
Panel-data deconvolution of the individual and idiosyncratic densities
Source:R/horowitz_native7.R
morie_panel_deconvolution.RdFor \(Y_{jt} = X_{jt}'\beta + U_j + \varepsilon_{jt}\), recovers \(f_U\) and \(f_\varepsilon\) nonparametrically via (5.21) through (5.26).
Usage
morie_panel_deconvolution(
y,
x,
beta,
nu_U = NULL,
nu_eps = NULL,
grid_u = NULL,
grid_z = NULL,
kernel = "fourfold"
)Arguments
- y
numeric matrix (n, T) of responses.
- x
numeric array (n, T, d) or matrix (n*T, d).
- beta
root-n consistent coefficients.
- nu_U, nu_eps
smoothing bandwidths; sigma_eps / sqrt(log n) for f_U and 0.5 sigma_eps N^(-1/5) for f_eps when NULL, sigma_eps = sd(eta) / sqrt(2).
- grid_u, grid_z
evaluation points.
- kernel
"fourfold"(default; the book's characteristic function, assumption PHU7) or"flattop"(indicator of \([-1, 1]\): outside PHU7, higher-order bias, 2-3 times smaller errors in simulation). Each has its own default bandwidths.
Value
list: grid_u, f_U, grid_z, f_eps, psi_eps_from_root, symmetry_required, nu_U, nu_eps, fastest_possible_rate, asymptotics_in, n, T, d, method.
Details
The levels residual estimates \(U + \varepsilon\), so \(\psi_W = \psi_U\psi_\varepsilon\); the within-individual difference removes \(U_j\) completely and estimates a difference of two independent copies of \(\varepsilon\), so \(\psi_\eta = |\psi_\varepsilon|^2\). Hence \(\psi_\varepsilon = \psi_\eta^{1/2}\).
The square root is what the symmetry assumption is for.
\(\psi_\eta\) determines \(\psi_\varepsilon\) only up to sign;
symmetry about zero makes it real and non-vanishing makes it
positive, which picks the root. This is a HARDER problem than
Sec. 5.1, where the contaminating distribution was known, and the
rates are just as slow – for normal \(\varepsilon\) the fastest
possible is \((\log n)^{-1}\). Asymptotics are in n with T
FIXED. Mirrors morie.fn.hrzpanel.