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Euclid: High-precision imaging astrometry and photometry from Early Release
Observations. I. Internal kinematics of NGC 6397 by combining Euclid and Gaia
data
    M. Libralato, L. R. Bedin, M. Griggio, D. Massari, J. Anderson,
    J.-C. Cuillandre, A. M. N. Ferguson, A. Lançon, S. S. Larsen, M. Schirmer,
    F. Annibali, E. Balbinot, E. Dalessandro, D. Erkal, P. B. Kuzma,
    T. Saifollahi, G. Verdoes Kleijn, M. Kümmel, R. Nakajima, M. Correnti,
    G. Battaglia, B. Altieri, A. Amara, S. Andreon, C. Baccigalupi, M. Baldi,
    A. Balestra, S. Bardelli, A. Basset, P. Battaglia, D. Bonino, E. Branchini,
    M. Brescia, J. Brinchmann, A. Caillat, S. Camera, V. Capobianco, C. Carbone,
    J. Carretero, S. Casas, M. Castellano, G. Castignani, S. Cavuoti,
    A. Cimatti, C. Colodro-Conde, G. Congedo, C. J. Conselice, L. Conversi,
    Y. Copin, F. Courbin, H. M. Courtois, M. Cropper, A. Da Silva,
    H. Degaudenzi, G. De Lucia, J. Dinis, F. Dubath, X. Dupac, S. Dusini,
    M. Fabricius, M. Farina, S. Farrens, F. Faustini, S. Ferriol, P. Fosalba,
    M. Frailis, E. Franceschi, M. Fumana, S. Galeotta, B. Garilli, K. George,
    W. Gillard, B. Gillis, C. Giocoli, P. Gómez-Alvarez, A. Grazian, F. Grupp,
    L. Guzzo, S. V. H. Haugan, J. Hoar, H. Hoekstra, W. Holmes, F. Hormuth,
    A. Construes, P. Hudelot, K. Jahnke, M. Jhabvala, E. Keihänen, S. Kermiche,
    A. Kiessling, M. Kilbinger, B. Kubik, M. Kunz, H. Kurki-Suonio, R. Laureijs,
    D. Le Mignant, S. Ligori, P. B. Lilje, V. Lindholm, I. Lloro, E. Maiorano,
    O. Mansutti, O. Marggraf, K. Markovic, M. Martinelli, N. Martinet,
    F. Marulli, R. Massey, E. Medinaceli, S. Mei,M. Melchior, Y. Mellier,
    M. Meneghetti, E. Merlin, G. Meylan, M. Moresco, L. Moscardini, C. Neissner,
    R. C. Nichol, S.-M. Niemi, J. W. Nightingale, C. Padilla, S. Paltani,
    F. Pasian, K. Pedersen, W. J. Percival, V. Pettorino, S. Pires, G. Polenta,
    M. Poncet, L. A. Popa, L. Pozzetti, F. Raison, R. Rebolo, A. Refregier,
    A. Renzi,J. Rhodes, G. Riccio, E. Romelli, M. Roncarelli, E. Rossetti,
    R. Saglia, Z. Sakr, A. G. Sánchez, D. Sapone, B. Sartoris, M. Sauvage,
    P. Schneider, T. Schrabback, A. Secroun, E. Sefusatti, G. Seidel,
    M. Seiffert, S. Serrano, C. Sirignano, G. Sirri, J. Skottfelt, L. Stanco,
    J. Steinwagner, P. Tallada-Crespí, A. N. Taylor, H. I. Teplitz, I. Tereno,
    R. Toledo-Moreo, F. Torradeflot, A. Tsyganov, I. Tutusaus, L. Valenziano,
    T. Vassallo, A. Veropalumbo, Y. Wang, J. Weller, G. Zamorani, E. Zucca,
    C. Burigana, V. Scottez,,D. Scott,and R. L. Smart,
    =References ?
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Keywords: astrometry – photometry – proper motions – stellar clusters –
	  globular clusters: individual: NGC 6397

