Abstract
In this article I describe the work done with Pushan Majumdar that provided a significant push towards identifying Yang–Mills flux tubes(our works only deal with flux tubes of pure gauge theory, i.e. without dynamical quarks) as the hadronic strings of early days. The main finding was that the static potential V(R) for large \(Q\) \({{\bar{Q}}}\) separations R has the form (D is the space-time dimensionality) \(\begin{aligned} V(R)=\sigma R-\frac{(D-2)\pi }{24R}-\frac{(D-2)^2\pi ^2}{1152\sigma R^3} \cdots \end{aligned}\) for SU(3) in \(D=4\) and SU(2) in \(D=3\). Remarkably this is also the \(\tfrac{1}{R}\) expansion of the ground state energy of the bosonic string theory as given by Arvis. While that derivation is supposed to be valid only in \(D=26\), the measured potentials are for QCD which is a consistent field theory in \(D=3,4\). In subsequent works with Peter Matlock and Yashas Bharadwaj, I resolved this issue within the framework of Polchinski–Strominger effective string theories. I conclude with a brief account of recent and related works.
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Notes
It is important to emphasize that LGT was independently discovered by Wegner, Polyakov and Jan Smit. I quote in verbatim the historical note in Wilson’s talk [10] at the Lepton-Photon symposium of 1983 held at Cornell. " the first studies of lattice gauge theories were carried out independently by Wegner [11], Smit [12], Polyakov [13], and finally myself [8]. The original feature of my paper is its discussion of quark confinement in the lattice theory for strong coupling."
We learnt of the Polchinski–Strominger approach from Prof. Julius Kuti.
I thank one of the referees of this paper for providing me with a concise and accurate account of them which has enabled me to add this very important post-script!
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Hari Dass, N.D. In search of QCD-strings. Indian J Phys 95, 1591–1598 (2021). https://doi.org/10.1007/s12648-021-02128-8
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DOI: https://doi.org/10.1007/s12648-021-02128-8