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class BPnP(torch.autograd.Function):
@staticmethod
def forward(ctx, x_2d, z_3d, K, initial_pose_guess=None):
# x_2d: (N, 2) tensor of 2D points
# z_3d: (N, 3) tensor of 3D points
# K: (3, 3) camera intrinsic matrix
# 1. Solve PnP (e.g., using LM algorithm)
# This is a non-differentiable operation in its standard form.
# y_pose = pnp_solver(x_2d, z_3d, K, initial_pose_guess)
# For OpenCV's solvePnP, ensure inputs/outputs are in correct format
# Example: Using an iterative solver like Levenberg-Marquardt
y_pose = solve_pnp_iterative(x_2d.detach().numpy(),
z_3d.detach().numpy(),
K.detach().numpy(),
initial_pose_guess) # convert to torch tensor
# Save inputs for backward pass
ctx.save_for_backward(x_2d, z_3d, K, y_pose)
return y_pose
@staticmethod
def backward(ctx, grad_output_y):
# grad_output_y is the gradient of the loss w.r.t. the output pose y
x_2d, z_3d, K, y_pose = ctx.saved_tensors
# 2. Construct the constraint function f and its Jacobians
# f(a,b) = d_objective / d_pose (where b=pose, a=inputs)
# We need d_f / d_pose (Hessian-like term) and d_f / d_inputs
# For y_pose = g(x_2d, z_3d, K)
# We need d_g/d_x2d, d_g/d_z3d, d_g/d_K
# Let o(x, y, z, K) be the PnP objective function (sum of squared reprojection errors)
# f(x, y, z, K) = grad_y o(x, y, z, K)
# df_dy = jacobian(f, y_pose) # This is effectively (d^2 o) / (dy^2)
# df_dx = jacobian(f, x_2d) # This is (d^2 o) / (dy dx)
# df_dz = jacobian(f, z_3d) # (d^2 o) / (dy dz)
# df_dK = jacobian(f, K) # (d^2 o) / (dy dK)
# These Jacobians can be computed using PyTorch's autograd on the reprojection error computation
# by re-evaluating at y_pose.
# Example for d_g/d_x2d:
# grad_y_pose_wrt_x2d = -inv(df_dy) @ df_dx
# Placeholder for actual Jacobian computations based on IFT:
# This requires careful implementation of the partial derivatives of f
# as described in Section 3.2 and 3.3 of the paper.
# For instance, to get df_dy and df_dx:
# Re-evaluate reprojection error r_i = x_i - pi(z_i | y, K)
# f_j = sum_i <r_i, -2 * (d pi_i / d y_j)>
# Then compute derivatives of f_j w.r.t y_k and x_l.
# grad_x2d = None
# grad_z3d = None
# grad_K = None
# if ctx.needs_input_grad[0]: # Gradient for x_2d
# J_yx = compute_jacobian_y_wrt_x(x_2d, z_3d, K, y_pose) # via IFT
# grad_x2d = J_yx.T @ grad_output_y
# if ctx.needs_input_grad[1]: # Gradient for z_3d
# J_yz = compute_jacobian_y_wrt_z(x_2d, z_3d, K, y_pose) # via IFT
# grad_z3d = J_yz.T @ grad_output_y
# if ctx.needs_input_grad[2]: # Gradient for K
# J_yK = compute_jacobian_y_wrt_K(x_2d, z_3d, K, y_pose) # via IFT
# grad_K = J_yK.T @ grad_output_y
# The actual implementation would involve setting up the equations from (10)-(14)
# and solving the linear system for the gradients. PyTorch's autograd can be
# leveraged to compute the partial derivatives of f.
# Simplified sketch of computing Jacobians (requires careful implementation of equations 10-14):
# Assume y is parameterized by m parameters (e.g., 6 for axis-angle)
# K_params could be focal lengths and principal point (4 parameters)
# Compute df_dy (m x m matrix), df_dx (m x 2n matrix), etc.
# using PyTorch's autograd on the expression for f_j
# inv_df_dy = torch.inverse(df_dy)
# J_yx = -inv_df_dy @ df_dx
# J_yz = -inv_df_dy @ df_dz
# J_yK = -inv_df_dy @ df_dK_params (if K is parameterized)
# grad_x2d = J_yx.T @ grad_output_y
# grad_z3d = J_yz.T @ grad_output_y
# grad_K_params = J_yK.T @ grad_output_y
# The authors provide their PyTorch implementation at http://github.com/BoChenYS/BPnP
# Return gradients for x_2d, z_3d, K, initial_pose_guess (None for last)
# return grad_x2d, grad_z3d, grad_K, None
raise NotImplementedError("Actual backward pass requires full IFT Jacobian computation as in the paper's code.")
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