Origins and Fundamental Physics of Supermassive Black Holes
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The US Extremely Large Telescope Program Origins and Fundamental Physics of Supermassive Black Holes Jenny E Greene GC Team:Tuan Do, Andrea Ghez, Jessica Lu, Matthew Hosek, Andrew Bellini, Sukanya Chakrabarti, Mark Morris, Shoko Sakai IMBH team: Tuan Do, Andrea Bellini, Jonelle Walsh, Kayhan Gultekin, Karl Gebhardt, Aaron Barth, Matthew Hosek, Dongwon Kim, Mattia Libralato, Jessica Lu, Matthew Malkan 01/07/2019 U.S. ELT Program - AAS #233 1
US-ELT: Transforming Black Hole Science Is GR the right description of black holes? Proper motions and radial velocities of stars at the Galactic Center How did supermassive black holes (SMBH) form? Search for intermediate-mass black holes Figure 3. Simulation of the central 0.5 arcsecond around the supermassive black hole Sgr A* (white cross) w adaptive optics with the Keck Telescopes (left) compared to that with TMT (right). The greater resolving pow How did SMBHs evolve through cosmic time? along with better AO correction will likely allow us to detect a factor of > 10 times more stars in this region. W how these orbit can be used simultaneously in a joint analysis to constraint tests of gravity and other science Search for SMBHs out to z~2 (won’t cover now) 01/07/2019 U.S. ELT Program - AAS #233 2 Figure 4. Overlay of a sample orbits from the simulations described in Section 3. TMT will likely discover
Zooming Into Stellar Nuclei Both angular resolution and depth are key From 17 to 120 stars to be monitored at the GC Reach the sphere of Influence of 1000 Msun Keck Today BHs in the MW and 10,000 1.1”=0.044pc Msun BHs to >5Mpc 01/07/2019 U.S. ELT Program - AAS #233 3
Zooming Into Stellar Nuclei Both angular resolution and depth are key From 17 to 120 stars to be monitored at the GC Reach the sphere of Influence of 1000 Msun BHs in the MW and 10,000 1.1”=0.044pc Msun BHs to >5Mpc 01/07/2019 U.S. ELT Program - AAS #233 4
Galactic Center Experiment Simulations: Instrumentation: Number of stars: 121 (TMT) vs 17 TMT/IRIS for astrometry+moderate (present-day) resolution spectroscopy Assumes: 5x better astrometry GMTNIRS for high-resolution 10x better radial velocities spectroscopy for shortest-period stars Cadence: 3 RV and 3 PM measurements/yr for three years Two-telescope system: provides complementary instrumentation, Total time: 360 hrs (IRIS) longer baseline modeling, insurance against weather 01/07/2019 U.S. ELT Program - AAS #233 5
>10 sigma detection Figure 4: The left panel shows the signal to noise ratio for the GR precession signal and the left panel displays the uncertainty on the extended mass parameter at the To 1000 Galactic Msun Center. The red precision curve shows the evolution with Keck and TMT data. The blue curve on the other hand is with only Keck data. The grey dashed horizontal line in the right panel is the extended mass value at the distance of semi–major axis of S0–2. Figure 4: The left panelToshows 2000 Msun precision the signal To +/- to noise ratio for the GR 5pc precision precession signal and the left panel displays the uncertainty on the extended mass parameter at the Galactic Center. The red curve shows the evolution with Keck and TMT data. The blue curve on the other hand is with only Keck data. The grey dashed horizontal line in the right panel is the extended mass value at the distance of semi–major axis of S0–2. U.S. ELT Program - AAS #233 6
How do SMBHs Form? ???????????????????????????????????????????? 