Abstract:
  The instruments at the focus of the Euclid space observatory offer
  superb, diffraction-limited imaging over an unprecedented (from
  space) wide field of view of 0.57 sq. deg. This exquisite image
  quality has the potential to produce high-precision astrometry for
  point sources once the undersampling of the Euclid's cameras is
  taken into account by means of accurate effective point spread
  function (ePSF) modelling. We present a complex, detailed workflow
  to simultaneously solve for the geometric distortion (GD) and model
  the undersampled ePSFs of the Euclid detectors.  Our procedure was
  successfully developed and tested with data from the Early Release
  Observations (ERO) programme focused on the nearby globular cluster
  NGC 6397. Our final one-dimensional astrometric precision for a
  well-measured star just below saturation is 0.7 mas (0.007 pixel)
  for the Visible Instrument (VIS) and 3 mas (0.01 pixel) for the
  Near-Infrared Spectrometer and Photometer (NISP). Finally, we
  present a specific scientific application of this high-precision
  astrometry: the combination of Euclid and Gaia data to compute
  proper motions and study the internal kinematics of NGC 6397. Future
  work, when more data become available, will allow for a better
  characterisation of the ePSFs and GD corrections that are derived
  here, along with assessing their temporal stability, and their
  dependencies on the spectral energy distribution of the sources as
  seen through the wide-band filters of Euclid.

Description:
  Astro-photometric catalogs and stacked images of NGC 6397. The astrometrized
  stacked images do not currently take into account for tangent-plane-projection
  effects. Also, fluxes are not properly resampled. Thus, these images are meant
  for visual reference only and not for scientific investigations.

File Summary:
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 FileName    Lrecl   Records    Explanations
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ReadMe          80        .  this file
ngc6397.dat    358   474706  NGC 6397 astro-photometric catalog
fits/*           .        4  Individual fits images

