Fine Art


The sum of all natural numbers 1 + 2 + 3 + 4 + · · · is a divergent series. The nth partial sum of the series is the triangular number

\( \sum_{k=1}^n k = \frac{n(n+1)}{2}, \)

which increases without bound as n goes to infinity. Because the sequence of partial sums fails to converge to a finite limit, the series does not have a sum.

Although the series seems at first sight not to have any meaningful value at all, it can be manipulated to yield a number of mathematically interesting results, some of which have applications in other fields such as complex analysis, quantum field theory, and string theory. Many summation methods are used in mathematics to assign numerical values even to a divergent series. In particular, the methods of zeta function regularization and Ramanujan summation assign the series a value of −1/12, which is expressed by a famous formula:[1]

\( 1+2+3+4+\cdots=-\frac{1}{12}. \)

In a monograph on moonshine theory, Terry Gannon calls this equation “one of the most remarkable formulae in science”.[2]

Partial sums
The first six triangular numbers
Main article: Triangular number

The partial sums of the series 1 + 2 + 3 + 4 + 5 + ⋯ are 1, 3, 6, 10, 15, etc. The nth partial sum is given by a simple formula:

\( \sum_{k=1}^n k = \frac{n(n+1)}{2}. \)

This equation was known to the Pythagoreans as early as the sixth century B.C.E.[3] Numbers of this form are called triangular numbers, because they can be arranged as an equilateral triangle.

The infinite sequence of triangular numbers diverges to +∞, so by definition, the infinite series 1 + 2 + 3 + 4 + ⋯ also diverges to +∞. The divergence is a simple consequence of the form of the series: the terms do not approach zero, so the series diverges by the term test.


Among the classical divergent series, 1 + 2 + 3 + 4 + · · · is relatively difficult to manipulate into a finite value. Many summation methods are used to assign numerical values to divergent series, some more powerful than others. For example, Cesàro summation is a well-known method that sums Grandi's series, the mildly divergent series 1 − 1 + 1 − 1 + ⋯, to 1/2. Abel summation is a more powerful method that not only sums Grandi's series to 1/2, but also sums the trickier series 1 − 2 + 3 − 4 + · · · to 1/4.

Unlike the above series, 1 + 2 + 3 + 4 + · · · is not Cesàro summable nor Abel summable. Those methods work on oscillating divergent series, but they cannot produce a finite answer for a series that diverges to +∞.[4] Most of the more elementary definitions of the sum of a divergent series are stable and linear, and any method that is both stable and linear cannot sum 1 + 2 + 3 +... to a finite value; see below. More advanced methods are required, such as zeta function regularization or Ramanujan summation. It is also possible to argue for the value of −1/12 using some rough heuristics related to these methods.


Passage from Ramanujan's first notebook describing the "constant" of the series

Srinivasa Ramanujan presented two derivations of "1 + 2 + 3 + 4 + ⋯ = −1/12" in chapter 8 of his first notebook.[5][6][7] The simpler, less rigorous derivation proceeds in two steps, as follows.

The first key insight is that the series of positive numbers 1 + 2 + 3 + 4 + · · · closely resembles the alternating series 1 − 2 + 3 − 4 + · · ·. The latter series is also divergent, but it is much easier to work with; there are several classical methods that assign it a value, which have been explored since the 18th century.[8]

In order to transform the series 1 + 2 + 3 + 4 + · · · into 1 − 2 + 3 − 4 + · · ·, one can subtract 4 from the second term, 8 from the fourth term, 12 from the sixth term, and so on. The total amount to be subtracted is 4 + 8 + 12 + 16 + · · ·, which is 4 times the original series. These relationships can be expressed with a bit of algebra. Whatever the "sum" of the series might be, call it c = 1 + 2 + 3 + 4 + ⋯. Then multiply this equation by 4 and subtract the second equation from the first:

\( \begin{alignat}{7} c&{}={}&1+2&&{}+3+4&&{}+5+6+\cdots \\ 4c&{}={}& 4&& {}+8&&{} +12+\cdots \\ -3c&{}={}&1-2&&{}+3-4&&{}+5-6+\cdots \\ \end{alignat} \)

The second key insight is that the alternating series 1 − 2 + 3 − 4 + · · · is the formal power series expansion of the function 1/(1 + x)2 but with x defined as 1. Accordingly, Ramanujan writes:

\( -3c=1-2+3-4+\cdots=\frac{1}{(1+1)^2}=\frac14 \)

Dividing both sides by −3, one gets c = −1/12.

