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Problem

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code template

Code

import sympy as sp

z, K = sp.symbols('z K')

def answer(z, K):
    r"""
    Return the expression of $\varphi$ in Sympy format.

    Inputs
    ----------
    z: sympy.Symbol, defined as $\log_2 t$
    K: sympy.Symbol, constant from the self-consistent equation
            $$\frac{1}{\ell^{\mu}(t)} \int_0^t \ell(\tau) \ell(t - \tau) d\tau = K$$

    Outputs
    ----------
    varphi: sympy.Expr, expansion of $\varphi$ in terms of $z$ for large $t$
        and retain terms up to constant order in $z$
    """

    # ------------------ FILL IN YOUR RESULTS BELOW ------------------
    varphi = ...  # SymPy expression in terms of z (and possibly K),
                  # retaining z, log_2(z), log_2(z)**2 terms; omit constants
    # ---------------------------------------------------------------

    return varphi

problem description

# Problem setup: In a long-range dispersal model, a cluster of species can grow from a single seed. The cluster expands into space with long-range power-law interactions. In one dimension, the asymptotic size of the cluster, denoted by (t)\ell(t), satisfies a self-consistent equation: \begin{equation} \frac{1}{\ell^{\mu}(t)} \int_0^t \ell(\tau) \ell(t - \tau) d\tau = K. \end{equation} Here, μ\mu is the power-law index of the long-range interaction, and KK is a constant independent of time. # Main problem: Consider the specific scenario where μ=2\mu = 2, and let us define φ=log2\varphi = \log_2 \ell and z=log2tz = \log_2 t. Expand φ\varphi in terms of zz for large tt and retain terms up to constant order in zz. That is, you should fix any polylog(z)\text{polylog}(z) corrections such as log2(z)\log_2(z) and log22(z)\log^2_2(z) if they are present; constant corrections can be ignored.
Plain-text mathematical notation (without MathML)

# Problem setup:
In a long-range dispersal model, a cluster of species can grow from a single seed. The cluster expands into space with long-range power-law interactions. In one dimension, the asymptotic size of the cluster,  denoted by ℓ(t), satisfies a self-consistent equation:
\begin{equation}
    \frac{1}{\ell^{\mu}(t)} \int_0^t \ell(\tau) \ell(t - \tau) d\tau = K.
\end{equation}
Here, μ is the power-law index of the long-range interaction, and K is a constant independent of time.

# Main problem:

Consider the specific scenario where μ=2, and let us define φ=log₂ℓ and z=log₂t. Expand φ in terms of z  for large t and retain terms up to constant order in z. That is, you should fix any polylog(z) corrections such as log₂(z) and log₂²(z) if they are present; constant corrections can be ignored.
Original LaTeX notation

# Problem setup:
In a long-range dispersal model, a cluster of species can grow from a single seed. The cluster expands into space with long-range power-law interactions. In one dimension, the asymptotic size of the cluster,  denoted by $\ell(t)$, satisfies a self-consistent equation:
\begin{equation}
    \frac{1}{\ell^{\mu}(t)} \int_0^t \ell(\tau) \ell(t - \tau) d\tau = K.
\end{equation}
Here, $\mu$ is the power-law index of the long-range interaction, and $K$ is a constant independent of time.

# Main problem:

Consider the specific scenario where $\mu = 2$, and let us define $\varphi = \log_2 \ell$ and $z = \log_2 t$. Expand $\varphi$ in terms of $z$  for large $t$ and retain terms up to constant order in $z$. That is, you should fix any $\text{polylog}(z)$ corrections such as $\log_2(z)$ and $\log^2_2(z)$ if they are present; constant corrections can be ignored.

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Source and history

Official source

initial import