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1,2,3-Dithiazolyl and 1,2,35-Dithiadiazolyl Radicals as Spin-Bearing ...

1,2,3-Dithiazolyl and 1,2,35-Dithiadiazolyl Radicals as Spin-Bearing ...

1,2,3-Dithiazolyl and 1,2,35-Dithiadiazolyl Radicals as Spin-Bearing ...

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linear relationship shown in Figure 1-1 with χT = C (J = 0). Interactions between<br />

unpaired electrons result in deviations from the ideal Curie Law which are more<br />

prominent at low temperatures. Real materials do not exhibit true Curie magnetism, <strong>and</strong><br />

are instead defined <strong>as</strong> having near Curie behaviour. Therefore a better way of describing<br />

these types of systems in a higher temperature regime is achieved by using the Curie-<br />

Weiss law which adds the additional parameter Θ <strong>and</strong> is written <strong>as</strong>:<br />

(1.4)<br />

where Θ is the Weiss constant. This constant is used when the temperature is<br />

much higher than the Curie temperature which is the temperature below which a<br />

compound will exhibit spontaneous magnetization. At higher temperatures the<br />

interactions with neighbouring magnetic domains must be considered <strong>and</strong> the value of Θ<br />

will provide some indication <strong>as</strong> to the nature of these interactions. If Θ = 0 then the<br />

equation becomes 1.3 <strong>and</strong> the material is considered paramagnetic. When Θ > 0 then the<br />

interaction is ferromagnetic <strong>and</strong> when Θ < 0 the interaction is antiferromagnetic.<br />

Bohr magnetons (β or μ B ) are the fundamental quantum of magnetic moment <strong>and</strong> h<strong>as</strong><br />

a value of 4.66864374 × 10 -5 cm -1 G -1 such that<br />

<strong>and</strong>:<br />

(1.5)<br />

according to:<br />

It is also important that the value of μ is related to the spin quantum number S<br />

(1.6)<br />

3

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