Generally speaking, it is dangerous to manipulate infinite series as if they were finite sums, and it is especially dangerous for divergent series. If zeroes are inserted into arbitrary positions of a divergent series, it is possible to arrive at results that are not self-consistent, let alone consistent with other methods. In particular, the step 4c = 0 + 4 + 0 + 8 + · · · is not justified by the additive identity law alone. For an extreme example, appending a single zero to the front of the series can lead to inconsistent results.[9]

One way to remedy this situation, and to constrain the places where zeroes may be inserted, is to keep track of each term in the series by attaching a dependence on some function.[10] In the series 1 + 2 + 3 + 4 + · · ·, each term n is just a number. If the term n is promoted to a function n−s, where s is a complex variable, then one can ensure that only like terms are added. The resulting series may be manipulated in a more rigorous fashion, and the variable s can be set to −1 later. The implementation of this strategy is called zeta function regularization.

Zeta function regularization
Plot of ζ(s). For s > 1, the series converges and ζ(s) > 1. Analytic continuation around the pole at s = 1 leads to a region of negative values, including ζ(−1) = −1/12

In zeta function regularization, the series \( \sum_{n=1}^\infty n \) is replaced by the series \( \sum_{n=1}^\infty n^{-s} \). The latter series is an example of a Dirichlet series. When the real part of s is greater than 1, the Dirichlet series converges, and its sum is the Riemann zeta function ζ(s). On the other hand, the Dirichlet series diverges when the real part of s is less than or equal to 1, so, in particular, the series 1 + 2 + 3 + 4 + · · · that results from setting s = –1 does not converge. The benefit of introducing the Riemann zeta function is that it can be defined for other values of s by analytic continuation. One can then define the zeta-regularized sum of 1 + 2 + 3 + 4 + · · · to be ζ(−1).

From this point, there are a few ways to prove that ζ(−1) = −1/12. One method, along the lines of Euler's reasoning,[11] uses the relationship between the Riemann zeta function and the Dirichlet eta function η(s). The eta function is defined by an alternating Dirichlet series, so this method parallels the earlier heuristics. Where both Dirichlet series converge, one has the identities:

\( \begin{alignat}{7} \zeta(s)&{}={}&1^{-s}+2^{-s}&&{}+3^{-s}+4^{-s}&&{}+5^{-s}+6^{-s}+\cdots& \\ 2\cdot2^{-s}\zeta(s)&{}={}& 2\cdot2^{-s}&& {}+2\cdot4^{-s}&&{} +2\cdot6^{-s}+\cdots& \\ \left(1-2^{1-s}\right)\zeta(s)&{}={}&1^{-s}-2^{-s}&&{}+3^{-s}-4^{-s}&&{}+5^{-s}-6^{-s}+\cdots&=\eta(s) \\ \end{alignat} \)

The identity \( (1-2^{1-s})\zeta(s)=\eta(s) \) continues to hold when both functions are extended by analytic continuation to include values of s for which the above series diverge. Substituting s = −1, one gets −3ζ(−1)=η(−1). Now, computing η(−1) is an easier task, as the eta function is equal to the Abel sum of its defining series,[12] which is a one-sided limit:

\( -3\zeta(-1)=\eta(-1)=\lim_{x\to 1^-}\left(1-2x+3x^2-4x^3+\cdots\right)=\lim_{x\to 1^-}\frac{1}{(1+x)^2}=\frac14 \)

Dividing both sides by −3, one gets ζ(−1) = −1/12.

Cutoff regularization
A graph depicting the series with layered boxes
The series 1 + 2 + 3 + 4 + ⋯
A graph depicting the smoothed series with layered curving stripes
After smoothing
A graph showing a parabola that dips just below the y-axis
Asymptotic behavior of the smoothing. The y-intercept of the parabola is −1/12.[9]

The method of regularization using a cutoff function can "smooth" the series to arrive at −1/12. Smoothing is a conceptual bridge between zeta function regularization, with its reliance on complex analysis, and Ramanujan summation, with its shortcut to the Euler–Maclaurin formula. Instead, the method operates directly on conservative transformations of the series, using methods from real analysis.

