Abstract
We discuss theoretically the magnetically ordered phase induced by magnetic and nonmagnetic impurities in three-dimensional and quasi-low-dimensional systems with singlet ground states separated by a gap from excited triplet states. Using ideas of the percolation theory, we estimate the transition temperature to the Néel phase at a small concentration of defects, derive the density of states of low-energy elementary excitations, and examine the contribution of these excitations to the specific heat and magnetization. Our expressions for and for the specific heat describe well available experimental findings obtained in various appropriate systems: spin- dimer materials, spin-ladder compounds, spin-Peierls and Haldane chain materials. However, our expression for differs considerably from many of those proposed before.
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