Solution 1 to problem over
Expressions |
Parameters |
Inequalities |
Relevance |
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Expressions
The solution is given through the following expressions:
r10=0
1
- ---*m2*n3*r333
4
r11=-------------------
2
a22
1
- ---*m1*n3*r333
4
r12=-------------------
2
a22
1 2
- ---*n3 *r333
4
r13=-----------------
2
a22
r14=0
r15=0
1 1
---*b31*m1*r333 + ---*b32*m2*r333
8 8
r20=-----------------------------------
2
a22
r21=0
r23=0
r24=0
r25=0
r26=0
1
- ---*b32*n3*r333
4
r27=--------------------
2
a22
1
- ---*b31*n3*r333
4
r28=--------------------
2
a22
- n3*r333
r29=------------
a22
1
- ---*m2*r333
2
r210=----------------
a22
r212=0
r213=0
r214=0
1
- ---*m1*r333
2
r215=----------------
a22
r216=0
r217=0
r218=0
r219=0
r30=0
r31=0
r32=0
r33=0
r34=0
r35=0
r36=0
r37=0
r38=0
r39=0
1 2 1 2
----*b31 *r333 + ----*b32 *r333
16 16
r310=---------------------------------
2
a22
r311=0
r312=0
r313=0
r314=0
r315=0
r316=0
r317=0
r318=0
r319=0
r320=0
r323=0
r325=0
1
- ---*b32*r333
2
r326=-----------------
a22
r328=0
r329=0
r330=0
r332=0
r334=0
r335=0
r336=0
r337=0
r338=0
r339=0
r340=0
1
- ---*b31*r333
2
r341=-----------------
a22
r342=0
r343=0
r344=0
r345=0
r347=0
r348=0
r349=0
r350=0
r351=0
r352=0
r353=r333
r354=0
r355=0
m3=0
n2=0
n1=0
1 2 1 2
- ----*b31 - ----*b32
16 16
c33=--------------------------
a22
c23=0
c22=0
c13=0
c12=0
c11=0
b33=0
b23=0
b22=0
b21=0
b13=0
b12=0
b11=0
a33=4*a22
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:
r333, m1, m2, n3, b32, b31, 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.
{r333,a22,a11}
Relevance for the application:
The new Hamiltonian in form of a list of vanishing expressions:
{a11 - a22,
a12,
a13,
a23,
- 4*a22 + a33,
b11,
b12,
b13,
b21,
b22,
b23,
b33,
c11,
c12,
c13,
c22,
c23,
a22*c33 + 1/16*b31**2 + 1/16*b32**2,
n1,
n2,
m3}$
The system of equations related to the Hamiltonian HAM:
2 2 2
HAM=u1 *a22 + u2 *a22 + 4*u3 *a22 + u3*v1*b31 + u3*v2*b32 + u3*n3 + v1*m1
1 2 1 2
- ----*b31 - ----*b32
2 16 16
+ v2*m2 + v3 *--------------------------
a22
has apart from the Hamiltonian and Casimirs only the following first integral:
2 2 1 1 2 2
FI=u1 *u3*a22 - ---*u1*u3*v3*a22*b31 - ---*u1*v3*a22*m1 + u2 *u3*a22
2 2
1 1 2 1
- ---*u2*u3*v3*a22*b32 - ---*u2*v3*a22*m2 - u3 *a22*n3 - ---*u3*v1*b31*n3
2 2 4
1 2 1 2 1 2 1 2
- ---*u3*v2*b32*n3 + u3*v3 *(----*b31 + ----*b32 ) - ---*u3*n3
4 16 16 4
1 1 2 1 1
- ---*v1*m1*n3 - ---*v2*m2*n3 + v3 *(---*b31*m1 + ---*b32*m2)
4 4 8 8
which the program can not factorize further.
{HAM,FI} = { - a22,
a22,
u1*v1 + u2*v2 + u3*v3,
- u1*u3*b32 - u1*m2 + u2*u3*b31 + u2*m1}
And again in machine readable form:
HAM=u1**2*a22 + u2**2*a22 + 4*u3**2*a22 + u3*v1*b31 + u3*v2*b32 + u3*n3 + v1*m1
+ v2*m2 + v3**2*( - 1/16*b31**2 - 1/16*b32**2)/a22$
FI=u1**2*u3*a22**2 - 1/2*u1*u3*v3*a22*b31 - 1/2*u1*v3*a22*m1 + u2**2*u3*a22**2 -
1/2*u2*u3*v3*a22*b32 - 1/2*u2*v3*a22*m2 - u3**2*a22*n3 - 1/4*u3*v1*b31*n3 - 1/4
*u3*v2*b32*n3 + u3*v3**2*(1/16*b31**2 + 1/16*b32**2) - 1/4*u3*n3**2 - 1/4*v1*m1*
n3 - 1/4*v2*m2*n3 + v3**2*(1/8*b31*m1 + 1/8*b32*m2)$