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By MaryAnn Bohland, Aleksey V. Matveyenko, Maziyar Saberi, Arshad M. Khan, Alan G. Watts, Casey M. Donovan

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Read or Download [Article] Activation of Hindbrain Neurons Is Mediated by Portal- Mesenteric Vein Glucosensors During Slow-Onset Hypoglycemia PDF

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The Ni atoms are strongly bounded to La atoms to generate a 2D network parallel to the {001} plane. 0 Introduction (Figures) [Ref. p. 429 For Fig. 61i see next page. Fig. 62i. Ce2Cu2P5–x. c. The crystal structure [81M2]. The structure is orthorhombic but is closely related to that of the PbFCl -ThCr2Si2 family. The slabs centered at z = 1/4 and 3/4 with the stackings of the Ce, P, Cu, P, Ce atoms are virtually identical to those found in the ThCr2Si2 structure. The differences arise through the clustering of the P atom layers around z = 0 and 1/2 (P atoms 5 to 8).

For Fig. 56i see next page. 43 Ln: La Ce Pr Nd Pm Sm Eu Gd Tb Dy Ho Er Tm Yb Lu L a nd o lt - B ö r ns t e in New Series III/27B4α Fig. 57i. LnT5P3. Cell volume of the YCo5P3-type compounds (T = Fe, Co) versus lanthanide atomic number [84J1]. Yb is trivalent in both compounds, but CeCo5P3 is probably in the mixed valent state. Open circle: data for LaCo5P3 type. 0 Introduction (Figures) [Ref. p. 429 Fig. 56i. YCo5P3. Projection of the crystal structure on the {x,z} plane and coordination polyhedra [84M1].

The lattice parameters of Yb3Cu8–xP6 [79K1] obey the dependence presented in Fig. very well, which indicates a valence state of 3+ for the ytterbium atoms. A good correlation between lattice parameters of Yb3Cu8–xP6 and those of Ln3Cu8–yP8 raises the questions of checking the structure since six phosphorus atoms in Yb3Cu8–xP6 should result in a smaller unit cell volume as compared to those of Ln3Cu8–yP8. 0 Introduction (Figures) [Ref. p. 429 Fig. 75i. Y3Cu8–yP8. c. The crystal structure (rhombohedral, space group R 3 m ) as viewed along the z-axis [98K1].

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