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Publications

Publications by Paulo Jorge Garcia

2017

Accretion-ejection morphology of the microquasar SS 433 resolved at sub-au scale

Authors
Petrucci, PO; Waisberg, I; Le Bouquin, JB; Dexter, J; Dubus, G; Perraut, K; Kervella, P; Abuter, R; Amorim, A; Anugu, N; Berger, JP; Blind, N; Bonnet, H; Brandner, W; Buron, A; Choquet, E; Clenet, Y; de Wit, W; Deen, C; Eckart, A; Eisenhauer, F; Finger, G; Garcia, P; Lopez, RG; Gendron, E; Genzel, R; Gillessen, S; Gonte, F; Haubois, X; Haug, M; Haussmann, F; Henning, T; Hippler, S; Horrobin, M; Hubert, Z; Jochum, L; Jocou, L; Kok, Y; Kolb, J; Kulas, M; Lacour, S; Lazareff, B; Lena, P; Lippa, M; Merand, A; Mueller, E; Ott, T; Panduro, J; Paumard, T; Perrin, G; Pfuhl, O; Ramos, J; Rau, C; Rohlo, RR; Rousset, G; Sanchez Bermudez, J; Scheithauer, S; Schoeller, M; Straubmeier, C; Sturm, E; Vincent, F; Wank, I; Wieprecht, E; Wiest, M; Wiezorrek, E; Wittkowski, M; Woillez, J; Yazici, S; Zins, G;

Publication
ASTRONOMY & ASTROPHYSICS

Abstract
We present the first optical observation of the microquasar SS 433 at sub-milliarcsecond (mas) scale obtained with the GRAVITY instrument on the Very Large Telescope interferometer (VLTI). The 3.5-h exposure reveals a rich K-band spectrum dominated by hydrogen Br gamma and He i lines, as well as (red-shifted) emission lines coming from the jets. The K-band-continuum-emitting region is dominated by a marginally resolved point source (<1 mas) embedded inside a diffuse background accounting for 10% of the total flux. The jet line positions agree well with the ones expected from the jet kinematic model, an interpretation also supported by the consistent sign (i.e., negative/positive for the receding/approaching jet component) of the phase shifts observed in the lines. The significant visibility drop across the jet lines, together with the small and nearly identical phases for all baselines, point toward a jet that is off set by less than 0.5 mas from the continuum source and resolved in the direction of propagation, with a typical size of 2 mas. The jet position angle of similar to 80 degrees is consistent with the expected one at the observation date. Jet emission so close to the central binary system would suggest that line locking, if relevant to explain the amplitude and stability of the 0.26c jet velocity, operates on elements heavier than hydrogen. The Br gamma profile is broad and double peaked. It is better resolved than the continuum and the change of the phase signal sign across the line on all baselines suggests an East-West-oriented geometry similar to the jet direction and supporting a (polar) disk wind origin.

