diff --git a/schrodinger1D.py b/schrodinger1D.py
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+++ b/schrodinger1D.py
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+"""
+Quantum Tunneling Simulation
+============================
+
+This example demonstrates how to solve the Time-Dependent Schrödinger Equation
+using Diffrax. It simulates a Gaussian wave packet tunneling through a 
+potential barrier.
+
+Key JAX features used:
+- `jax.jit` for compilation
+- `diffrax.Tsit5` solver
+- Complex number arithmetic in ODEs
+
+![Simulation Result](simulation_result.png)
+"""
+
+import dataclasses
+import jax
+import jax.numpy as jnp
+import diffrax
+import matplotlib.pyplot as plt
+
+
+# configure sim we use @dataclass to not write the __init__ method
+@dataclasses.dataclass(frozen=True)
+class SimConfig:
+    N: int = 500  # Grid points
+    L: float = 40.0  # Box size
+    t0: float = 0.0  # Start time
+    t1: float = 4.0  # End time
+    num_frames: int = 200  # Number of frames to save (Fixed integer is safer than dt)
+
+    # dx function can be called without () because of @property
+    @property
+    def dx(self):
+        return self.L / self.N
+
+    @property
+    def x_grid(self):
+        return jnp.linspace(-self.L / 2, self.L / 2, self.N)
+
+
+# Physics
+
+
+def get_potential(x_grid):
+    return jnp.where((x_grid > -0.5) & (x_grid < 0.5), 20.0, 0.0)
+
+
+def build_hamiltonian(config: SimConfig):
+    x = config.x_grid
+    V_arr = get_potential(x)
+    V_matrix = jnp.diag(V_arr)
+
+    main_diag = jnp.full(config.N, -2.0)
+    off_diag = jnp.ones(config.N - 1)
+
+    M = jnp.diag(main_diag, k=0) + jnp.diag(off_diag, k=1) + jnp.diag(off_diag, k=-1)
+    KE = (-1.0 / (2.0 * config.dx**2)) * M
+
+    H = KE + V_matrix
+    return H, V_arr
+
+
+def get_initial_psi(config: SimConfig, x0=-10.0, k0=5.0, sigma=1.0):
+    x = config.x_grid
+    norm = 1.0 / (jnp.pi * sigma**2) ** 0.25
+    psi = norm * jnp.exp(-((x - x0) ** 2) / (2 * sigma**2)) * jnp.exp(1j * k0 * x)
+    return psi
+
+
+def vector_field(t, psi, args):
+    H = args
+    return -1j * (H @ psi)
+
+
+# compile jit
+@jax.jit
+def run_simulation(hamiltonian, psi0, t0, t1, save_times):
+
+    term = diffrax.ODETerm(vector_field)
+    solver = diffrax.Tsit5()
+
+    # Use the passed-in array instead of creating one inside
+    saveat = diffrax.SaveAt(ts=save_times)
+
+    step_controller = diffrax.PIDController(rtol=1e-8, atol=1e-8)
+
+    sol = diffrax.diffeqsolve(
+        term,
+        solver,
+        t0,
+        t1,
+        dt0=0.01,
+        y0=psi0,
+        args=hamiltonian,
+        saveat=saveat,
+        stepsize_controller=step_controller,
+    )
+    return sol
+
+
+# Visualization
+
+
+def create_plot(sol, config, V_arr, psi0):
+    x = config.x_grid
+    psi_final = sol.ys[-1]
+
+    fig, (ax1, ax2) = plt.subplots(2, 1, figsize=(10, 8), sharex=True)
+
+    # Plot 1
+    ax1.set_title(f"Quantum Tunneling (t={config.t1})", fontsize=14)
+    ax1.fill_between(
+        x, 0, V_arr * 0.01, color="gray", alpha=0.3, label="Potential Barrier (Scaled)"
+    )
+    ax1.plot(x, jnp.abs(psi0) ** 2, "b--", alpha=0.6, label="Initial |$\psi$|$^2$")
+    ax1.plot(x, jnp.abs(psi_final) ** 2, "r-", linewidth=2, label=f"Final |$\psi$|$^2$")
+    ax1.set_ylabel("Probability Density")
+    ax1.legend(loc="upper right")
+    ax1.grid(True, alpha=0.3)
+
+    # Plot 2
+    ax2.set_title("Wave Function Components", fontsize=12)
+    ax2.plot(x, jnp.real(psi_final), "g-", alpha=0.7, label="Real Part")
+    ax2.plot(x, jnp.imag(psi_final), "orange", alpha=0.7, label="Imaginary Part")
+    ax2.set_xlabel("Position ($x$)")
+    ax2.set_ylabel("Amplitude")
+    ax2.legend(loc="upper right")
+    ax2.grid(True, alpha=0.3)
+
+    plt.tight_layout()
+    plt.savefig("simulation_result.png", dpi=150)
+    print("Plot saved as simulation_result.png")
+    plt.show()
+
+
+# main
+def main():
+    print("Initializing Quantum Simulation...")
+    config = SimConfig(N=500, L=40.0, t0=0.0, t1=4.0, num_frames=200)
+
+    print("Building Hamiltonian...")
+    H_matrix, V_array = build_hamiltonian(config)
+    psi0 = get_initial_psi(config)
+
+    # always initialize outside the helper functions because helper functions are for abstractions
+    save_times = jnp.linspace(config.t0, config.t1, config.num_frames)
+
+    print("Solving Schrödinger Equation (JIT Compiled)...")
+    # Pass 'save_times' into the function
+    sol = run_simulation(H_matrix, psi0, config.t0, config.t1, save_times)
+
+    print("Generating Plots...")
+    create_plot(sol, config, V_array, psi0)
+
+
+if __name__ == "__main__":
+    main()
diff --git a/simulation_result.png b/simulation_result.png
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