Abstract
We solve the closed Schwinger–Dyson equation for the 2-point function of a tensor field theory with a quartic melonic interaction, in terms of Lambert’s W function, using a perturbative expansion and Lagrange–Bürmann resummation. Higher-point functions are then obtained recursively.
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Notes
Not to be confused with tensor fields living on a space-time such as in [4].
We computed the expansion up to order 9 in the coupling using Mathematica.
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Acknowledgements
The author would like to thank Raimar Wulkenhaar for his guidance throughout this project, Adrian Tanasa for his advice and comments on the manuscript and Alexander Hock for helpful discussions.
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Funded by the Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) under Germany’s Excellence Strategy EXC 2044–390685587, Mathematics Münster: Dynamics–Geometry–Structure and partially supported by the CNRS Infiniti ModTens Grant.
Appendix A: Recurrence relations
Appendix A: Recurrence relations
In this section, we will use the recursive equation (11) to determine recurrence relations on the numbers \(a_{n,k,m}\). We first perform the integration
where for \(p=1\) the sum on r does not appear. Plugging back the ansatz (19) in the recurrence relation (11) with \(c=1\) gives
The first term of (44) gives
where we sent \(k \rightarrow k+1\) and \(m \rightarrow m+1\) to get to the last line. The second term of (44) gives
Setting \(r=p+k\) in the line of the previous equation, let us rewrite the double sum as
Then, we send \(m \rightarrow m+1\) and rewrite double sum to get
Hence, sending \(p \rightarrow n-p\) and collecting the results, we get
The third term of (44) gives
The first term of Eq. (50) gives
by setting \(k=p-r\). Then, by setting \(l=n-1-k\) and rewriting the sums, we get
Then, we set \(k = l-r+1\) and obtain
The second term of (50) gives, by rewriting the sums,
First by setting \(q=k+r\) and by several rewriting of the sums, we get
where we send \(l \rightarrow l+1\) in the last line.
Now, collecting all the results, we obtain recurrence relations on \(a_{n,k,m}\):
Rewriting these equations gives explicit relations on Stirling numbers of the first kind, harmonic numbers and binomial coefficients. Indeed, from Eq. (60), we recover
which corresponds to equation (6.21) in [16].
Setting \(l=n-2-r \), \(k = n-m-1 \) and sending \(n-3 \rightarrow n\), Eq. (59) gives
Sending \(r \rightarrow k-l\) and in the last term \(l \rightarrow r\) of Eq. (61), we get
for \(k \in \llbracket 2,n-3 \rrbracket \) and \(m \in \llbracket 2,k \rrbracket \).
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Pascalie, R. A solvable tensor field theory. Lett Math Phys 110, 925–943 (2020). https://doi.org/10.1007/s11005-019-01245-0
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DOI: https://doi.org/10.1007/s11005-019-01245-0