Clean up TODOs and FIXMEs

desc/backend.py

@@ -65,7 +65,7 @@
     )
 )
 
-if use_jax:  # noqa: C901 - FIXME: simplify this, define globally and then assign?
+if use_jax:  # noqa: C901
     from jax import custom_jvp, jit, vmap
 
     imap = jax.lax.map

desc/basis.py

@@ -1098,13 +1098,13 @@ def evaluate(
         if not len(modes):
             return np.array([]).reshape((len(nodes), 0))
 
-        # TODO: avoid duplicate calculations when mixing derivatives
+        # TODO(#1243): avoid duplicate calculations when mixing derivatives
         r, t, z = nodes.T
         l, m, n = modes.T
         lm = modes[:, :2]
 
         if unique:
-            # TODO: can avoid this here by using grid.unique_idx etc
+            # TODO(#1243): can avoid this here by using grid.unique_idx etc
             # and adding unique_modes attributes to basis
             _, ridx, routidx = np.unique(
                 r, return_index=True, return_inverse=True, axis=0
@@ -1364,7 +1364,6 @@ def polyval_vec(p, x, prec=None):
 def _polyval_exact(p, x, prec):
     p = np.atleast_2d(p)
     x = np.atleast_1d(x).flatten()
-    # TODO: possibly multithread this bit
     mpmath.mp.dps = prec
     y = np.array([np.asarray(mpmath.polyval(list(pi), x)) for pi in p])
     return y.astype(float)

desc/batching.py

@@ -102,7 +102,6 @@ def f_(carry, x):
     return res_append
 
 
-# TODO in_axes a la vmap?
 def _scanmap(fun, scan_fun, argnums=0):
     """A helper function to wrap f with a scan_fun."""
 

desc/coils.py

@@ -1901,8 +1901,8 @@ def save_in_makegrid_format(self, coilsFilename, NFP=None, grid=None):
             if None, will default to the coil compute functions's
             default grid
         """
-        # TODO: name each group based off of CoilSet name?
-        # TODO: have CoilGroup be automatically assigned based off of
+        # TODO(#1376): name each group based off of CoilSet name?
+        # TODO(#1376): have CoilGroup be automatically assigned based off of
         # CoilSet if current coilset is a collection of coilsets?
 
         NFP = 1 if NFP is None else NFP
@@ -2697,7 +2697,7 @@ def insert(self, i, new_item):
         self._coils.insert(i, new_item)
 
     @classmethod
-    def from_makegrid_coilfile(  # noqa: C901 - FIXME: simplify this
+    def from_makegrid_coilfile(  # noqa: C901
         cls, coil_file, method="cubic", ignore_groups=False, check_intersection=True
     ):
         """Create a MixedCoilSet of SplineXYZCoils from a MAKEGRID coil txtfile.

desc/compute/_geometry.py

@@ -194,7 +194,7 @@ def _A_of_z(params, transforms, profiles, data, **kwargs):
     data=["Z", "n_rho", "e_theta|r,p", "rho"],
     parameterization=["desc.geometry.surface.FourierRZToroidalSurface"],
     resolution_requirement="rt",  # just need max(rho) near 1
-    # FIXME: Add source grid requirement once omega is nonzero.
+    # TODO(#568): Add source grid requirement once omega is nonzero.
 )
 def _A_of_z_FourierRZToroidalSurface(params, transforms, profiles, data, **kwargs):
     # Denote any vector v = [vᴿ, v^ϕ, vᶻ] with a tuple of its contravariant components.
@@ -213,7 +213,7 @@ def _A_of_z_FourierRZToroidalSurface(params, transforms, profiles, data, **kwarg
         line_integrals(
             transforms["grid"],
             data["Z"] * n[:, 2] * safenorm(data["e_theta|r,p"], axis=-1),
-            # FIXME: Works currently for omega = zero, but for nonzero omega
+            # TODO(#568): Works currently for omega = zero, but for nonzero omega
             #  we need to integrate over theta at constant phi.
             #  Should be simple once we have coordinate mapping and source grid
             #  logic from GitHub pull request #1024.
@@ -449,7 +449,7 @@ def _perimeter_of_z(params, transforms, profiles, data, **kwargs):
         line_integrals(
             transforms["grid"],
             safenorm(data["e_theta|r,p"], axis=-1),
-            # FIXME: Works currently for omega = zero, but for nonzero omega
+            # TODO(#568): Works currently for omega = zero, but for nonzero omega
             #  we need to integrate over theta at constant phi.
             #  Should be simple once we have coordinate mapping and source grid
             #  logic from GitHub pull request #1024.

