ライフサイエンスコーパス: rotatory

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1 METHODS AND LR was suggested by small rotatory activations (carousels) containing the full spe

2 meteoritical evidence for an excess of laevo-rotatory amino acids is hard to understand in the contex

3 ion of the responses in the insula, with the rotatory and translational VSs being evoked at more post

4 catalytic sites achieve cooperativity during rotatory catalysis.

5 vicinity of the active site, have different rotatory configurations.

6 tion primarily in spinal cord, whereas axial-rotatory disease involves inflammation and demyelination

7 Axial-rotatory disease, characterized by uncontrolled axial ro

8 ime-resolved absorption and magnetic optical rotatory dispersion (MORD) measurements of photolyzed my

9 rison of calculated and experimental optical rotatory dispersion (ORD) data provides the most straigh

10 tronic circular dichroism (ECD), and optical rotatory dispersion (ORD) spectroscopy.

11 guration using a combination of NMR, optical rotatory dispersion (ORD), and circular dichroism (CD) s

12 ar dichroism (ECD) spectroscopy, and optical rotatory dispersion (ORD).

13 lowed using nanosecond time-resolved optical rotatory dispersion (ORD).

14 ave been studied using time-resolved optical rotatory dispersion (TRORD) spectroscopy in the visible

15 he protein, nanosecond time-resolved optical rotatory dispersion (TRORD) spectroscopy, which is a dir

16 Previous far-UV time-resolved optical rotatory dispersion (TRORD) studies of the sub-milliseco

17 In 1919, Perucca reported anomalous optical rotatory dispersion from chiral NaClO(3) crystals that w

18 , electronic circular dichroism, and optical rotatory dispersion spectra and corresponding quantum ch

19 udied using nanosecond time-resolved optical rotatory dispersion spectroscopy.

20 ction reproducing solvent-mediated trends in rotatory dispersion surprisingly well, whereas more mode

21 m, electronic circular dichroism and optical rotatory dispersion.

22 merical modelling we determine the origin of rotatory effects in these two structures.

23 y incoming, dendritic signals in the case of rotatory flow fields and to reduce them in the case of o

24 to compensate for the confounding effects of rotatory head movements on optic flow.

25 ive, noninvasive diagnosis of posterolateral rotatory instability.

26 The TS is formed simultaneously with the rotatory motion enabling the translocation of the A-site

27 mple, turn with the direction of large-field rotatory motion, an optomotor reflex that is thought to

28 essing to a severe head tilt, spinning, or a rotatory motion.

29 t are carried out, a mathematical feature of rotatory motions known as noncommutativity.

30 f the tubules and supercoiling, suggesting a rotatory movement of the helix turns relative to each ot

31 hVOR and resulted in a prolongation of post-rotatory nystagmus in darkness.

32 nments, and while their visual processing of rotatory optic flow is understood in exquisite detail, h

33 c nanocolloids, whose nanoscale geometry and rotatory optical activity can be reversibly reconfigured

34 ral, chiral metamaterials can exhibit strong rotatory power at or around resonances, they convert lin

35 ral core that is manifested by lower optical rotatory power.

36 Their conglomerate domains exhibit optical rotatory powers comparable to the highest ever found for

37 stibular systems both encode translatory and rotatory self-motion, their coordinate systems differ.

38 of the cilium may be modeled as a nonlinear rotatory spring, with the linear spring constant k of th

39 Optical rotations and rotatory strengths are calculated for achiral, conjugate

40 ining to what extent the sum-over-pi --> pi* rotatory strengths are sufficient to account for nonreso

41 nvagination, C1-C2 instability, atlantoaxial rotatory subluxation, congenital occipitocervical synost

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