Simone Lotti

Dr. Simone Lotti

orcid

Research Focus & Metrics

Academic Career Length

17Years (2010-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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13 April 2018 in Monthly Notices of the Royal Astronomical Society: Letters
Verified
Journal Article
Open access
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ETE Troja
E Troja
LPL Piro
L Piro
GRG Ryan
G Ryan
HEH van Eerten
H van Eerten
RRR Ricci
R Ricci
SCS B Cenko
S B Cenko
We present our broad-band study of GW170817 from radio to hard X-rays, including NuSTAR and Chandra observations up to 165 d after the merger, and a multimessenger analysis including LIGO constraints. The data are compared with predictions from a wide range of models, providing the first detailed comparison between non-trivial cocoon and jet models. Homogeneous and power-law shaped jets, as well as simple cocoon models are ruled out by the data, while both a Gaussian shaped jet and a cocoon with energy injection can describe the current data set for a reasonable range of physical parameters, consistent with the typical values derived from short GRB afterglows. We propose that these models can be unambiguously discriminated by future observations measuring the post-peak behaviour, with Fν ∝ t∼−1.0 for the cocoon and Fν∝ t∼−2.5 for the jet model.

20 November 2019 in Nature
Verified
Journal Article
Closed access
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PVP. Veres
P. Veres
PBP. N. Bhat
P. N. Bhat
MBM. S. Briggs
M. S. Briggs
WCW. H. Cleveland
W. H. Cleveland
RHR. Hamburg
R. Hamburg
JRJavier Rico
Javier Rico

31 July 2018
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Conference Paper
Closed access
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DBDidier Barret
Didier Barret
JHJan-Willem Den Herder
Jan-Willem Den Herder
TTThien Lam Trong
Thien Lam Trong
LPLuigi Piro
Luigi Piro
MCMassimo Cappi
Massimo Cappi
LNLorenzo Natalucci
Lorenzo Natalucci
The X-ray Integral Field Unit (X-IFU) is the high resolution X-ray spectrometer of the ESA Athena X-ray observatory. Over a field of view of 5’ equivalent diameter, it will deliver X-ray spectra from 0.2 to 12 keV with a spectral resolution of 2.5 eV up to 7 keV on ∼ 5” pixels. The X-IFU is based on a large format array of super-conducting molybdenum-gold Transition Edge Sensors cooled at ∼ 90 mK, each coupled with an absorber made of gold and bismuth with a pitch of 249 μm. A cryogenic anti-coincidence detector located underneath the prime TES array enables the non X-ray background to be reduced. A bath temperature of ∼ 50 mK is obtained by a series of mechanical coolers combining 15K Pulse Tubes, 4K and 2K Joule-Thomson coolers which pre-cool a sub Kelvin cooler made of a 3He sorption cooler coupled with an Adiabatic Demagnetization Refrigerator. Frequency domain multiplexing enables to read out 40 pixels in one single channel. A photon interacting with an absorber leads to a current pulse, amplified by the readout electronics and whose shape is reconstructed on board to recover its energy with high accuracy. The defocusing capability offered by the Athena movable mirror assembly enables the X-IFU to observe the brightest X-ray sources of the sky (up to Crab-like intensities) by spreading the telescope point spread function over hundreds of pixels. Thus the X-IFU delivers low pile-up, high throughput (< 50%), and typically 10 eV spectral resolution at 1 Crab intensities, i.e. a factor of 10 or more better than Silicon based X-ray detectors. In this paper, the current X-IFU baseline is presented, together with an assessment of its anticipated performance in terms of spectral resolution, background, and count rate capability. The X-IFU baseline configuration will be subject to a preliminary requirement review that is scheduled at the end of 2018.

11 January 2019
Verified
Journal Article
Closed access
KNKirpal Nandra
Kirpal Nandra
DBDidier Barret
Didier Barret
XBXavier Barcons
Xavier Barcons
AFAndy Fabian
Andy Fabian
JHJan-Willem Den Herder
Jan-Willem Den Herder
IZIrina Zhuravleva
Irina Zhuravleva

17 August 2016
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Conference Paper
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DBDidier Barret
Didier Barret
TTThien Lam Trong
Thien Lam Trong
JHJan-Willem Den Herder
Jan-Willem Den Herder
LPLuigi Piro
Luigi Piro
XBXavier Barcons
Xavier Barcons
ECEdoardo Cucchetti
Edoardo Cucchetti
The X-ray Integral Field Unit (X-IFU) on board the Advanced Telescope for High-ENergy Astrophysics (Athena) will provide spatially resolved high-resolution X-ray spectroscopy from 0.2 to 12 keV, with ~ 5" pixels over a field of view of 5 arc minute equivalent diameter and a spectral resolution of 2.5 eV up to 7 keV. In this paper, we first review the core scientific objectives of Athena, driving the main performance parameters of the X-IFU, namely the spectral resolution, the field of view, the effective area, the count rate capabilities, the instrumental background. We also illustrate the breakthrough potential of the X-IFU for some observatory science goals. Then we brie y describe the X-IFU design as defined at the time of the mission consolidation review concluded in May 2016, and report on its predicted performance. Finally, we discuss some options to improve the instrument performance while not increasing its complexity and resource demands (e.g. count rate capability, spectral resolution).

24 July 2014
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Conference Paper
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LRL. Ravera
L. Ravera
DBD. Barret
D. Barret
JHJ. Den Herder
J. Den Herder
LPL. Piro
L. Piro
RCR. Clédassou
R. Clédassou
CSC. Schmid
C. Schmid
Athena is designed to implement the Hot and Energetic Universe science theme selected by the European Space Agency for the second large mission of its Cosmic Vision program. The Athena science payload consists of a large aperture high angular resolution X-ray optics (2 m2 at 1 keV) and twelve meters away, two interchangeable focal plane instruments: the X-ray Integral Field Unit (X-IFU) and the Wide Field Imager. The X-IFU is a cryogenic X-ray spectrometer, based on a large array of Transition Edge Sensors (TES), offering 2:5 eV spectral resolution, with ~5" pixels, over a field of view of 50 in diameter. In this paper, we present the X-IFU detector and readout electronics principles, some elements of the current design for the focal plane assembly and the cooling chain. We describe the current performance estimates, in terms of spectral resolution, effective area, particle background rejection and count rate capability. Finally, we emphasize on the technology developments necessary to meet the demanding requirements of the X-IFU, both for the sensor, readout electronics and cooling chain