The focal plane assembly for the ATHENA x-ray integral field unit instrument (Conference Presentation)

Author(s):  
Brian D. Jackson ◽  
Roland H. den Hartog ◽  
Jan van der Kuur ◽  
Henk J. van Weers ◽  
Hiroki Akamatsu ◽  
...  
Keyword(s):  
X Ray ◽  
2016 ◽  
Author(s):  
B. D. Jackson ◽  
H. van Weers ◽  
J. van der Kuur ◽  
R. den Hartog ◽  
H. Akamatsu ◽  
...  
Keyword(s):  
X Ray ◽  

2019 ◽  
Vol 628 ◽  
pp. A5 ◽  
Author(s):  
Didier Barret ◽  
Massimo Cappi

Context. Active galactic nuclei (AGNs) display complex X-ray spectra that exhibit a variety of emission and absorption features. These are commonly interpreted as a combination of (i) a relativistically smeared reflection component, resulting from the irradiation of an accretion disk by a compact hard X-ray source; (ii) one or several warm or ionized absorption components produced by AGN-driven outflows crossing our line of sight; and (iii) a nonrelativistic reflection component produced by more distant material. Disentangling these components via detailed model fitting could be used to constrain the black hole spin, geometry, and characteristics of the accretion flow, as well as of the outflows and surroundings of the black hole. Aims. We investigate how a high-throughput high-resolution X-ray spectrometer such as the Athena X-ray Integral Field Unit (X-IFU) can be used to this aim, using the state-of-the-art reflection model relxill in a lamp-post geometrical configuration. Methods. We simulated a representative sample of AGN spectra, including all necessary model complexities, as well as a range of model parameters going from standard to more extreme values, and considered X-ray fluxes that are representative of known AGN and quasar populations. We also present a method to estimate the systematic errors related to the uncertainties in the calibration of the X-IFU. Results. In a conservative setting, in which the reflection component is computed self consistently by the relxill model from the pre-set geometry and no iron overabundance, the mean errors on the spin and height of the irradiating source are < 0.05 and ∼0.2 Rg (in units of gravitational radius). Similarly, the absorber parameters (column density, ionization parameter, covering factor, and velocity) are measured to an accuracy typically less than ∼5% over their allowed range of variations. Extending the simulations to include blueshifted ultra-fast outflows, we show that X-IFU could measure their velocity with statistical errors < 1%, even for high-redshift objects (e.g., at redshifts ∼2.5). Conclusion. The simulations presented here demonstrate the potential of the X-IFU to understand how black holes are powered and how they shape their host galaxies. The accuracy in recovering the physical model parameters encoded in their X-ray emission is reached thanks to the unique capability of X-IFU to separate and constrain narrow and broad emission and absorption components.


2017 ◽  
Vol 13 (S334) ◽  
pp. 242-247
Author(s):  
Luca Pasquini ◽  
B. Delabre ◽  
R. S. Ellis ◽  
J. Marrero ◽  
L. Cavaller ◽  
...  

AbstractWe present the concept of a novel facility dedicated to massively-multiplexed spectroscopy. The telescope has a very wide field Cassegrain focus optimised for fibre feeding. With a Field of View (FoV) of 2.5 degrees diameter and a 11.4m pupil, it will be the largest etendue telescope. The large focal plane can easily host up to 16.000 fibres. In addition, a gravity invariant focus for the central 10 arc-minutes is available to host a giant integral field unit (IFU). The 3 lenses corrector includes an ADC, and has good performance in the 360-1300 nm wavelength range. The top level science requirements were developed by a dedicated ESO working group, and one of the primary cases is high resolution spectroscopy of GAIA stars and, in general, how our Galaxy formed and evolves. The facility will therefore be equipped with both, high and low resolution spectrographs. We stress the importance of developing the telescope and instrument designs simultaneously. The most relevant R&amp;D aspect is also briefly discussed.


2014 ◽  
Author(s):  
L. Gottardi ◽  
H. Akamatsu ◽  
D. Barret ◽  
M. P. Bruijn ◽  
R. H. den Hartog ◽  
...  
Keyword(s):  
X Ray ◽  

2016 ◽  
Author(s):  
S. J. Smith ◽  
J. S. Adams ◽  
S. R. Bandler ◽  
G. L. Betancourt-Martinez ◽  
J. A. Chervenak ◽  
...  

Author(s):  
Edoardo Cucchetti ◽  
Etienne Pointecouteau ◽  
Didier Barret ◽  
Simone Lotti ◽  
Claudio Macculi ◽  
...  

2016 ◽  
Vol 2 (4) ◽  
pp. 046002 ◽  
Author(s):  
Damien Prêle ◽  
Fabrice Voisin ◽  
Cyril Beillimaz ◽  
Si Chen ◽  
Andrea Goldwurm

Author(s):  
Edoardo Cucchetti ◽  
Philippe Peille ◽  
Nicolas Clerc ◽  
Elena Rasia ◽  
Veronica Biffi ◽  
...  

Author(s):  
Philippe Peille ◽  
Didier Barret ◽  
Vincent Albouys ◽  
Jan-Willem A. den Herder ◽  
Luigi Piro ◽  
...  
Keyword(s):  
X Ray ◽  

2020 ◽  
Vol 200 (5-6) ◽  
pp. 277-285 ◽  
Author(s):  
M. Lorenz ◽  
C. Kirsch ◽  
P. E. Merino-Alonso ◽  
P. Peille ◽  
T. Dauser ◽  
...  

Abstract We present numerical simulations of full transition-edge sensor (TES) arrays utilizing graphical processing units (GPUs). With the support of GPUs, it is possible to perform simulations of large pixel arrays to assist detector development. Comparisons with TES small-signal and noise theory confirm the representativity of the simulated data. In order to demonstrate the capabilities of this approach, we present its implementation in , a simulator for the X-ray Integral Field Unit, a cryogenic X-ray spectrometer on board the future Athena X-ray observatory.


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