@@ -219,6 +219,51 @@ function hhjacob!(J, u, p, t)
219219end
220220
221221
222+ """
223+ qbh(u0=[]; A=1., B=0.55, D=0.4)
224+
225+ ```math
226+ \\ begin{aligned}
227+ \\ dot{q}_0 &= A p_0 \\\\
228+ \\ dot{q}_2 &= A p_2 \\\\
229+ \\ dot{p}_0 &= -A q_0 -3 \\ frac{B}{\\ sqrt{2}} (q_2^2 - q_1^2) - D q_1 (q_1^2 + q_2^2) \\\\
230+ \\ dot{p}_2 &= -q_2 (A + 3\\ sqrt{2} B q_1 + D (q_1^2 + q_2^2)) (x^2 - y^2)
231+ \\ end{aligned}
232+ ```
233+
234+ These equations of motion correspond to a Hamiltonian used [1,2] in nuclear
235+ physics to study the quadrupole vibrations of the nuclear surface.
236+
237+ ```math
238+ H(p_0, p_2, q_0, q_2) = \\ frac{A}{2}\\ left(p_0^2+p_2^2\\ right)+\\ frac{A}{2}\\ left(q_0^2+q_2^2\\ right)
239+ +\\ frac{B}{\\ sqrt{2}}q_0\\ left(3q_2^2-q_0^2\\ right) +\\ frac{D}{4}\\ left(q_0^2+q_2^2\\ right)^2
240+ ```
241+
242+ The Hamiltonian has a similar structure with the Henon-Heiles one, but it has an added fourth order term
243+ and presents a nontrivial dependence of chaoticity with the increase of energy [3].
244+ The default initial condition is chaotic.
245+
246+ [1]: Eisenberg, J.M., & Greiner, W., Nuclear theory 2 rev ed. Netherlands: North-Holland pp 80 (1975)
247+ [2]: Baran V. and Raduta A. A., International Journal of Modern Physics E, **7**, pp 527--551 (1998)
248+ [3]: Micluta-Campeanu S., Raportaru M.C., Nicolin A.I., Baran V., Rom. Rep. Phys. **70**, pp 105 (2018)
249+ """
250+ function qbh (u0= [0. , - 2.5830294658973876 , 1.3873470962626937 , - 4.743416490252585 ]; A= 1. , B= 0.55 , D= 0.4 )
251+ return CDS (qeom, u0, [A, B, D])
252+ end
253+ function qeom (z, p, t)
254+ @inbounds begin
255+ A, B, D = p
256+ p₀, p₂ = z[1 ], z[2 ]
257+ q₀, q₂ = z[3 ], z[4 ]
258+
259+ return SVector {4} (
260+ - A * q₀ - 3 * B / √ 2 * (q₂^ 2 - q₀^ 2 ) - D * q₀ * (q₀^ 2 + q₂^ 2 ),
261+ - q₂ * (A + 3 * √ 2 * B * q₀ + D * (q₀^ 2 + q₂^ 2 )),
262+ A * p₀,
263+ A * p₂
264+ )
265+ end
266+ end
222267
223268"""
224269 lorenz96(N::Int, u0 = rand(M); F=0.01)
0 commit comments