Solution 1 to problem over


Expressions | Parameters | Inequalities | Relevance | Back to problem over

Expressions

The solution is given through the following expressions:

r10=0


         1
      - ---*b33*n2*r29
         2
r11=-------------------
         2
      a22  - a22*a33


         1
      - ---*b33*n1*r29
         2
r12=-------------------
         2
      a22  - a22*a33


      - n3*r29
r13=-----------
     a22 - a33


      - n2*r29
r14=-----------
     a22 - a33


      - n1*r29
r15=-----------
     a22 - a33


r20=0


r21=0


r23=0


r24=0


r25=0


r26=0


r27=0


r28=0


r210=0


r212=0


r213=0


r214=0


r215=0


r216=0


r217=0


r218=0


r219=0


     - b33*n3
m3=-----------
    a22 - a33


        1                1
     - ---*a22*b33*n2 - ---*a33*b33*n2
        2                2
m2=------------------------------------
                 2
              a22  - a22*a33


        1                1
     - ---*a22*b33*n1 - ---*a33*b33*n1
        2                2
m1=------------------------------------
                 2
              a22  - a22*a33


         1     2
      - ---*b33
         4
c33=-------------
         a22


c23=0


c22=0


c13=0


c12=0


c11=0


b32=0


b31=0


b23=0


b22=0


b21=0


b13=0


b12=0


b11=0


a23=0


a13=0


a12=0


a11=a22


Parameters

Apart from the condition that they must not vanish to give a non-trivial solution and a non-singular solution with non-vanishing denominators, the following parameters are free:
 r29, n3, n1, b33, n2, a33, a22

Inequalities

In the following not identically vanishing expressions are shown. Any auxiliary variables g00?? are used to express that at least one of their coefficients must not vanish, e.g. g0019*p4 + g0020*p3 means that either p4 or p3 or both are non-vanishing.
 
{a11,a22 - a33,a22,a33,r29}


Relevance for the application:

The new Hamiltonian in form of a list of vanishing expressions: 

{a11 - a22,
a12,
a13,
a23,
b11,
b12,
b13,
b21,
b22,
b23,
b31,
b32,
c11,
c12,
c13,
c22,
c23,
a22*c33 + 1/4*b33**2,
a22**2*m1 - a22*a33*m1 + 1/2*a22*b33*n1 + 1/2*a33*b33*n1,
a22**2*m2 - a22*a33*m2 + 1/2*a22*b33*n2 + 1/2*a33*b33*n2,
a22*m3 - a33*m3 + b33*n3}$

The system of equations related to the Hamiltonian HAM:

      2                 2                 2
HAM=u1 *a22 + u1*n1 + u2 *a22 + u2*n2 + u3 *a33 + u3*v3*b33 + u3*n3

               1                1
            - ---*a22*b33*n1 - ---*a33*b33*n1
               2                2
     + v1*------------------------------------
                        2
                     a22  - a22*a33

               1                1                     1    2    2
            - ---*a22*b33*n2 - ---*a33*b33*n2      - ---*v3 *b33
               2                2                     4
     + v2*------------------------------------ + -----------------
                        2                               a22
                     a22  - a22*a33

         - v3*b33*n3
     + --------------
         a22 - a33

has apart from the Hamiltonian and Casimirs only the following first integral: 

                                2     2                           1
FI= - u1*a22*n1 - u2*a22*n2 + u3 *(a22  - a22*a33) - u3*a22*n3 - ---*v1*b33*n1
                                                                  2

       1
    - ---*v2*b33*n2
       2

which the program can not factorize further.

{HAM,FI} = 0





And again in machine readable form:



HAM=u1**2*a22 + u1*n1 + u2**2*a22 + u2*n2 + u3**2*a33 + u3*v3*b33 + u3*n3 + v1*(
 - 1/2*a22*b33*n1 - 1/2*a33*b33*n1)/(a22**2 - a22*a33) + v2*( - 1/2*a22*b33*n2 -
 1/2*a33*b33*n2)/(a22**2 - a22*a33) + ( - 1/4*v3**2*b33**2)/a22 + ( - v3*b33*n3)
/(a22 - a33)$

FI= - u1*a22*n1 - u2*a22*n2 + u3**2*(a22**2 - a22*a33) - u3*a22*n3 - 1/2*v1*b33*
n1 - 1/2*v2*b33*n2$