From f0458070a336b4c4c9bc2c4183a48957327ae3d1 Mon Sep 17 00:00:00 2001 From: =?UTF-8?q?Fabiana=20=F0=9F=9A=80=20=20Campanari?= <113218619+FabianaCampanari@users.noreply.github.com> Date: Tue, 4 Feb 2025 23:48:28 -0300 Subject: [PATCH] Update README.md MIME-Version: 1.0 Content-Type: text/plain; charset=UTF-8 Content-Transfer-Encoding: 8bit Signed-off-by: Fabiana 🚀 Campanari <113218619+FabianaCampanari@users.noreply.github.com> --- README.md | 3 +++ 1 file changed, 3 insertions(+) diff --git a/README.md b/README.md index 43c6bcb..831c688 100644 --- a/README.md +++ b/README.md @@ -311,6 +311,7 @@ Ramanujan's deep insights into infinite series and modular forms continue to inf $\huge \color{DeepSkyBlue} E_n = -\frac{13.6 \, \text{eV}}{n^2}$ +
[Where](): - $$\large \color{DeepSkyBlue} E_n$$ is the energy of the $$n$$-th level. @@ -327,6 +328,8 @@ Time-dependent form of Schrödinger’s equation: $\huge \color{DeepSkyBlue} i\hbar \frac{\partial}{\partial t} \psi(r, t) = \hat{H} \psi(r, t)$ +
+ [Where](): - $\large \color{DeepSkyBlue} \psi(r, t)$ is the wave function of the system. - $\large \color{DeepSkyBlue} \hat{H}$ is the Hamiltonian operator.