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1        METHODS AND LR was suggested by small rotatory activations (carousels) containing the full spe
2                                              Rotatory actomyosin flows during division have been impl
3 meteoritical evidence for an excess of laevo-rotatory amino acids is hard to understand in the contex
4 ion of the responses in the insula, with the rotatory and translational VSs being evoked at more post
5 ave shown that the angle between the central rotatory axes of the monomeric complexes varies between
6 catalytic sites achieve cooperativity during rotatory catalysis.
7  vicinity of the active site, have different rotatory configurations.
8 l superposition-could be used to deconvolute rotatory contributions, designated as [M(X)] and [M(Y)]
9 tion primarily in spinal cord, whereas axial-rotatory disease involves inflammation and demyelination
10                                        Axial-rotatory disease, characterized by uncontrolled axial ro
11 ime-resolved absorption and magnetic optical rotatory dispersion (MORD) measurements of photolyzed my
12 rison of calculated and experimental optical rotatory dispersion (ORD) data provides the most straigh
13 tronic circular dichroism (ECD), and optical rotatory dispersion (ORD) spectroscopy.
14 guration using a combination of NMR, optical rotatory dispersion (ORD), and circular dichroism (CD) s
15 tronic circular dichroism (ECD), and optical rotatory dispersion (ORD).
16 ar dichroism (ECD) spectroscopy, and optical rotatory dispersion (ORD).
17 lowed using nanosecond time-resolved optical rotatory dispersion (ORD).
18 uration, which was also supported by optical rotatory dispersion (ORD).
19 ave been studied using time-resolved optical rotatory dispersion (TRORD) spectroscopy in the visible
20 he protein, nanosecond time-resolved optical rotatory dispersion (TRORD) spectroscopy, which is a dir
21        Previous far-UV time-resolved optical rotatory dispersion (TRORD) studies of the sub-milliseco
22  In 1919, Perucca reported anomalous optical rotatory dispersion from chiral NaClO(3) crystals that w
23 ely due to the belief that molecular optical rotatory dispersion is too insignificant to create the s
24  demonstrate the characterization of optical rotatory dispersion of glucose solutions at two-peak and
25 , electronic circular dichroism, and optical rotatory dispersion spectra and corresponding quantum ch
26 udied using nanosecond time-resolved optical rotatory dispersion spectroscopy.
27 ction reproducing solvent-mediated trends in rotatory dispersion surprisingly well, whereas more mode
28 hirality such as circular dichroism, optical rotatory dispersion, and circularly polarized luminescen
29 m, electronic circular dichroism and optical rotatory dispersion.
30 ross initiating different words, followed by rotatory dynamics during speaking.
31 merical modelling we determine the origin of rotatory effects in these two structures.
32 y incoming, dendritic signals in the case of rotatory flow fields and to reduce them in the case of o
33 to compensate for the confounding effects of rotatory head movements on optic flow.
34 ive, noninvasive diagnosis of posterolateral rotatory instability.
35 le mechanisms for atomization of fluids from rotatory instrumentation exist, but parameters can be co
36           The key actuator is a light-driven rotatory molecular motor linked to polymer chains, which
37     The TS is formed simultaneously with the rotatory motion enabling the translocation of the A-site
38 mple, turn with the direction of large-field rotatory motion, an optomotor reflex that is thought to
39 essing to a severe head tilt, spinning, or a rotatory motion.
40 t are carried out, a mathematical feature of rotatory motions known as noncommutativity.
41 cess is mediated by ATP hydrolysis-triggered rotatory motions of the TRIP13 ATPase, thereby resulting
42 f the tubules and supercoiling, suggesting a rotatory movement of the helix turns relative to each ot
43  hVOR and resulted in a prolongation of post-rotatory nystagmus in darkness.
44 nments, and while their visual processing of rotatory optic flow is understood in exquisite detail, h
45 c nanocolloids, whose nanoscale geometry and rotatory optical activity can be reversibly reconfigured
46 ral, chiral metamaterials can exhibit strong rotatory power at or around resonances, they convert lin
47 s, and metasurfaces have shown giant optical rotatory power but are generally passive and beset with
48  for such synthetic routes due to the strong rotatory power of highly delocalized plasmonic states (M
49 oad transmission maxima accompanied by giant rotatory power, thereby enabling large (>n) polarization
50 ral core that is manifested by lower optical rotatory power.
51   Their conglomerate domains exhibit optical rotatory powers comparable to the highest ever found for
52 stibular systems both encode translatory and rotatory self-motion, their coordinate systems differ.
53  of the cilium may be modeled as a nonlinear rotatory spring, with the linear spring constant k of th
54                        Optical rotations and rotatory strengths are calculated for achiral, conjugate
55 ining to what extent the sum-over-pi --> pi* rotatory strengths are sufficient to account for nonreso
56 nvagination, C1-C2 instability, atlantoaxial rotatory subluxation, congenital occipitocervical synost
57 em coupled to a liquid sample chamber with a rotatory wheel that presents the liquid to the laser bea