2007
DOI: 10.1016/j.physleta.2006.10.055
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Theta and Riemann xi function representations from harmonic oscillator eigensolutions

Abstract: From eigensolutions of the harmonic oscillator or Kepler-Coulomb Hamiltonian we extend the functional equation for the Riemann zeta function and develop integral representations for the Riemann xi function that is the completed classical zeta function. A key result provides a basis for generalizing the important Riemann-Siegel integral formula.

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Cited by 10 publications
(13 citation statements)
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“…In particular, there are at least four, albeit related, points of view that could connect the h coefficients of equations (2.9) and (3.12), other series coefficients and the sum S 2 , with the theories of diffusion, Brownian motion and random walk. Underlying much of this connection is the fact that a Jacobi theta function (Coffey 2002), a solution of the heat equation, provides a basis for a (Mellin transform) representation of the Riemann xi function (Riemann 1859;Biane et al 2001;Coffey 2005aCoffey , 2007c). …”
Section: A Probabilistic Setting For the S And H Valuesmentioning
confidence: 99%
“…In particular, there are at least four, albeit related, points of view that could connect the h coefficients of equations (2.9) and (3.12), other series coefficients and the sum S 2 , with the theories of diffusion, Brownian motion and random walk. Underlying much of this connection is the fact that a Jacobi theta function (Coffey 2002), a solution of the heat equation, provides a basis for a (Mellin transform) representation of the Riemann xi function (Riemann 1859;Biane et al 2001;Coffey 2005aCoffey , 2007c). …”
Section: A Probabilistic Setting For the S And H Valuesmentioning
confidence: 99%
“…From the explicit form of Eq. (2.34) depicting the inner product of two arbitrary states, by choosing for example that l = −2 ⇒ k = 1 4 , one concludes that the pseudo-norm The Mellin transform based on the weighted Θ 2j (t) [41] requires once again to extract the zero mode n = 0 contribution of Θ 2j (t) (to regularize the divergent integrals) in order to arrive at …”
Section: And the Hamiltonian Operators Hmentioning
confidence: 99%
“…The polynomial P j (s) has simple zeros on the critical line Re s = 1 2 , obeys the functional relation P j (s) = (−1) j P j (1 − s) and in particular P j (s = 1 2 ) = 0 when j = odd [41]. It is only when j = even that P j (s = 1 2 ) = 0 and when we can implement CT invariance resulting from the relation (2.39) and which is consistent with the results of Eqs.…”
Section: And the Hamiltonian Operators Hmentioning
confidence: 99%
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“…Our work is related to the development of extended theta function representations of the Riemann zeta function ζ. We have very recently shown how to correspondingly generalize the important Riemann-Siegel integral formula [9]. Bump and Ng [5] and Keating [14] have shown how to generalize Riemann's second proof of the functional equation of ζ(s) by using Mellin and Fourier transforms of Hermite polynomials.…”
Section: Introductionmentioning
confidence: 99%