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'}$| scalars possessing |$ H $|-singlet up to |$ N =26$| are listed in Table 6 (note there the isomorphisms |$U\hspace{-0.125em}Sp( 2 )\simeq SO( 3 )\simeq SU( 2 )$|, |$SO(5)\simeq U\hspace{-0.125em}Sp(4)$|, and |$U(1 ...
of the modified method is presented in Section 2 . The main part of this article is Section 3 , which describes possible scenarios one could encounter in a planetary system, and provides results for the dimensional ...
, topological quantum states, high Chern number, high temperature INTRODUCTION The quantum Hall effect (QHE) with quantized Hall resistance plateaus of height h /νe2 was first observed in two- dimensional (2D ...
of the sialylα( 2 - 3 /6) N -acetyllactosamine structural element in glycoproteins, by two- dimensional NOE 1H-NMR spectrocopy in combination with energy calculations by hard-sphere exo-anomeric and molecular mechanics ...
amyloid fibrils at a neutral pH. J. Am. Soc. Nephrol. 15, 126–133 Google Scholar 3 . Yamaguchi, I., Hasegawa, K., Takahashi, N ., Gejyo, F., and Naiki, H . ( 2001) Apolipoprotein E inhibits ...
of full length Gal- 3 to RG-I-4 Figure 2 shows 15N–1H heteronuclear single quantum coherence (HSQC) spectral overlays of 15N-Gal- 3 (80 μM) in the absence (black peaks) and presence (red peaks) of RG-I-4 ...
growth-light conditions and in state 2 . The maximal photosynthetic capacity and the quantum efficiency of oxygen evolution were diminished by 8–14% in the PSI- H -less plants. Under growth-light conditions ...
for particle physics) and in many approaches to quantum gravity. 3 Lorentz symmetry is a particular sort of symmetry that constrains the way physical systems can be transformed. These so-called Lorentz ...
the structure and dynamics of the disordered histone tails, which play a pivotal role for nucleosome integrity. This is a gap filling experimental FRET study from the perspective of the histone H3 N -terminal tail ...
. . . . . . . . . . . . . . . . . . . . . . . . . . . . [Fe i] a5D1–a5D0 111.24 89.90 111.18 +150 400 1.61 Tentative; weak H i 14–13 111.80 89.45 111.86 −140 520 6.60 . . . . . . . . . . . . . . . . . . . . . . . . . . . . OH N = 2 +–1−, J = 5/ 2 - 3 / 2 119.25 ...
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