2018

Multiple star systems in the Orion nebula

Authors
Karl, M; Pfuhl, O; Eisenhauer, F; Genzel, R; Grellmann, R; Habibi, M; Abuter, R; Accardo, M; Amorim, A; Anugu, N; Avila, G; Benisty, M; Berger, JP; Blind, N; Bonnet, H; Bourget, P; Brandner, W; Brast, R; Buron, A; Garatti, ACO; Chapron, F; Clenet, Y; Collin, C; du Foresto, VC; de Wit, WJ; de Zeeuw, T; Deen, C; Delplancke Stroebele, F; Dembet, R; Derie, F; Dexter, J; Duvert, G; Ebert, M; Eckart, A; Esselborn, M; Fedou, P; Finger, G; Garcia, P; Dabo, CEG; Lopez, RG; Gao, F; Gendron, E; Gillessen, S; Gonte, F; Gordo, P; Groezinger, U; Guajardo, P; Guieu, S; Haguenauer, P; Hans, O; Haubois, X; Haug, M; Haussmann, F; Henning, T; Hippler, S; Horrobin, M; Huber, A; Hubert, Z; Hubin, N; Jakob, G; Jochum, L; Jocou, L; Kaufer, A; Kellner, S; Kendrew, S; Kern, L; Kervella, P; Kiekebusch, M; Klein, R; Koehler, R; Kolb, J; Kulas, M; Lacour, S; Lapeyrere, V; Lazareff, B; Le Bouquin, JB; Lena, P; Lenzen, R; Leveque, S; Lin, CC; Lippa, M; Magnard, Y; Mehrgan, L; Merand, A; Moulin, T; Mueller, E; Mueller, F; Neumann, U; Oberti, S; Ott, T; Pallanca, L; Panduro, J; Pasquini, L; Paumard, T; Percheron, I; Perraut, K; Perrin, G; Pflueger, A; Duc, TP; Plewa, PM; Popovic, D; Rabien, S; Ramirez, A; Ramos, J; Rau, C; Riquelme, M; Rodriguez Coira, G; Rohloff, RR; Rosales, A; Rousset, G; Sanchez Bermudez, J; Scheithauer, S; Schoeller, M; Schuhler, N; Spyromilio, J; Straub, O; Straubmeier, C; Sturm, E; Suarez, M; Tristram, KRW; Ventura, N; Vincent, F; Waisberg, I; Wank, I; Widmann, F; Wieprecht, E; Wiest, M; Wiezorrek, E; Wittkowski, M; Woillez, J; Wolff, B; Yazici, S; Ziegler, D; Zins, G;

Publication
ASTRONOMY & ASTROPHYSICS

Abstract
This work presents an interferometric study of the massive-binary fraction in the Orion Trapezium cluster with the recently comissioned GRAVITY instrument. We observed a total of 16 stars of mainly OB spectral type. We find three previously unknown companions for theta(1) Ori B, theta(2) Ori B, and theta(2) Ori C. We determined a separation for the previously suspected companion of NU Ori. We confirm four companions for theta(1) Ori A, theta(1) Ori C, theta(1) Ori D, and theta(2) Ori A, all with substantially improved astrometry and photometric mass estimates. We refined the orbit of the eccentric high-mass binary theta(1) Ori C and we are able to derive a new orbit for theta(1) Ori D. We find a system mass of 21.7 M-circle dot and a period of 53 days. Together with other previously detected companions seen in spectroscopy or direct imaging, eleven of the 16 high-mass stars are multiple systems. We obtain a total number of 22 companions with separations up to 600 AU. The companion fraction of the early B and O stars in our sample is about two, significantly higher than in earlier studies of mostly OB associations. The separation distribution hints toward a bimodality. Such a bimodality has been previously found in A stars, but rarely in OB binaries, which up to this point have been assumed to be mostly compact with a tail of wider companions. We also do not find a substantial population of equal-mass binaries. The observed distribution of mass ratios declines steeply with mass, and like the direct star counts, indicates that our companions follow a standard power law initial mass function. Again, this is in contrast to earlier findings of flat mass ratio distributions in OB associations. We excluded collision as a dominant formation mechanism but find no clear preference for core accretion or competitive accretion.

2018

Detection of orbital motions near the last stable circular orbit of the massive black hole SgrA*

Authors
Abuter, R; Amorim, A; Bauboeck, M; Berger, JP; Bonnet, H; Brandner, W; Clenet, Y; du Foresto, VC; de Zeeuw, PT; Deen, C; Dexter, J; Duvert, G; Eckart, A; Eisenhauer, F; Schreiber, NMF; Garcia, P; Gao, F; Gendron, E; Genzel, R; Gillessen, S; Guajardo, P; Habibi, M; Haubois, X; Henning, T; Hippler, S; Horrobin, M; Huber, A; Jimenez Rosales, A; Jocou, L; Kervella, P; Lacour, S; Lapeyrere, V; Lazareff, B; Le Bouquin, JB; Lena, P; Lippa, M; Ott, T; Panduro, J; Paumard, T; Perraut, K; Perrin, G; Pfuhl, O; Plewa, PM; Rabien, S; Rodriguez Coira, G; Rousset, G; Sternberg, A; Straub, O; Straubmeier, C; Sturm, E; Tacconi, LJ; Vincent, F; von Fellenberg, S; Waisberg, I; Widmann, F; Wieprecht, E; Wiezorrek, E; Woillez, J; Yazici, S;

