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Fig. 4.

Fig. 4. Refer to the following caption and surrounding text.

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Cumulative S/N forecasts for detecting the gravitomagnetic lensing signal as a function of maximum angular multipole, . All forecasts assume a sky fraction of fsky ≈ 0.25. Left: S/N for the cross-correlation of the lensing convergence with the reconstructed momentum convergence field for different galaxy number densities ( n ¯ g Mathematical equation: $ \bar{n}_g $, in units of Mpc−3); solid lines show cosmic-variance-limited lensing noise, while dashed lines show stage-four lensing survey noise. Middle: Cosmic-variance-limited S/N for three different momentum field tracers: the true, noiseless field (κj)∥); the reconstructed field ( κ ̂ j ) Mathematical equation: $ \hat{\kappa}_{j){\parallel}} $), assuming a galaxy density of n ¯ g = 10 2 Mathematical equation: $ \bar{n}_g = 10^{-2} $ Mpc−3; and the kinetic Sunyaev-Zel’dovich (kSZ) effect. Right: S/N for the cross-correlation after subtracting a reconstructed density convergence field ( κ ̂ ϕ Mathematical equation: $ \hat{\kappa}_{\phi} $), where the different lines show the effect of varying the galaxy density used for the density reconstruction.

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