UNCERTAINTIES IN THE DEPROJECTION OF THE OBSERVED BAR PROPERTIES - - PowerPoint PPT Presentation

uncertainties in the deprojection of the observed bar
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UNCERTAINTIES IN THE DEPROJECTION OF THE OBSERVED BAR PROPERTIES - - PowerPoint PPT Presentation

UNCERTAINTIES IN THE DEPROJECTION OF THE OBSERVED BAR PROPERTIES Yanfei Zou 1 Juntai Shen 1 and Zhao-Yu Li 1 1.Shanghai Astronomical Observatory, China 2013.10.21 MOTIVATION ~2/3 of disk galaxies are barred Composition of the bar


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SLIDE 1

UNCERTAINTIES IN THE DEPROJECTION OF THE OBSERVED BAR PROPERTIES

Yanfei Zou1

Juntai Shen1 and Zhao-Yu Li1

1.Shanghai Astronomical Observatory, China 2013.10.21

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SLIDE 2

MOTIVATION

 ~2/3 of disk galaxies are

barred

 Composition of the bar

 old stars

 Bar pattern rotates rapidly  Internal driver of disk galaxies

 gas inflow, central starburst, etc.  energy and angular momentum

exchange

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SLIDE 3

 Deproject the inclined bar to

face-on.

 Basic assumption of the

deprojection

 The outer parts of the bar are

vertically thin.

 Observed galaxies: projected

2D information

MOTIVATION

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SLIDE 4

 Simulated galaxies: 3D

information

 So we know the true face-on

values of the bar length and ellipticity.

 Observe the simulated galaxy

from different viewing angles

 The uncertainties of

deprojection can be examined.

MOTIVATION

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SLIDE 5

 3D information

 true face-on values of

the bar length and ellipticity.

 Observe the

simulated galaxies from different viewing angles

 We reduce the data

in the same way as

  • bservations

METHODS

Model A Model B

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106 particles rigid dark matter halo potential T = 1.8 Gyr 2*106 particles live halo T = 2.4 Gyr

Data

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SLIDE 6

 IRAF ellipse fitting

 amax : Maximum ellipticity (Sheth et al. 2003)  amin : Minimum ellipticity (Erwin 2005)  a10 : Position angle (PA) deviates by 10° (Erwin 2005)

METHODS

Measure bar properties (length and ellipticity)

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SLIDE 7

 1-D analytical deprojection

(Martin 1995)

 Assuming the bar is a straight line

segment

 2-D analytical deprojection

(Gadotti et al. 2007)

 Assuming the bar is a planar

elliptical structure

 2-D image deprojection  Other Fourier-based

deprojections

 Fourier decomposition

(Li Z-Y et al. 2011)

 Bar-interbar contrast

(Ohta et al. 1990)

METHODS

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Deproject bar properties to face-on

1. Deproject the image using GEOTRAN 2. Measure the deprojected bar properties

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SLIDE 8

RESULTS

 Assuming the bar is a planar

elliptical structure

 The deviation of adep/aint

increases with the i

 The deprojected amax tends to

  • verestimate the true face-on
  • amax. There is no clear trend

for amin and a10.

 i >60°, the deviation becomes

large

 ~10%

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2-D analytical deprojection of the bar length

Φbar

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SLIDE 9

RESULTS

 A reflection of the strength of

the bar

 The deviation of edep/eint

becomes large with i

 As Φbar increases from 0° to

90°, the deprojected ellipticity gradually transition from under-estimate to over- estimate

 ~10%

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2-D analytical deprojection of the bar ellipticity

Φbar

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SLIDE 10

RESULTS

 1D deprojection has the

largest uncertainty ~20%.

 2D deprojection is more

  • accurate. The uncertainty is

~10%.

 Uncertainty of Fourier

decompostion:~5%.

 Bar-interbar contrast has large

uncertainty, which is ~10%.

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Typical scatter in the deprojection

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TOY MODEL

 Bar structure: triaxial ellipsoid

shell.

 Axis ratio: a:b:h

 Project the shell of the triaxial

ellipsoid from different i and Φbar.

 1D and 2D analytical

deprojection are tested using this simple toy model

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TOY MODEL

 2D analytical deprojection of

the toy bar length

 Uncertainties increase with i

and Φbar.

 Similar trend and scatter as

the simulation results of 2D analytical deprojection.

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TOY MODEL

 2D analytical deprojection of

the toy bar ellipticity

 Uncertainties increase with i.  Deprojected ellipticity

transition from under-estimate to over-estimate in the ellipticity deprojection as Φbar increases from 0◦ to 90◦.

 Similar trend and scatter as

the simulation results of 2D analytical deprojection.

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TOY MODEL

 Solid line: thick bar.  Dashed line: 2D planar bar.  Small residual at small i.  Large residual at large i.  Uncertainties mainly stem from

the vertical structure of the bar.

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SUMMARY

 Uncertainties of deprojection increase with i. All deprojection methods have

trouble recovering the bar properties when i>60°.

 For amax, both the 1D and 2D methods overestimate the intrinsic bar length.

There is no clear trend for amin and a10.

 As Φbar increases from 0 ° to 90 °, the deprojected emax and emin from 2D

methods transition from underestimate to overestimate. The deprojected e10 is generally underestimated.

 Uncertainties of the deprojection can be reproduced by a simple toy model,

which confirms that it mainly stems from the vertical structure of the bar.

 The uncertainty and application range of popular methods are given (lower

limit).

 Provide guidelines for the sample selection and error estimation of future

statistical research on barred galaxies.

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