TY - JOUR
T1 - Feynman diagrams for stochastic inflation and quantum field theory in de Sitter space
AU - Garbrecht, Björn
AU - Gautier, Florian
AU - Rigopoulos, Gerasimos
AU - Zhu, Yi
N1 - Publisher Copyright:
© 2015 American Physical Society.
PY - 2015/3/19
Y1 - 2015/3/19
N2 - We consider a massive scalar field with quartic self-interaction λ/4!φ4 in de Sitter spacetime and present a diagrammatic expansion that describes the field as driven by stochastic noise. This is compared with the Feynman diagrams in the Keldysh basis of the amphichronous (closed-time-path) field theoretical formalism. For all orders in the expansion, we find that the diagrams agree when evaluated in the leading infrared approximation, i.e. to leading order in m2/H2, where m is the mass of the scalar field and H is the Hubble rate. As a consequence, the correlation functions computed in both approaches also agree to leading infrared order. This perturbative correspondence shows that the stochastic theory is exactly equivalent to the field theory in the infrared. The former can then offer a nonperturbative resummation of the field theoretical Feynman diagram expansion, including fields with 0≤m2λH2 for which the perturbation expansion fails at late times.
AB - We consider a massive scalar field with quartic self-interaction λ/4!φ4 in de Sitter spacetime and present a diagrammatic expansion that describes the field as driven by stochastic noise. This is compared with the Feynman diagrams in the Keldysh basis of the amphichronous (closed-time-path) field theoretical formalism. For all orders in the expansion, we find that the diagrams agree when evaluated in the leading infrared approximation, i.e. to leading order in m2/H2, where m is the mass of the scalar field and H is the Hubble rate. As a consequence, the correlation functions computed in both approaches also agree to leading infrared order. This perturbative correspondence shows that the stochastic theory is exactly equivalent to the field theory in the infrared. The former can then offer a nonperturbative resummation of the field theoretical Feynman diagram expansion, including fields with 0≤m2λH2 for which the perturbation expansion fails at late times.
UR - https://www.scopus.com/pages/publications/84927668572
U2 - 10.1103/PhysRevD.91.063520
DO - 10.1103/PhysRevD.91.063520
M3 - Article
AN - SCOPUS:84927668572
SN - 1550-7998
VL - 91
JO - Physical Review D - Particles, Fields, Gravitation and Cosmology
JF - Physical Review D - Particles, Fields, Gravitation and Cosmology
IS - 6
M1 - 063520
ER -