Publication
ASTRONOMY & ASTROPHYSICS

Abstract
We report the detection of continuous positional and polarization changes of the compact source SgrA* in high states ("flares") of its variable near-infrared emission with the near-infrared GRAVITY-Very Large Telescope Interferometer (VLTI) beam-combining instrument. In three prominent bright flares, the position centroids exhibit clockwise looped motion on the sky, on scales of typically 150 mu as over a few tens of minutes, corresponding to about 30% the speed of light. At the same time, the flares exhibit continuous rotation of the polarization angle, with about the same 45(+/- 15) min period as that of the centroid motions. Modelling with relativistic ray tracing shows that these findings are all consistent with a near face-on, circular orbit of a compact polarized "hot spot" of infrared synchrotron emission at approximately six to ten times the gravitational radius of a black hole of 4 million solar masses. This corresponds to the region just outside the innermost, stable, prograde circular orbit (ISCO) of a Schwarzschild-Kerr black hole, or near the retrograde ISCO of a highly spun-up Kerr hole. The polarization signature is consistent with orbital motion in a strong poloidal magnetic field.

2019

A geometric distance measurement to the Galactic center black hole with 0.3% uncertainty

Authors
Abuter, R; Amorim, A; Bauboeeck, M; Berger, JP; Bonnet, H; Brandner, W; Clenet, Y; du Foresto, VC; de Zeeuw, PT; Dexter, J; Duvert, G; Eckart, A; Eisenhauer, F; Schreiber, NMF; Garcia, P; Gao, F; Gendron, E; Genzel, R; Gerhard, O; Gillessen, S; Habibi, M; Haubois, X; Henning, T; Hippler, S; Horrobin, M; Jimenez Rosales, A; Jocou, L; Kervella, P; Lacour, S; Lapeyrere, V; Le Bouquin, JB; Lena, P; Ott, T; Paumard, T; Perraut, K; Perrin, G; Pfuhl, O; Rabien, S; Coira, GR; Rousset, G; Scheithauer, S; Sternberg, A; Straub, O; Straubmeier, C; Sturm, E; Tacconi, LJ; Vincent, F; von Fellenberg, S; Waisberg, I; Widmann, F; Wieprecht, E; Wiezorrek, E; Woillez, J; Yazici, S;

Publication
ASTRONOMY & ASTROPHYSICS

Abstract
We present a 0.16% precise and 0.27% accurate determination of R-0, the distance to the Galactic center. Our measurement uses the star S2 on its 16-year orbit around the massive black hole Sgr A* that we followed astrometrically and spectroscopically for 27 years. Since 2017, we added near-infrared interferometry with the VLTI beam combiner GRAVITY, yielding a direct measurement of the separation vector between S2 and Sgr A* with an accuracy as good as 20 mu as in the best cases. S2 passed the pericenter of its highly eccentric orbit in May 2018, and we followed the passage with dense sampling throughout the year. Together with our spectroscopy, in the best cases with an error of 7 km s(-1), this yields a geometric distance estimate of R-0 = 8178 +/- 13(stat.) +/- 22(sys.) pc. This work updates our previous publication, in which we reported the first detection of the gravitational redshift in the S2 data. The redshift term is now detected with a significance level of 20 sigma with f(redshift) = 1.04 +/- 0.05.

