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Similarly to what done in the previous section, we decompose the force coupling matrix and the mobil- ity matrix into their diagonal and non-diagonal parts, ˆK= ˆKd + ˆKnd and ˆµ= ˆµd","work_id":"84079ba1-9096-4476-8617-43cd203d1bf3","year":null},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":4,"title":"A. Hilfinger and J. Paulsson, Separating intrinsic from extrinsic fluctuations in dynamic biological systems, Pro- ceedings of the National Academy of Sciences108, 12167 (2011)","work_id":"26319361-52c9-4c9c-a0db-9cbc207a5c67","year":2011},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":5,"title":"P. Thomas, N. Popovi´ c, and R. 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