Phys man

Author: giadarol

docs/physics_manual/physics_man.pdf

@@ -305,7 +305,8 @@ \subsection{Hamiltonians of the implemented maps}
 Knh & kn, ks, h  & Curved Multipoles & 
 Not yet available\\
 M   & k0, k1, l, h & 2nd order Hamiltonian & 
-$H_{Kn} = \frac{p_\tau}{\beta_0} +  \frac{1}{2}\frac{p_x^2 + p_y^2}{(1 + \delta)} + (k_0 -h)x + \frac{k0hx^2}{2}\right) + k_1 \frac{x^2-y^2}{2} $\\
+$H_{Kn} = \frac{p_\tau}{\beta_0} +  \frac{1}{2}\frac{p_x^2 + p_y^2}{(1 + \delta)} + (k_0 -h)x + \frac{k_0hx^2}{2} + k_1 \frac{x^2-y^2}{2} $
+\\
 S   & ks,l          & Solenoid & 
 $H_{S} = \frac{p_\tau}{\beta_0} - \sqrt{(1 + \delta)^2 - \left(p_x-\frac{k_s}{2} y\right)^2 - \left(p_y+\frac{k_s}{2}\right)^2}$
 \\