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Dive into the research topics where G. Ballardin is active.

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Featured researches published by G. Ballardin.


Astronomy and Astrophysics | 2012

Implementation and testing of the first prompt search for gravitational wave transients with electromagnetic counterparts

J. Abadie; B. Abbott; R. Abbott; T. D. Abbott; M. Abernathy; T. Accadia; F. Acernese; C. Adams; R. Adhikari; C. Affeldt; M. Agathos; P. Ajith; B. Allen; G. Allen; E. Amador Ceron; D. Amariutei; R. Amin; S. Anderson; W. G. Anderson; K. Arai; M. A. Arain; M. C. Araya; S. Aston; P. Astone; D. Atkinson; P. Aufmuth; C. Aulbert; B. E. Aylott; S. Babak; P. Baker

Aims. A transient astrophysical event observed in both gravitational wave (GW) and electromagnetic (EM) channels would yield rich scientific rewards. A first program initiating EM follow-ups to possible transient GW events has been developed and exercised by the LIGO and Virgo community in association with several partners. In this paper, we describe and evaluate the methods used to promptly identify and localize GW event candidates and to request images of targeted sky locations. Methods. During two observing periods (Dec. 17, 2009 to Jan. 8, 2010 and Sep. 2 to Oct. 20, 2010), a low-latency analysis pipeline was used to identify GW event candidates and to reconstruct maps of possible sky locations. A catalog of nearby galaxies and Milky Way globular clusters was used to select the most promising sky positions to be imaged, and this directional information was delivered to EM observatories with time lags of about thirty minutes. A Monte Carlo simulation has been used to evaluate the low-latency GW pipelines ability to reconstruct source positions correctly. Results. For signals near the detection threshold, our low-latency algorithms often localized simulated GW burst signals to tens of square degrees, while neutron star/neutron star inspirals and neutron star/black hole inspirals were localized to a few hundred square degrees. Localization precision improves for moderately stronger signals. The correct sky location of signals well above threshold and originating from nearby galaxies may be observed with similar to 50% or better probability with a few pointings of wide-field telescopes.Aims. A transient astrophysical event observed in both gravitational wave (GW) and electromagnetic (EM) channels would yield rich scientific rewards. A first program initiating EM follow-ups to possible transient GW events has been developed and exercised by the LIGO and Virgo community in association with several partners. In this paper, we describe and evaluate the methods used to promptly identify and localize GW event candidates and to request images of targeted sky locations. Methods. During two observing periods (Dec 17 2009 to Jan 8 2010 and Sep 2 to Oct 20 2010), a low-latency analysis pipeline was used to identify GW event candidates and to reconstruct maps of possible sky locations. A catalog of nearby galaxies and Milky Way globular clusters was used to select the most promising sky positions to be imaged, and this directional information was delivered to EM observatories with time lags of about thirty minutes. A Monte Carlo simulation has been used to evaluate the low-latency GW pipelines ability to reconstruct source positions correctly. Results. For signals near the detection threshold, our low-latency algorithms often localized simulated GW burst signals to tens of square degrees, while neutron star/neutron star inspirals and neutron star/black hole inspirals were localized to a few hundred square degrees. Localization precision improves for moderately stronger signals. The correct sky location of signals well above threshold and originating from nearby galaxies may be observed with ~50% or better probability with a few pointings of wide-field telescopes.


Review of Scientific Instruments | 2001

Measurement of the VIRGO superattenuator performance for seismic noise suppression

G. Ballardin; L. Bracci; S. Braccini; C. Bradaschia; C. Casciano; G. Calamai; R. Cavalieri; R. Cecchi; G. Cella; Elena Cuoco; E. D’Ambrosio; V. Dattilo; A. Di Virgilio; L. Fabbroni; F. Fidecaro; F. Frasconi; A. Gaddi; A. Gennai; G. Gennaro; A. Giazotto; G. Losurdo; L. Holloway; P. La Penna; F. Lelli; E. Majorana; M. Mazzoni; F. Paoletti; M. Pasotti; A. Pasqualetti; R. Passaquieti

Below a few tens of hertz interferometric detection of gravitational waves is masked by seismic vibrations of the optical components. In order to isolate the mirrors of the VIRGO interferometer, a sophisticated suspension system, called superattenuator, has been developed. Its working principle is based on a multistage pendulum acting on seismic vibrations as a chain of second order mechanical low-pass filters. A complete superattenuator has been built and tested. This apparatus allows extending the VIRGO detection band down to a few Hz. A detailed description of the attenuation system and its performance are presented in this article.


The Astrophysical Journal | 2010

Search for gravitational-wave bursts associated with gamma-ray bursts using data from LIGO science run 5 and VIRGO science run 1.

