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Magnetic susceptibility temperature-independent

CrN 300-100 3.9 Gouy at room temperature magnetic transition observed near 7i=273 K, below susceptibility temperature independent 73W5, Fig. 51... [Pg.103]

Neptunium dioxide crystallizes in the cubic fluorite structure and magnetic measurements have been reported from 4 to 300 K [16,74,75]. There is a magnetic transition at 2S.4K. Above 60 K, the susceptibility follows the Curie-Weiss law pgn = 2.95-3.00/ig, 0 = —22 K). Below 10-12 K, the magnetic susceptibility becomes independent of temperature (xm = ... [Pg.502]

In his thesis (1895) Pierre Curie [64] investigated the magnetic properties of a number of different materials. He found that the magnetic susceptibility is independent of temperature for diamagnetic materials. For paramagnetic materials (like oxygen) he found a relation of the type of Eq. (5). A different relation... [Pg.1545]

The magnetic susceptibility of Na[Pu02(CH3COO)3] was measured by Dawson between 90 and 333 K (3). The resulting magnetic moment, yjff = 8.0 Ug, is temperature independent and corresponds to = 8.70 Ug, which is calculated from EPR measurements on a... [Pg.32]

Magnetic measurements of PuFi, between 4.2 and 300 K are consistent at high temperatures with older measurements (10-12). The large temperature dependent diamagnetism observed earlier was not found. Up to 100 K the susceptibility is nearly temperature independent with a value of X ip 2940 x 10-6 emu. The Curie-Weiss behavior near room temperature indicates population of a higher first excited state. The structure of PuFi, is isomorphic with that of UFi, (13), where two different sets of actinide atoms are 8-fold coordinated by a distorted antiprism. [Pg.35]

With respect to the physical properties mentioned, band-structure calculations have attracted considerable interest, e.g., for SbSBr, SbSI, and SbSel (234). For the compounds having reference 22i in column 4 of Table XXIX, a temperature-independent diamagnetism has been found, with values of about 10 cm" g between 77 and 340 K. A small temperature-dependence is exhibited by BiTel, a narrow-gap semiconductor (41). The anisotropy of the magnetic susceptibility has been studied for SbSI, BiSel, and BiTel (41, 420). [Pg.412]

Variable-temperature measurements of the magnetic susceptibility at 0.1 and 1.0 T between 2 and 290 K indicated temperature-independent diamagnetism 44). That is, flat % versus T curves, for both 3 (Xdiayrip(3) =-10.2 X lO emumor ) and 4 (Xdia/Tip(4) =-9.8 x 10 emu mol were obtained. By comparison these numbers for the... [Pg.259]

The above statements apply to an assembly of independent spins. Deviation from proportionality, if any is observed, suggests the presence of cooperative magnetic phenomena, i.e. ferro-, antiferro-, ferri-, meta-, micto-magnetism, and so on. The magnetic susceptibility at above the spinordering temperature (Tq) can be usually fitted by the Curie-Weiss expression (18) with the Weiss temperature 0 > 0 for the sample with dominant... [Pg.205]

Diamagnetism is a basic property of all substances and involves a slight repulsion by a magnetic field. The magnetic susceptibility of a diamagnetic substance is small (-10 ), negative and independent of temperature. Iron oxides display additional types of magnetism. [Pg.119]

Another additive term in the magnetic susceptibility arises from the temperature-independent core diamagnetism of all the ions in a solid. For YBa2Cu307 the core diamagnetism is approximately -2 x 10 7 based on a calculation using Pascal s constants (9). This small negative contribution serves to reduce the total susceptibility. A third possible contribution arises from Van Vleck paramagnetism (10) caused by excited states in the atoms of the... [Pg.679]

Rhenium metal exhibits a very low paramagnetism which is field-independent and almost temperature-independent. In the range 79—471 K, magnetic susceptibility data for two independent samples were shown to correspond, when Tis in Kelvin, to the following equations (5) ... [Pg.161]


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