220220
221221
222222"""
223- qbh(u0=[ ]; A=1., B=0.55, D=0.4)
223+ qbh([u0 ]; A=1.0 , B=0.55, D=0.4)
224224
225225```math
226226\\ begin{aligned}
231231\\ end{aligned}
232232```
233233
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.
234+ These equations of motion correspond to a Hamiltonian used in nuclear
235+ physics to study the quadrupole vibrations of the nuclear surface [1,2] .
236236
237237```math
238238H(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)
@@ -244,7 +244,9 @@ and presents a nontrivial dependence of chaoticity with the increase of energy [
244244The default initial condition is chaotic.
245245
246246[1]: Eisenberg, J.M., & Greiner, W., Nuclear theory 2 rev ed. Netherlands: North-Holland pp 80 (1975)
247+
247248[2]: Baran V. and Raduta A. A., International Journal of Modern Physics E, **7**, pp 527--551 (1998)
249+
248250[3]: Micluta-Campeanu S., Raportaru M.C., Nicolin A.I., Baran V., Rom. Rep. Phys. **70**, pp 105 (2018)
249251"""
250252function qbh (u0= [0. , - 2.5830294658973876 , 1.3873470962626937 , - 4.743416490252585 ]; A= 1. , B= 0.55 , D= 0.4 )
@@ -418,7 +420,7 @@ nosehoover(u0 = [0, 0.1, 0])
418420\\ begin{aligned}
419421\\ dot{x} &= y \\\\
420422\\ dot{y} &= yz - x \\\\
421- \\ dot{V } &= 1 - y^2
423+ \\ dot{z } &= 1 - y^2
422424\\ end{aligned}
423425```
424426Three dimensional conservative continuous system, taken from the book
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