Abstract
We construct for the linearized Higgs model a representation of the field operators in a Hilbert space H with the following features: (1) H has a positive definite metric but is nonseparable. (2) The vacuum is gauge invariant. (3) The gauge variant operators exist only in their exponentiated form as unitaries. (4) There is a subspace of H where A{sub {mu}}`{sup {mu}} is represented by 0. (authors).
Citation Formats
Thirring, W, and Narnhofer, H.
Covariant QED without indefinite metric.
Austria: N. p.,
1992.
Web.
Thirring, W, & Narnhofer, H.
Covariant QED without indefinite metric.
Austria.
Thirring, W, and Narnhofer, H.
1992.
"Covariant QED without indefinite metric."
Austria.
@misc{etde_10125478,
title = {Covariant QED without indefinite metric}
author = {Thirring, W, and Narnhofer, H}
abstractNote = {We construct for the linearized Higgs model a representation of the field operators in a Hilbert space H with the following features: (1) H has a positive definite metric but is nonseparable. (2) The vacuum is gauge invariant. (3) The gauge variant operators exist only in their exponentiated form as unitaries. (4) There is a subspace of H where A{sub {mu}}`{sup {mu}} is represented by 0. (authors).}
place = {Austria}
year = {1992}
month = {Apr}
}
title = {Covariant QED without indefinite metric}
author = {Thirring, W, and Narnhofer, H}
abstractNote = {We construct for the linearized Higgs model a representation of the field operators in a Hilbert space H with the following features: (1) H has a positive definite metric but is nonseparable. (2) The vacuum is gauge invariant. (3) The gauge variant operators exist only in their exponentiated form as unitaries. (4) There is a subspace of H where A{sub {mu}}`{sup {mu}} is represented by 0. (authors).}
place = {Austria}
year = {1992}
month = {Apr}
}