Initial commit

Co-authored-by: Aradhana Dube <a.dube@rug.nl>
Co-authored-by: Renzo I. Barraza Altamirano <r.i.barraza.altamirano@rug.nl>
Co-authored-by: Paolo Gibertini <p.gibertini@rug.nl>
Co-authored-by: Luca D. Fehlings <l.d.fehlings@rug.nl>
This commit is contained in:
2026-02-26 18:30:32 +01:00
commit 9fabbdefc0
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import marimo
__generated_with = "0.19.4"
app = marimo.App(width="medium")
@app.cell
def _():
import marimo as mo
from wigglystuff import Slider2D
return Slider2D, mo
@app.cell
def _():
import diffrax
import jax
import jax.numpy as jnp
import matplotlib.pyplot as plt
import numpy as np
return diffrax, jax, jnp, np, plt
@app.cell
def _(diffrax, jax, jnp):
def vector_field(t, state, args):
u, v = state
alpha, beta, gamma, kappa, sigma, delta = args
z = jax.nn.tanh(kappa * (v - u))
# Prey dynamics
du = (1 - alpha * jnp.exp(beta * v) * (1 - gamma * (0.3 - u))) + sigma * z
# Predator dynamics
dv = (-1 + alpha * jnp.exp(beta * u) * (1 + gamma * (0.3 - v))) + sigma * z
return jnp.array([du, dv])
def compute_nullclines(vector_field, u_range, v_range, args, resolution=200):
"""
Compute nullclines
du/dt = 0 (u-nullcline)
dv/dt = 0 (v-nullcline)
"""
alpha, beta, gamma, kappa, sigma, delta = args
u_vals = jnp.linspace(u_range[0], u_range[1], resolution)
v_vals = jnp.linspace(v_range[0], v_range[1], resolution)
U, V = jnp.meshgrid(u_vals, v_vals)
dU, dV = vector_field(0, [U, V], args)
return U, V, dU, dV
def solve(dyn, y0, p, T, n=500):
sol = diffrax.diffeqsolve(
diffrax.ODETerm(dyn),
diffrax.Tsit5(),
t0=0.0,
t1=T,
dt0=0.0001,
y0=y0,
args=p,
saveat=diffrax.SaveAt(ts=jnp.linspace(0, T, n)),
stepsize_controller=diffrax.PIDController(rtol=1e-7, atol=1e-8),
max_steps=50000,
)
return sol.ts, sol.ys
return compute_nullclines, solve, vector_field
@app.cell
def _(Slider2D, mo):
# alpha = 0.5 # I_n0 / I_bias ratio
# beta = 0.39/0.025 # k / U_t (inverse thermal scale)
# gamma = 0.26 # coupling coefficient
# kappa = 5.0 # tanh steepness
# sigma = 0.6 # bias scaling (s * I_bias normalized)
# y0 = jnp.array([0.2, 0.4])
# ts, ys = solve(vector_field, y0, params, 140)
alpha = mo.ui.slider(
0.0004, 0.012, 0.00001, 0.00129, label="alpha", orientation="vertical"
)
beta = mo.ui.slider(
0.0, 30, 0.00001, 0.39 / 0.025, label="beta", orientation="vertical"
)
gamma = mo.ui.slider(0, 1, 0.01, 0.26, label="gamma", orientation="vertical")
kappa = mo.ui.slider(0, 30, 1.0, 10.0, label="kappa", orientation="vertical")
sigma = mo.ui.slider(0, 1, 0.01, 0.6, label="sigma", orientation="vertical")
delta = mo.ui.slider(1, 100.0, 1, 10, label="delta", orientation="vertical")
# v0 = mo.ui.slider(0, 1.0, 0.01, 0.3, label="v0")
# u0 = mo.ui.slider(0, 1.0, 0.01, 0.2, label="u0", orientation="vertical")
state0 = mo.ui.anywidget(
Slider2D(
x=0.34,