106 10 10 10 76 10 10 10 1087 89 9 Direct Collapse Direct Directcollapse? Collapse The Astrophysical Journal Letters, 824:L8 (7pp), 2016 June 10 Rodriguez et al. rophysical Journal Letters, 824:L8 (7pp), 2016 June 10 Rodriguez et al. Supermassive Supermassive Supermassive Accretion Accretion Stellar Mass Stellar Mass Stellar Mass Black Holes Black Holes gravitational! Tidal ! gravitational gravitational! Rodriguez+2016 Tidal ! runaway disruption Rodriguez+2016 runaway disruption runaway? Accretion Accretion PopIII SNe? dynamical ! Figure 2. Distribution of BBH total masses from GCs. In gray, we show the CHE distribution of all mergers that occur at z 0.5 (for GCs that form at z 3.5), dynamical ! interactions Figure 2. Distribution of BBH total masses from GCs.weIn show gray, the we distribution show the of sources detectable with Advanced CHE while in blue distribution of all mergers that occur at z 0.5 (for GCs that form at z 3.5), interactions while in blue we show the distribution of LIGO during its first observing run. The median and 90% credible regions for thesources detectable total mass with Advanced of GW150914 are shown in red (The LIGO Scientific LIGO during its first observing run. The median and 90% & credible regions for 105 Msun Collaboration The Virgo Collaboration 2016b). We also show the the total mass of GW150914 are shown in red (The trigger, LIGO LVT151012, Scientific in purple (where we have computed Collaboration & The Virgo Collaboration gravitational-wave 2016b). the median and We (where alsoregions credible show bythe Accretion adding the component mass median and gravitational-wave trigger, LVT151012, in explosion the median and credible regions by adding 90%purple Thethe credible component Virgo Accretion we have interval computed boundaries mass median Collaboration from The LIGO Scientific Collaboration & 2016a). and Note that while LVT151012 is below the SN01/07/2019 explosion 90% credible interval boundaries from The The Virgo Collaboration 2016a). Note that LIGO thresholdU.S. while signal to ELTCollaboration Scientific Program be considered was LVT151012 of astrophysical & - there a detection, is below the origin (Abbott AASexists#233 a 84% chance that the et al. 2016d). 7 threshold to be considered a detection, there exists a 84% chance that the
Search for . ELT Key Science Program Intermediate-mass Black Holes Page 4 Draft SgrA* 6 Two Experiments: 10 15 Cluster BHs = ! Proper motion measurements More Common of 43 MW GCs TOTAL NUMBER i! cle t Nu ) entection s 2e3 Msun limits with 3 epochs 105 ?? Intermediate-mass MBH (M ) r r Heavy BHs ! Cu de(3 100 total hrs* Black Holes?? 10 = rare gh t! U.S. ELT Key Science Program Page 5 NucDraft Current GC ! li 104 (6 possible ! t. ) - in sed HST ACS/WFC 202x202 arcsec2 HST WFC3/UVIS 40 mas/pixel TMT/IRIS 4 mas/pixel Ts propo Integrated-light observations of 25 stellar detections) L E 25 ( MWGC ELT PM ! 103 (43 proposed) nuclei in galaxies 5 with TMT/IRIS+GMTIFS
Search for . ELT Key Science Program Intermediate-mass Black Holes Page 4 Draft SgrA* 10 6 Two Experiments: Cluster BHs = ! 15 Integrated-light observations of 25 TOTAL NUMBER i! More Common cle 105 t Nu ) entection s stellar nuclei inHeavy galaxies
Solve the Seed Problem U.S. ELT Key Science Program Page 4 Draft SgrA* 106 15 Cluster BHs = ! TOTAL NUMBER i! More Common ucle t N ) s 105 entection ?? Intermediate-mass MBH (M ) r r Heavy BHs ! Cu de(3 Black Holes?? 10 = rare ht! Nuc 4 Current GC ! t. )lig 10 (6 possible ! - inposed detections) s T ro EL 25 p ( ELT PM ! MWGC (43 proposed) 103 5 Nuc MWGC 102 LIGO ! Binaries 10 3 10 2 10 1 100 0 3 10 104 105 D (Mpc) log (M /M ) 01/07/2019 U.S. ELT Program - AAS #233 10
US-ELT: Transforming Black Hole Science Is GR the right description of black holes? Proper motions and radial velocities of stars at the Galactic Center Extended mass distributions and GR tests: 360 hrs How did supermassive black holes (SMBH) form? Search for intermediate-mass black holes Mass function and environments, first-ever detections of IMBHs: 200-300hrs Figure 3. Simulation of the central 0.5 arcsecond around the supermassive black hole Sgr A* (white cross) w adaptive optics with the Keck Telescopes (left) compared to that with TMT (right). The greater resolving pow along with better AO correction will likely allow us to detect a factor of > 10 times more stars in this region. W how these orbit can be used simultaneously in a joint analysis to constraint tests of gravity and other science The combination of angular resolution and sensitivity will transform BH science 01/07/2019 U.S. ELT Program - AAS #233 11 Figure 4. Overlay of a sample orbits from the simulations described in Section 3. TMT will likely discover
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