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Byte-by-byte Description of file: ngc6397.dat
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  Bytes   Format Units  Label    Explanations
--------------------------------------------------------------------------------
  1- 14   F14.10 ---    ra       Right Ascension (ICRS) at Ep=2023
 16- 29   F14.10 ---    dec      Declination (ICRS) at Ep=2023
 31- 36   I6     ---    idvis    ID number of the source
 38- 47   F10.4  ---    xvis     VIS X master-frame position (100mas/pixel)
 49- 58   F10.4  ---    yvis     VIS Y master-frame position (100mas/pixel)
 60- 66   F7.4   ---    mvis     Calibrated VIS I_E magnitude (1)
 68- 73   F6.4   ---    sxvis    VIS X position rms (5)
 75- 80   F6.4   ---    syvis    VIS Y position rms (5)
 82- 87   F6.4   ---    smvis    VIS I_E magnitude rms (5)
 89- 94   F6.4   ---    qvis     VIS I_E quality-of-PSF-fit parameter (5)
 96- 96   I1     ---    nfvis    Number of individual VIS I_E exposures in
                                 which an object was found (5)
 98- 98   I1     ---    nuvis    Number of individual VIS I_E exposures
                                 used to measure an object (5)
100-109   F10.4  ---    xnispy   NISP Y_E X master-frame position (300mas/pixel)
                                 (6)
111-120   F10.4  ---    ynispy   NISP Y_E Y master-frame position (300mas/pixel)
                                 (6)
122-128   F7.4   ---    mnispy   Calibrated NISP Y_E magnitude (2) (6)
130-135   F6.4   ---    sxnispy  NISP Y_E X position rms (5) (6)
137-142   F6.4   ---    synispy  NISP Y_E Y position rms (5) (6)
144-149   F6.4   ---    smnispy  NISP Y_E magnitude rms (5) (6)
151-156   F6.4   ---    qnispy   NISP Y_E quality-of-PSF-fit parameter (5) (6)
158-158   I1     ---    nfnispy  Number of individual NISP Y_E exposures in
                                 which an object was found (5) (6)
160-160   I1     ---    nunispy  Number of individual NISP Y_E exposures
                                 used to measure an object (5) (6)
162-171   F10.4  ---    xnispj   NISP J_E X master-frame position (300mas/pixel)
                                 (6)
173-182   F10.4  ---    ynispj   NISP J_E X master-frame position (300mas/pixel)
                                 (6)
184-190   F7.4   ---    mnispj   Calibrated NISP J_E magnitude (3) (6)
192-197   F6.4   ---    sxnispj  NISP J_E X position rms (5) (6)
199-204   F6.4   ---    synispj  NISP J_E Y position rms (5) (6)
206-211   F6.4   ---    smnispj  NISP J_E magnitude rms (5) (6)
213-218   F6.4   ---    qnispj   NISP J_E quality-of-PSF-fit parameter (5) (6)
220-220   I1     ---    nfnispj  Number of individual NISP J_E exposures in
                                 which an object was found (5) (6)
222-222   I1     ---    nunispj  Number of individual NISP J_E exposures
                                 used to measure an object (5) (6)
224-233   F10.4  ---    xnisph   NISP H_E X master-frame position (300mas/pixel)
                                 (6)
235-244   F10.4  ---    ynisph   NISP H_E X master-frame position (300mas/pixel)
                                 (6)
246-252   F7.4   ---    mnisph   Calibrated NISP H_E magnitude (4) (6)
254-259   F6.4   ---    sxnisph  NISP H_E X position rms (5) (6)
261-266   F6.4   ---    synisph  NISP H_E Y position rms (5) (6)
268-273   F6.4   ---    smnisph  NISP H_E magnitude rms (5) (6)
275-280   F6.4   ---    qnisph   NISP H_E quality-of-PSF-fit parameter (5) (6)
282-282   I1     ---    nfnisph  Number of individual NISP H_E exposures in
                                 which an object was found (5) (6)
284-284   I1     ---    nunisph  Number of individual NISP H_E exposures
                                 used to measure an object (5) (6)
286-294   F9.5   ---    pmra     Proper motion along R.A. cos(Dec.) (mas/yr) (7)
296-304   F9.5   ---    pmdec    Proper motion along Dec. (mas/yr) (7)
306-313   F8.5   ---    epmra    Error on the proper motion along R.A. cos(Dec.)
                                 (mas/yr) (7)
315-321   F7.5   ---    epmdec   Error on the proper motion along Dec. (mas/yr)
                                 (7)
323-331   F9.5   ---    pmrac    Proper motion along R.A. cos(Dec.) corrected for
                                 the color-dependent systematic (mas/yr) (7)
333-341   F9.5   ---    pmdecc   Proper motion along Dec. corrected for the 
                                 color-dependent systematic (mas/yr) (7)
343-350   F8.5   ---    epmrac   Error on the proper motion along R.A. cos(Dec.)
                                 corrected for the color-dependent systematic
				 (mas/yr) (7)
352-358   F7.5   ---    epmdecc  Error on the proper motion along Dec. corrected
                                 for the color-dependent systematic (mas/yr) (7)
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Note (1): Stars saturated in the VIS I_E catalog have a magnitude <= ~18.8.
Note (2): Stars saturated in the NISP Y_E catalog have a magnitude <= ~16.2.
Note (3): Stars saturated in the NISP J_E catalog have a magnitude <= ~16.5.
Note (4): Stars saturated in the NISP H_E catalog have a magnitude <= ~16.5.
Note (5): Saturated stars have positional rms, magnitude rms,
          quality-of-PSF-fit and/or proper motions that can be set to a value
	  greater or equal to 0. We advise extreme caution when dealing with
	  saturated stars.
Note (6): Stars not measured in a NISP filter have all the corresponding
          parameters set to 0.
Note (7): Stars without a proper-motion measurement have proper motions and
          corresponding errors set to 0.
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Acknowledgements:
    Mattia Libralato, mattia.libralato(at)inaf.it

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