B. Abbott; R. Abbott; F. Acernese; R. Adhikari; P. Ajith; B. Allen; G. Allen; R. Amin; S. Anderson; W. G. Anderson; F. Antonucci; S. Aoudia; M. C. Araya; H. Armandula; P. Armor; K. G. Arun; Y. Aso; S. Aston; P. Astone; P. Aufmuth; C. Aulbert; S. Babak; P. Baker; G. Ballardin; S. Ballmer; C. Barker; D. Barker; F. Barone; B. Barr; P. Barriga

We present the results of a search for gravitational-wave bursts associated with 137 gamma-ray bursts (GRBs) that were detected by satellite-based gamma-ray experiments during the fifth LIGO science run and first Virgo science run. The data used in this analysis were collected from 2005 November 4 to 2007 October 1, and most of the GRB triggers were from the Swift satellite. The search uses a coherent network analysis method that takes into account the different locations and orientations of the interferometers at the three LIGO-Virgo sites. We find no evidence for gravitational-wave burst signals associated with this sample of GRBs. Using simulated short-duration (<1 s) waveforms, we set upper limits on the amplitude of gravitational waves associated with each GRB. We also place lower bounds on the distance to each GRB under the assumption of a fixed energy emission in gravitational waves, with typical limits of D ~ 15 Mpc (E_GW^iso / 0.01 M_o c^2)^1/2 for emission at frequencies around 150 Hz, where the LIGO-Virgo detector network has best sensitivity. We present astrophysical interpretations and implications of these results, and prospects for corresponding searches during future LIGO-Virgo runs.


Review of Scientific Instruments | 2001

Inertial control of the mirror suspensions of the VIRGO interferometer for gravitational wave detection

G. Losurdo; G. Calamai; Elena Cuoco; L. Fabbroni; G. Guidi; M. Mazzoni; R. Stanga; F. Vetrano; L. Holloway; D. Passuello; G. Ballardin; S. Braccini; C. Bradaschia; R. Cavalieri; R. Cecchi; G. Cella; V. Dattilo; A. Di Virgilio; F. Fidecaro; F. Frasconi; A. Gennai; A. Giazotto; I. Ferrante; P. La Penna; F. Lelli; T. Lomtadze; A. Marin; S. Mancini; F. Paoletti; A. Pasqualetti

In order to achieve full detection sensitivity at low frequencies, the mirrors of interferometric gravitational wave detectors must be isolated from seismic noise. The VIRGO vibration isolator, called the superattenuator, is fully effective at frequencies above 4 Hz. But the residual motion of the mirror at the mechanical resonant frequencies of the system is too large for the interferometer locking system and must be damped. A multidimensional feedback system, using inertial sensors and digital processing, has been designed for this purpose. An experimental procedure for determining the feedback control of the system has been defined. In this article a full description of the system is given and experimental results are presented.


Review of Scientific Instruments | 2001

Measurement of the transfer function of the steering filter of the Virgo super attenuator suspension

G. Ballardin; S. Braccini; C. Bradaschia; C. Casciano; R. Cavalieri; R. Cecchi; V.S. Chickarmane; V. Dattilo; A. Di Virgilio; I. Ferrante; F. Fidecaro; F. Frasconi; A. Gaddi; A. Gennai; A. Giazotto; L. Holloway; T. Lomtazde; F. Paoletti; A. Pasqualetti; R. Passaquieti; D. Passuello; R. Poggiani; R. Taddei; A. Viceré; Z. Zhang; E. Cuoco; G. Losurdo; Wei-Tou Ni; Jeah-Sheng Wu; Chun-Hsiung Chang

The optical elements of the Virgo antenna are supported and isolated from seismic noise disturbances by super attenuator (SA) suspensions. The steering filter (SF) is a component of the SA, designed for the mirror control. The dynamical properties of the SF are described by transfer functions, which have been measured in order to define the control strategy; the results have made it possible to set and tune the parameters of a simulation of the SA. The measuring devices were linear voltage differential transducers: they were found to be quite effective and flexible in usage. An auto-regressive model was used to fit the experimental data, implementing the linear relation between the input forces and the resulting motion. The ability of the model to reproduce the experimental behavior was a clear indication of the good data quality, showing that the contaminating noise was under control. The simulation was able to reproduce the qualitative behavior, and the simulation parameters were estimated, with 10% and...


Physical Review D | 2015

All-sky search for long-duration gravitational wave transients with LIGO

B. Abbott; R. Abbott; T. D. Abbott; M. Abernathy; F. Acernese; K. Ackley; C. Adams; T. Adams; P. Addesso; R. Adhikari; V. B. Adya; C. Affeldt; M. Agathos; K. Agatsuma; N. Aggarwal; O. D. Aguiar; A. Ain; P. Ajith; B. Allen; A. Allocca; D. Amariutei; S. Anderson; W. G. Anderson; Koji Arai; M. C. Araya; C. C. Arceneaux; J. S. Areeda; N. Arnaud; K. G. Arun; G. Ashton

We present the results of a search for long-duration gravitational wave transients in two sets of data collected by the LIGO Hanford and LIGO Livingston detectors between November 5, 2005 and September 30, 2007, and July 7, 2009 and October 20, 2010, with a total observational time of 283.0 days and 132.9 days, respectively. The search targets gravitational wave transients of duration 10 - 500 seconds in a frequency band of 40 - 1000 Hz, with minimal assumptions about the signal waveform, polarization, source direction, or time of occurrence. All candidate triggers were consistent with the expected background; as a result we set 90% confidence upper limits on the rate of long-duration gravitational wave transients for different types of gravitational wave signals. We also report upper limits on the source rate density per year per Mpc^3 for specific signal models. These are the first results from an all-sky search for unmodeled long-duration transient gravitational waves.


