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Causality and supersymmetry in the superstring theory

M D Pollock

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Reduction of the ten-dimensional, heterotic-superstring effective action hat S, including quartic higher-derivative terms \hat{\calR}^4, yields a physical four-action S which is tachyon-free up to quadratic order Script R2—the masses M0 and M2 of the spin-0 and spin-2 particles are both real—when the internal six-space is a Calabi–Yau metric bar gμν and N = 1 supersymmetry is preserved via the equation dbar H ≡ tr(bar R wedge bar R) − Tr(bar F wedge bar F)/30 = 0, where bar Hμνξ is the totally antisymmetric three-index field (while the bosonic string and type-II superstring may contain a spin-2 tachyon and a spin-0 tachyon, respectively). Here, we show that this crucial feature is independent of imposing supersymmetry, for if dbar H ≠ 0, there is an additional contribution to Script R2 which, however, produces no tachyons. Thus, the requirement of a stable, causal theory singles out the heterotic superstring irrespective of the requirement of N = 1 supersymmetry, which is essential at high energies rather for its roles in the vanishing of the cosmological constant and the maintenance of the gauge hierarchy.


PACS

11.30.Pb Supersymmetry

11.15.-q Gauge field theories

14.80.-j Other particles (including hypothetical)

11.25.-w Strings and branes

02.40.Sf Manifolds and cell complexes

MSC

14J32 Calabi-Yau manifolds, mirror symmetry

81T60 Supersymmetric field theories

81T30 String and superstring theories; other extended objects (e.g., branes) (See also 83E30)

Subjects

Mathematical physics

Particle physics and field theory

Dates

Issue 13 (7 July 2003)

Received 20 September 2002, in final form 2 April 2003

Published 23 May 2003



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