Update src/7_tight_binding_model_sol.md

src/7_tight_binding_model_sol.md

@@ -81,63 +81,3 @@ The Schrödinger equation is given as: $|\Psi\rangle = \sum_n \phi_n |n\rangle$
 
 Solving the Schrödinger equation yields dispersion: $$E(k) = E_0 -t\cos(ka) -t'\cos(2ka)$$
 
-### Subquestiion 3
-
-$$m_{eff} = \frac{\hbar^2}{2a^2}\frac{1}{t\cos(ka)+4t'\cos(2ka)}$$
-
-Plot for t=t':
-
-```python
-k1 = np.linspace(-pi, -pi/2-0.01, 300);
-k2 = np.linspace(-pi/2+0.01, pi/2-0.01, 300);
-k3 = np.linspace(pi/2+0.01, pi, 300);
-
-pyplot.plot(k1, 1/(5*np.cos(k1)),'b');
-pyplot.plot(k2, 1/(5*np.cos(k2)),'b');
-pyplot.plot(k3, 1/(5*np.cos(k3)),'b');
-pyplot.xlabel('$k$'); pyplot.ylabel('$m_{eff}(k)$');
-pyplot.xticks([-pi,0,pi],[r'$-\pi/a$',0,r'$\pi/a$']);
-pyplot.yticks([],[]);
-pyplot.tight_layout();
-```
-
-### Subquestion 4
-
-Plots for 2t'=t, 4t'=t and 10t'=t:
-
-```python
-def m(k,t):
-    return 1/(np.cos(k)+4*t*np.cos(2*k))
- 
-k1 = np.linspace(-1.6, -0.83, 300);
-k2 = np.linspace(-0.826, 0.826, 300);
-k3 = np.linspace(0.83, 1.6, 300);
-
-pyplot.plot(k1, m(k1,2),'b');
-pyplot.plot(k2, m(k2,2),'b');
-pyplot.plot(k3, m(k3,2),'b',label='t=2t\'');
-pyplot.xlabel('$k$'); pyplot.ylabel('$m_{eff}(k)$');
-pyplot.xticks([-pi,0,pi],[r'$-\pi/a$',0,r'$\pi/a$']);
-pyplot.yticks([-10,10],[]);
-pyplot.tight_layout();
-
-k1 = np.linspace(-1.58, -0.81, 300);
-k2 = np.linspace(-0.804, 0.804, 300);
-k3 = np.linspace(0.81, 1.58, 300);
-
-pyplot.plot(k1, m(k1,4),'r');
-pyplot.plot(k2, m(k2,4),'r');
-pyplot.plot(k3, m(k3,4),'r',label='t=4t\'');
-
-k1 = np.linspace(-1.575, -0.798, 300);
-k2 = np.linspace(-0.790, 0.790, 300);
-k3 = np.linspace(0.798, 1.575, 300);
-
-pyplot.plot(k1, m(k1,10),'k');
-pyplot.plot(k2, m(k2,10),'k');
-pyplot.plot(k3, m(k3,10),'k',label='t=10t\'');
-
-pyplot.legend()
-```
-
-