TY - JOUR
T1 - Quantum linearization instabilities of de Sitter spacetime. I
AU - Higuchi, A.
PY - 1991
Y1 - 1991
N2 - It is known that all the physical states in linearized gravity are required to be invariant under the continuous isometries of the background spacetime if it is spatially compact. For example, all the physical states in linearized gravity in de Sitter spacetime are required to be SO(4, 1) invariant. A detailed derivation of SO(4, 1) invariance of the physical state is presented. Also, it is found that normal ordering of operators is unnecessary in the constraints which demand SO(4, 1) invariance. Then it is proved that there are no normalizable SO(4, 1)-invariant states other than the vacuum state in the Fock space. This appears to suggest that there would be no dynamics in de Sitter spacetime. A step towards a possible resolution of this paradox will be presented in the sequel to this article.
AB - It is known that all the physical states in linearized gravity are required to be invariant under the continuous isometries of the background spacetime if it is spatially compact. For example, all the physical states in linearized gravity in de Sitter spacetime are required to be SO(4, 1) invariant. A detailed derivation of SO(4, 1) invariance of the physical state is presented. Also, it is found that normal ordering of operators is unnecessary in the constraints which demand SO(4, 1) invariance. Then it is proved that there are no normalizable SO(4, 1)-invariant states other than the vacuum state in the Fock space. This appears to suggest that there would be no dynamics in de Sitter spacetime. A step towards a possible resolution of this paradox will be presented in the sequel to this article.
UR - http://www.scopus.com/inward/record.url?scp=0642385601&partnerID=8YFLogxK
U2 - 10.1088/0264-9381/8/11/009
DO - 10.1088/0264-9381/8/11/009
M3 - Article
AN - SCOPUS:0642385601
SN - 0264-9381
VL - 8
SP - 1961
EP - 1981
JO - Classical and Quantum Gravity
JF - Classical and Quantum Gravity
IS - 11
M1 - 009
ER -