Class

NumCosmoWLEllipticitySeriesTrace

Description [src]

final class NumCosmo.WLEllipticitySeriesTrace : GObject.Object
{
  /* No available fields */
}

Truncated $g$-Taylor series of nc_wl_ellipticity.h’s own closed-form reduced-shear kernels: $\chi_I(\chi_L,g)$ (via apply_shear_inv) and the linear (not log) Jacobian $\mathrm{Jac}(\chi_L,g)=|\det J|$ (via det_jac), one object per ellipticity convention, mirroring that file’s own _trace/_trace_det split.

Both conventions have closed forms in $g$ (no finite differences anywhere) — see docs/theory/wl_shape_marginalization_series.qmd and dev-notes/wl_shape_series_marginalization_derivation.py sections 10-11 (verify_chi_closed_form_pieces, verify_eps_closed_form_pieces) for the derivation and symbolic/numeric verification these two classes mirror:

  • TRACE_DET (epsilon): $\chi_I=(\chi_L-g)/(1-g\chi_L)$, holomorphic, so $\mathrm{Jac}=|f’(\chi_L,-g)|^2$; both closed-form power series in $g$ with no recursion needed at all.
  • TRACE (chi): $\chi_I(\chi_L,g)=f_\chi(\chi_L,-g)$ is a ratio of two QUADRATICS in $g$ ($\chi_L,\bar\chi_L$ fixed), so its Taylor series follows a 2-term power-series-division recursion; the chi map is NOT holomorphic in $\chi_L$ (involves $\bar\chi_L$ too), so the Jacobian needs the full real $2\times2$ determinant, itself a closed-form reciprocal-series-cubed construction. Both closed forms match the already-shipped nc_wl_ellipticity_apply_shear_inv_trace/nc_wl_ellipticity_det_jac_trace to machine precision (see dev-notes’ verify_inverse_map_and_jacobian_match_production and this module’s own test suite, tests/c/nc/lss/wl/test_nc_wl_ellipticity_series.c, which checks eval()+Horner-evaluate-at-small-g directly against those already-shipped closed forms).

Every intermediate NcmLaurentSeriesTPS/NcmLaurentSeries this needs is owned directly and allocated once at construction (order is CONSTRUCT_ONLY): eval() only ever refills already-existing storage, never allocates. TRACE_DET’s chi and TRACE_DET’s own $\chi_L$/$\bar\chi_L$/d1 quantities (shared between its chi and jac computation, since both run sequentially against the same $\rho$ within one eval() call) are the only scratch either class needs beyond the named NcmLaurentSeriesTPS series themselves.

Ancestors

Constructors

nc_wl_ellipticity_series_trace_new
No description available.

Functions

nc_wl_ellipticity_series_trace_clear
No description available.

Instance methods

nc_wl_ellipticity_series_trace_eval

Refills sers chi and jac series (see nc_wl_ellipticity_series_trace_get_chi()/ _get_jac()) at $\chi_L=\rho\,w$. $\chi_L,\bar\chi_L,d_1=-(\chi_L+\bar\chi_L)$ are computed once here and shared by both the chi and jac recursions (identical quantities, same $\rho$, never needed concurrently). Also fills nc_wl_ellipticity_series_trace_get_abs_sq() ($|\chi_I(\chi_L,g)|^2= \chi_I\overline{\chi_I}$, population-independent, exactly the $\rho^2(g)$ input nc_galaxy_shape_pop_eval_p_rho2_g_series() needs).

nc_wl_ellipticity_series_trace_free
No description available.

nc_wl_ellipticity_series_trace_get_abs_sq
No description available.

nc_wl_ellipticity_series_trace_get_chi
No description available.

nc_wl_ellipticity_series_trace_get_jac
No description available.

nc_wl_ellipticity_series_trace_get_order
No description available.

nc_wl_ellipticity_series_trace_ref
No description available.

Methods inherited from GObject (43)

Please see GObject for a full list of methods.

Properties

NumCosmo.WLEllipticitySeriesTrace:order

Truncation order $N$ of the $g$-power series. Immutable for the object’s whole life — every NcmLaurentSeriesTPS/NcmLaurentSeries this needs is sized and allocated once, here.

Signals

Signals inherited from GObject (1)
GObject::notify

The notify signal is emitted on an object when one of its properties has its value set through g_object_set_property(), g_object_set(), et al.

Class structure

struct NumCosmoWLEllipticitySeriesTraceClass {
  GObjectClass parent_class;
  
}

No description available.

Class members
parent_class: GObjectClass

No description available.