 17) is one and the same equation for both choices of the sign in u = ω ± ε. Owing to this fact, we have two Miura transformations of ( 17) into (1), namely, where u and v are solutions of (1) if ω satisfies (17).Eliminating ω from ( 18), ( 19) and ( 17), we get where w = u − v, z = u + v, and α(y, t) is any solution of (4).One can check that the system (20)-( 21) is compatible in v if u satisfies (1), and vice versa.Therefore the equations ( 20) and ( 21) constitute a Bäcklund transformation of the PDE (1) into itself.
We have shown that the method of truncated singular expansions does not lead to the simplest auto-Bäcklund transformation of the Calogero equation ( 1), related to the equation's Lax pair, and one may only guess that the transformation (20)-( 21) can be derived from the transformation ( 15)-( 16).

Conclusion
In this paper, we used the Calogero equation to illustrate the following two aspects of the Painlevé analysis of nonlinear PDEs.
First, if a nonlinear equation passes the Painlevé test for integrability, the singular expansions of its solutions around characteristic hypersurfaces can be neither single-valued functions of independent variables nor single-valued functionals of data.Of course, if the Painlevé property is considered as an abstract analytic property, one may give any definition of it.However, if the Painlevé property is defined to be used as an indicator of integrability of nonlinear equations, the adequacy of its definition becomes an experimental result.By the singularity analysis of the Calogero equation, we have shown that the Ward's definition of the Painlevé property for PDEs is well founded.
Second, if the truncation of singular expansions of solutions is consistent, the truncation not necessarily leads to the simplest, or elementary, auto-Bäcklund transformation related to the Lax pair.We have found two different Bäcklund transformations of the Calogero equation into itself: one follows from the truncated singular expansion, the other one follows from the Lax pair, and the former turns out to be a special case of the square of the latter.In other words, the way from the truncated singular expansions to Bäcklund transformations and Lax pairs is not so straightforward as it is sometimes stated in the literature.