desc/compute/_omnigenity.py

@@ -47,7 +47,7 @@ def fitfun(x):
     return data
 
 
-# TODO: do math to change definition of nu so that we can just use B_zeta_mn here
+# TODO (#568): do math to change definition of nu so that we can just use B_zeta_mn here
 @register_compute_fun(
     name="B_phi_mn",
     label="B_{\\phi, m, n}",
@@ -63,7 +63,7 @@ def fitfun(x):
     data=["B_phi|r,t"],
     resolution_requirement="tz",
     grid_requirement={"is_meshgrid": True},
-    aliases="B_zeta_mn",  # TODO: remove when phi != zeta
+    aliases="B_zeta_mn",  # TODO(#568): remove when phi != zeta
     M_booz="int: Maximum poloidal mode number for Boozer harmonics. Default 2*eq.M",
     N_booz="int: Maximum toroidal mode number for Boozer harmonics. Default 2*eq.N",
 )

desc/compute/_profiles.py

@@ -1378,7 +1378,7 @@ def _iota_num_rrr(params, transforms, profiles, data, **kwargs):
                 - beta * data["sqrt(g)_rrr"],
                 data["sqrt(g)"],
             ),
-            # Todo: axis limit of beta_rrr
+            # TODO(#587): axis limit of beta_rrr
             #   Computed with four applications of l’Hôpital’s rule.
             #   Requires sqrt(g)_rrrr and fourth derivatives of basis vectors.
             jnp.nan,
@@ -1656,7 +1656,7 @@ def _iota_den_rrr(params, transforms, profiles, data, **kwargs):
             - gamma * data["sqrt(g)_rrr"],
             data["sqrt(g)"],
         ),
-        # Todo: axis limit
+        # TODO(#587): axis limit
         #   Computed with four applications of l’Hôpital’s rule.
         #   Requires sqrt(g)_rrrr and fourth derivatives of basis vectors.
         jnp.nan,
@@ -1713,7 +1713,7 @@ def _q(params, transforms, profiles, data, **kwargs):
     return data
 
 
-# TODO: add K(rho,theta,zeta)*grad(rho) term
+# TODO (#1381): add K(rho,theta,zeta)*grad(rho) term
 @register_compute_fun(
     name="I",
     label="I",

desc/compute/_stability.py

@@ -76,7 +76,7 @@ def _D_current(params, transforms, profiles, data, **kwargs):
                 / data["|grad(psi)|"] ** 3
                 * dot(Xi, data["B"])
             ),
-            # Todo: implement equivalent of equation 4.3 in desc coordinates
+            # TODO(#671): implement equivalent of equation 4.3 in desc coordinates
             jnp.nan,
         )
     )

desc/compute/_surface.py

@@ -3,7 +3,7 @@
 from .data_index import register_compute_fun
 from .geom_utils import rpz2xyz
 
-# TODO: review when zeta no longer equals phi
+# TODO(#568): review when zeta no longer equals phi
 
 
 @register_compute_fun(
@@ -27,7 +27,7 @@
 def _x_FourierRZToroidalSurface(params, transforms, profiles, data, **kwargs):
     R = transforms["R"].transform(params["R_lmn"])
     Z = transforms["Z"].transform(params["Z_lmn"])
-    # TODO: change when zeta no longer equals phi
+    # TODO(#568): change when zeta no longer equals phi
     phi = transforms["grid"].nodes[:, 2]
     coords = jnp.stack([R, phi, Z], axis=1)
     # default basis for "x" is rpz, the conversion will be done

desc/continuation.py

@@ -748,7 +748,6 @@ def solve_continuation(  # noqa: C901
         if len(deltas) > 0:
             if verbose > 0:
                 print("Perturbing equilibrium")
-            # TODO: pass Jx if available
             eqp = eqfam[ii - 1].copy()
             objective_i = get_equilibrium_objective(
                 eq=eqp, mode=objective, jac_chunk_size=jac_chunk_size

desc/equilibrium/coords.py

@@ -107,7 +107,7 @@ def map_coordinates(  # noqa: C901
 
     profiles = get_profiles(inbasis + basis_derivs, eq)
 
