2022
DOI: 10.1088/1475-7516/2022/11/054
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What do gravitational wave detectors say about polymer quantum effects?

Abstract: We compute the expected response of detector arms of gravitational wave observatories to polymerized gravitational waves. The mathematical and theoretical features of these waves were discussed in our previous work. In the present manuscript, we find both perturbative analytical, and full nonperturbative numerical solutions to the equations of motion of the detector arms using the method of geodesic deviations. These results show the modifications to both frequency and amplitude of the signal measured by the d… Show more

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Cited by 2 publications
(8 citation statements)
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“…The reality conditions on the fields indicates that not all the modes are independent. To have an independent expansion for each mode and write the Hamiltonian as a set of decoupled harmonic oscillators, we introduce new variables A λ,k and E λ,k and split the lattice L into positive and negative sectors; for more details see [11,12]. In terms of these new variables, the Hamiltonian of the perturbation field reads…”
Section: Brief Review Of the Theorymentioning
confidence: 99%
See 4 more Smart Citations
“…The reality conditions on the fields indicates that not all the modes are independent. To have an independent expansion for each mode and write the Hamiltonian as a set of decoupled harmonic oscillators, we introduce new variables A λ,k and E λ,k and split the lattice L into positive and negative sectors; for more details see [11,12]. In terms of these new variables, the Hamiltonian of the perturbation field reads…”
Section: Brief Review Of the Theorymentioning
confidence: 99%
“…Actually, in the standard representation one can recover the fundamental operators A and E due to the weak continuity condition of the Stone-von Neumann theorem is satisfied. However, polymer quantization violates such a condition and therefore, it is not unitarily equivalent to the standard quantum mechanics [11,12]. In this case, the Hilbert space is given by L 2 (R, dx Bohr ), where the configuration space, R, is the Bohr compactification of the real line and dx Bohr is the Haar measure.…”
Section: Brief Review Of the Theorymentioning
confidence: 99%
See 3 more Smart Citations