词条 | Euler–Mascheroni constant | ||||||||
释义 |
The Euler–Mascheroni constant (also called Euler's constant) is a mathematical constant recurring in analysis and number theory, usually denoted by the lowercase Greek letter gamma ({{mvar|γ}}). It is defined as the limiting difference between the harmonic series and the natural logarithm: Here, represents the floor function. The numerical value of the Euler–Mascheroni constant, to 50 decimal places, is: {{gaps|0.57721|56649|01532|86060|65120|90082|40243|10421|59335|93992|...}} {{nowrap|{{OEIS|A001620}}}}
HistoryThe constant first appeared in a 1734 paper by the Swiss mathematician Leonhard Euler, titled De Progressionibus harmonicis observationes (Eneström Index 43). Euler used the notations {{math|C}} and {{math|O}} for the constant. In 1790, Italian mathematician Lorenzo Mascheroni used the notations {{math|A}} and {{math|a}} for the constant. The notation {{mvar|γ}} appears nowhere in the writings of either Euler or Mascheroni, and was chosen at a later time perhaps because of the constant's connection to the gamma function.[2] For example, the German mathematician Carl Anton Bretschneider used the notation {{mvar|γ}} in 1835[3] and Augustus De Morgan used it in a textbook published in parts from 1836 to 1842.[4] AppearancesThe Euler–Mascheroni constant appears, among other places, in the following ('*' means that this entry contains an explicit equation):
PropertiesThe number {{mvar|γ}} has not been proved algebraic or transcendental. In fact, it is not even known whether {{mvar|γ}} is irrational. Continued fraction analysis reveals that if {{mvar|γ}} is rational, its denominator must be greater than 10242080.[6] The ubiquity of {{mvar|γ}} revealed by the large number of equations below makes the irrationality of {{mvar|γ}} a major open question in mathematics. Also see Sondow (2003a). Relation to gamma function{{mvar|γ}} is related to the digamma function {{math|Ψ}}, and hence the derivative of the gamma function {{math|Γ}}, when both functions are evaluated at 1. Thus:This is equal to the limits: Further limit results are (Krämer, 2005): A limit related to the beta function (expressed in terms of gamma functions) is Relation to the zeta function{{mvar|γ}} can also be expressed as an infinite sum whose terms involve the Riemann zeta function evaluated at positive integers:Other series related to the zeta function include: The error term in the last equation is a rapidly decreasing function of {{math|n}}. As a result, the formula is well-suited for efficient computation of the constant to high precision. Other interesting limits equaling the Euler–Mascheroni constant are the antisymmetric limit (Sondow, 1998): and de la Vallée-Poussin's formula where are ceiling brackets. Closely related to this is the rational zeta series expression. By taking separately the first few terms of the series above, one obtains an estimate for the classical series limit: where {{math|ζ(s,k)}} is the Hurwitz zeta function. The sum in this equation involves the harmonic numbers, {{math|Hn}}. Expanding some of the terms in the Hurwitz zeta function gives: where {{math|0 < ε < {{sfrac|1|252n6}}.}} {{mvar|γ}} can also be expressed as follows where {{math|A}} is the Glaisher–Kinkelin constant:Integrals{{mvar|γ}} equals the value of a number of definite integrals:where {{math|Hx}} is the fractional harmonic number. Definite integrals in which {{mvar|γ}} appears include: One can express {{mvar|γ}} using a special case of Hadjicostas's formula as a double integral (Sondow 2003a, 2005) with equivalent series: An interesting comparison by J. Sondow (2005) is the double integral and alternating series It shows that {{math|ln {{sfrac|4|π}}}} may be thought of as an "alternating Euler constant". The two constants are also related by the pair of series (see Sondow 2005 #2) where {{math|N1(n)}} and {{math|N0(n)}} are the number of 1s and 0s, respectively, in the base 2 expansion of {{math|n}}. We have also Catalan's 1875 integral (see Sondow and Zudilin) Series expansionsIn general, for any . However, the rate of convergence of this expansion depends significantly on . In particular, exhibits much more rapid convergence than the conventional expansion .