2018

Status of the Mid-IR ELT Imager and Spectrograph (METIS)

Authors
Brandl, BR; Absil, O; Agocs, T; Baccichet, N; Bertram, T; Bettonvil, F; van Boekel, R; Burtscher, L; van Dishoeck, E; Feldt, M; Garcia, PJV; Glasse, A; Glauser, A; Guedel, M; Haupt, C; Kenworthy, MA; Labadie, L; Laun, W; Lesman, D; Pantin, E; Quanz, SP; Snellen, I; Siebenmorgen, R; van Winckel, H;

Publication
GROUND-BASED AND AIRBORNE INSTRUMENTATION FOR ASTRONOMY VII

Abstract
METIS is one of the first three scientific instruments on the ELT, expected to see first light in 2025. METIS will provide diffraction limited imaging, coronagraphy, and low resolution slit spectroscopy over the 3 - 19 mu m range. Furthermore, METIS will provide a unique combination of high resolution (R similar to 100,000) integral field spectroscopy and coronagraphy from 2.9 - 5.3 mu m. The latter can be reconfigured to obtain a wider instantaneous wavelength coverage in exchange for integral field coverage. While METIS is a multi-purpose instrument for a wide range of infrared astronomy, its greatest strengths will be in the studies of exoplanets and proto-planetary disks. After two years into the preliminary design phase, the design of METIS has reached an advanced stage. This paper provides an update on the areas which have most advanced in the recent past: the main science drivers, the optical and opto-mechanical design, adaptive optics and the coronagraphy concept. We also describe the calibration of the instrument, give an overview of its observation modes, and present the schedule toward first light.

2017

The wind and the magnetospheric accretion onto the T Tauri star S Coronae Australis at sub-au resolution

Authors
Lopez, RG; Perraut, K; Garatti, ACO; Lazareff, B; Sanchez Bermudez, J; Benisty, M; Dougados, C; Labadie, L; Brandner, W; Garcia, PJV; Henning, T; Ray, TP; Abuter, R; Amorim, A; Anugu, N; Berger, JP; Bonnet, H; Buron, A; Caselli, P; Clenet, Y; du Foresto, VC; de Wit, W; Deen, C; Delplancke Stroebele, F; Dexter, J; Eckart, A; Eisenhauer, F; Dabo, CEG; Gendron, E; Genzel, R; Gillessen, S; Haubois, X; Haug, M; Haussmann, F; Hippler, S; Hubert, Z; Hummel, CA; Horrobin, M; Jocou, L; Kellner, S; Kervella, P; Kulas, M; Kolb, J; Lacour, S; Le Bouquin, JB; Lena, P; Lippa, M; Merand, A; Mueller, E; Ott, T; Panduro, J; Paumard, T; Perrin, G; Pfuhl, O; Ramirez, A; Rau, C; Rohloff, RR; Rousset, G; Scheithauer, S; Schoeller, M; Straubmeier, C; Sturm, E; Thi, WF; van Dishoeck, E; Vincent, F; Waisberg, I; Wank, I; Wieprecht, E; Wiest, M; Wiezorrek, E; Woillez, J; Yazici, S; Zins, G;

Publication
ASTRONOMY & ASTROPHYSICS

Abstract
Aims. To investigate the inner regions of protoplanetary discs, we performed near-infrared interferometric observations of the classical T Tauri binary system S CrA. Methods. We present the first VLTI-GRAVITY high spectral resolution (R similar to 4000) observations of a classical T Tauri binary, S CrA (composed of S CrAN and S CrA S and separated by similar to 1".4), combining the four 8m telescopes in dual-field mode. Results. Our observations in the near-infrared K-band continuum reveal a disc around each binary component, with similar halfflux radii of about 0.1 au at d similar to 130 pc, inclinations (i = 28 +/- 3 degrees and i = 22 +/- 6 degrees), and position angles (PA = 0 degrees +/- 6 degrees and PA = -2 degrees +/- 12 degrees), suggesting that they formed from the fragmentation of a common disc. The S CrAN spectrum shows bright He i and Br gamma line emission exhibiting inverse PCygni profiles, typically associated with infalling gas. The continuum-compensated Br gamma line visibilities of S CrAN show the presence of a compact Br gamma emitting region whose radius is about similar to 0.06 au, which is twice as big as the truncation radius. This component is mostly tracing a wind. Moreover, a slight radius change between the blue-and red-shifted Br gamma line components is marginally detected. Conclusions. The presence of an inverse PCygni profile in the He i and Br gamma lines, along with the tentative detection of a slightly larger size of the blue-shifted Br gamma line component, hint at the simultaneous presence of a wind and magnetospheric accretion in S CrA N.

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