Single Crystals Temperatures

Fig. 2 a, b. EPR and ENDOR spectrum of the low-spin Co(II) Schiff base complex Co(acacen) diluted into a Ni(acacen) 1/2 H20 single crystal, temperature 8K. a) EPR spectrum the two magnetically nonequivalent sites coincide for this particular orientation (EPR observer is marked by an arrow) b) ENDOR spectrum of H, 13C (enriched) and 14N ligand nuclei vp free proton frequency denote the AmN = 2 nitrogen ENDOR transitions. (From Ref. 12)... 

Blaurock and Carothers (1990) and Blaurock and Wan (1990) described a simple way, valid for butteroil, of analyzing isothermal DSC data to characterize the kinetics of early crystallization in a supercooled oil. This approach yielded a single crystallization-temperature dependent combined nucleation/crystal growth constant (which they called NG). The temperature dependence of NG could be modeled with the Arrhenius equation. 

Zeeman-perturbed NQR on a single crystal. Temperature dependence also studied. 

Fig. 20. VjOj, single crystal. Temperature dependence of VXfj (average values) for the perpendicular direction. Solid curve is a least-squares (it by a cubic equation, the dashed lines correspond to a Curie-Weiss law [68A8].

Fig. 106. CsiMnClj 2H,0, single crystal. Temperature dependence of 1/xn and 1/X [68S37]. Fig. 107 sec next page...

Fig. 119. Mn(HCOO)2 2H2O, single crystal Temperature dependence of l/z along three crystallographic axes [65Y5].

Fig. 125. Na MniSi Ov, single crystal. Temperature depen- Fig. 126. NajMnjSijO, single crystal. Temperature dependence of Xm (open circle), full circle in the plane of sym- dence of spontaneous magnetization [68K1]. metry triangle along the b axis [68K1].

Fig. 177. Fc3(P04),-413,0, single crystal. Temperature dependence of x, in the directions of the three prindpal magnetic axes. Crystal 1 1, full triangle Xi, Z full triangle Z full circle /j, crystal II I, open triangle 2, open triangle Xz, 3, open circle Xi [68M12].

Fig. 258. CsjCoCls, CsiCoC, and K2Co(CNS)4 4H2O, single crystals. Temperature dependence of [64F].

Fig. 263. CsjCoCIs, single crystal. Temperature dependence Xm/C measured along the c axis [67M22].

Fig. 274. CotCHjCOO), -4FI,0 single crystal. Temperature dependence of the square of the principal magnetic moments parallel and perpendicular to the tetragonal axis [65M8].

Fig. 284. [Co(H20)6]F2 SHF, single crystal. Temperature dependence of magnetic anisotropy where (Xi—X2) s measured perpendicular to c axis c and h represent cooling and heating respectively [68D11].

Fig. 286. [CoCHjOypj -SHF, single crystal. Temperature dependence of principal magnetic moment squared p -along c axis, Pj, and perpendicular to c axis, Pi > pj [68D11].

Fig. 317. NiSiF6 6H20, single crystal. Temperature de- Fig. 318. Ni(CN)2 NHj CsH. Temperature dependence pendencel/x andx . 7 whereZmisfor =0.Field parallel of l/z . p = 2.18 Ib p=-2.7 K [68W5]. to the crystallographic c axis [66H23].

Fig. 344. NaNiO, single crystal. Temperature dependence Fig. 345. NaNiO, single crystal. Magnetization <7 of a...

Fig. 1. VjOj single crystal. Temperature dependence of Fig. 2. VjOj single crystal. Temperature dependence of Ay, Ay,. The circles, both filled and unfilled, are data for [71G30]. lowering of temperature, the triangles are data for increasing of temperature. Filled and unfilled circles due to different sets of measurements [71G30].

Fig. 28. CsMnCl3 2H20 single crystal. Temperature dependence of magnetic anisotropy Zn Xf Zt Solid curve calculated on the basis of the Heisenberg model [72N1].

Fig. 40. (NH4)2MnF5 single crystal. Temperature dependence of Xm- The open circles are in [010] and full points are in [100] [71K14].

Fig. 41. MnjB4 single crystal. Temperature dependence of Zg(Za. Zt- Xc) [71K6].

Fig. 67. RbFeF4 single crystal. Temperature dependence of Xn parallel and perpendicular to crystallographic b axis [71E2],...

Fig. 109. CsCoClj-ZHjO single crystal. Temperature dependence of y, (left scale and open symbols) and 1/y, (right hand scale and solid symbols. Circles H u squares H l6 triangles H If [72H18],...

Fig. 115. [CoCljfHjOlA] 2 HjO single crystal. Temperature dependence of p ,, p. Curves fitted to d crystal...

Fig. 136. NiSnClj 6HjO powder and single crystal. Temperature dependence of (j , Xn > Zi)-Magnetism fitted to...

Fig. 143. NiWOj single crystal. Temperature dependence Fig. 144. KNiP04. Temperature dependence of l/x ...

Fig. 204. [Co(NH3)6][CuBr3Cl2]. Temperature dependence Fig. 206. Cu(CH3COO)2 H2O single crystal. Temperature of [72J3]. dependence of principal molecular susceptibilities. Curves...

Fig. 207. CaCu(CHjC00)4-6H20 single crystal. Temperature dependence of z i, Xml- Th dahed curves illustrate the Curie-Weiss fit using...

Fig. 3. Ti(urea)gl3 single crystal. Temperature dependence of P and Px- The solid curves are the smoothed experimental data, the dashed line is calculated for py, the dotted line is calculated for pj, from the theory for the term with Dg = 1700cm" J=-600cm fc = 0.45, A = 75cm" , C7 g < 50 cm fc is the orbital angular momentum reduction factor, A is the splitting of the term, 17 q is a trigonal ligand field parameter [73F6].

Fig. 79. CsMnClj 2 HjO single crystal. Temperature dependence of Xm Lines fitted according to a model see original literature for details [73K18].

Fig. 80. CsMnClj 2DjO single crystal. Temperature dependence of Curve fitted for a Heisenberg linear chain antiferromagnet by the method of Weng and Griffith using J/k= -3.00 K. S= [73K18].

Fig. 83. (CH3NH3)2MnCl4 p, single crystal. Temperature dependence of ( ) and Xmi (o)- Zmii ( ) calculated [73H9].

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