Non-Noether symmetry of the modified Boussinesq equations

George Chavchanidze
Department of Theoretical Physics,A. Razmadze Institute of Mathematics,1 Aleksidze Street, Tbilisi 0193, Georgia
abstract. We investigate one-parameter non-Noether symmetry group of the modified Boussinesq equationsand show that this symmetry naturally yields infinite sequence of conservation laws.
keywords. Non-Noether symmetry; Conservation laws; Modified Boussinesq system;
msc. 70H33; 70H06; 58J70; 53Z05; 35A30
In Hamiltonian systems, conservation laws are closely related to symmetries of evolutionary equations.In case of modified Boussinesq hierarchy this relationship is especially tight as its entire infinite set of conservation laws forms a single involutive orbit of a simple one-parameter symmetry group. We discuss some geometric properties of this symmetry and show how its properties ensure involutivity of conservation laws.
Recall that the modified Boussinesq system is formed by the following set of partial differential equationsut = cvxx + uxv + uvxvt = − cuxx + uux + kvvxwhere u = u(x, t), v = v(x, t) are smooth functions on 2subjected to zero boundary conditions u(±∞, t) = v(±∞, t) = 0, while c and k are some real constants.In cases k = − 1 and k = 3 modified Boussinesq system has non-trivial bi-Hamiltonian structure that drastically simplifies analysis of the system in these sectors. The first case is described in [2],[5],[6],while in the present paper we focus on the second sector and show that in case k = 3 bi-Hamiltonian structure of modified Boussinesq system is related to non-Noether symmetry [1] of equations (1).Thus in case k = 3 modified Boussinesq equationsut = cvxx + uxv + uvxvt = − cuxx + uux + 3vvxcan be rewritten in bi-Hamiltonian formut = W(dh ∧ du) = Ŵ(dĥ ∧ du)vt = W(dh ∧ dv) = Ŵ(dĥ ∧ dv)where W and Ŵ are compatible Poison bivector fields, i.e.[W , W] = [W , Ŵ] = [Ŵ , Ŵ] = 0defined as followsW = + ∞− ∞ ½(A ∧ Ax + B ∧ Bx)dxŴ = + ∞− ∞ (uB ∧ Ax + vB ∧ Bx − cAx ∧ Bx)dxNote that A, B are vector fields that for every smooth functional R = R(u) are definedvia variational derivatives A(R) = δRδu,          B(R) = δRδv.Corresponding Hamiltonians in bi-Hamiltonian realization (3) are h = ½+ ∞− ∞ (u2v + v3 + 2cuvx)dxĥ = ½+ ∞− ∞ (u2 + v2)dxThis bi-Hamiltonian structure is related to symmetry of equations (2), but before we proceed letus remind that symmetry of evolutionary equations is given by the group of transformations(u , v) ↦ (g(u) , g(v))which commutes with time evolutionddtg(u) = g(ut),          ddtg(v) = g(vt)In case of continuous one-parameter groups of transformation g(u) = ezLE(u) = u + zLEu + ½z2(LE)2u + ⋯g(v) = ezLE(v) = v + zLEv + ½z2(LE)2v + ⋯generated by some vector field E, relation (9) gives rise to the followingconditions for the generator of symmetry EE(u)t = cE(v)xx + E(u)xv + uE(v)x + uxE(v) + E(u)vxE(v)t = − cE(u)xx + uE(u)x + 3vE(v)x + E(u)ux + 3E(v)vxAmong solutions of equations (11) there is one important vector field —the generator of non-Noether symmetry which has the following formE = + ∞− ∞ {[xuv + 2t(u3 + 3uv2 + 6cvvx − 2c2uxx)]Ax − cxvAxx+ (xuux + xvvx)B + [xu2 + 2xv2 + 2t(5v3 + 3u2v − 6cvux − 2c2vxx)]Bx+ cxuBxx}dxApplying one-parameter group of transformations g(z) = ezLEgenerated by the vector field E to the centre of Poisson algebra which in our case is formed by functional J = + ∞− ∞ (ku + mv)dxwhere k, m are arbitrary constants, produces one-parameter family of functionsJ(z) = ezLEJ = J + zLEJ+ ½(zLE)2J + ⋯(actually this is the orbit of non-Noether symmetry group that passes centre of Poisson algebra).It is interesting that the functionals (LE)mJ are in involution.
theorem. The orbit (15) of the non-Noether symmetry group generated by the vector field (12) is involutive{J(x) , J(y)} = 0          ∀x, y ∈ ℝand the functionalsJ(m) = (LE)mJform Lenard scheme with respect to bi-Hamiltonian structure (5)and produce involutive sequence of conservation laws of the modified Boussinesq hierarchy.
proof. The theorem follows from simple geometric properties of the vector field E. In particular taking the Lie derivative of Poisson bivector field W along E one gets the second Poisson bivector involved in bi-Hamiltonian system (5) Ŵ = [E , W]while the Lie derivative of Ŵ along E vanishes [E , Ŵ] = 0These properties ensure that the functionals (17) are in involution (the Poisson bracket of arbitrary two conservation laws from infinite family (17) vanishes){J(k) , J(m)} = 0          k, m = 0, 1, 2 ...Indeed, by applying m-th order Lie derivative (LE)m to the relationW(dJ(0)) = 0 which reflects the fact that J(0) belongs to the centre of Poisson algebra,its easy to prove that the functionals (17) form Lenard scheme W(dJ(m + 1)) = − (1 + m)[E , W](dJ(m))with respect to bi-Hamiltonian system (5)From the other hand it is well known [4] that functionals involved in Lenard scheme arein involution. In the same time calculating the functional J(2) = (LE)2J(0) = m+ ∞− ∞ (u2v + v3 + 2cuvx)dx = 2mHgives rise to Hamiltonian of the modified Boussinesq system and functionals J(m) being in involution with Hamiltonian must be conservation laws.
By calculating Lie derivatives of J(0) along the vector field E one can get explicit form of the conservation laws of the modified Boussinesq system:J(0) = + ∞− ∞ (ku + mv)dxJ(1) = LEJ(0) = m2+ ∞− ∞(u2 + v2)dxJ(2) = (LE)2J(0) = m+ ∞− ∞ (u2v + v3 + 2cuvx)dxJ(3) = (LE)3J(0) = 3m4+ ∞− ∞ (u4 + 5v4 + 6u2v2 − 12cv2ux + 4c2ux2 + 4c2vx2)dxJ(m) = (LE)mJ(0) = LEJ(m − 1)
summary. The fact that the infinite sequence of conservation laws of modified Boussinesq hierarchyform single orbit of the one-parameter non-Noether symmetry group indicates thatnon-Noether symmetries may play an important role in analysis of certain integrablemodels where they drastically simplify calculation of conservation laws and shed more light on geometric origin of integrable hierarchies. Basic results of the paper can be extendedto the case of periodic boundary conditions u(− ∞) = u(+ ∞) and v(− ∞) = v(+ ∞)when the modified Boussinesq equations can be considered as bi-Hamiltonian system on a loop space[4]. Note however that in the periodic case the symmetry (12) does not seem topreserve boundary conditions.
acknowledgements. The research described in this publication was made possible in part byAward No. GEP1-3327-TB-03 of the Georgian Research and Development Foundation (GRDF) and the U.S. Civilian Research & Development Foundation for the Independent States of the Former Soviet Union (CRDF).


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