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MAPPING THE SMALL - SCALE STRUCTURE OF D ARK M ATTER HALOS WITH ALMA - PowerPoint PPT Presentation

MAPPING THE SMALL - SCALE STRUCTURE OF D ARK M ATTER HALOS WITH ALMA O BSERVATIONS OF S TRONG L ENSES Y ASHAR H EZAVEH H UBBLE F ELLOW - KIPAC - S TANFORD U NIVERSITY R ENCONTRE DU V IETNAM - Q UI N HON - 2016 N. D ALAL , D. M ARRONE , G. H OLDER ,


  1. MAPPING THE SMALL - SCALE STRUCTURE OF D ARK M ATTER HALOS WITH ALMA O BSERVATIONS OF S TRONG L ENSES Y ASHAR H EZAVEH H UBBLE F ELLOW - KIPAC - S TANFORD U NIVERSITY R ENCONTRE DU V IETNAM - Q UI N HON - 2016 N. D ALAL , D. M ARRONE , G. H OLDER , Y. M AO , W. M ORNINGSTAR R. B LANDFORD , J. C ARLSTROM , C. F ASSNACHT , P. M ARSHALL , N. M URRAY L. P ERREAULT L EVASSEUR , J. V IEIRA , R. W ECHSLER AND THE S OUTH P OLE T ELESCOPE DMS TEAM

  2. S MALL -S CALE S TRUCTURE OF D ARK M ATTER Small scale distribution of Large scale structure is very dark matter is not well well constrained. understood.

  3. M OTIVATION C OMPARING MW DWARF GALAXIES TO DM SUBHALOS N BODY SIMULATIONS O BSERVED MW SATELLITES T HEORY : N>> 1000 O BSERVATION N~10

  4. T HE M ISSING S ATELLITE P ROBLEM L ONG STANDING PROBLEM FOR CDM S TRIGARI ET AL . 2007 A P J. 669, 676

  5. S OLUTIONS B ARYONIC G ASTROPHYSICS D ARK M ATTER P HYSICS 2 keV Warm Dark Matter Cold Dark Matter L OVELL ET AL 2012, MNRAS 420, 3

  6. S TRONG G RAVITATIONAL L ENSING

  7. S TRONG G RAVITATIONAL L ENSING M ULTIPLY I MAGED F ISH

  8. S TRONG G RAVITATIONAL L ENSING

  9. S UBSTRUCTURE L ENSING

  10. S UBSTRUCTURE L ENSING

  11. A SENSE OF SCALE … Cold Dark Matter

  12. SDP.81

  13. SDP.81

  14. L ENS M ODELING P OSTULATE A S OURCE M ORPHOLOGY ( WITH PARAMETERS P S ) RAY - TRACING MODEL SIMULATION P OSTULATE A M ASS G ENERATE THE LENSED DISTRIBUTION IN THE LENS IMAGE OF THE SOURCE ( WITH PARAMETERS P M ) DATA M AXIMIZE THE LIKELIHOOD OF THE MODEL PARAMETERS GIVEN THE DATA

  15. I NTERFEROMETRY : ( WHAT DOES ALMA MEASURE ?)

  16. I NTERFEROMETRY : ( WHAT DOES ALMA MEASURE ?)

  17. I NTERFEROMETRY : ( WHAT DOES ALMA MEASURE ?) 1 0.5 v [M λ ] 0 − 0.5 − 1 − 1 − 0.5 0 0.5 1 u [M λ ] F OURIER SPACE P OSITION SPACE ( SKY )

