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Related papers: The Ultraviolet Finiteness of N=8 Supergravity

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The Lorentz covariant all-loop counterterms built in the 4+32 on shell superspace of N=8 supergravity imply that the theory is not UV finite. Meanwhile, the relevant counterterms depending on the light-cone superfields in 4+16 superspace…

High Energy Physics - Theory · Physics 2008-11-16 Renata Kallosh

We study candidate counterterms (CT)'s in maximal supergravities in diverse integer dimensions $d \geq 4 $. We find that UV divergences in these theories occur at the number of loops $L$ below certain critical value $L_{cr}$. At $L\geq…

High Energy Physics - Theory · Physics 2023-05-02 Renata Kallosh

We construct the generating functional for the light-cone superfield amplitudes in a chiral momentum superspace. It generates the n-point particle amplitudes which on shell are equivalent to the covariant ones. Based on the action depending…

High Energy Physics - Theory · Physics 2013-05-29 Renata Kallosh

We study N=8 supergravity deformed by the presence of the candidate counterterms. We show that even though they are invariant under undeformed E{7(7)}, all of the candidate counterterms violate the deformed E{7(7)} current conservation. The…

High Energy Physics - Theory · Physics 2015-05-27 Renata Kallosh

We review the development of understanding for the problem of ultraviolet divergences in supergravity. This history proceeds from initial constructions of counterterms invariant under the relevant degrees of local supersymmetry, through a…

High Energy Physics - Theory · Physics 2025-03-04 G. Bossard , K. S. Stelle

According to the recent pure spinor analysis of the UV divergences by Karlsson, there are no divergent 1PI structures beyond 6 loops in D=4 N=8 supergravity. In combination with the common expectation that the UV divergences do not appear…

High Energy Physics - Theory · Physics 2014-12-23 Renata Kallosh

We present a pedagogical review of our current understanding of the ultraviolet structure of N = (1,1) 6D supersymmetric Yang-Mills theory and of N = 8 4D supergravity. These theories are not renormalizable, they involve power ultraviolet…

High Energy Physics - Theory · Physics 2017-04-05 A. V. Smilga

Conventional wisdom holds that no four-dimensional gravity field theory can be ultraviolet finite. This understanding is based mainly on power counting. Recent studies confirm that one-loop N = 8 supergravity amplitudes satisfy the…

High Energy Physics - Theory · Physics 2008-11-26 Zvi Bern , Lance J. Dixon , Radu Roiban

We describe the construction of the complete four-loop four-particle amplitude of N=8 supergravity. The amplitude is ultraviolet finite, not only in four dimensions, but in five dimensions as well. The observed extra cancellations provide…

High Energy Physics - Theory · Physics 2015-03-13 Z. Bern , J. J. Carrasco , L. J. Dixon , H. Johansson , R. Roiban

We discuss various approaches to the problem of determining which supersymmetric invariants are permitted as counterterms in maximally supersymmetric super Yang--Mills and supergravity theories in various dimensions. We review the…

High Energy Physics - Theory · Physics 2009-05-07 G. Bossard , P. S. Howe , K. S. Stelle

We present the explicit expressions in N=8 supergravity for the bosonic 4-particle tree and 1-loop amplitudes including vectors and scalars. We also present the candidate 4-point UV divergences in a form of helicity amplitudes,…

High Energy Physics - Theory · Physics 2009-09-29 Renata Kallosh , Ching Hua Lee , Tomas Rube

The 4-loop 4-point amplitude in N=8 d=4 supergravity is UV finite due to supersymmetry. Even better UV behavior of the 4-loop 4-point amplitude, analogous to that of N=4 SYM theory, has been recently established by computation in [1]. All…

High Energy Physics - Theory · Physics 2009-10-02 Renata Kallosh

We examine conservation of the E7(7) Noether-Gaillard-Zumino current in the presence of N=8 supergravity counterterms using the momentum space helicity formalism, which significantly simplifies the calculations. The main result is that the…

High Energy Physics - Theory · Physics 2011-06-20 Renata Kallosh

We hereby introduce and extensively study a class of non-polynomial higher derivative theories of gravity that realize a ultraviolet (UV) completion of Einstein general relativity. These theories are unitary (ghost free) and at most only…

High Energy Physics - Theory · Physics 2018-09-03 Leonardo Modesto , Leslaw Rachwal

We consider the ultra-violet divergence structure of general noncommutative supersymmetric $U(N_c)$ gauge theories, and seek theories which are all-orders finite.

High Energy Physics - Theory · Physics 2008-11-26 I. Jack , D. R. T. Jones

The UV finiteness found in calculations of the 4-point amplitude in $\mathcal N=5$ supergravity at loop order $L=3, 4$ has not been explained, which motivates our study of the relevant superspace invariants and on-shell superamplitudes for…

High Energy Physics - Theory · Physics 2018-10-09 Daniel Z. Freedman , Renata Kallosh , Yusuke Yamada

We give a relatively simple explanation of the light-cone supergraph prediction for the UV properties of the maximally supersymmetric theories. It is based on the existence of a dynamical supersymmetry which is not manifest in the…

High Energy Physics - Theory · Physics 2010-06-25 Renata Kallosh , Pierre Ramond

We show that the four-loop four-point amplitudes of N = 5 supergravity are ultraviolet finite in four dimensions, contrary to expectations based on supersymmetry and duality-symmetry arguments. We explain why the diagrams of any covariant…

High Energy Physics - Theory · Physics 2014-11-19 Zvi Bern , Scott Davies , Tristan Dennen

Investigation of on-shell superinvariants is the standard way to identify the candidate UV divergences in supergravity. Geometric on-shell superinvariants in 4d supergravity at $N\geq 4$ are available starting at the critical loop order.…

High Energy Physics - Theory · Physics 2023-12-13 Renata Kallosh

We argue that N=4 supergravity is 3-loop UV finite because the relevant supersymmetric candidate counterterm is known to be SL(2, R)x SO(6) invariant, which violates the Noether-Gaillard-Zumino current conservation. Analogous arguments,…

High Energy Physics - Theory · Physics 2013-05-30 Renata Kallosh
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