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Algebra Universalis, 1977
Let \(L\) be a bounded distributive lattice; \({\mathcal P}\) and \({\mathcal M}\) are respectively the prime spectrum and maximal spectrum of \(L\). If every prime ideal of \(L\) is contained in a unique maximal ideal of \(L\) then \(L\) is called a \(pm\)-lattice.
Pawar, Y. S., Thakare, N. K.
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Let \(L\) be a bounded distributive lattice; \({\mathcal P}\) and \({\mathcal M}\) are respectively the prime spectrum and maximal spectrum of \(L\). If every prime ideal of \(L\) is contained in a unique maximal ideal of \(L\) then \(L\) is called a \(pm\)-lattice.
Pawar, Y. S., Thakare, N. K.
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Acta Crystallographica Section A Foundations of Crystallography, 2004
Most of the sharp peaks, recently reported by Constant & Shlichta [Acta Cryst. (2003), A59, 281-282], in the frequency distribution of known tetrahedral and hexagonal-rhombohedral inorganic compounds apparently correspond to integral lattices. These are characterized by an integral metric tensor of their basis vectors (up to a unit-length factor ...
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Most of the sharp peaks, recently reported by Constant & Shlichta [Acta Cryst. (2003), A59, 281-282], in the frequency distribution of known tetrahedral and hexagonal-rhombohedral inorganic compounds apparently correspond to integral lattices. These are characterized by an integral metric tensor of their basis vectors (up to a unit-length factor ...
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Acta Crystallographica Section B Structural Science, 2005
A modified choice of unit-cell vectors resolves an apparent discrepancy in the indexation of the most intense para-sexiphenyl reflections compared with other known para-phenylenes.
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A modified choice of unit-cell vectors resolves an apparent discrepancy in the indexation of the most intense para-sexiphenyl reflections compared with other known para-phenylenes.
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Lattices and Lattice Complexes
1991A lattice is an array of points each of which has identical environment in identical orientation. The points of a lattice are related to each other by a translation: by moving the entire lattice parallel to itself through an appropriate distance it can be brought into coincidence with itself (cf. Fig. 15-1).
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