y=0.38,
width=150,
height=150,
x_bounds=(0.0, 0.6),
y_bounds=(0.0, 0.6),
)
)
mo.hstack(
[
mo.plain_text("""
alpha: I_n0 / I_bias ratio
beta: k / U_t ratio
gamma: coupling coefficient
kappa: tanh steepness
sigma: bias scaling (s * I_bias)
"""),
mo.hstack(
[state0, alpha, beta, gamma, kappa, sigma, delta], justify="start"
),
]
)
return alpha, beta, delta, gamma, kappa, sigma, state0
@app.cell
def _(
alpha,
beta,
compute_nullclines,
delta,
gamma,
jnp,
kappa,
np,
plt,
sigma,
solve,
state0,
vector_field,
):
params = (
alpha.value,
beta.value,
gamma.value,
kappa.value,
sigma.value,
delta.value,
)
ic_neuro = [state0.x, state0.y]
u_range = [0.0, 0.6]
v_range = [0.0, 0.6]
u_sparse = jnp.linspace(u_range[0], u_range[1], 20)
v_sparse = jnp.linspace(v_range[0], v_range[1], 20)
Us, Vs = jnp.meshgrid(u_sparse, v_sparse)
def plot_vf(ax, vector_field):
U, V, dU, dV = compute_nullclines(vector_field, u_range, v_range, params)
dUs, dVs = vector_field(0, [Us, Vs], params)
# Normalize for visualization
magnitude = np.sqrt(dUs**2 + dVs**2)
magnitude[magnitude == 0] = 1
dUs_norm = dUs / magnitude
dVs_norm = dVs / magnitude
# Nullclines
ax.contour(U, V, dU, levels=[0], colors="blue", linewidths=2, linestyles="-")
ax.contour(U, V, dV, levels=[0], colors="red", linewidths=2, linestyles="-")
ax.quiver(Us, Vs, dUs_norm, dVs_norm, magnitude, cmap="viridis", alpha=0.6)
# Trajectories
color = plt.cm.plasma(0.2)
ts, ys = solve(vector_field, jnp.array(ic_neuro), params, delta.value)
ax.plot(ys[:, 0], ys[:, 1], "-", color=color, linewidth=1.5, alpha=0.8)
ax.plot(ic_neuro[0], ic_neuro[1], "o", color=color, markersize=6)
ax.set_xlabel("u (Prey)")
ax.set_ylabel("v (Predator)")
ax.set_title("Wererabbit: Phase Portrait")
ax.legend(["u-nullcline (du/dt=0)", "v-nullcline (dv/dt=0)"], loc="upper right")
ax.set_xlim(u_range)
ax.set_ylim(v_range)
ax.axhline(y=0, color="gray", linestyle="--", alpha=0.3)
ax.axvline(x=0, color="gray", linestyle="--", alpha=0.3)
def plot_trj(ax, vector_field):
ts, ys = solve(vector_field, jnp.array(ic_neuro), params, delta.value)
ax.plot(ts, ys[:, 0], "b-", linewidth=2, label="u (Prey)")
ax.plot(ts, ys[:, 1], "r-", linewidth=2, label="v (Predator)")
ax.set_xlabel("Time τ")
ax.set_ylabel("Population")
ax.set_title(
f"Wererabbit: Time Series (IC: u₀={ic_neuro[0]:.2f}, v₀={ic_neuro[1]:.2f})"
)
ax.legend()
ax.axhline(y=0, color="gray", linestyle="--", alpha=0.3)
fig = plt.figure(figsize=(10, 4))
# --- Plot 1: Wererabbit Phase Portrait ---
ax1 = fig.add_subplot(1, 2, 1)
plot_vf(ax1, vector_field)
ax2 = fig.add_subplot(1, 2, 2)
plot_trj(ax2, vector_field)
# ax3 = fig.add_subplot(3, 2, 3)
# plot_vf(ax3, vector_field_prod)
# ax4 = fig.add_subplot(3, 2, 4)
# plot_trj(ax4, vector_field_prod)
# ax5 = fig.add_subplot(3, 2, 5)
# plot_vf(ax5, vector_field_exp)
# ax6 = fig.add_subplot(3, 2, 6)
# plot_trj(ax6, vector_field_exp)
plt.tight_layout()
