1 Despite being
roused a similar number of times, dream frequency was re
2 reported and is neglected in the widely used
Rouse and Zimm approximations.
3 Furthermore, the hypothesis of the
Rouse formula's applicability for floating and sinking p
4 The theory extends the generalized
Rouse (
GR) model used to study the dynamics of polymers
5 e orexin neurons have narcolepsy and fail to
rouse in response to hunger.
6 which inflammation is resolved has begun to
rouse interest.
7 rough mitochondrial replacement therapy have
roused interest in the organellar genome.
8 oefficients of DNA show a clear shift from a
Rouse-
like behavior (DG congruent with N0-0.5) to a rept
9 Rheological data also show a sticky
Rouse-
like relaxation at long times due to collective re
10 solved using a theory based on a Generalized
Rouse Model for Chromosomes (GRMC).
11 omes based on tethered polymers and with the
Rouse model from polymer physics, respectively.
12 the electric field is removed agree with the
Rouse model prediction, which neglects hydrodynamic inte
13 polymer end-to-end distance dynamics from a
Rouse model that includes internal friction.
14 rinsic free-energy profile for a generalized
Rouse model, which mimics the two-state behavior in nucl
15 guish between the Zimm model and the HI-free
Rouse model.
16 rgodic phase transition is predicted for all
Rouse modes at a finite temperature T(A).
17 densimetric Froude number or decreasing the
Rouse number of turbidity currents.
18 velocity, vertical turbulence intensity, and
Rouse number.
19 tio of inertial to gravitational forces) and
Rouse numbers (ratio of settling velocity of sediments t
20 Using numerical simulations of a
Rouse polymer and live cell imaging of the MAT-locus loc
21 fluctuations and timescales of relaxation of
Rouse polymer chains, one can recapitulate the dominant
22 odel for segregation of chromosomal DNA as a
Rouse polymer in a viscoelastic medium with a force appl
23 conewton forces, which are consistent with a
Rouse polymer model.
24 ensin, chromatin behaves as an unconstrained
Rouse polymer with excluded volume, while condensin cons
25 The
Rouse profile was adapted to show that fluvial transport
26 The modified
Rouse profile was applied to describe the positively buo
27 y of physiological responses that ultimately
rouse psychological, cardiovascular, and metabolic impai
28 Our results show that the
Rouse relaxation remains unchanged in a weakly attractiv
29 he manner of a spear, rather than a probe or
rousing tool.
30 l-Ferry model, the activation model, and the
Rouse-
Zimm model based, respectively, on concepts of fre
31 on of activation, Williams-Landel-Ferry, and
Rouse-
Zimm models shows the material to be quite differe