Classical and Quantum Gravity | 2002

Status of the low frequency facility experiment

L. Bracci; G. Calamai; Elena Cuoco; P Dominici; L. Fabbroni; G. M. Guidi; G. Losurdo; F Martelli; M. Mazzoni; R. Stanga; Flavio Vetrano; A Porzio; I. Ricciardi; S. Solimeno; G. Ballardin; S. Braccini; C. Bradaschia; C. Casciano; R. Cavalieri; R. Cecchi; G. Cella; V. Dattilo; A. Di Virgilio; M Fazzi; I. Ferrante; F. Fidecaro; F. Frasconi; G. Gennaro; A. Giazotto; L. Holloway

The low frequency facility is a VIRGO R&D experiment having the goal of performing a direct measurement of the thermal noise of the VIRGO suspensions by means of a two-mirror Fabry–Perot cavity suspended to the last stage of the attenuating chain. The present status of advancement of this experiment is reported: the apparatus, including mechanical and optical parts, has been completely built and put into operation. Vacuum facilities and the first control loops are active. First measurements on the suspended cavity are in progress.


Classical and Quantum Gravity | 2004

First results of the low frequency facility experiment

A. Di Virgilio; S. Braccini; G. Ballardin; C. Bradaschia; G. Cella; E. Cuoco; V. Dattilo; M Fazzi; I. Ferrante; F. Fidecaro; F. Frasconi; A. Giazotto; A. Gennai; L. Holloway; H A Mei; Wei-Tou Ni; P. La Penna; T. Lomtadze; G. Losurdo; R. Passaquieti; D. Passuello; R. Poggiani; A Porzio; P. Puppo; F. Raffaelli; P. Rapagnani; F. Ricci; I. Ricciardi; S. Solimeno; R. Stanga

The first low frequency facility (LFF) data are presented; the main purpose of the LFF is to study the pendulum thermal noise around 10 Hz. The displacement noise floor is at the level of 10−13 m Hz−1x/2 at 10 Hz, and at about 11 Hz enters the 10−14 m Hz−1/2 sensitivity region; this level is compatible with the electronic noise of the drivers of the actuators used to lock the apparatus. The calibration method and the seismic noise contribution are discussed.


Physics Letters A | 2003

The low frequency facility Fabry-Perot cavity used as a speed-meter

A. Di Virgilio; S. Braccini; G. Ballardin; C. Bradaschia; G. Cella; E. Cuoco; V. Dattilo; M Fazzi; I. Ferrante; F. Fidecaro; F. Frasconi; A. Giazotto; A. Gennai; L. Holloway; P. La Penna; T. Lomtadze; G. Losurdo; R. Passaquieti; D. Passuello; R. Poggiani; A Porzio; P. Puppo; F. Raffaelli; P. Rapagnani; F. Ricci; I. Ricciardi; S. Solimeno; R. Stanga; Flavio Vetrano; Z Zhou

Fabry–Perot cavities have many different applications as scientific instruments. In the gravitational waves research field they are extensively used to frequency stabilize lasers and to measure very small distance variations. In the present Letter a method to evaluate from the transmitted power only the relative speed and position of the mirrors of a cavity, having finesse F > 40, is described. A displacement spectral sensitivity of the order of about 3 × 10 −10 m/Hz −1/2 at 10 Hz is obtained with the cavity of the low frequency facility.  2003 Elsevier B.V. All rights reserved.


Physics Letters A | 2003

Status report of the low frequency facility experiment, Virgo R&D

A. Di Virgilio; G. Ballardin; S. Braccini; C. Bradaschia; G. Calamai; C. Casciano; R. Cavalieri; R. Cecchi; G. Cella; Sheng-Jui Chen; Elena Cuoco; V. Dattilo; P. Dominici; L. Fabbroni; M Fazzi; S. Frasca; I. Ferrante; F. Fidecaro; F. Frasconi; G. Gennaro; A. Giazotto; G. M. Guidi; L. Holloway; P. La Penna; T. Lomtadze; G. Losurdo; E. Majorana; F. Martelli; M. Mazzoni; F. Nenci

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A. Di Virgilio

Istituto Nazionale di Fisica Nucleare

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C. Bradaschia

Scuola Normale Superiore di Pisa

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F. Fidecaro

Istituto Nazionale di Fisica Nucleare

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F. Frasconi

Istituto Nazionale di Fisica Nucleare

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G. Losurdo

Istituto Nazionale di Fisica Nucleare

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S. Braccini

Istituto Nazionale di Fisica Nucleare

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G. Cella

Istituto Nazionale di Fisica Nucleare

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V. Dattilo

Istituto Nazionale di Fisica Nucleare

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