1 reported and is neglected in the widely used Rouse and Zimm approximations.

2           The theory extends the generalized Rouse (GR) model used to study the dynamics of polymers

3 e orexin neurons have narcolepsy and fail to rouse in response to hunger.

4 rough mitochondrial replacement therapy have roused interest in the organellar genome.

5 oefficients of DNA show a clear shift from a Rouse-like behavior (DG congruent with N0-0.5) to a rept

6          Rheological data also show a sticky Rouse-like relaxation at long times due to collective re

7 omes based on tethered polymers and with the Rouse model from polymer physics, respectively.

8 the electric field is removed agree with the Rouse model prediction, which neglects hydrodynamic inte

9  polymer end-to-end distance dynamics from a Rouse model that includes internal friction.

10 rinsic free-energy profile for a generalized Rouse model, which mimics the two-state behavior in nucl

11 guish between the Zimm model and the HI-free Rouse model.

12 rgodic phase transition is predicted for all Rouse modes at a finite temperature T(A).

13             Using numerical simulations of a Rouse polymer and live cell imaging of the MAT-locus loc

14 odel for segregation of chromosomal DNA as a Rouse polymer in a viscoelastic medium with a force appl

15 y of physiological responses that ultimately rouse psychological, cardiovascular, and metabolic impai

16                    Our results show that the Rouse relaxation remains unchanged in a weakly attractiv

17 he manner of a spear, rather than a probe or rousing tool.

18 l-Ferry model, the activation model, and the Rouse-Zimm model based, respectively, on concepts of fre

19 on of activation, Williams-Landel-Ferry, and Rouse-Zimm models shows the material to be quite differe