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We prove that the unique shift ε = φ − 1 — where φ = (1 + √5)/2 is the Golden Ratio — makes the 2-regularized Fredholm determinant of the diagonal operator Aₛ+ε on ℓ²(primes) equal (up to an entire, nowhere-vanishing factor) to ζ(s)⁻¹. Explicitly, det₂(I − Aₛ+φ−1 · E_φ(s)) = ζ(s)⁻¹, for Re s > ½, where E_φ is an elementary exponential built ...
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Nature, 1952
The Theory of the Riemann Zeta-Function By Prof. E. C. Titchmarsh. Pp. vii + 346. (Oxford: Clarendon Press; London: Oxford University Press, 1951.) 40s. net.
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The Theory of the Riemann Zeta-Function By Prof. E. C. Titchmarsh. Pp. vii + 346. (Oxford: Clarendon Press; London: Oxford University Press, 1951.) 40s. net.
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2011
The Riemann zeta function is one of the most important functions of classical mathematics, with a variety of applications in analytic number theory. In this lecture, we shall study some of its elementary properties.
Ravi P. Agarwal +2 more
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The Riemann zeta function is one of the most important functions of classical mathematics, with a variety of applications in analytic number theory. In this lecture, we shall study some of its elementary properties.
Ravi P. Agarwal +2 more
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1998
In order to make progress in number theory, it is sometimes necessary to use techniques from other areas of mathematics, such as algebra, analysis or geometry. In this chapter we give some number-theoretic applications of the theory of infinite series.
Gareth A. Jones, J. Mary Jones
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In order to make progress in number theory, it is sometimes necessary to use techniques from other areas of mathematics, such as algebra, analysis or geometry. In this chapter we give some number-theoretic applications of the theory of infinite series.
Gareth A. Jones, J. Mary Jones
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Riemann’s Zeta Function Regularization
2018In this final section, we want to introduce the concept of the zeta function in connection with regularizing certain problems in quantum physics where infinities occur.
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2001
Abstract The theory we presented in Chapter 10 works globally over the adeles by simply taking the product of the local theories for p ≥ η .
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Abstract The theory we presented in Chapter 10 works globally over the adeles by simply taking the product of the local theories for p ≥ η .
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1999
The surface is a graph of the reciprocal of the absolute value of the Riemann zeta function ζ (s). The spikes correspond to the zeros on the critical line ½ + iy. Recall that the global behavior of π(x), the prime distribution function, is well approximated by Riemann’s smooth function R(x) (discussed in Chapter 2). More delicate information about π(x),
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The surface is a graph of the reciprocal of the absolute value of the Riemann zeta function ζ (s). The spikes correspond to the zeros on the critical line ½ + iy. Recall that the global behavior of π(x), the prime distribution function, is well approximated by Riemann’s smooth function R(x) (discussed in Chapter 2). More delicate information about π(x),
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