-    # TODO: make this work for permutations of in/out basis
+    # TODO (#1382): make this work for permutations of in/out basis
     if outbasis == ("rho", "theta", "zeta"):
         if inbasis == ("rho", "alpha", "zeta"):
             if "iota" in kwargs:
@@ -286,7 +286,7 @@ def _distance_body(i, idx):
     return yg[idx]
 
 
-# TODO: decide later whether to assume given phi instead of zeta.
+# TODO(#568): decide later whether to assume given phi instead of zeta.
 def _map_PEST_coordinates(
     coords,
     L_lmn,
@@ -395,7 +395,7 @@ def fixup(x, *args):
     return out
 
 
-# TODO: decide later whether to assume given phi instead of zeta.
+# TODO(#568): decide later whether to assume given phi instead of zeta.
 def _map_clebsch_coordinates(
     coords,
     iota,
@@ -766,7 +766,7 @@ def get_rtz_grid(
     return desc_grid
 
 
-# TODO: deprecated, remove eventually
+# TODO(#1383): deprecated, remove eventually
 def compute_theta_coords(
     eq, flux_coords, L_lmn=None, tol=1e-6, maxiter=20, full_output=False, **kwargs
 ):

desc/equilibrium/equilibrium.py

@@ -1443,7 +1443,6 @@ def axis(self, new):
     @property
     def spectral_indexing(self):
         """str: Type of indexing used for the spectral basis."""
-        # TODO: allow this to change?
         return self._spectral_indexing
 
     @property
@@ -1972,8 +1971,6 @@ def from_near_axis(
             raise ValueError("Input must be a pyQSC or pyQIC solution.") from e
 
         rho, _ = special.js_roots(L, 2, 2)
-        # TODO: could make this an OCS grid to improve fitting, need to figure out
-        # how concentric grids work with QSC
         grid = LinearGrid(rho=rho, theta=ntheta, zeta=na_eq.phi, NFP=na_eq.nfp)
         basis_R = FourierZernikeBasis(
             L=L,

desc/equilibrium/initial_guess.py

@@ -20,7 +20,7 @@
 from desc.utils import copy_coeffs, warnif
 
 
-def set_initial_guess(eq, *args, ensure_nested=True):  # noqa: C901 - FIXME: simplify
+def set_initial_guess(eq, *args, ensure_nested=True):  # noqa: C901
     """Set the initial guess for the flux surfaces, eg R_lmn, Z_lmn, L_lmn.
 
     Parameters

desc/equilibrium/utils.py

@@ -146,7 +146,7 @@ def parse_axis(axis, NFP=1, sym=True, surface=None):
             name="axis",
         )
     elif axis is None:  # use the center of surface
-        # TODO: make this method of surface, surface.get_axis()?
+        # TODO (#1384): make this method of surface, surface.get_axis()?
         if isinstance(surface, FourierRZToroidalSurface):
             axis = FourierRZCurve(
                 R_n=surface.R_lmn[np.where(surface.R_basis.modes[:, 1] == 0)],
@@ -160,7 +160,7 @@ def parse_axis(axis, NFP=1, sym=True, surface=None):
                 NFP=NFP,
             )
         elif isinstance(surface, ZernikeRZToroidalSection):
-            # FIXME: include m=0 l!=0 modes
+            # TODO (#782): include m=0 l!=0 modes
             axis = FourierRZCurve(
                 R_n=surface.R_lmn[
                     np.where(

desc/geometry/surface.py

@@ -339,7 +339,7 @@ def from_input_file(cls, path, **kwargs):
         )
         return surf
 
-    # TODO: add k value for number of rotations per field period
+    # TODO (#1385): add k value for number of rotations per field period
     @classmethod
     def from_qp_model(
         cls,

desc/grid.py

@@ -22,7 +22,6 @@
 class _Grid(IOAble, ABC):
     """Base class for collocation grids."""
 
