词条 | Chebyshev function |
释义 |
In mathematics, the Chebyshev function is either of two related functions. The first Chebyshev function {{math|ϑ(x)}} or {{math|θ(x)}} is given by with the sum extending over all prime numbers {{mvar|p}} that are less than or equal to {{mvar|x}}. The second Chebyshev function {{math|ψ(x)}} is defined similarly, with the sum extending over all prime powers not exceeding {{mvar|x}}: where {{mvar|Λ}} is the von Mangoldt function. The Chebyshev functions, especially the second one {{math|ψ(x)}}, are often used in proofs related to prime numbers, because it is typically simpler to work with them than with the prime-counting function, {{math|π(x)}} (See the exact formula, below.) Both Chebyshev functions are asymptotic to {{mvar|x}}, a statement equivalent to the prime number theorem. Both functions are named in honour of Pafnuty Chebyshev. RelationshipsThe second Chebyshev function can be seen to be related to the first by writing it as where {{mvar|k}} is the unique integer such that {{math|pk ≤ x}} and {{math|x < pk + 1}}. The values of {{mvar|k}} are given in {{OEIS2C|id=A206722}}. A more direct relationship is given by Note that this last sum has only a finite number of non-vanishing terms, as The second Chebyshev function is the logarithm of the least common multiple of the integers from 1 to {{mvar|n}}. Values of {{math|lcm(1,2,...,n)}} for the integer variable {{mvar|n}} is given at {{OEIS2C|id=A003418}}. Asymptotics and boundsThe following bounds are known for the Chebyshev functions:{{ref|Dusart1999}}{{ref|Dusart2010}} (in these formulas {{math|pk}} is the {{mvar|k}}th prime number {{math|p1 {{=}} 2}}, {{math|p2 {{=}} 3}}, etc.) Furthermore, under the Riemann hypothesis, for any {{math|ε > 0}}. Upper bounds exist for both {{math|ϑ(x)}} and {{math|ψ(x)}} such that,[1] {{ref|Dusart2010}} for any {{math|x > 0}}. An explanation of the constant 1.03883 is given at {{OEIS2C|id=A206431}}. The exact formulaIn 1895, Hans Carl Friedrich von Mangoldt proved{{ref|Dav104}} an explicit expression for {{math|ψ(x)}} as a sum over the nontrivial zeros of the Riemann zeta function: (The numerical value of {{math|{{sfrac|ζ′(0)|ζ(0)}}}} is {{math|log(2π)}}.) Here {{mvar|ρ}} runs over the nontrivial zeros of the zeta function, and {{math|ψ0}} is the same as {{mvar|ψ}}, except that at its jump discontinuities (the prime powers) it takes the value halfway between the values to the left and the right: From the Taylor series for the logarithm, the last term in the explicit formula can be understood as a summation of {{math|{{sfrac|xω|ω}}}} over the trivial zeros of the zeta function, {{math|ω {{=}} −2, −4, −6, ...}}, i.e. Similarly, the first term, {{math|x {{=}} {{sfrac|x1|1}}}}, corresponds to the simple pole of the zeta function at 1. It being a pole rather than a zero accounts for the opposite sign of the term. PropertiesA theorem due to Erhard Schmidt states that, for some explicit positive constant {{mvar|K}}, there are infinitely many natural numbers {{mvar|x}} such that and infinitely many natural numbers {{mvar|x}} such that {{ref|Sch03}}{{ref|Hard16}} In little-{{mvar|o}} notation, one may write the above as Hardy and Littlewood{{ref|Hard16}} prove the stronger result, that Relation to primorialsThe first Chebyshev function is the logarithm of the primorial of {{mvar|x}}, denoted {{math|x#}}: This proves that the primorial {{math|x#}} is asymptotically equal to {{math|e(1 + o(1))x}}, where "{{mvar|o}}" is the little-{{mvar|o}} notation (see big {{mvar|O}} notation) and together with the prime number theorem establishes the asymptotic behavior of {{math|pn#}}. Relation to the prime-counting functionThe Chebyshev function can be related to the prime-counting function as follows. Define Then The transition from {{mvar|Π}} to the prime-counting function, {{mvar|π}}, is made through the equation Certainly {{math|π(x) ≤ x}}, so for the sake of approximation, this last relation can be recast in the form The Riemann hypothesisThe Riemann hypothesis states that all nontrivial zeros of the zeta function have real part {{sfrac|1|2}}. In this case, {{math|{{abs|xρ}} {{=}} {{sqrt|x}}}}, and it can be shown that By the above, this implies Good evidence that the hypothesis could be true comes from the fact proposed by Alain Connes and others, that if we differentiate the von Mangoldt formula with respect to {{mvar|x}} we get {{math|x {{=}} eu}}. Manipulating, we have the "Trace formula" for the exponential of the Hamiltonian operator satisfying and where the "trigonometric sum" can be considered to be the trace of the operator (statistical mechanics) {{math|eiuĤ}}, which is only true if {{math|ρ {{=}} {{sfrac|1|2}} + iE(n)}}. Using the semiclassical approach the potential of {{math|H {{=}} T + V}} satisfies: with {{math|Z(u) → 0}} as {{math|u → ∞}}. solution to this nonlinear integral equation can be obtained (among others) by in order to obtain the inverse of the potential: Smoothing functionThe smoothing function is defined as It can be shown that Variational formulationThe Chebyshev function evaluated at {{math|x {{=}} et}} minimizes the functional so Notes1. ^{{Cite journal | last = Rosser | first = J. Barkley | author-link1 = J. Barkley Rosser | last2 = Schoenfeld | first2 = Lowell | author-link2 = Lowell Schoenfeld | title = Approximate formulas for some functions of prime numbers. | journal = Illinois J. Math. | year = 1962 | volume = 6 | pages = 64–94. | url = http://projecteuclid.org/DPubS?service=UI&version=1.0&verb=Display&handle=euclid.ijm/1255631807}} * {{note|Dusart2010}} Pierre Dusart, "Estimates of some functions over primes without R.H.". {{arxiv|1002.0442}}
References
External links
1 : Arithmetic functions |
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