[6][7] This is because while Even so, there exist other series expansions which converge more rapidly than this; some of these are discussed below. Euler showed that the following infinite series approaches {{mvar|γ}}: The series for {{mvar|γ}} is equivalent to a series Nielsen found in 1897:[8] In 1910, Vacca found the closely related series[9] where {{math|log2}} is the logarithm to base 2 and {{math|⌊ ⌋}} is the floor function. In 1926 he found a second series: From the Malmsten–Kummer expansion for the logarithm of the gamma function[10] we get: An important expansion for Euler's constant is due to Fontana and Mascheroni where {{math|Gn}} are Gregory coefficients.[11] This series is the special case of the expansions convergent for A similar series with the Cauchy numbers of the second kind {{math|Cn}} is[12] Blagouchine (2018) found an interesting generalisation of the Fontana-Mascheroni series where {{math|ψn(a)}} are the Bernoulli polynomials of the second kind, which are defined by the generating function For any rational {{math|a}} this series contains rational terms only. For example, at {{math|a {{=}} 1}}, it becomes see OEIS {{OEIS2C|id=A302120}} and {{OEIS2C|id=A302121}}. Other series with the same polynomials include these examples: and where {{math|Γ(a)}} is the gamma function.[13] A series related to the Akiyama-Tanigawa algorithm is where {{math|Gn(2)}} are the Gregory coefficients of the second order.[13] Series of prime numbers: Asymptotic expansions{{mvar|γ}} equals the following asymptotic formulas (where {{math|Hn}} is the {{math|n}}th harmonic number):(Euler) (Negoi) (Cesàro) The third formula is also called the Ramanujan expansion. ExponentialThe constant {{math|e{{isup|γ}}}} is important in number theory. Some authors denote this quantity simply as {{math|γ′}}. {{math|e{{isup|γ}}}} equals the following limit, where {{math|pn}} is the {{math|n}}th prime number: This restates the third of Mertens' theorems.[14] The numerical value of {{math|e{{isup|γ}}}} is: {{gaps|1.78107|24179|90197|98523|65041|03107|17954|91696|45214|30343|...}} {{OEIS2C|id=A073004}}. Other infinite products relating to {{math|e{{isup|γ}}}} include: These products result from the Barnes {{math|G}}-function. We also have where the {{math|n}}th factor is the {{math|(n + 1)}}th root of This infinite product, first discovered by Ser in 1926, was rediscovered by Sondow (2003) using hypergeometric functions. Continued fractionThe continued fraction expansion of {{mvar|γ}} is of the form {{nowrap|[0; 1, 1, 2, 1, 2, 1, 4, 3, 13, 5, 1, 1, 8, 1, 2, 4, 1, 1, 40, ...]}} {{OEIS2C|id=A002852}}, which has no apparent pattern. The continued fraction is known to have at least 470,000 terms,[15] and it has infinitely many terms if and only if {{mvar|γ}} is irrational. GeneralizationsEuler's generalized constants are given by for {{math|0 < α < 1}}, with {{mvar|γ}} as the special case {{math|α {{=}} 1}}.[16] This can be further generalized to for some arbitrary decreasing function {{math|f}}. For example, gives rise to the Stieltjes constants, and gives where again the limit appears. A two-dimensional limit generalization is the Masser–Gramain constant. Euler–Lehmer constants are given by summation of inverses of numbers in a common modulo class:[17][18] The basic properties are and if {{math|gcd(a,q) {{=}} d}} then Published digitsEuler initially calculated the constant's value to 6 decimal places. In 1781, he calculated it to 16 decimal places. Mascheroni attempted to calculate the constant to 32 decimal places, but made errors in the 20th–22nd and 31st-32nd decimal places; starting from the 20th digit, he calculated ...1811209008239 when the correct value is ...0651209008240. Notes
