It seems that the array notation is not suited for pattern matching in Maple ?

@jalal 
More intuiative with complex numbers ...

corrected code

restart;
with(DEtools);
with(plots);
with(LinearAlgebra);
f := y -> y^2*(1 - y^2);
sys := [diff(x(t), t) = -x(t), diff(y(t), t) = f(y(t))];
trajectories := [[x(0) = 1, y(0) = 1.5], [x(0) = -1, y(0) = 0.5], [x(0) = 0.5, y(0) = -1.5]];
phase_plot := DEplot(sys, [x(t), y(t)], t = 0 .. 10, trajectories, x = -2 .. 2, y = -2 .. 2, arrows = medium, dirfield = [20, 20], linecolor = blue, title = "Phase Portrait with Equilibrium Points");
equilibrium_points := pointplot([[0, 0], [0, 1], [0, -1]], symbol = solidcircle, color = black, symbolsize = 15);
display([phase_plot, equilibrium_points], scaling = constrained);
print("\n### DETAILED STABILITY ANALYSIS ###");
F := [-x, -y^4 + y^2];
J := Matrix([[diff(F[1], x), diff(F[1], y)], [diff(F[2], x), diff(F[2], y)]]);
print("\n1. Analysis for (0,0):");
J0 := eval(J, {x = 0, y = 0});
print("Jacobian:", J0);
print("Eigenvalues:", Eigenvalues(J0));
print("Conclusion:");
print("   - Eigenvalues: -1 and 0");
print("   - Non-hyperbolic point");
print("   - dy/dt ≈ y^2 > 0 for y ≈ 0");
print("   - ⇒ (0,0) is UNSTABLE");
print("\n2. Analysis for (0,1):");
J1 := eval(J, {x = 0, y = 1});
print("Jacobian:", J1);
print("Eigenvalues:", Eigenvalues(J1));
print("Conclusion:");
print("   - Eigenvalues: -1 and -2");
print("   - Both negative ⇒ STABLE NODE");
print("   - All nearby trajectories converge to this point");
print("\n3. Analysis for (0,-1):");
Jm1 := eval(J, {x = 0, y = -1});
print("Jacobian:", Jm1);
print("Eigenvalues:", Eigenvalues(Jm1));
print("Conclusion:");
print("   - Eigenvalues: -1 and +2");
print("   - Mixed eigenvalues ⇒ SADDLE POINT");
print("   - Stable in x-direction, unstable in y-direction");
print("   - ⇒ (0,-1) is UNSTABLE");
print("\n### VISUAL INTERPRETATION ###");
print("1. (0,0): Arrows point away in y-direction - unstable");
print("2. (0,1): All arrows point toward this point - stable");
print("3. (0,-1): Arrows approach in x-direction but diverge in y-direction - saddle point");
print("\n### SYSTEM BEHAVIOR SUMMARY ###");
print("The system exhibits:");
print("- One stable equilibrium at (0,1)");
print("- One unstable equilibrium at (0,0)");
print("- One saddle point at (0,-1)");
print("- Bistability between y=1 and y=-1 states");
print("- All x-values decay to 0 over time");
print("- y-direction determines long-term behavior");

Never trust ai , because node ( 0,-1) is not stable , when i examine it 

@salim-barzani 
You need help from a specialist , i don't know what you are after for.? 

do_loop_met_absoluutfunctie_complex_herschreven7-6-2025mprimes.mw

@salim-barzani 

 

restart;
expr := abs(U[i](x, t))^n*diff(U[i](x, t), x);
expr_rewritten := subs(abs(U[i](x, t))^n = (U[i](x, t)*conjugate(U[i](x, t)))^(n/2), expr);
print(expr_rewritten);

"in here i want to seperate abs(U[i](x,t))^n=U[i](x,t)^n/2*conjugate(U[i](x,t))"   
I am guessing here, no direction where you are after for?

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@salim-barzani 
berekening_u1_u2_etc_6-6-2025mprimes.mw

@salim-barzani 

It is not yet a definitive code that can handle all non-linear pdes .
The procedure code must be modified for certain types of pde 
So specify the pde ...

Kunda_Eckhaus5-6-2025mprimes.mw

Download onderzoek_termen_in_niet_linear_pde5-6-2025mprimes.mw

Checked the procedure with the classical  non -lineair schrodinger eq 
Do you have a idea what are the lineair and non linear parts of your pde

splitsing_pde_conjugate_vorm_4-6-2025mprimes_A.mw

"Ai is trash in 100 time just one time work , when i am stuck i will post here and my work is rare i cant find it any where i have to do step by step,  many thanks for you"

You can't use ai , so this is not a good  attitude , rather simplistic 

@salim-barzani 

Download G25_via_maple_nu_-wel_in_mathematica_mprimes3-6-2025.mw