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Self-assembled Transition Metal Coordination Frameworks of ...

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Chapter I W _ _<br />

Traditional magnets are based on metallic or ionic systems, but recently it has<br />

been discovered that even individual molecules can behave like tiny magnets.<br />

Magnetic molecules are a new class <strong>of</strong> fascinating materials. These molecules contain<br />

a finite number <strong>of</strong> interacting spin centers (e.g. paramagnetic ions) and thus provide<br />

ideal opportunities to study basic concepts <strong>of</strong> magnetism. One <strong>of</strong> the characteristic<br />

features <strong>of</strong> molecular magnetism is its deeply interdisciplinary character, bringing<br />

together organic, organometallic and inorganic synthetic chemists as well as<br />

theoreticians from both the chemistry and physics communities, and materials and<br />

life-science specialists. This interdisciplinary nature confers a special appeal to this<br />

field. Nobody alone can make a crucial contribution [99].<br />

Paramagnetic metal ions with covalent radii <strong>of</strong> the order <strong>of</strong> l A (0.1 nm) can<br />

be brought into close proximity with suitable diamagnetic single atom bridging<br />

ligands, and with appropriate magnetic orbital overlap situations can produce parallel<br />

or antiparallel alignment <strong>of</strong> the metal centered spins (ferromagnetic or<br />

antiferromagnetic behavior respectively). Increasing the number <strong>of</strong> spin centers in a<br />

polynuclear bridged arrangement is more <strong>of</strong> a challenge, but can be achieved using<br />

polydentate ligands <strong>of</strong> various types. One approach uses well-defined polydentate<br />

ligands to impose specific geometries on the resulting arrays, while another approach<br />

uses simple ligands, and essentially is controlled by properties <strong>of</strong> the metal ion. An<br />

intermediate approach uses coordinatively flexible ligands [21].<br />

Magnetic measurements can be performed in ac or dc modes. In the dc mode<br />

a static magnetic field H is applied, and the induced magnetization, M, is studied as a<br />

function <strong>of</strong> this magnetic field and <strong>of</strong> temperature [99]. In the present study variable<br />

temperature and field dependent magnetization were carried out in dc mode at the<br />

Department <strong>of</strong> Physics, Boise State University, Boise, USA in the powder state on a<br />

Quantum Design PPMS superconducting magnetometer at 500 Oe field strength.<br />

Diamagnetic corrections were made using Pascal's constants [I00].<br />

28

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