The idea is to replace the ill-behaved discrete series \sum_{n=0}^Nn with a smoothed version \( \sum_{n=0}^\infty nf(n/N) \), where f is a cutoff function with appropriate properties. The cutoff function must be normalized to f(0) = 1; this is a different normalization from the one used in differential equations. The cutoff function should have enough bounded derivatives to smooth out the wrinkles in the series, and it should decay to 0 faster than the series grows. For convenience, one may require that f is smooth, bounded, and compactly supported. One can then prove that this smoothed sum is asymptotic to −1/12 + CN2, where C is a constant that depends on f. The constant term of the asymptotic expansion does not depend on f: it is necessarily the same value given by analytic continuation, −1/12.[9]
Ramanujan summation

The Ramanujan sum of 1 + 2 + 3 + 4 + · · · is also −1/12. Ramanujan wrote in his second letter to G. H. Hardy, dated 27 February 1913:

"Dear Sir, I am very much gratified on perusing your letter of the 8th February 1913. I was expecting a reply from you similar to the one which a Mathematics Professor at London wrote asking me to study carefully Bromwich's Infinite Series and not fall into the pitfalls of divergent series. … I told him that the sum of an infinite number of terms of the series: 1 + 2 + 3 + 4 + · · · = −1/12 under my theory. If I tell you this you will at once point out to me the lunatic asylum as my goal. I dilate on this simply to convince you that you will not be able to follow my methods of proof if I indicate the lines on which I proceed in a single letter. …"[13]

Ramanujan summation is a method to isolate the constant term in the Euler–Maclaurin formula for the partial sums of a series. For a function f, the classical Ramanujan sum of the series \( \sum_{k=1}^\infty f(k) \) is defined as

\( c=-\frac{1}{2}f(0)-\sum_{k=1}^{\infty}\frac{B_{2k}}{(2k)!}f^{(2k-1)}(0), \)

where f(2k−1) is the (2k−1)-th derivative of f and B2k is the 2k-th Bernoulli number: B2 = 1/6, B4 = −1/30, and so on. Setting f(x) = x, the first derivative of f is 1, and every other term vanishes, so:[14]

\( c=-\frac16\cdot\frac{1}{2!} = -\frac{1}{12}. \)

To avoid inconsistencies, the modern theory of Ramanujan summation requires that f is "regular" in the sense that the higher-order derivatives of f decay quickly enough for the remainder terms in the Euler–Maclaurin formula to tend to 0. Ramanujan tacitly assumed this property.[14] The regularity requirement prevents the use of Ramanujan summation upon spaced-out series like 0 + 2 + 0 + 4 + · · ·, because no regular function takes those values. Instead, such a series must be interpreted by zeta function regularization. For this reason, Hardy recommends "great caution" when applying the Ramanujan sums of known series to find the sums of related series.[15]

Failure of stable linear summation methods
This section does not cite any references or sources. Please help improve this section by adding citations to reliable sources. Unsourced material may be challenged and removed. (January 2015)

A summation method that is linear and stable cannot sum the series 1 + 2 + 3 + ... to any finite value. (Stable means that adding a term to the beginning of the series increases the sum by the same amount.) This can be seen as follows. If

1 + 2 + 3 + ... = x

then adding 0 to both sides gives

0 + 1 + 2 + ... = 0 + x = x by stability.

By linearity, one may subtract the second equation from the first to give

1 + 1 + 1 + ... = x – x = 0.

Adding 0 to both sides again gives

0 + 1 + 1 + 1 + ... = 0,

and subtracting the last two series gives

1 + 0 + 0 + ... = 0

contradicting stability.

The methods used above to sum 1 + 2 + 3 + ... are either not stable or not linear. For example, there are two different methods called zeta function regularization. The first, which defines the sum a + b + c + ... of a set of numbers to be the value of the analytic continuation of 1/as + 1/bs + 1/cs + ... at s = –1 (if this exists), is stable but not linear. The second, which defines the sum a + b + c + ... of a sequence of numbers to be the value of the analytic continuation of a/1s + b/2s + c/3s + ... at s = 0 (if this exists), is linear but not stable. (Both methods assign to the series 1 + 2 + 3 + ... the value ζ(–1) = –1/12.)

In bosonic string theory, the attempt is to compute the possible energy levels of a string, in particular the lowest energy level. Speaking informally, each harmonic of the string can be viewed as a collection of D-2 independent quantum harmonic oscillators, one for each transverse direction, where D is the dimension of spacetime. If the fundamental oscillation frequency is \omega then the energy in an oscillator contributing to the nth harmonic is n\hbar\omega/2. So using the divergent series, the sum over all harmonics is -\hbar\omega (D-2)/24. Ultimately it is this fact, combined with the Goddard–Thorn theorem, which leads to bosonic string theory failing to be consistent in dimensions other than 26.[16]

The regularization of 1 + 2 + 3 + 4 + ⋯ is also involved in computing the Casimir force for a scalar field in one dimension.[17] An exponential cutoff function suffices to smooth the series, representing the fact that arbitrarily high-energy modes are not blocked by the conducting plates. The spatial symmetry of the problem is responsible for canceling the quadratic term of the expansion. All that is left is the constant term −1/12, and the negative sign of this result reflects the fact that the Casimir force is attractive.[18]

