Optimal finite duration pulses for OFDM
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Cites background or methods from "Optimal finite duration pulses for ..."
...As for OFDPs, their expression in continuous-time is as follows [6], [20]:...
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...where is the th prolate spheroidal wave function truncated to the interval and where are some real-valued coefficients obtained thanks to an optimization procedure [20]....
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...Let us refer to the optimization method of the lattice coefficients according to the criterion as the optimized lattice (OL), knowing naturally that more generally, the optimization of the lattice coefficients can be carried out with different types of criteria, including, as in [20], the maximization of the in-band energy....
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...for instance, [19]); 2) a family of pulses introduced by Vahlin and Holte in [20], which we will call optimal finite duration pulses (OFDPs); 3) a new family of functions called extended Gaussian functions (EGFs); see [21]....
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...These prototype filters have been computed thanks to the values of the coefficients given in [20]....
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388 citations
Cites methods from "Optimal finite duration pulses for ..."
...Reference [ 9 ] recommends the use of time-limited prolate spheroidal wave function which offers minimum bandwidth for a fixed temporal support....
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Cites background or methods from "Optimal finite duration pulses for ..."
...Some of the proposed pulse shape design methods, however, involve the solution of highly nonlinear optimization problems [ 6 ], [7]....
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...Following other work on pulse-shaping OFDM [ 6 ]‐[8], [10], [23], we consider transmission systems with spectral efficiency (in practice, a higher spectral...
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...3 Alternatively, we can use a slightly different modulation scheme, known as OQAM-OFDM, see [ 6 ]....
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291 citations
Cites methods from "Optimal finite duration pulses for ..."
...0 0.5 1 1.5 2 2.5 3 3.5 4 −160 −140 −120 −100 −80 −60 −40 −20 0 f/F 10 lo g 1 0 (| P (f )| 2 ) Gaussian IOTA Hermite Prolate (K = 4) OFDP (K = 4) Kaiser (β = 10) (b) Energy distribution in frequency....
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...In this context, a basic single-tap equalization per subcarrier may be employed to recover the symbols [16], [21], [22], [74], [92]–[94]....
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...It is shown that these coefficients can be computed (for finite number of coefficientsbk,j) as dk,ρ,υ0 = jk∑ j=0 bk,je −(πρ/2ν2 0 )(2j+k) , 0 ≤ k ≤ K , (16) 0 0.5 1 1.5 2 2.5 3 3.5 4 −160 −140 −120 −100 −80 −60 −40 −20 0 10 lo g 1 0 |p (t )| 2 t/T Gaussian IOTA Hermite Prolate (K = 4) OFDP (K = 4) Kaiser (β = 10) (a) Energy distribution in time....
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...Equalization [52], [54], [55], [61], [106]–[108], [110], [112]– [115], [121] [167] [39], [40], [45], [46], [50], [51], [106], [107], [109], [110], [113]–[115], [123] [108], [111], [112], [121], [157], [168] [134], [165] [51], [106] [16], [21], [22], [93], [94] [74] [47]...
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...Considering this fact, Vahlin exploits PSWFs to realize a new family which is referred as optimal finite duration pulse (OFDP) [74] by generalizing the optimization procedure given for single carrier, presented in [73]....
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"Optimal finite duration pulses for ..." refers background or methods in this paper
...which corresponds to the integral equation ( 9 )....
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...As h(t) is assumed even, coefficients a, are zero for odd z. Substituting the series expansion (10) in ( 9 ), using only even indices, the condition for h(t) becomes...
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...equations, defined by (16) and (17), gives the coefficients a, in the series expansion of an h(t) which satisfies equations ( 9 ) and (6)....
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...Orthogonality conditions for this category were presented in [SI and an application with offset QAM (OQAM) can be found in [ 9 ]....
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...As the integral operator on the left-hand side of ( 9 ) is compact and self adjoint, there exists a complete set of orthogonal eigenfunctions &(t), which are known as prolate spheroidal wave functions (PSWF’s), and corresponding distinct eigenvalues y; [12]....
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