fig
return
@app.cell
def _():
return
@app.cell
def _():
return
@app.cell
def _():
return
if __name__ == "__main__":
app.run()

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import marimo
__generated_with = "0.19.4"
app = marimo.App(width="medium")
@app.cell
def _():
import diffrax as dfx
import jax.numpy as jnp
import marimo as mo
import matplotlib.pyplot as plt
import numpy as np
from jax import jit
return dfx, jit, jnp, mo, np, plt
@app.cell
def _(dfx, jnp):
def vector_field(t, y, args):
v, vslow = y
ipasive = args["gmax"] * (v - args["Erev"])
ifast = args["af"] * jnp.tanh(v - args["Ef"])
islow = args["as"] * jnp.tanh(vslow - args["Es"])
dv = (-ipasive - ifast - islow) / args["C"]
dvs = (v - vslow) / args["ts"]
return jnp.array([dv, dvs])
term = dfx.ODETerm(vector_field)
return term, vector_field
@app.cell
def _(mo):
p1 = mo.ui.slider(0.0, 5.0, value=1.0, step=0.1, label="gmax")
p2 = mo.ui.slider(-1.0, 1.0, value=0.0, step=0.1, label="Erev")
p3 = mo.ui.slider(-5.0, 5.0, value=-2.0, step=0.05, label="af")
p4 = mo.ui.slider(-1.0, 1.0, value=0.0, step=0.05, label="Ef")
p5 = mo.ui.slider(-5.0, 5.0, value=2.0, step=0.05, label="as")
p6 = mo.ui.slider(-1.0, 1.0, value=0.0, step=0.05, label="Es")
p7 = mo.ui.slider(1.0, 100.0, value=50.0, step=0.1, label="ts")
p8 = mo.ui.slider(0.0, 1.0, value=1.0, step=0.01, label="C")
mo.hstack(
[
mo.vstack([p1, p2, p3, p4], justify="start", gap=1),
mo.vstack([p5, p6, p7, p8], justify="start", gap=1),
]
)
return p1, p2, p3, p4, p5, p6, p7, p8
@app.cell
def _(mo):
mo.md("""
### Initial Conditions & Simulation
""")
return
@app.cell
def _(mo):
x0 = mo.ui.slider(-5.0, 5.0, value=2.0, step=0.1, label="x₀")
y0 = mo.ui.slider(-5.0, 5.0, value=0.0, step=0.1, label="y₀")
t_max = mo.ui.slider(10, 100, value=30, step=5, label="t_max")
mo.hstack([x0, y0, t_max], justify="start", gap=2)
return t_max, x0, y0
@app.cell
def _(dfx, jit, jnp, p1, p2, p3, p4, p5, p6, p7, p8, t_max, term, x0, y0):
@jit
def solve_ode(y_init, args, t_end):
solver = dfx.Tsit5()
saveat = dfx.SaveAt(ts=jnp.linspace(0, t_end, 2000))
sol = dfx.diffeqsolve(
term,
solver,
t0=0,
t1=t_end,
dt0=0.01,
y0=y_init,
args=args,
saveat=saveat,
max_steps=100000,
)
return sol.ts, sol.ys
args = {
"gmax": p1.value,
"Erev": p2.value,
"af": p3.value,
"Ef": p4.value,
"as": p5.value,
"Es": p6.value,
"ts": p7.value,
"C": p8.value,
}
y_init = jnp.array([x0.value, y0.value])
t, ys = solve_ode(y_init, args, float(t_max.value))
x_sol = ys[:, 0]
y_sol = ys[:, 1]
return args, t, x_sol, y_sol
@app.cell
def _(args, jnp, np, plt, t, vector_field, x0, x_sol, y0, y_sol):
fig, (ax1, ax2) = plt.subplots(1, 2, figsize=(14, 5))
# Time series
ax1.plot(t, x_sol, "b-", lw=1.5, label="x(t)")
ax1.plot(t, y_sol, "r-", lw=1.5, label="y(t)")
ax1.set_xlabel("Time t")
