Seminars and Journal Clubs

The quantum enhanced Virgo interferometer

by Dr Marco Vardaro (Universita' di Padova, Italy)

Europe/Brussels
E/3rd floor-E.349 - Seminar room (E.349) (Marc de Hemptinne (chemin du Cyclotron, 2, Louvain-la-Neuve))

E/3rd floor-E.349 - Seminar room (E.349)

Marc de Hemptinne (chemin du Cyclotron, 2, Louvain-la-Neuve)

30
Description

Virgo is a giant laser interferometer designed to detect gravitational waves (GW). It is built in Cascina, in Italy near Pisa. Gravitational waves can be produced by different astrophysical sources in different frequency bandwidths. Terrestrial interferometers are sensitive in the bandwidth between 10 Hz and 10 kHz, thus the main astrophyiscal sources that can be detected by GW interferometers are supernova explosions and the merger of binary system composed by black holes or neutron stars.

However, the detection of this phenomena is not an easy task. The mirrors displacement, induced by a gravitational wave in a terrestrial interferometer is of the order of 10^-19 m. Thus, more than fifty years of experimental and technology developments were needed before the first direct gravitational wave detection by the two LIGO interferometer in the 2015.


The sensitivity of a GW interferometer is limited both by classical noises (i.e. seismic, thermal and Newtonian noise) and quantum noies. Quantum noise that limits GW-interferometers, in the form of shot noise and quantum radiation pressure, is ultimately due to the interaction of the main laser field with quantum vacuum fluctuations that enter the instruments through the ”dark” output port. A key towards better sensitivity in GW detectors is to suppress the quantum noise. One way to improve the sensitivity of GW detectors, without minimal modification to their optical configuration, is to inject squeezed vacuum states through the dark port.
Squeezed vacuum states are special quantum states of the electromagnetic fields in which quantum vacuum fluctuations, rather than being equally distributed among the two quadratures that describe the EM field, are reduced in one quadrature at the expense of the other. Which quadrature is chosen has a different effect on the observed level of shot or radiation-pressure noise. Such states can be generated by a nonlinear crystal via
the Optical Parametric Amplification process (OPA). Injection of squeezed vacuum states through the interferometer dark port has been already demonstrated to effectively reduce quantum noise in the large-scale interferometric GW detectors GEO600, LIGO and more recently in Virgo.
The upgrade program of the Advanced Virgo detector foresees the injection of squeezed vacuum to reduce quantum noise. In a first phase (observing run 3, or O3), frequency-independent squeezed vacuum will be injected; in this case the ”squeezed” quadrature is the same at all frequencies, leading to a decrease in the detector shot noise contribution at high frequencies while increasing, at low frequency, radiation pressure noise, which is however not yet a dominant contribution. The squeezing light source used for this
purpose was developed by the AEI collaboration. I will present the main features and performance of the low-loss squeezed-vacuum injection subsystem and related controls system. Moreover the first Advanced Virgo long-term results related to the use of squeezed light will be discussed.

Organised by

Giacomo Bruno