Mehreen Mahmud Denise Gabuzda University College Cork, Ireland Searching for Helical Magnetic Fields...

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Mehreen Mahmud Denise Gabuzda University College Cork, Ireland Searching for Helical Magnetic Fields in Several BL Lac Objects

Transcript of Mehreen Mahmud Denise Gabuzda University College Cork, Ireland Searching for Helical Magnetic Fields...

Mehreen Mahmud Denise Gabuzda

University College Cork, Ireland

Searching for Helical Magnetic Fields in Several BL Lac Objects

Outline

● Introduction - Overview of previous work

● Faraday Rotation

● Data Reduction - Observations, Calibration, Imaging and Rotation Measure (RM) determination

● Results To Date - Sources with transverse rotation measure gradients : 0256+075, 0735+178 ,1418+546, 1803+784, 2155-152

● Conclusions and current work

● Polarization important because it shows the ordering of the magnetic field

associated with the radio emission.

● BL Lac Objects show a tendency for the magnetic fields in their parsec-scale

jets to be perpendicular to the jet direction.

● Gabuzda, Murray and Cronin (2004), showed systematic Faraday- Rotation

gradients across the parsec-scale jets of several BL Lac Objects,

- Interpreted as evidence for helical magnetic fields – the gradients were

taken to be due to the systematic variation of the line-of-sight magnetic

field component across the jet.

- Used three frequencies at 2 cm, 4 cm and 6 cm, observed in 1997.

● Shock Model: Series of relativistic shocks each of which enhances local

transverse B field.

Introduction

Gabuzda, D., Murray,E. & Cronin,P. (2004)

● RM map of 1652+398 observed at 2cm, 4cm and 6cm.

● Example of 'spine-sheath' B-field structure

● Transverse RM gradient ranging from ~ -63 rads/m2 to 131 rads/m2

Faraday Rotation

The amount of rotation is proportional to the integral of the density of free electrons ne multiplied by the line-of-sight magnetic field B • dl, the square of the

observing wavelength, and various physical constants; the coefficient of 2 is called the rotation measure, RM:

2 ne B • dl RM 2

Thus, the intrinsic polarization of the source, 0 can be obtained:

obs

= 0 + RM ( 2 )

where obs is the observed polarization angle, 0 is the intrinsic polarization

angle observed if no rotation occurred and is the observing wavelength.

● VLBA polarisation observations of 37 BL Lac objects observed between August 2003 and September 2004.

● 'Snap shot' mode, each source observed for about 25-30 minutes, several scans over the observing time period.

● 6 wavelengths; 2 at each of the 2cm, 4cm and 6cm bands.

● Objective to verify earlier results and get more refined Faraday Rotation gradients and identify new sources with the FR gradients.

Data Observation and Reduction I

Data Observation and Reduction II

● After calibration, for each wavelength, total intensity (I) and polarization images (distribution of Stokes parameters Q and U) mapped ● Polarization angle images combined to make rotation measure maps after matching their parameters (beam size, image size, cell size)

● Before final RM maps made, contributions from known integrated (Galactic) Faraday Rotation subtracted at each wavelength.

● Calibration, Imaging and Rotation Measure determination done with AIPS package using standard techniques.

Map of 1803+784 by Zavala R. & Taylor G. (2003)

● Observed at seven frequencies between 8.1 and 15.2 GHz on June 27th, 2000.

● RM of -201 rad/m2 at core, 14 rad/m2 in jet.

● Compare RM map to my map observed ~ 4 years later.

Detection of transverse gradients in 1803+784

● North-South RM gradient at ~2 mas from core.● Hints of transverse RM gradient further along jet (at ~ 5 mas).● Direction of North-South gradient reversed as compared to Zavala and Taylor (2003)● Possible explanation: Kink in magnetic field followed by reconnection.

0735+178 2155-152

0256+075 1418+546

Conclusions and current/future work

● Transverse rotation measure gradients in 1803+784 verified, and evidence for gradient further out in the jet (which still need verification). Orientation of rotation measure gradients may change over time (may indicate kinks in B-field).

● Possible transverse gradients in 0256+075, 0735+178,1418+546, 2155-152

● Simplest explanation is of helical magnetic fields wrapped around jet.

Acknowledgments

Radio Astronomy Lab at UCC

This work is supported by a Basic Research Grant from Science

Foundation Ireland. The VLBA is operated by the National Radio

Astronomy Observatory, which is a facility of the National Science

Foundation operated under cooperative agreement by Associated

Universities, Inc.

References

Gabuzda, D., Murray,E. & Cronin,P. 2004, MNRAS,351,L90

Zavala R. & Taylor G. 2003, ApJ, 589, 126Z

“Searching for Helical Magnetic Fields in Several BL Lac objects” Denise Gabuzda, Mehreen Mahmud and Askea O'Dowd (Poster presented at conference Ultra-Relativistic Jets in Astrophysics, Banff, Canada, July 2005 )

Pushkarev A. 2001, Astron. Rep., 45, 667

Rusk R. 1988, PhD Thesis, University of Toronto