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Weak gravitational lensing is the only filament probe that weighs total mass directly, dark and baryonic alike. This paper computes the lensing budget for a stated stacked detection: an excess surface density of 1.0 solar mass per square parsec at a projected radius of one megaparsec around the filament axis, for lenses at redshift 0.4 and sources at redshift 1.0. The critical surface density for that geometry is 2.75e+03 solar masses per square parsec, so the tangential shear at one megaparsec is 0.0003641 — a distortion of a few parts in ten thousand, far below any single-filament measurement and accessible only by stacking thousands of systems. Integrating the stated profile, falling as inverse radius between 0.3 and 2 megaparsecs, over a ten-megaparsec segment gives a segment mass of 1.07e+14 solar masses and a line mass of 1.07e+13 solar masses per megaparsec, of which the cosmic baryon share is 1.67e+12. The angular diameter distances entering the geometry, 1.15e+03 megaparsecs to the lens and 1.7e+03 to the sources, are computed by numerical integration over the stated expansion history.
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William Alexander Aldred (2026) studied this question.
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