ax1.set_ylabel("State")
ax1.set_title("Transient Response")
ax1.legend()
ax1.grid(True, alpha=0.3)
# Phase plane bounds
# pad = 1.0
xmin, xmax = -4, 4
ymin, ymax = -2.5, 2.5
# Vector field
X, Y = jnp.meshgrid(jnp.linspace(xmin, xmax, 20), jnp.linspace(ymin, ymax, 20))
U, V = jnp.zeros_like(X), np.zeros_like(Y)
state = jnp.stack([X, Y], axis=0)
deriv = vector_field(0.0, state, args)
dx, dy = deriv[0], deriv[1]
mag = jnp.sqrt(dx**2 + dy**2)
U = jnp.where(mag > 0, dx / mag, U)
V = jnp.where(mag > 0, dy / mag, V)
ax2.quiver(X, Y, U, V, alpha=0.4, color="gray", scale=25)
# Nullclines
Xf, Yf = jnp.meshgrid(jnp.linspace(xmin, xmax, 150), jnp.linspace(ymin, ymax, 150))
DX, DY = jnp.zeros_like(Xf), jnp.zeros_like(Yf)
state = jnp.stack([Xf, Yf], axis=0)
deriv = vector_field(0.0, state, args)
DX, DY = deriv[0], deriv[1]
ax2.contour(
Xf,
Yf,
DX,
levels=[0],
colors="blue",
linestyles="--",
linewidths=1.5,
alpha=0.7,
)
ax2.contour(
Xf, Yf, DY, levels=[0], colors="red", linestyles="--", linewidths=1.5, alpha=0.7
)
# Trajectory
ax2.plot(x_sol, y_sol, "b-", lw=2)
ax2.plot(x0.value, y0.value, "go", ms=10, label="Start")
ax2.plot(x_sol[-1], y_sol[-1], "r*", ms=12, label="End")
ax2.set_xlabel("x")
ax2.set_ylabel("y")
ax2.set_title("Phase Plane")
ax2.legend()
ax2.grid(True, alpha=0.3)
ax2.set_xlim(xmin, xmax)
ax2.set_ylim(ymin, ymax)
plt.tight_layout()
fig
return
@app.cell
def _():
return
if __name__ == "__main__":
app.run()

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import marimo
__generated_with = "0.19.4"
app = marimo.App(width="medium")
@app.cell
def _():
import marimo as mo
from wigglystuff import Slider2D
return Slider2D, mo
@app.cell
def _():
import diffrax
import jax
import jax.numpy as jnp
import matplotlib.pyplot as plt
import numpy as np
return diffrax, jax, jnp, np, plt
@app.cell
def _(diffrax, jax, jnp):
def vector_field(t, state, args):
u, v = state
alpha, beta, gamma, kappa, sigma, delta = args
z = jax.nn.tanh(kappa * (u - v))
# Prey dynamics
du = z * (1 - alpha * jnp.exp(beta * v) * (1 + gamma * (0.5 - u))) - sigma
# Predator dynamics
dv = z * (-1 + alpha * jnp.exp(beta * u) * u * (1 + gamma * (0.5 - v))) - sigma
return jnp.array([du, dv])
def vector_field_prod(t, state, args):
u, v = state
alpha, beta, gamma, kappa, sigma, delta = args
z = jax.nn.tanh(kappa * (u - v))
# Prey dynamics
du = (
z * (1 - alpha * jnp.exp(beta * v) * (1 + gamma * (0.5 - u))) - sigma
# + sigma * jnp.maximum(0, delta - u) / (delta + 1e-16)
)
# Predator dynamics
dv = (
z * (-1 + alpha * jnp.exp(beta * u) * (1 + gamma * (0.5 - v))) - sigma
# + sigma * jnp.maximum(0, delta - v) / (delta + 1e-16)
)
dv = jnp.where(jnp.allclose(z, 0.0), dv * jnp.sign(v), dv)
du = jnp.where(jnp.allclose(z, 0.0), du * jnp.sign(u), du)
return jnp.array([du, dv])
def vector_field_exp(t, state, args):
