Let $H \in C^{\infty}(\mathbb{R}, \mathbb{R}^{3})$ such that $\|H^{\prime}(x)\| = 1$ and $\|H^{\prime\prime}(x)\| \neq 0$ for all $x \in \mathbb{R}$. We denote $T_{H}(x) = H^{\prime}(x)$, $n_{H}(x) = T_{H}^{\prime}(x)/\|T_{H}^{\prime}(x)\|$ and $b_{H}(x) = T_{H}(x) \wedge n_{H}(x)$. We admit that there exist $k_{H}(x)$ and $\tau_{H}(x)$ such that $$\left\{\begin{array}{l} T_{H}^{\prime}(x) = k_{H}(x)\, n_{H}(x) \\ n_{H}^{\prime}(x) = -k_{H}(x)\, T_{H}(x) + \tau_{H}(x)\, b_{H}(x) \\ b_{H}^{\prime}(x) = -\tau_{H}(x)\, n_{H}(x) \end{array}\right.$$
We assume that $m = 0$ and there exists $\lambda > 0$ such that $G(0) = (0,0,2\lambda)$, $G^{\prime}(0) = (1,0,0)$, and $G \in C^{\infty}(\mathbb{R}, \mathbb{R}^{3})$ satisfies $\forall x \in \mathbb{R},\, G^{\prime\prime}(x) = \frac{1}{2}G(x) \wedge G^{\prime}(x)$, with $T(x) = G^{\prime}(x)$, $n(x) = T^{\prime}(x)/\lambda$, $b(x) = T(x) \wedge n(x)$.
Express $k_{G}$ and $\tau_{G}$, then show that there exists $\alpha \in \mathbb{R}$ such that the function $$\Psi(t, x) = \frac{1}{\sqrt{t}}\, k_{G}\!\left(\frac{x}{\sqrt{t}}\right) \exp\!\left(i\int_{0}^{x} \frac{1}{\sqrt{t}}\, \tau_{G}\!\left(\frac{y}{\sqrt{t}}\right) dy\right)$$ is a solution of equation $(F_{\alpha})$, that is $$\forall (t, x) \in \mathbb{R}_{+}^{*} \times \mathbb{R}, \quad i\frac{\partial \Psi}{\partial t}(t, x) + \frac{\partial^{2} \Psi}{\partial x^{2}}(t, x) + \frac{1}{2}\Psi(t, x)\left(\alpha|\Psi(t, x)|^{2} + \frac{1}{t}\right) = 0$$