Triple-lens analysis of event OB07349/MB07379

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Transcript Triple-lens analysis of event OB07349/MB07379

Triple-lens analysis of event OB07349/MB07379 Yvette Perrott, MOA group

Magnification map technique  This technique was developed at Auckland, by Lydia Philpott, Christine Botzler, Ian Bond, Nick Rattenbury and Phil Yock.

 It was developed for high magnification events with multiple lenses.

Three maps - high, medium, low resolution  The three maps cover roughly the FWHM, t E , and bulge season respectively.

L 4 x t E 0.8 x t E M H 0.08 x t E

A typical high-resolution map and track

Advantages and disadvantages of the method  It is straightforward conceptually, and can be applied to any combination of lens and source geometries.

 Many tracks can be laid across the same map.

 It is not the fastest way.

Cluster usage  We use a cluster of teaching computers during weeknights, weekends and holidays. This keeps the cost down, but they are not always available or reliable.

 The codes are written in C# for reliability, at the cost of speed.

 First analysis of OB07349/MB07379 Started with one-planet solution found by Dave Bennett, and searched for second planet to fit visible deviation.

2nd planet search procedure (1st stage)  Searched for low mass planets fairly near to the ring, and higher mass planets further away.  Only solutions with both planets inside the ring were considered.

 Only u min negative solutions were considered.

 Low resolution maps were used, with accuracy in chi 2 ~ 20.

2nd planet search procedure cont’d  The search procedure used for the track parameters was neither steepest descent or MCMC. Chi found.

2 values are calculated over a grid of track parameter values until a minimum not using an edge value in any parameter is  Three trials are conducted using randomised starting points and coarse step sizes, then the best minimum found in this way is used as a starting point for a final minimisation using fine step sizes.

q 2 = 10 -5 search results q=1 b 1 q 1 b 2 a 2 q 2 Delta chi 2 values (from 1-planet minimum) < -600 -600 0

q 2 = 10 -4 q 1 q=1 b 1 a 2 b 2 q 2 Delta chi 2 values (from 1-planet minimum) < -600 -600 0

q 2 = 10 -3 q 1 q=1 b 1 a 2 b 2 q 2 Delta chi 2 values (from 1-planet minimum) < -600 -600 0

q 2 = 10 -2 q 1 q=1 b 1 a 2 b 2 q 2 Delta chi 2 values (from 1-planet minimum) < -600 -600 0

2nd stage of search  Mass and position of both planets varied.

 Orbital and terrestrial parallax effects included.

 Higher resolution maps used to increase accuracy to chi 2 ~ a few.

 u min positive and negative solutions explored.

Method of including parallax Ecliptic March Earth at December

Z

Sun

Y

23.5

X n

September (RA = 0) June To galactic bulge

e

 The sun’s apparent motion around the Earth is calculated as in Gould, A. “Resolution of the MACHO-LMC-5 Puzzle: the Jerk-Parallax Microlens Degeneracy.” Astrophys.J.

606 (2004): 319-325.

Parallax method cont’d  The corrections to the track of the source star are then given by  (  ,  ) = ( 

E

  s, 

E

 s)  where r E = AU/|  E |, and the direction of Non-parallax track of source    E is the direction of motion of the source.

Lens u min Parallax track of source

Terrestrial parallax - similar  Add the small displacement from the Earth’s centre to the position and velocity functions, taking into account the Earth’s translation and rotation.

Results of 2nd stage - Sol #1,  2 = 902 (u min negative) Planet parameters: q 0.80689; q 2 1 = 0.0003841; b 1 = 1.3x10

-5 ; b 2 = 0.73; a 2 = = 194

Track parameters  u min = -0.00181; 4348.7366; t E  = 0.325; ssr = 0.00062; t 0 = 111.61;  E,E = 0.11;  E,N = = 0.21

 u min

Results of 2nd stage - Sol #2,  2 = 870 (u min negative) Planet parameters: q q 2 = 7x10 -6 ; b 2 1 = 0.000397; b 1 = 0.955; a 2 = -3.5

= 0.794;

Track parameters  u min = -0.00181; 4348.7341; t E  = 0.317; ssr = 0.000615; t 0 = 110.66;  E,E = 0.11;  E,N = 0.11

=  u min

Results of 2nd stage - Sol #2,  2 = 873 (u min positive) Planet parameters: q q 2 = 8.5x10

-6 ; b 2 1 = 0.000395; b = 0.952; a 2 1 = 0.794; = 183.5

Track parameters  u min = 0.00181; 4348.7341; t E  = -0.315; ssr = 0.00062; t 0 = 110.41;  E,E = 0.12;  E,N = = -0.06

 u min

Results of 2nd stage - Sol #3,  2 = 881 (u min negative) Planet parameters: q 0.80569; q 2 1 = 0.0003851; b 1 = 0.0010; b 2 = 0.2; a 2 = = 213

Track parameters  u min = -0.00192; 4348.7521; t E  = -0.341; ssr = 0.000625; t 0 = 111.31;  E,E = 0.10;  E,N = 0.38

=  u min

Parallax from the wings  Only OGLE and MOA data used (older reduction)  Consistent with all solutions so far (negative u min ) 3 1 2 3 2 1  2 levels are at 1, 4, 9, 16, 25

Comparison with Subo Dong’s results (Ohio State)  6 solutions, of which 2 correspond to ours  Note different conventions: our results for u min , t 0 converted to US system; b 1 , b 2 not converted q 1 q 1 b 1 b 1 Lens star u min Lens star Centre of mass u min Source at t 0 Source at t 0 NZ system US system

Sol # q 1 1 3 (Subo) b 1 0.0003841 0.80689

q 2 1.3x10

-5 0.0003791 0.8073938 0.504x10

-5 b 2 0.73

a 2 194 0.871897 193.1

u min -0.00210

-0.0020802

 0.325

0.322

ssr 0.00062

0.0006177

t 0 4348.7472

4348.7471829

t E 111.61

112.12765

 E,E 0.11

0.119

 E,N 0.21

0.107

 2 902 796.67

Sol # q 1 2 (-ve) 0.000397

b 1 0.794

q 2 7x10 -6 b 2 0.955

a 2 -3.5

5 (Subo) u min -0.00210

0.0004034 0.7962501 8.10x10

-6  0.317

ssr 0.000615

-0.0021945

0.321

0.0006444

0.9526577 -3.51

t 0 4348.7447

4348.7460743

t E 110.66

106.61081

 E,E 0.11

0.117

 E,N 0.11

0.009

 2 870 769.09

Sol # q 1 2 (+ve) 0.000395

5 (Subo) b 1 0.794

q 2 8.5x10

-6 0.0003731 0.7946362 8.68x10

-6 b 2 0.952

a 2 183.5

0.9454526 183.72

u min 0.00210

0.0020265

 -0.315

-0.321

ssr 0.00062

0.0005883

t 0 4348.7447

4348.7459452

t E 110.41

115.31758

 E,E 0.12

0.114

 E,N -0.06

-0.256

 2 873 758.10

Sol #3,  2 = 881 Doesn’t appear to correspond to any of Subo’s solutions.

Future plans  Finish analysing the remaining minima  Use MCMC for track parameters for speed and better  2 accuracy  Include HST data to identify lens

Thanks  To the observatories and groups that provided data: OGLE, Bronberg, FTN, CTIO, MOA, Palomar, UTAS, Perth, VintageLane  To Ian Bond and Subo Dong for data reductions  To Andy Gould and Subo Dong for discussion  To the IT department at Auckland University for use of the cluster  To the North Harbour Club who helped to fund my trip