  18. I NTERFEROMETRY : ( WHAT DOES ALMA MEASURE ?) 1 0.5 v [M λ ] 0 − 0.5 − 1 − 1 − 0.5 0 0.5 1 u [M λ ]

  19. I NTERFEROMETRY : ( WHAT DOES ALMA MEASURE ?) 1 0.5 v [M λ ] 0 − 0.5 − 1 − 1 − 0.5 0 0.5 1 u [M λ ]

  20. I NTERFEROMETRY : ( WHAT DOES ALMA MEASURE ?) 1 0.5 v [M λ ] 0 − 0.5 − 1 − 1 − 0.5 0 0.5 1 u [M λ ]

  21. I NTERFEROMETRY : ( WHAT DOES ALMA MEASURE ?) 1 0.5 v [M λ ] 0 − 0.5 − 1 − 1 − 0.5 0 0.5 1 u [M λ ]

  22. I NTERFEROMETRY : ( WHAT DOES ALMA MEASURE ?) 1 0.5 v [M λ ] 0 − 0.5 − 1 − 1 − 0.5 0 0.5 1 u [M λ ]

  23. I NTERFEROMETRY : ( WHAT DOES ALMA MEASURE ?) 1 0.5 v [M λ ] 0 − 0.5 − 1 − 1 − 0.5 0 0.5 1 u [M λ ]

  24. I NTERFEROMETRY : ( WHAT DOES ALMA MEASURE ?) 1 0.5 v [M λ ] 0 − 0.5 − 1 − 1 − 0.5 0 0.5 1 u [M λ ]

  25. I NTERFEROMETRY : ( WHAT DOES ALMA MEASURE ?) 1 0.5 v [M λ ] 0 − 0.5 − 1 − 1 − 0.5 0 0.5 1 u [M λ ]

  26. I NTERFEROMETRY : ( WHAT DOES ALMA MEASURE ?) 1 0.5 v [M λ ] 0 − 0.5 − 1 − 1 − 0.5 0 0.5 1 u [M λ ] NOT NOISE

  27. L ENS M ODELING FOR I NTERFEROMETRIC D ATA 1 - Postulate Sky Model 2 - Predict the Visibilities on Parameterized by the measured uv coverage Source and Lens Properties 5 x 10 − 6 − 4 − 2 0 2 4 1 arcsec 6 − 6 − 4 − 2 0 2 4 6 5 x 10 4 - Form a χ2 likelihood and 3 - Add additional Sample the posterior using a parameters for antenna parameter exploration phases method (MCMC, etc.)

  28. M ODEL P ARAMETERS parameters describing the light distribution in the background source (P source ) sky emission parameters describing the mass distribution in the foreground lens (P lens )

  29. L ENS MODELING WITH PIXELATED SOURCES p source = L ( p lens ) × = L ( p lens ) × p source sky surface brightness

  30. L ENS M ODELING WITH PIXELATED SOURCES matter distribution in the lens v = F L ( p lens ) × p source |{z} |{z} e − i ~ " # k ~ r ... ∼ 10 6 . . . |{z} background source ∼ 10 4

  31. SUCCESSFULLY TESTED ON MOCKS GENERATED WITH AN INDEPENDENT CODE W ARREN M ORNINGSTAR ( GRAD @ S TANFORD )

  32. EXAMPLE : SOURCE RECONSTRUCTION mock data (dirty image)

  33. EXAMPLE : SOURCE RECONSTRUCTION reconstructed source

  34. EXAMPLE : SOURCE RECONSTRUCTION true source (mock)

  35. EXAMPLE : SOURCE RECONSTRUCTION reconstructed source true source (mock) − 1 ⇤ − 1 ⇥ − 1 ( FBL ) + C s − 1 D ⇥ ( FBL ) T C N ( FBL ) T C N ⇤ S = For realistic ALMA data, solving this requires thousands of cpu-cores.

  36. L INEARIZING THE M ODEL ( SUBHALO FINDER ) Generally, likelihood evaluation is computationally very expensive. In a small neighborhood of the maximum posterior model, all parameters could be treated linearly for small perturbation to the fiducial model. We can use this linearized model to estimate the marginalized posterior for different subhalo models.

  37. P ROBABILITY OF THE PRESENCE OF A SUBHALO greyscale: difference in log posterior between a model which includes a subhalo and a smooth model (no subhalos) H EZAVEH ET AL . 2016

  38. SDP 81 
 (ALMA SCIENCE VERIFICATION DATA ) B LUE : HST D UST CO 8-7 R ED : ALMA

  39. SDP 81 
 R ECONSTRUCTED B ACKGROUND S OURCE H EZAVEH ET AL . 2016

  40. F IRST D ETECTION OF A DM S UBHALO WITH ALMA H EZAVEH ET AL . 2016

  41. F IRST D ETECTION OF A DM S UBHALO WITH ALMA H EZAVEH ET AL . 2016

  42. P ROBABILITY OF A SECOND S UBHALO H EZAVEH ET AL . 2016

  43. C ONSTRAINTS ON THE M ASS F UNCTION OF S UBHALOS IN THE H OST H ALO H EZAVEH ET AL . 2016

  44. C ONSTRAINTS ON THE M ASS F UNCTION OF S UBHALOS IN THE H OST H ALO T HEORY : Y AO -Y UAN M AO H EZAVEH ET AL . 2016

  45. C OMPARISON TO T HEORETICAL P REDICTIONS T HEORY : Y AO -Y UAN M AO H EZAVEH ET AL . 2016

  46. C ONSTRAINTS ON THE M ASS F UNCTION OF S UBHALOS IN THE H OST H ALO H EZAVEH ET AL . 2016

  47. C ONSTRAINTS ON THE M ASS F UNCTION OF S UBHALOS IN THE H OST H ALO H EZAVEH ET AL . 2016

  48. ALMA OBSERVATIONS OF SPT- DISCOVERED SOURCES B LUE : HST ( OPTICAL ), R ED : ALMA (C YCLE 0) V IEIRA ET AL . N ATURE 2013 H EZAVEH ET AL . A P J. 2013

