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use crateld;
use crate;
use crate;
use IauLdBody;
/// Light deflection by multiple solar−system bodies
///
/// For a star, apply light deflection by multiple solar-system bodies,
/// as part of transforming coordinate direction into natural direction.
///
/// This function is part of the International Astronomical Union's
/// SOFA (Standards of Fundamental Astronomy) software collection.
///
/// Status: support function.
///
/// Given:
/// ```
/// n int number of bodies (note 1)
/// b iauLDBODY[n] data for each of the n bodies (Notes 1,2):
/// bm double mass of the body (solar masses, Note 3)
/// dl double deflection limiter (Note 4)
/// pv [2][3] barycentric PV of the body (au, au/day)
/// ob double[3] barycentric position of the observer (au)
/// sc double[3] observer to star coord direction (unit vector)
/// ```
/// Returned:
/// ```
/// sn double[3] observer to deflected star (unit vector)
/// ```
/// 1) The array b contains n entries, one for each body to be
/// considered. If n = 0, no gravitational light deflection will be
/// applied, not even for the Sun.
///
/// 2) The array b should include an entry for the Sun as well as for
/// any planet or other body to be taken into account. The entries
/// should be in the order in which the light passes the body.
///
/// 3) In the entry in the b array for body i, the mass parameter
/// b[i].bm can, as required, be adjusted in order to allow for such
/// effects as quadrupole field.
///
/// 4) The deflection limiter parameter b[i].dl is phi^2/2, where phi is
/// the angular separation (in radians) between star and body at
/// which limiting is applied. As phi shrinks below the chosen
/// threshold, the deflection is artificially reduced, reaching zero
/// for phi = 0. Example values suitable for a terrestrial
/// observer, together with masses, are as follows:
/// ```
/// body i b[i].bm b[i].dl
///
/// Sun 1.0 6e-6
/// Jupiter 0.00095435 3e-9
/// Saturn 0.00028574 3e-10
/// ```
/// 5) For cases where the starlight passes the body before reaching the
/// observer, the body is placed back along its barycentric track by
/// the light time from that point to the observer. For cases where
/// the body is "behind" the observer no such shift is applied. If
/// a different treatment is preferred, the user has the option of
/// instead using the iauLd function. Similarly, iauLd can be used
/// for cases where the source is nearby, not a star.
///
/// 6) The returned vector sn is not normalized, but the consequential
/// departure from unit magnitude is always negligible.
///
/// 7) The arguments sc and sn can be the same array.
///
/// 8) For efficiency, validation is omitted. The supplied masses must
/// be greater than zero, the position and velocity vectors must be
/// right, and the deflection limiter greater than zero.
///
/// Reference:
///
/// Urban, S. & Seidelmann, P. K. (eds), Explanatory Supplement to
/// the Astronomical Almanac, 3rd ed., University Science Books
/// (2013), Section 7.2.4.
///
/// Called:
/// ```
/// iauCp copy p-vector
/// iauPdp scalar product of two p-vectors
/// iauPmp p-vector minus p-vector
/// iauPpsp p-vector plus scaled p-vector
/// iauPn decompose p-vector into modulus and direction
/// iauLd light deflection by a solar-system body
/// ```