Quantum field theory is a highly successful and experimentally well-tested framework for describing elementary particles and the four fundamental forces of nature. In quantum field theory, the primary objects of interest are scattering amplitudes. These amplitudes are plagued by ultraviolet divergences at high energies. Enhancing the symmetry in the theory improves the ultraviolet properties. Supersymmetric quantum field theories are of great interest in this context as they exhibit dramatically improved ultraviolet behavior. The theme of my current research, thus, focuses on studying the aspects of maximally supersymmetric theories, particularly concerning N=4 super Yang-Mills theory in four dimensions.


Supersymmetry without anti-commuting variables

Pure supersymmetric Yang-Mills theories exist in D = 3,4,6 and 10 dimensions. The maximally extended N=4; D=4 theory is ultraviolet finite and conformally invariant. It is related under the AdS/CFT correspondence to type II superstring theory compactified on a 5-sphere to an asymptotically anti-de Sitter space-time. All these links motivate us to investigate supersymmetric Yang-Mills theories and their properties from every possible angle.

Supersymmetric theories can be formulated without the use of anti-commuting variables. In this approach, supersymmetric gauge theories are characterized by a Nicolai map – a transformation of the bosonic fields such that the Jacobian determinant of the transformation exactly cancels against the product of the Matthews-Salam-Seiler (MSS) and Faddeev-Popov determinants. The formalism avoids any use of anti-commuting objects thus offering an alternate perspective on the physics of gauge theories.

We took up an old thread of development concerning the characterization of supersymmetric theories without any use of anticommuting variables. Our special focus was on the formulation of supersymmetric Yang-Mills theories, extending previous results beyond D = 4 dimensions.


  • We derived for the first time the map up to the second order in the coupling constant and extended it to all pure supersymmetric Yang-Mills theories. The above construction makes use of a method called R prescription. As a new result, we recovered the classical result that interacting pure supersymmetric Yang-Mills theories can exist only in space-time dimensions D = 3, 4, 6, 10. The above result is quite remarkable in the sense that we can entirely formulate supersymmetric Yang-Mills theories in these space-time dimensions without using anti-commuting variables.

  • We also extended the map and the framework itself to the third order in the coupling constant by deriving an explicit formula for the transformation. The Feynman-like graphical approach was outlined using tree diagrams, which in principle allow one to extend the construction to all orders in the coupling constant.

  • We addressed the uniqueness of the Nicolai map by finding a new transformation, also to the third order in the coupling constant, but valid exclusively in six dimensions. We arrived at the map by starting with an educated guess. This new map is simpler than the one obtained using the R operator thus highlighting a potential ambiguity in the formalism.


I plan to study and understand how the symmetries in the theory are reflected in this new `mapped’ formalism. This approach yields new insights beyond those obtained using the traditional formulation: specifically for objects of interest to a physicist, like scattering amplitudes and correlation functions