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Table H.1.

Physical viability and geometric consistency of BNS population models.

Universal top-hat Non-univ. flat Non-univ. log-normal Universal structured
αCE 0.5 1.0 3.0 5.0 0.5 1.0 3.0 5.0 0.5 1.0 3.0 5.0 0.5 1.0 3.0 5.0
F ×a ✓ ✓ × × ✓ ✓ × ✓ ✓ ✓ ✓ × ✓ ✓ ×
K265 ×a × × ×a × × × × ✓b ✓ ✓ ✓b × × × ×
K150 × × ✓ × × × × × ✓ ✓ ✓ ✓ × × × ×
QCBSE ×a, c × ×a ×a × × × × ×b ✓ ✓b ✓b × × × ×
QCBB ✓ × × × ✓ ✓a × × ✓ ✓ ✓ ✓b × × × ×
RBSE × ×a ✓ × ×a ✓ ✓ ×a ✓b ✓ ✓ ✓b × ✓ ✓ ×
LK ×a, c ×c × ✓ × × ✓ ✓ ×b ✓b ✓ ✓ × × × ✓
LC ×a × ✓ ✓ × × ✓ ✓ ✓b ✓ ✓ ✓ × × ✓ ✓
LX ×a, c × ✓ ✓ × × ✓ ✓ ×b ✓b ✓ ✓ × × ✓ ✓
OPT ×a, c × ✓ ×c × × ✓ ✓ ×b ✓ ✓ ✓ × × ✓ ✓
F19 ×a ✓ ✓ × ×a ✓ ✓ × ✓ ✓ ✓ ✓ × ✓ ✓ ×
F5M ×a ✓ ✓ ×a × ✓ ✓ × ✓ ✓ ✓ ✓ × ✓ ✓ ×
SND × ×c ✓ × ×a ✓ ✓ × ✓ ✓ ✓ ✓ × ✓ ✓ ×
QHE × ✓ ✓ × × ✓ ✓ × ✓ ✓ ✓ ✓ × ✓ ✓ ×
NT × ×c ×c × × ✓ ✓ × ✓ ✓ ✓ ✓ × ✓ ✓ ×
NTC × ✓ ✓ ✓ × ✓ ✓ ✓ ✓ ✓ ✓ ✓ × ✓ ✓ ×

Notes. Checkmarks (✓) indicate physical median jet fractions (fj ≤ 1). Crosses (×) indicate non-physical scenarios with median fj > 1. The aperture angle is fixed at 6.1° for top-hat models and the distribution median for non-universal models, following Rouco Escorial et al. (2023).

a

Required θ* > 15.4°.

b

More than 10% of the inferred jet population exceeds θc = 15°.

c

Required θ* exceeded prior bounds.

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