u, v = state
alpha, beta, gamma, kappa, sigma, delta = args
z = jax.nn.tanh(kappa * (u - v))
# Prey dynamics
du = (
z * (1 - alpha * jnp.exp(beta * v) * (1 + gamma * (0.5 - u)))
- sigma
+ sigma * jnp.exp(-u / delta)
)
# Predator dynamics
dv = (
z * (-1 + alpha * jnp.exp(beta * u) * u * (1 + gamma * (0.5 - v)))
- sigma
+ sigma * jnp.exp(-v / delta)
)
return jnp.array([du, dv])
def physical_vector_field(t, state, args):
x1, x2 = state
alpha, beta, gamma, kappa, sigma, delta = args
In0 = 129e-15 # fixed by design
C = 0.1e-12 # fixed by design
kk = 0.39 # fixed by tech
Ut = 0.025 # temperature dependent
Ibias = In0 / alpha
Ia = Ibias * sigma
x3 = jax.nn.tanh(kappa * (x1 - x2))
dx1 = (
x3 * Ibias
- (In0 * jnp.exp(kk * x2 / Ut)) * (x3 + 26e-2 * (0.5 - x1) * x3)
- Ia
) / C
dx2 = (
-x3 * Ibias
+ In0 * jnp.exp(kk * x1 / Ut) * (x3 + 26e-2 * (0.5 - x2) * x3)
- Ia
) / C
return jnp.array([dx1, dx2])
def compute_nullclines(vector_field, u_range, v_range, args, resolution=200):
"""
Compute nullclines
du/dt = 0 (u-nullcline)
dv/dt = 0 (v-nullcline)
"""
alpha, beta, gamma, kappa, sigma, delta = args
u_vals = jnp.linspace(u_range[0], u_range[1], resolution)
v_vals = jnp.linspace(v_range[0], v_range[1], resolution)
U, V = jnp.meshgrid(u_vals, v_vals)
dU, dV = vector_field(0, [U, V], args)
return U, V, dU, dV
def solve(dyn, y0, p, T, n=1000):
sol = diffrax.diffeqsolve(
diffrax.ODETerm(dyn),
diffrax.Tsit5(),
t0=0.0,
t1=T,
dt0=0.01,
y0=y0,
args=p,
saveat=diffrax.SaveAt(ts=jnp.linspace(0, T, n)),
stepsize_controller=diffrax.PIDController(rtol=1e-7, atol=1e-8),
max_steps=50000,
)
return sol.ts, sol.ys
return compute_nullclines, solve, vector_field_prod
@app.cell
def _(Slider2D, mo):
# alpha = 0.5 # I_n0 / I_bias ratio
# beta = 0.39/0.025 # k / U_t (inverse thermal scale)
# gamma = 0.26 # coupling coefficient
# kappa = 5.0 # tanh steepness
# sigma = 0.6 # bias scaling (s * I_bias normalized)
# y0 = jnp.array([0.2, 0.4])
# ts, ys = solve(vector_field, y0, params, 140)
alpha = mo.ui.slider(
0.0004, 0.012, 0.00001, 0.00129, label="alpha", orientation="vertical"
)
beta = mo.ui.slider(
0.0, 30, 0.00001, 0.39 / 0.025, label="beta", orientation="vertical"
)
gamma = mo.ui.slider(0, 1, 0.01, 0.26, label="gamma", orientation="vertical")
kappa = mo.ui.slider(0, 10, 0.1, 5.0, label="kappa", orientation="vertical")
sigma = mo.ui.slider(0, 1, 0.01, 0.6, label="sigma", orientation="vertical")
delta = mo.ui.slider(0, 0.1, 0.001, 0.02, label="delta", orientation="vertical")
# v0 = mo.ui.slider(0, 1.0, 0.01, 0.3, label="v0")
# u0 = mo.ui.slider(0, 1.0, 0.01, 0.2, label="u0", orientation="vertical")
state0 = mo.ui.anywidget(
Slider2D(
width=150,
height=150,
x_bounds=(-1.0, 1.5),
y_bounds=(-1.0, 1.5),
)
)
mo.hstack(
[
mo.plain_text("""
alpha: I_n0 / I_bias ratio
beta: k / U_t ratio
gamma: coupling coefficient
