Our starting point for constructing perturbative quantum gravity is the Kawai, Lewellen, and Tye (KLT)
relations [86
] between closed and open string tree-level amplitudes. Since closed string theories are theories
of gravity and open string theories include gauge bosons, in the low energy limit, where string theory
reduces to field theory, these relations then necessarily imply relations between gravity and gauge
theories. The realization that ordinary gauge and gravity field theories emerge from the low
energy limit of string theories has been appreciated for nearly three decades. (See, for example,
Refs. [144, 118, 117
, 69
, 70
, 110
, 111
].)
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