The five-dimensional Watson integral
Find a closed form for the five-dimensional Watson integral W5 ≈ 0.2312616250, which fixes the return probability of a random walk on Z^5.
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| 1 | +# The five-dimensional Watson integral | |
| 2 | + | |
| 3 | +A simple random walk on the five-dimensional integer lattice returns to its starting point with probability about 0.135. That probability is fixed by the Watson integral $W_5 \approx 0.2312616$, which is, up to normalization, the lattice Green function of $\mathbb{Z}^5$ at the origin. Watson's integral has a closed form in three dimensions, and since 2019 one in four dimensions as well. In five dimensions none is known. | |
| 4 | + | |
| 5 | +## Problem | |
| 6 | + | |
| 7 | +For $d \ge 3$ let | |
| 8 | + | |
| 9 | +$$ | |
| 10 | +W_d = \frac{1}{\pi^d} \int_0^\pi \!\!\cdots\! \int_0^\pi \frac{dx_1 \cdots dx_d}{d - \cos x_1 - \cdots - \cos x_d} = \int_0^\infty e^{-dt} \, I_0(t)^d \, dt, | |
| 11 | +$$ | |
| 12 | + | |
| 13 | +where $I_0$ is the modified Bessel function. The second form follows from $1/a = \int_0^\infty e^{-at}\,dt$ and $\frac{1}{\pi}\int_0^\pi e^{t\cos x}\,dx = I_0(t)$. Find a closed-form expression for | |
| 14 | + | |
| 15 | +$$ | |
| 16 | +W_5 = 0.23126162496804623574142702438771339710\ldots | |
| 17 | +$$ | |
| 18 | + | |
| 19 | +in terms of standard constants and special functions. The probability that the simple random walk on $\mathbb{Z}^d$ ever returns to the origin is $1 - 1/(d\,W_d)$ [3], which is about $0.13518$ for $d = 5$. | |
| 20 | + | |
| 21 | +## Background | |
| 22 | + | |
| 23 | +The product $d\,W_d$ is the hypercubic lattice Green function $P(\vec 0; z)$ at $z = 1$. Such Green functions give return probabilities of random walks and effective resistances of resistor networks [3]. For $d = 3$, Watson evaluated the cubic-lattice integrals in 1939 [1], and Glasser and Zucker reduced the simple-cubic case to a product of Gamma values in 1977 [2]. Laporta conjectured that the four-dimensional integral is, up to a constant, a four-loop sunrise Feynman diagram of two-dimensional quantum field theory. Zhou proved this, together with a reduction to special values of Euler's Gamma function and generalized hypergeometric series [4]. Five dimensions is the next case. | |
| 24 | + | |
| 25 | +## What is known | |
| 26 | + | |
| 27 | +- $d = 3$: Watson (1939) evaluated the integral with elliptic integrals [1], and Glasser and Zucker (1977) gave a closed form in Gamma values [2, 3]. | |
| 28 | +- $d = 4$: Laporta's conjectured formulae were proved by Zhou (2019). They link $W_4$ to the four-loop sunrise integral and reduce it to Gamma values and generalized hypergeometric series [4]. | |
| 29 | +- $d = 5$: Guttmann (2010) treated lattice Green functions in all dimensions. The five-dimensional hypercubic one satisfies a linear differential equation of order 5 [3]. No closed form for $W_5$ is known. HorizonMath's reference value has 110 digits. | |
| 30 | + | |
| 31 | +## What would count as progress | |
| 32 | + | |
| 33 | +- A closed-form expression that agrees with $W_5$ to 20 significant digits, HorizonMath's acceptance threshold. Its evaluator checks this at 100-digit precision and rejects numerical shortcuts such as quadrature, root-finding, infinite series and fitted constants. The Bessel form lets anyone compute $W_5$ to many more digits, so candidates can be tested far beyond 20. | |
| 34 | +- A proof of such an evaluation, or an exact reduction of $W_5$ to Bessel moments or periods that are already understood. | |
| 35 | + | |
| 36 | +## References | |
| 37 | + | |
| 38 | +1. G. N. Watson, "Three triple integrals", *Q. J. Math.* 10 (1939), 266–276. [doi:10.1093/qmath/os-10.1.266](https://doi.org/10.1093/qmath/os-10.1.266) | |
| 39 | +2. M. L. Glasser and I. J. Zucker, "Extended Watson integrals for the cubic lattices", *Proc. Natl. Acad. Sci. USA* 74 (1977), 1800–1801. [doi:10.1073/pnas.74.5.1800](https://doi.org/10.1073/pnas.74.5.1800) | |
| 40 | +3. A. J. Guttmann, "Lattice Green's functions in all dimensions", *J. Phys. A* 43 (2010), 305205. [doi:10.1088/1751-8113/43/30/305205](https://doi.org/10.1088/1751-8113/43/30/305205), [arXiv:1004.1435](https://arxiv.org/abs/1004.1435) | |
| 41 | +4. Y. Zhou, "On Laporta's 4-loop sunrise formulae", *Ramanujan J.* 50 (2019), 465–503. [doi:10.1007/s11139-018-0090-z](https://doi.org/10.1007/s11139-018-0090-z), [arXiv:1801.02182](https://arxiv.org/abs/1801.02182) | |
| 42 | + | |
| 43 | +## Source | |
| 44 | + | |
| 45 | +Imported from [HorizonMath w5_watson_integral](https://github.com/ewang26/HorizonMath/blob/4ef0b61a8a6d4c5ded661fab7c2e896af84abe6e/data/problems_full.json#L13-L23), curated by Erik Y. Wang, Sumeet R. Motwani et al. Open according to the source as of 2026-10-20. The statement above is written in our own words; see the source for the original wording, history and discussion. | |