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A058632
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Coefficients of replicable function number "32b".
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1
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1, 2, 3, 6, 7, 10, 16, 20, 29, 40, 52, 70, 91, 116, 149, 190, 242, 306, 383, 478, 590, 730, 897, 1096, 1342, 1630, 1975, 2390, 2873, 3448, 4133, 4932, 5880, 6994, 8290, 9814, 11587, 13650, 16058, 18848, 22089, 25842, 30178, 35186, 40950, 47594, 55231, 63996, 74068, 85592, 98776, 113864
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OFFSET
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-1,2
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COMMENTS
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LINKS
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FORMULA
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Expansion of q^(1/4)*(eta(q^2)*eta(q^4)/(eta(q)*eta(q^8)))^2 in powers of q. -G. C. Greubel, Jun 23 2018
Expansion of (psi(x)/psi(-x^2))^2 = (phi(-x^4)/psi(-x))^2 = (chi(x)*chi(x^2))^2 = (chi(-x^4)/chi(-x))^2 in powers of x where phi(), psi(), chi() are Ramanujan theta functions.
G.f. is a period 1 Fourier series which satisfies f(-1 / (128 t)) = f(t) where q = exp(2 Pi i t). (End)
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EXAMPLE
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T32b = 1/q + 2*q^3 + 3*q^7 + 6*q^11 + 7*q^15 + 10*q^19 + 16*q^23 + 20*q^27 + ...
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MATHEMATICA
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eta[q_] := q^(1/24)*QPochhammer[q]; a := CoefficientList[Series[q^(1/4)*(eta[q^2]*eta[q^4]/(eta[q]*eta[q^8]))^2, {q, 0, 60}], q]; Table[a[[n]], {n, 0, 50}] (* G. C. Greubel, Jun 23 2018 *)
a[ n_] := SeriesCoefficient[ (EllipticTheta[2, 0, q^(1/2)]/EllipticTheta[2, Pi/4, q])^2 / (2/q^(1/4)), {q, 0, n}];
a[ n_] := SeriesCoefficient[ (EllipticTheta[3, 0, -q^4]/EllipticTheta[2, Pi/4, q^(1/2)])^2 *(2*q^(1/4)), {q, 0, n}];
a[ n_] := SeriesCoefficient[ (QPochhammer[-q, q^2]*QPochhammer[-q^2, q^4])^2, {q, 0, n}];
a[ n_] := SeriesCoefficient[ (QPochhammer[+q^4, q^8]/QPochhammer[+q, q^2])^2, {q, 0, n}]; (End)
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PROG
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(PARI) q='q+O('q^50); Vec((eta(q^2)*eta(q^4)/(eta(q)*eta(q^8)))^2) \\ G. C. Greubel, Jun 23 2018
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CROSSREFS
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KEYWORD
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nonn
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AUTHOR
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EXTENSIONS
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STATUS
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approved
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