Shaping Multidimensional Signal Spaces-Part I : Optimum Shaping , Shell Mapping
Shaping Multidimensional Signal Spaces-Part I : Optimum Shaping , Shell Mapping
复制标题
塑造多维信号空间 - 第一部分:最佳塑造、壳映射
DOI:
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发表时间:
1998
期刊:
影响因子:
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通讯作者:
P. Kabal
中科院分区:
文献类型:
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作者:
Arnir;K. Kbandani;P. Kabal
In selecting the boundary of a signal constellation used for data transmission, one tries to minimize the average energy of the constellation for a given number of points from a given packing. The reduction in the average energy per two dimensions due to the use of a region ‘Z as the boundary instead of a hypercube is called the shaping gain y, of L?‘. The price to be paid for shaping involves: 1) an increase in the factor constellation-expansion ratio (CER,), 2) an increase in the factor peak-to-average-power ratio (PAR), and 3) an increase in the addressing complexity. In general, there exists a tradeoff between ys and CER,, PAR. In this work, the structure of the region which simultaneously optimizes both of these tradeoffs is introduced. In an N-D (N-dimensional) optimum shaping region (N even), a 2-D sphere is the boundary of the 2-D subspaces and an N-D sphere is the boundary of the whole space. Analytical expressions are derived for the optimum tradeoff curves. By applying a change of variable denoted as shell mapping, the optimum shaping region is mapped to a hypercube truncated within a simplex. This mapping facilitates the performance computation, and also the addressing of the optimum shaping region. Using shell mapping, we introduce an addressing scheme with low complexity to achieve a point on the optimum tradeoff curves. To obtain more flexibility in selecting the tradeoff point, a second shaping method with more degrees of freedom is used. In this method, a 2-D sphere is the boundary of the 2-D subspaces, an N’-D sphere, N’ 2 2, is the boundary of the N’-D subspaces, and an N-D sphere is the boundary of the whole space. Index Temts-Optimum shaping, shell mapping, truncated cube, uniform density, optimum tradeoff.