kappa: tanh steepness
sigma: bias scaling (s * I_bias)
"""),
mo.hstack(
[state0, alpha, beta, gamma, kappa, sigma, delta], justify="start"
),
]
)
return alpha, beta, delta, gamma, kappa, sigma, state0
@app.cell
def _(
alpha,
beta,
compute_nullclines,
delta,
gamma,
jnp,
kappa,
np,
plt,
sigma,
solve,
state0,
vector_field_prod,
):
params = (
alpha.value,
beta.value,
gamma.value,
kappa.value,
sigma.value,
delta.value,
)
ic_neuro = [state0.x, state0.y]
u_range = [-1.0, 1.5]
v_range = [-1.0, 1.5]
u_sparse = jnp.linspace(u_range[0], u_range[1], 20)
v_sparse = jnp.linspace(v_range[0], v_range[1], 20)
Us, Vs = jnp.meshgrid(u_sparse, v_sparse)
def plot_vf(ax, vector_field):
U, V, dU, dV = compute_nullclines(vector_field, u_range, v_range, params)
dUs, dVs = vector_field(0, [Us, Vs], params)
# Normalize for visualization
magnitude = np.sqrt(dUs**2 + dVs**2)
magnitude[magnitude == 0] = 1
dUs_norm = dUs / magnitude
dVs_norm = dVs / magnitude
# Nullclines
ax.contour(U, V, dU, levels=[0], colors="blue", linewidths=2, linestyles="-")
ax.contour(U, V, dV, levels=[0], colors="red", linewidths=2, linestyles="-")
ax.quiver(Us, Vs, dUs_norm, dVs_norm, magnitude, cmap="viridis", alpha=0.6)
# Trajectories
color = plt.cm.plasma(0.2)
ts, ys = solve(vector_field, jnp.array(ic_neuro), params, 50)
ax.plot(ys[:, 0], ys[:, 1], "-", color=color, linewidth=1.5, alpha=0.8)
ax.plot(ic_neuro[0], ic_neuro[1], "o", color=color, markersize=6)
ax.set_xlabel("u (Prey)")
ax.set_ylabel("v (Predator)")
ax.set_title("Wererabbit: Phase Portrait")
ax.legend(["u-nullcline (du/dt=0)", "v-nullcline (dv/dt=0)"], loc="upper right")
ax.set_xlim(u_range)
ax.set_ylim(v_range)
ax.axhline(y=0, color="gray", linestyle="--", alpha=0.3)
ax.axvline(x=0, color="gray", linestyle="--", alpha=0.3)
def plot_trj(ax, vector_field):
ts, ys = solve(vector_field, jnp.array(ic_neuro), params, 50)
ax.plot(ts, ys[:, 0], "b-", linewidth=2, label="u (Prey)")
ax.plot(ts, ys[:, 1], "r-", linewidth=2, label="v (Predator)")
ax.set_xlabel("Time τ")
ax.set_ylabel("Population")
ax.set_title(
f"Wererabbit: Time Series (IC: u₀={ic_neuro[0]:.2f}, v₀={ic_neuro[1]:.2f})"
)
ax.legend()
ax.axhline(y=0, color="gray", linestyle="--", alpha=0.3)
fig = plt.figure(figsize=(10, 4))
# --- Plot 1: Wererabbit Phase Portrait ---
ax1 = fig.add_subplot(1, 2, 1)
plot_vf(ax1, vector_field_prod)
ax2 = fig.add_subplot(1, 2, 2)
plot_trj(ax2, vector_field_prod)
# ax3 = fig.add_subplot(3, 2, 3)
# plot_vf(ax3, vector_field_prod)
# ax4 = fig.add_subplot(3, 2, 4)
# plot_trj(ax4, vector_field_prod)
# ax5 = fig.add_subplot(3, 2, 5)
# plot_vf(ax5, vector_field_exp)
# ax6 = fig.add_subplot(3, 2, 6)
# plot_trj(ax6, vector_field_exp)
plt.tight_layout()
fig
return
@app.cell
def _():
return
@app.cell
def _():
return
@app.cell
def _():
return
if __name__ == "__main__":
app.run()