Abstract

According to the KKLT scenario, metastable dS vacua are formed as a result of uplifting of supersymmetric AdS vacua by D3‾\overline {D3} branes. I describe an extended version of this scenario where metastable dS vacua appear after an uplift from a state where the potential of the volume modulus in the absence of D3‾\overline {D3} branes would be unbounded below. This mechanism may considerably strengthen vacuum stabilization in the early universe.

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