000877303 001__ 877303 000877303 005__ 20240610121159.0 000877303 0247_ $$2doi$$a10.1103/PhysRevE.101.052612 000877303 0247_ $$2ISSN$$a1063-651X 000877303 0247_ $$2ISSN$$a1095-3787 000877303 0247_ $$2ISSN$$a1538-4519 000877303 0247_ $$2ISSN$$a1539-3755 000877303 0247_ $$2ISSN$$a1550-2376 000877303 0247_ $$2ISSN$$a2470-0045 000877303 0247_ $$2ISSN$$a2470-0053 000877303 0247_ $$2ISSN$$a2470-0061 000877303 0247_ $$2Handle$$a2128/24959 000877303 0247_ $$2WOS$$aWOS:000535461000011 000877303 0247_ $$2altmetric$$aaltmetric:77063609 000877303 037__ $$aFZJ-2020-02119 000877303 082__ $$a530 000877303 1001_ $$0P:(DE-Juel1)171524$$aMartin-Gomez, Aitor$$b0 000877303 245__ $$aHydrodynamics of polymers in an active bath 000877303 260__ $$aWoodbury, NY$$bInst.$$c2020 000877303 264_1 $$2Crossref$$3online$$bAmerican Physical Society (APS)$$c2020-05-26 000877303 264_1 $$2Crossref$$3print$$bAmerican Physical Society (APS)$$c2020-05-01 000877303 3367_ $$2DRIVER$$aarticle 000877303 3367_ $$2DataCite$$aOutput Types/Journal article 000877303 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1591172381_4524 000877303 3367_ $$2BibTeX$$aARTICLE 000877303 3367_ $$2ORCID$$aJOURNAL_ARTICLE 000877303 3367_ $$00$$2EndNote$$aJournal Article 000877303 520__ $$aThe conformational and dynamical properties of active polymers in solution are determined by the nature of the activity. Here, the behavior of polymers with self-propelled, active Brownian particle-type monomers differs qualitatively from that of polymers with monomers driven externally by colored-noise forces. We present simulation and theoretical results for polymers in solution in the presence of external active noise. In simulations, a semiflexible bead-spring chain is considered, in analytical calculations, a continuous linear wormlike chain. Activity is taken into account by independent monomer or site velocities, with orientations changing in a diffusive manner. In simulations, hydrodynamic interactions (HIs) are taken into account by the Rotne-Prager-Yamakawa tensor or by an implementation of the active polymer in the multiparticle-collision-dynamics approach for fluids. To arrive at an analytical solution, the preaveraged Oseen tensor is employed. The active process implies a dependence of the stationary-state properties on HIs via the polymer relaxation times. With increasing activity, HIs lead to an enhanced swelling of flexible polymers, and the conformational properties differ substantially from those of polymers with self-propelled monomers in the presence of HIs, or free-draining polymers. The polymer mean-square displacement is enhanced by HIs. Over a wide range of timescales, hydrodynamics leads to a subdiffusive regime of the site mean-square displacement for flexible active polymers, with an exponent of 5/7, larger than that of the Rouse (1/2) and Zimm (2/3) models of passive polymers. 000877303 536__ $$0G:(DE-HGF)POF3-551$$a551 - Functional Macromolecules and Complexes (POF3-551)$$cPOF3-551$$fPOF III$$x0 000877303 542__ $$2Crossref$$i2020-05-26$$uhttps://link.aps.org/licenses/aps-default-license 000877303 588__ $$aDataset connected to CrossRef 000877303 7001_ $$0P:(DE-Juel1)164141$$aEisenstecken, Thomas$$b1 000877303 7001_ $$0P:(DE-Juel1)130665$$aGompper, Gerhard$$b2$$eCorresponding author 000877303 7001_ $$0P:(DE-Juel1)131039$$aWinkler, Roland G.$$b3$$eCorresponding author 000877303 77318 $$2Crossref$$3journal-article$$a10.1103/physreve.101.052612$$bAmerican Physical Society (APS)$$d2020-05-26$$n5$$p052612$$tPhysical Review E$$v101$$x2470-0045$$y2020 000877303 773__ 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Doi$$2Crossref$$oM. Doi The Theory of Polymer Dynamics 1986$$tThe Theory of Polymer Dynamics$$y1986 000877303 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1063/1.436761 000877303 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1063/1.5001886 000877303 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevE.67.066705 000877303 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1016/j.jcp.2009.09.024 000877303 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1063/1.3077860 000877303 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevE.90.033314 000877303 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1063/1.4893766 000877303 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1063/1.4996525 000877303 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevLett.97.258101 000877303 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1063/1.469027 000877303 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1063/1.1537247 000877303 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1021/ma802017g 000877303 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1063/1.2753160 000877303 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1088/1361-6633/aab3ed 000877303 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1038/nature01935 000877303 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1126/science.1072133