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Finally, we output ((mathsf {actor}), (mathsf {actress})) pairs connected to the same (mathsf {country}) in (V_{1}).
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More precisely, (mathbf {R}_{mathsf {D}_{i}}phantom {dot {i}!}) is formed by concatenating the transmit vectors of the sources that are connected to D i.
(mathbf {R}_{mathsf {V}_{j}}phantom {dot {i}!}) is formed by concatenating the transmit vectors of the sources that are connected to V j.
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