Physical characterization of Kuiper belt objects from stellar occultations and thermal measurements
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1 Physical characterization of Kuiper belt objects from stellar occultations and thermal measurements Pablo Santos-Sanz & the SBNAF team
2 Stellar occultations Simple method to: -Obtain high precision sizes/shapes (unc. ~km) -Detect/characterize atmospheres/rings -Obtain albedo, density -Improve the orbit of the body this looks like very nice but...the reality is harder (at least for TNOs and Centaurs)
3 Stellar occultations Titan 10 mas Quaoar Pluto arsec (33 mas) Diameter of 1 Euro coin at 140 km Eris Charon Makemake Pablo Santos-Sanz
4 Stellar occultations ~25 occultations by 15 TNOs (+ Pluto/Charon + Chariklo + Chiron GZ 32 ) Namaka Dysnomia Hi iaka Ixion Pluto Chiron Eris Haumea 2007 UK126 Chariklo Vanth 2014 MU GZ VS KX TV AZ TX 300
5 Stellar occultations: Eris & Chariklo Eris: 6 November 2010 Size ~ Plutón Albedo= 96% Density= 2.5 g/cm 3 Atmosphere < 1nbar (10-4 x Pluto) Eris radius 1163±6 km Pluto s radius ±1.6 km (Nimmo et al. 2016) Chariklo: 3 June 2014 It has rings! Danish 1.54-m telescope (La Silla) Braga-Ribas et al (Nature) Sicardy et al (Nature)
6 Stellar occultations: Makemake 23 April 2011 Geometric Albedo = 77% (betwen Pluto and Eris) Possible local atmosphere! Ortiz et al (Nature)
7 Stellar occultations: latest catches 2007 UK 126 : 15 November AZ 84 : 8 Jan single, 3 Feb multi, 2 Dec single, 15 Nov multi. Benedetti-Rossi et al (7-chords) D eq = km p V = % Maclaurin spheroid (e= ) r < 1.74 g cm 3 (P = h) Schindler et al (3-chords) D eq = km p V = 15.0 ± 1.6% Maclaurin spheroid (a/c ) r 0.73 g cm -3 (P 8 h) Dias-Oliveira et al (multi-chord) D eq = 772 ± 12 km p V = 9.7 ± 0.9% Jacobi ellipsoid (470 x 383 x 245 km) r = 0.87 ± 0.01 g cm -3 (P = 6.75 h) Possible detection of a chasm! Pablo Santos-Sanz
8 Stellar occultations: latest catches 2003 VS 2 : 7 November MU 69 : 17 July 2017 Credit: NASA/JHUAPL/SwRI/Alex Parker Santos-Sanz et al (4-chords) D eq = 562 km Jacobi ellipsoid r= g cm 3 (P = 7.42 h) Preliminary results: Very irregular shape Close or contact binary? 2 "lobes", with D s of ~20 km and ~18 km Pablo Santos-Sanz
9 Stellar occultations from JWST? JWST/NIRCam, cadence ~6.7 Hz, 64x64 subarray, 0.7 to 4.8mm Stellar occultations by KBOs: JWST-GTO time approved!
10 Thermal measurements Thermal emission of TNOs (T= K) have their maxima at mm Thermal emission of few TNOs from ground (Jewitt et al. 2001, Lellouch et al. 2002, Margot et al. 2002, Bertoldi et al. 2006, Gerdes et al. 2017, Brown & Butler 2017, Lellouch et al. 2017) Thermal observations of ~60 TNOs w/ Spitzer/MIPS and μm) Herschel: observed 140 TNOs/Centaurs within the open time key programme TNOs are Cool: a survey of the Transneptunian region Main goal: determine Diameters and Albedos by means of: 3-band photometry w/ Herschel/PACS (@ 70.0, and μm) + Thermal and/or Thermophysical modeling (TPM) 1996 TL 66 Santos-Sanz et al Herschel observations expand / complement Spitzer observations Pablo Santos-Sanz
11 Thermal measurements TNOs are Cool! sizes, albedos, thermal properties and mass densities Typical uncertainties ~10% Diameters and ~ 20% Albedos (Müller et al. 2010, Lellouch et al. 2010, Lim et al. 2010, Santos-Sanz et al. 2012, Mommert et al. 2012, Vilenius et al. 2012, Pal et al. 2012, Fornasier et al. 2013, Lellouch et al. 2013, Vilenius et al. 2014, Duffard et al. 2014, Santos-Sanz et al. 2017) Pablo Santos-Sanz
12 Thermal measurements: mass density Object r (g cm -3 ) Reference (136199) Eris Santos-Sanz et al (50000) Quaoar Fornasier at al (90482) Orcus Fornasier et al (120347) Salacia Fornasier et al (174567) Varda Vilenius et al (47171) 1999 TC Mommert et al (79360) Sila-Nunam 0.73 ± 0.28 Vilenius et al (148780) Altjira Vilenius et al QC Vilenius et al (26308) 1998 SM Stansberry et al. 2008, Spencer et al (65489) Ceto Santos-Sanz et al (275809) 2001 QY Vilenius et al XR Vilenius et al (88611) Teharonhiawako Vilenius et al (66652) Borasisi Vilenius et al (42355) Typhon Stansberry et al (42355) Typhon Santos-Sanz et al Pablo Santos-Sanz
13 Thermal measurements h range <1 to 2.5 surface roughness effects important Lellouch, Santos-Sanz et al G mean = (2.5 ± 0.5) MKS Strong suggestion that T.I. (G) decreases with heliocentric distance (r h ) G s 2-3 orders of magnitude lower than expected for compact ices Pablo Santos-Sanz
14 Thermal measurements h range <1 to 2.5 surface roughness effects important Our results suggests strongly porous surfaces, in which the heat transfer is affected by radiative conductivity within pores and increases with depth in the subsurface. G mean = (2.5 ± 0.5) MKS Lellouch, Santos-Sanz et al Strong suggestion that T.I. (G) decreases with heliocentric distance (r h ) G s 2-3 orders of magnitude lower than expected for compact ices Pablo Santos-Sanz
15 Merging techniques Stellar occultations and thermal measurements are complementary techniques with clear and important synergies: Refining of TPMs using results from occultations Obtaining a detailed physical and thermal characterization of selected TNOs/Centaurs: diameter, albedo, shape, mass density, surface properties (G, roughness, emissivity), etc. Pablo Santos-Sanz
16 Merging techniques Borasisi or deriving general properties for the whole TNO/Centaur populations Pablo Santos-Sanz
17 Pablo Santos-Sanz Merging techniques
18 Merging techniques within SBNAF 2007 UK126 (Schindler et al. 2017) 3-chords stellar occultation + thermal data Results from the occultation used to constrain the TPM (assuming P = 8 h): D eff = km, a/c = T ss ~ K Orientation near equator-on (q=45-90º) Surface T distribution on 2007 UK 126, as predicted by the best TPM 2003 AZ84 (Santos-Sanz et al. 2017) thermal data + multi-chord stellar occultation Results from the occultation used to constrain the TPMs (P = 6.78 h): Orientation near pole-on ±30º Absolute PACS and MIPS fluxes for 2003 AZ84 w/ various TPMs: pole-on, pole-on +30, pole-on +60, equator-on Pablo Santos-Sanz
19 KBOs from occ. & thermal Thank you! Pablo Santos-Sanz:
(1,2), E. (1), T. (3), P. (1,4), P. (5), C. (6), T. (7), M. (8), E. (3), D. (1), J.
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