1. ^{{OEIS2C|id=A002852|name=Continued fraction for Euler's constant}} 2. ^{{cite journal| last = Lagarias | first = Jeffrey C. |date=October 2013 | title = Euler's constant: Euler's work and modern developments | journal = Bulletin of the American Mathematical Society | volume = 50 | issue = 4 | page = 556 | url = http://www.ams.org/journals/bull/2013-50-04/S0273-0979-2013-01423-X/S0273-0979-2013-01423-X.pdf | doi=10.1090/s0273-0979-2013-01423-x| arxiv = 1303.1856| bibcode = 1994BAMaS..30..205W }} 3. ^Carl Anton Bretschneider: Theoriae logarithmi integralis lineamenta nova (13 October 1835), Journal für die reine und angewandte Mathematik 17, 1837, pp. 257–285 (in Latin; "{{mvar|γ}} = {{math|c}} = {{nowrap|0,577215 664901 532860 618112 090082 3..}}" on [{{Google |plainurl=yes |id=OAoPAAAAIAAJ |page=260 }} p. 260]) 4. ^Augustus De Morgan: The differential and integral calculus, Baldwin and Craddock, London 1836–1842 ("{{mvar|γ}}" on [https://books.google.com/books?id=95x4IrIcHrgC&pg=PA578 p. 578]) 5. ^{{cite book|last1=Caves |first1=Carlton M. |author-link1=Carlton M. Caves |last2=Fuchs |first2=Christopher A. |chapter=Quantum information: How much information in a state vector? |title=The Dilemma of Einstein, Podolsky and Rosen – 60 Years Later |year=1996 |isbn=9780750303941 |oclc=36922834 |publisher=Israel Physical Society |arxiv=quant-ph/9601025|bibcode=1996quant.ph..1025C }} 6. ^{{cite journal|last=DeTemple|first=Duane W.|date=May 1993|title=A Quicker Convergence to Euler's Constant|journal=The American Mathematical Monthly|volume=100|issue=5|pages=468–470|doi=10.2307/2324300|issn=0002-9890|jstor=2324300}} 7. ^Havil (2003), pp. 75-78 8. ^Krämer (2005), Blagouchine (2016). 9. ^Vacca (1910), Glaisher (1910), Hardy (1912), Vacca (1925), Kluyver (1927), Krämer (2005), Blagouchine (2016). 10. ^Blagouchine (2014). 11. ^Krämer (2005), Blagouchine (2016), Blagouchine (2018). 12. ^Blagouchine (2016), Alabdulmohsin (2018), pp. 147-148. 13. ^1 Blagouchine (2018). 14. ^http://mathworld.wolfram.com/MertensConstant.html (14) 15. ^1 Havil (2003) p. 97. 16. ^Havil (2003), pp. 117–118 17. ^{{cite journal|first1=M. | last1=Ram Murty | first2=N. | last2=Saradha | title=Euler–Lehmer constants and a conjecture of Erdos| journal = JNT| doi=10.1016/j.jnt.2010.07.004| year=2010|volume=130| issue=12 |pages=2671–2681}} 18. ^{{cite journal| first1=D. H. | last1=Lehmer|year=1975|title=Euler constants for arithmetical progressions | journal=Acta Arith. |volume=27 |number=1| pages=125–142|url=http://matwbn.icm.edu.pl/ksiazki/aa/aa27/aa27121.pdf| doi=10.4064/aa-27-1-125-142}} 19. ^1 {{cite web|url=http://www.numberworld.org/nagisa_runs/computations.html|title=Nagisa - Large Computations|author=|date=|website=www.numberworld.org}} }}
|journal=Journal of Computational and Applied Mathematics |year=2000 |volume=121 |issue=1–2 |pages=11 |url=http://www.maths.ex.ac.uk/~mwatkins/zeta/borwein1.pdf |doi=10.1016/s0377-0427(00)00336-8|bibcode=2000JCoAM.121..247B}} Derives {{mvar|γ}} as sums over Riemann zeta functions.
|year=1969|journal=Amer. Math. Monthly|doi=10.2307/2316370|volume=76|issue=3|pages=237–275|jstor=2316370}}
External links
3 : Mathematical constants|Unsolved problems in mathematics|Leonhard Euler |
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