A similar calculation is involved in three dimensions, using the Epstein zeta-function in place of the Riemann zeta function.[19]

It is unclear whether Leonhard Euler summed the series to −1/12. According to Morris Kline, Euler's early work on divergent series relied on function expansions, from which he concluded 1 + 2 + 3 + 4 + · · · = ∞.[20] According to Raymond Ayoub, the fact that the divergent zeta series is not Abel summable prevented Euler from using the zeta function as freely as the eta function, and he "could not have attached a meaning" to the series.[21] Other authors have credited Euler with the sum, suggesting that Euler would have extended the relationship between the zeta and eta functions to negative integers.[22][23][24] In the primary literature, the series 1 + 2 + 3 + 4 + ⋯ is mentioned in Euler's 1760 publication De seriebus divergentibus alongside the divergent geometric series 1 + 2 + 4 + 8 + ⋯. Euler hints that series of this type have finite, negative sums, and he explains what this means for geometric series, but he does not return to discuss 1 + 2 + 3 + 4 + ⋯. In the same publication, Euler writes that the sum of 1 + 1 + 1 + 1 + ⋯ is infinite.[25]
Popular media

David Leavitt's 2007 novel The Indian Clerk includes a scene where Hardy and Littlewood discuss the meaning of this series. They conclude that Ramanujan has rediscovered ζ(−1), and they take the "lunatic asylum" line in his second letter as a sign that Ramanujan is toying with them.[26]

Simon McBurney's 2007 play A Disappearing Number focuses on the series in the opening scene. The main character, Ruth, walks into a lecture hall and introduces the idea of a divergent series before proclaiming, "I'm going to show you something really thrilling," namely 1 + 2 + 3 + 4 + · · · = −1/12. As Ruth launches into a derivation of the functional equation of the zeta function, another actor addresses the audience, admitting that they are actors: "But the mathematics is real. It's terrifying, but it's real."[27][28]

In January 2014, Numberphile produced a YouTube video on the series, which gathered over 1.5 million views in its first month.[29] The 8-minute video is narrated by Tony Padilla, a physicist at the University of Nottingham. Padilla begins with 1 − 1 + 1 − 1 + · · · and 1 − 2 + 3 − 4 + · · · and relates the latter to 1 + 2 + 3 + 4 + · · · using a term-by-term subtraction similar to Ramanujan's argument.[30] Numberphile also released a 21-minute version of the video featuring Nottingham physicist Ed Copeland, who describes in more detail how 1 − 2 + 3 − 4 + · · · = 1/4 as an Abel sum and 1 + 2 + 3 + 4 + · · · = −1/12 as ζ(−1).[31] After receiving complaints about the lack of rigor in the first video, Padilla also wrote an explanation on his webpage relating the manipulations in the video to identities between the analytic continuations of the relevant Dirichlet series.[32]

In the New York Times coverage of the Numberphile video, mathematician Edward Frenkel commented, "This calculation is one of the best-kept secrets in math. No one on the outside knows about it."[29]


