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005 | 20250730145615.0 | ||
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088 | _ | _ | |a DESY-14-132 |2 DESY |
100 | 1 | _ | |a Dudas, Emilian |0 P:(DE-H253)PIP1022049 |b 0 |e Corresponding Author |u desy |
245 | _ | _ | |a Three-Form Multiplet and Inflation |
260 | _ | _ | |a Berlin |c 2014 |b Springer |
336 | 7 | _ | |a article |2 DRIVER |
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500 | _ | _ | |a OA |
520 | _ | _ | |a Most successful models of inflation in supergravity have a shift symmetry for the inflaton and contain a stabilizer field coupled to the inflaton in a particular way. We argue that the natural interpretation of the stabilizer, from the viewpoint of the shift symmetry, is a three-form multiplet. Its coupling to the inflaton is uniquely determined by the shift symmetry and the invariance under three-form gauge transformations and has a natural string theory interpretation. |
536 | _ | _ | |a 514 - Theoretical Particle Physics (POF2-514) |0 G:(DE-HGF)POF2-514 |c POF2-514 |f POF II |x 0 |
536 | _ | _ | |a MASSTEV - Mass hierarchy and particle physics at the TeV scale (226371) |0 G:(EU-Grant)226371 |c 226371 |f ERC-2008-AdG |x 1 |
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650 | _ | 7 | |a differential forms: 3 |2 autogen |
650 | _ | 7 | |a transformation: gauge |2 autogen |
650 | _ | 7 | |a inflation: model |2 autogen |
650 | _ | 7 | |a inflaton |2 autogen |
650 | _ | 7 | |a stability |2 autogen |
650 | _ | 7 | |a multiplet |2 autogen |
650 | _ | 7 | |a string model |2 autogen |
650 | _ | 7 | |a supergravity |2 autogen |
650 | 2 | 0 | |a Supergravity Models |2 Author |
650 | 2 | 0 | |a Supersymmetric Effective Theories |2 Author |
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773 | _ | _ | |a 10.1007/JHEP12(2014)014 |g Vol. 2014, no. 12, p. 14 |0 PERI:(DE-600)2027350-2 |n 12 |p 14 |t Journal of high energy physics |v 2014 |y 2014 |x 1029-8479 |
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