diff --git a/scri/pn/boosted_comcharge.py b/scri/pn/boosted_comcharge.py
new file mode 100644
index 00000000..79a5f30d
--- /dev/null
+++ b/scri/pn/boosted_comcharge.py
@@ -0,0 +1,144 @@
+import numpy as np
+
+
+def PN_charges(m, ν):
+    """
+    Determine a tuple of callables for a specific input of mass (m) and
+    symmetric mass ratio (ν).
+
+    Parameters
+    ----------
+    m: float, real
+        Total mass of the binary.
+    ν: float, real
+        Symmetric mass ratio of the binary.
+
+    Returns
+    -------
+    energy_pn : callable
+        Returns PN approximation for energy up to 2PN order
+    angular_momentum_pn : callable
+        Returns PN approximation for angular momentum up to 3PN order
+    com_charge_pn : callable
+        Returns PN approximation for CoM charge up to leading order
+    phase : callable
+        Returns the phase obtained from the (2,1) mode of the strain
+
+    All returned callables accept an `ABD` object as an input parameter and
+    return their respective quantities evaluated at the same time steps as the
+    `ABD` object. The PN expressions for energy and angular momentum are taken
+    from Eqs. (337) and (338) of Blanchet's Living Review (2014)
+    <https://arxiv.org/abs/1310.1528>. The PN expression for CoM charge is
+    derived in Khairnar et al. <add_arXiv_link>. The tuple of these callables
+    can be passed as the `Gargsfun` keyword argument to
+    `map_to_superrest_frame`. These callables are then used to determine the
+    Gargs parameters to `transformation_from_CoM_charge`. They are called as
+    Gargs = [func(abd) for func in Gargsfun] if Gargsfun else None
+    within the `com_transformation_to_map_to_superrest_frame` function.
+
+    Notes
+    ------
+    Our conventions for defining the orbital phase differ from the standard
+    conventions used in PN theory.  This stems from the fact that SpEC uses
+    h_{ab} to define the metric perturbation while PN theory uses h^{ab} for
+    the metric perturbation, which results in h^{NR}_{l,m} = − h^{PN}_{l,m}.
+    Also, the π/2 phase difference is due to the leading-order complex phase
+    of h_{2,1} mode from PN theory.
+
+    """
+
+    def compute_x(abd):
+        """Helper function to extract PN parameter x."""
+        h = abd.h
+        ω_mag = np.linalg.norm(h.angular_velocity(), axis=1)
+        x = (m * ω_mag) ** (2.0 / 3.0)
+        return x
+
+    def energy_pn(abd):
+        x = compute_x(abd)
+        E = m - (m * ν * x) / 2 * (1 + (-3 / 4 - ν / 12) * x + (-27 / 8 + 19 / 8 * ν - ν**2 / 24) * x**2)
+        return E
+
+    def angular_momentum_pn(abd):
+        x = compute_x(abd)
+        J_mag = (m**2 * ν * x ** (-1 / 2)) * (
+            1
+            + (3 / 2 + ν / 6) * x
+            + (-27 / 8 + 19 / 8 * ν - ν**2 / 24) * x**2
+            + (135 / 16 + (-6889 / 144 + 41 / 24 * np.pi**2) * ν + 31 / 24 * ν**2 + 7 / 1296 * ν**3) * x**3
+        )
+        return J_mag
+
+    def G_mag_pn(abd):
+        x = compute_x(abd)
+        G_mag = -(1142 / 105) * x ** (5 / 2) * m**2 * np.sqrt(1 - 4 * ν) * ν**2
+        return G_mag
+
+    def orbital_phase(abd):
+        h = abd.h
+        h_21 = h.data[:, h.index(2, 1)]
+        ψ = (-1) * np.unwrap(np.angle(-h_21) - np.pi / 2)
+        return ψ
+
+    return energy_pn, angular_momentum_pn, G_mag_pn, orbital_phase
+
+
+def analytical_CoM_func(θ, t, E, J_mag, G_mag, ψ):
+    """
+    Compute a model time series for boosted center-of-mass (CoM) charge using PN
+    expressions of energy, angular momentum, and CoM charge, along with the
+    phase computed from the h_{21} mode.
+
+    This model timeseries is derived in Khairnar et al. <add_arXiv_link>.
+    It serves as a fitting function that can be passed as the `Gfun` keyword
+    argument to the `map_to_superrest_frame` function. All the arguments are
+    computed over the window used for fixing the frame.
+
+    Parameters
+    ----------
+    θ: ndarray, real, shape(8,)
+        Parameters of the model.
+        - θ[0:3] : components of the boost velocity
+        - θ[3:6] : components of the spatial translation
+        - θ[6:]  : two additional fit parameters referred to as the nuisance
+                   parameters in Khairnar et al. <add_arXiv_link>; their
+                   fitted values are ignored.
+    t: ndarray, real
+        Time array corresponding to the window over which the frame fixing is
+        performed.
+    E: ndarray, real
+        PN approximation for the energy computed over the fitting window.
+    J_mag: ndarray, real
+        PN approximation for the magnitude of angular momentum computed over the
+        fitting window.
+    G_mag: ndarray, real
+        PN approximation for the magnitude of the CoM charge computed over the
+        fitting window.
+    ψ: ndarray, real
+        Unwrapped orbital phase obtained from the (2,1) mode of the strain over
+        the fitting window.
+
+    Returns
+    -------
+    G: ndarray, real, shape(..., 3)
+        Model time series of the boosted center-of-mass charge.
+    """
+    β = θ[0:3][np.newaxis]
+    X = θ[3:6][np.newaxis]
+    α1, α2 = θ[6:]
+
+    # Get the orbital direction vectors, and the angular momentum vector.
+    cosψ, sinψ = np.cos(ψ), np.sin(ψ)
+    nvec = np.array([cosψ, sinψ, 0 * ψ]).T
+    λvec = np.array([-sinψ, cosψ, 0 * ψ]).T
+    J = np.array([0 * t, 0 * t, J_mag]).T
+
+    G = (
+        α1 * (G_mag / E)[:, np.newaxis] * λvec
+        + α2 * (G_mag / E)[:, np.newaxis] * nvec
+        - np.cross(β, J / E[:, np.newaxis])
+        - (t[:, np.newaxis] @ β)
+        + X
+    )
+
+    return G