  49. SPT2134-50 (ALMA C YCLE 2) B AND 6 ( RED : ALMA CONTINUUM , BLUE : HST) M ORNINGSTAR LEADING THE ANALYSIS

  50. SPT2134-50 (ALMA C YCLE 2) B AND 6 ( CONTINUUM ) M ORNINGSTAR LEADING THE ANALYSIS

  51. C ONSTRAINTS ON THE M ASS F UNCTION OF S UBHALOS IN THE H OST H ALO lensed by a fi eld lensed by a fi eld smooth density fi eld with low-k power with high-k power H EZAVEH ET AL . 2016

  52. E FFECT OF S OURCE S IZE : L ARGER S OURCE = L OWER S ENSITIVITY

  53. W E NEED A SMALL SOURCE , OR A SOURCE WITH SMALL FEATURES ...

  54. W E NEED A SMALL SOURCE , OR A SOURCE WITH SMALL FEATURES ... VELOCITY STRUCTURE E NGEL ET AL 2010, A P J

  55. 3D LENS MODELING (3 RD DIMENSION = WAVELENGTH )

  56. S ENSITIVITY A NALYSIS OF D ETECTING DM S UBHALOS 0.35 0.3 ϵ 0.25 angle [degree] 110 109 108 107 106 9 log M s [M ⊙ ] 8.5 8 7.5 7 1 x s [ arcsec ] 0.8 0.6 0.4 1.3 y s [ arcsec ] 1.2 1.1 1 0.9 11.598 11.6 11.60211.60411.606 0.25 0.3 0.35 106 108 110 7 8 9 0.4 0.6 0.8 1 0.9 1 1.1 1.2 1.3 7 8 9 log M [M ⊙ ] ϵ angle [degree] log M s [M ⊙ ] x s [ arcsec ] y s [ arcsec ] ] log M s [M ⊙ ] A FTER MARGINALIZING OVER ~60 SOURCE PARAMETERS H EZAVEH , D ALAL ET AL 2013, A P J. 767, 9

  57. SPT2134-50 (ALMA C YCLE 2) B AND 6 (CO 7-6) M ORNINGSTAR LEADING THE ANALYSIS

  58. C ONSTRAINTS ON THE M ASS F UNCTION OF S UBHALOS IN THE H OST H ALO lensed by a fi eld lensed by a fi eld smooth density fi eld with low-k power with high-k power H EZAVEH ET AL . 2016

  59. W E CAN DETECT AND MODEL MASSIVE SUBHALOS W HAT ABOUT THE THOUSANDS OF LOWER MASS ONES ? C AN WE DETECT THEM AS A WHOLE ? 5 10 4 10 3 10 N( > M) 2 10 1 10 0 10 5 6 7 8 9 10 M [ M ⊙ ]

  60. R ESIDUALS FROM M ODELING WITH A S MOOTH L ENS : lensed by a fi eld lensed by a fi eld smooth density fi eld with low-k power with high-k power

  61. C OVARIANCE OF D ENSITY P OWER SPECTRUM DEFLECTIONS

  62. DM SUBHALO DENSITY P OWER S PECTRUM 2 10 1 10 0 10 P ( k ) [pc 2 ] − 1 10 − 2 10 − 3 10 − 4 10 − 5 10 − 6 10 − 4 − 3 − 2 − 1 10 10 10 10 k [pc − 1 ]

  63. DM SUBHALO DENSITY P OWER S PECTRUM

  64. DM SUBHALO DENSITY P OWER S PECTRUM 2 2 10 10 1 1 10 10 0 0 10 10 P ( k ) [pc 2 ] P ( k ) [pc 2 ] − 1 − 1 10 10 − 2 − 2 10 10 − 3 − 3 10 10 − 4 − 4 10 10 − 5 − 5 10 10 − 6 − 6 10 10 − 4 − 4 − 3 − 3 − 2 − 2 − 1 − 1 10 10 10 10 10 10 10 10 k [pc − 1 ] k [pc − 1 ]

  65. DM SUBHALO DENSITY P OWER S PECTRUM 2 2 2 10 10 10 1 1 1 10 10 10 0 0 0 10 10 10 P ( k ) [pc 2 ] P ( k ) [pc 2 ] P ( k ) [pc 2 ] − 1 − 1 − 1 10 10 10 − 2 − 2 − 2 10 10 10 − 3 − 3 − 3 10 10 10 − 4 − 4 − 4 10 10 10 − 5 − 5 − 5 10 10 10 − 6 − 6 − 6 10 10 10 − 4 − 4 − 4 − 3 − 3 − 3 − 2 − 2 − 2 − 1 − 1 − 1 10 10 10 10 10 10 10 10 10 10 10 10 k [pc − 1 ] k [pc − 1 ] k [pc − 1 ]

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