Lepowsky, J. (1999), Naihuan Jing and Kailash C. Misra, ed., Vertex operator algebras and the zeta function, Contemporary Mathematics 248, pp. 327–340, arXiv:math/9909178
Gannon, Terry (April 2010), Moonshine Beyond the Monster: The Bridge Connecting Algebra, Modular Forms and Physics, Cambridge University Press, p. 140
Pengelley, David J. (2002), Otto Bekken et al., eds., The bridge between the continuous and the discrete via original sources, National Center for Mathematics Education, University of Gothenburg, Sweden, p. 3
Hardy p.10
Ramanujan's Notebooks, retrieved January 26, 2014
Abdi, Wazir Hasan (1992), Toils and triumphs of Srinivasa Ramanujan, the man and the mathematician, National, p. 41
Berndt, Bruce C. (1985), Ramanujan’s Notebooks: Part 1, Springer-Verlag, pp. 135–136
Euler, Leonhard; Lucas Willis; and Thomas J Osler (2006). "Translation with notes of Euler's paper: Remarks on a beautiful relation between direct as well as reciprocal power series". The Euler Archive. Retrieved 2007-03-22. Originally published as Euler, Leonhard (1768). "Remarques sur un beau rapport entre les séries des puissances tant directes que réciproques". Memoires de l'academie des sciences de Berlin 17: 83–106.
Tao, Terence (April 10, 2010), The Euler-Maclaurin formula, Bernoulli numbers, the zeta function, and real-variable analytic continuation, retrieved January 30, 2014
Promoting numbers to functions is identified as one of two broad classes of summation methods, including Abel and Borel summation, by Knopp, Konrad (1990) [1922]. Theory and Application of Infinite Series. Dover. pp. 475–476. ISBN 0-486-66165-2.
Stopple, Jeffrey (2003), A Primer of Analytic Number Theory: From Pythagoras to Riemann, p. 202, ISBN 0-521-81309-3
Knopp, Konrad (1990) [1922]. Theory and Application of Infinite Series. Dover. pp. 490–492. ISBN 0-486-66165-2.
Berndt et al. p.53.
Berndt, Bruce C. (1985), Ramanujan’s Notebooks: Part 1, Springer-Verlag, pp. 13,134
Hardy p.346
Barbiellini, Bernardo (1987), "The Casimir effect in conformal field theories", Physics Letters B 190 (1-2): 137–139, doi:10.1016/0370-2693(87)90854-9
See v:Quantum mechanics/Casimir effect in one dimension
Zee pp.65–67
Zeidler, Eberhard (2007), Quantum Field Theory I: Basics in Mathematics and Physics: A Bridge between Mathematicians and Physicists, Springer, pp. 305–306, ISBN 9783540347644.
Kline, Morris (November 1983), "Euler and Infinite Series", Mathematics Magazine 56 (5): 307–314, doi:10.2307/2690371
Ayoub, Raymond (December 1974), "Euler and the Zeta Function" (PDF), The American Mathematical Monthly 81 (10): 1067–1086, doi:10.2307/2319041, retrieved February 14, 2014
Lefort, Jean, "Les séries divergentes chez Euler" (PDF), l'Ouvert (IREM de Strasbourg) (31): 15–25, retrieved February 14, 2014
Kaneko, Masanobu; Kurokawa, Nobushige; Wakayama, Masato (2003), "A variation of Euler's approach to values of the Riemann zeta function" (PDF), Kyushu Journal of Mathematics 57 (1): 175–192, arXiv:math/0206171, doi:10.2206/kyushujm.57.175, retrieved January 31, 2014
Sondow, Jonathan (February 1994), "Analytic continuation of Riemann's zeta function and values at negative integers via Euler's transformation of series", Proceedings of the American Mathematical Society 120 (4): 421–424, doi:10.1090/S0002-9939-1994-1172954-7, retrieved February 14, 2014
Barbeau, E.J.; Leah, P.J. (May 1976), "Euler's 1760 paper on divergent series", Historia Mathematica 3 (2): 141–160, doi:10.1016/0315-0860(76)90030-6
Leavitt, David (2007), The Indian Clerk, Bloomsbury, pp. 61–62
Complicite (April 2012), A Disappearing Number, Oberon
Thomas, Rachel (December 1, 2008), "A disappearing number", Plus, retrieved February 5, 2014
Overbye, Dennis (February 3, 2014), "In the End, It All Adds Up to – 1/12", New York TImes, retrieved February 3, 2014
ASTOUNDING: 1 + 2 + 3 + 4 + 5 + ... = -1/12 on YouTube
Sum of Natural Numbers (second proof and extra footage) on YouTube

Padilla, Tony, What do we get if we sum all the natural numbers?, retrieved February 3, 2014


Berndt, Bruce C., Srinivasa Ramanujan Aiyangar, and Robert A. Rankin (1995). Ramanujan: letters and commentary. American Mathematical Society. ISBN 0-8218-0287-9.
Hardy, G.H. (1949). Divergent Series. Clarendon Press. LCC QA295 .H29 1967.
Zee, A. (2003). Quantum field theory in a nutshell. Princeton UP. ISBN 0-691-01019-6.

Further reading

Lepowsky, James (1999). "Vertex operator algebras and the zeta function". Contemporary Mathematics 248: 327–340. arXiv:math/9909178. doi:10.1090/conm/248/03829.
Zwiebach, Barton (2004). A First Course in String Theory. Cambridge UP. ISBN 0-521-83143-1. See p. 293.
Elizalde, Emilio (2004). "Cosmology: Techniques and Applications". Proceedings of the II International Conference on Fundamental Interactions. arXiv:gr-qc/0409076.
Watson, G. N. (April 1929), "Theorems stated by Ramanujan (VIII): Theorems on Divergent Series", Journal of the London Mathematical Society, 1 4 (2): 82–86, doi:10.1112/jlms/s1-4.14.82

Mathematics Encyclopedia

Retrieved from ""
All text is available under the terms of the GNU Free Documentation License

Home - Hellenica World