-    # TODO: calculate weights automatically using voronoi / delaunay triangulation
     _io_attrs_ = [
         "_L",
         "_M",

desc/input_reader.py

@@ -137,7 +137,7 @@ def _get_parser_(self):
         """
         return get_parser()
 
-    def parse_inputs(self, fname=None):  # noqa: C901 - FIXME: simplify this
+    def parse_inputs(self, fname=None):  # noqa: C901
         """Read input from DESC input file; converts from VMEC input if necessary.
 
         Parameters
@@ -386,7 +386,6 @@ def parse_inputs(self, fname=None):  # noqa: C901 - FIXME: simplify this
             if match:
                 inputs["bdry_mode"] = words[0].lower()
                 flag = True
-                # TODO: set bdry_mode automatically based on bdry coeffs
 
             # coefficient indices
             match = re.search(r"l\s*:\s*" + num_form, command, re.IGNORECASE)
@@ -970,7 +969,7 @@ def vmec_to_desc_input(vmec_fname, desc_fname):
         InputReader.write_desc_input(desc_fname, inputs, header)
 
     @staticmethod
-    def parse_vmec_inputs(vmec_fname, threshold=0):  # noqa: C901 - FIXME: simplify this
+    def parse_vmec_inputs(vmec_fname, threshold=0):  # noqa: C901
         """Parse a VMEC input file into a dictionary of DESC inputs.
 
         Parameters

desc/integrals/bounce_utils.py

@@ -83,7 +83,7 @@ def _check_spline_shape(knots, g, dg_dz, pitch_inv=None):
         to that field line.
 
     """
-    errorif(knots.ndim != 1, msg=f"knots should be 1d; got shape {knots.shape}.")
+    errorif(knots.ndim != 1, msg=f"knots should be 1d, got shape {knots.shape}.")
     errorif(
         g.shape[-2] != (knots.size - 1),
         msg=(
@@ -390,7 +390,8 @@ def loop(z):  # over num well axis
             )
 
         result = jnp.moveaxis(
-            # TODO: Use batch_size arg of imap after increasing JAX version requirement.
+            # TODO (#1386): Use batch_size arg of imap after
+            #  increasing JAX version requirement.
             imap(loop, (jnp.moveaxis(z1, -1, 0), jnp.moveaxis(z2, -1, 0)))[1],
             source=0,
             destination=-1,

desc/integrals/interp_utils.py

@@ -82,7 +82,7 @@ def polyval_vec(*, x, c):
     )
 
 
-# TODO: Eventually do a PR to move this stuff into interpax.
+# TODO (#1388): Eventually do a PR to move this stuff into interpax.
 
 
 def _subtract_last(c, k):

desc/integrals/surface_integral.py

@@ -8,8 +8,8 @@
 from desc.grid import ConcentricGrid, LinearGrid
 from desc.utils import errorif, warnif
 
-# TODO: Make the surface integral stuff objects with a callable method instead of
-#       returning functions. Would make simpler, allow users to actually see the
+# TODO (#1389): Make the surface integral stuff objects with a callable method instead
+#       of returning functions. Would make simpler, allow users to actually see the
 #       docstrings of the methods, and less bookkeeping to default to more
 #       efficient methods on tensor product grids.
 
@@ -227,8 +227,6 @@ def surface_integrals_map(grid, surface_label="rho", expand_out=True, tol=1e-14)
     )
     spacing = jnp.prod(spacing, axis=1)
 
-    # Todo: Define mask as a sparse matrix once sparse matrices are no longer
-    #       experimental in jax.
     if has_idx:
         # The ith row of masks is True only at the indices which correspond to the
         # ith surface. The integral over the ith surface is the dot product of the

desc/magnetic_fields/_core.py

@@ -2401,7 +2401,7 @@ def __init__(
             assert len(x_lmn) == self.x_basis.num_modes
             self._x_lmn = x_lmn
 
-        # TODO: should we not allow some types of helicity?
+        # TODO (#1390): should we not allow some types of helicity?
         helicity_sign = sign(helicity[0]) * sign(helicity[1])
         warnif(
             self.helicity != (0, self.NFP * helicity_sign)