Polarization in Interferometry

Size: px
Start display at page:

Download "Polarization in Interferometry"

Transcription

1 Polarization in Interferometry Calibration Tutorial Ivan Martı -Vidal Onsala Space Observatory Chalmers University of Technology (Sweden) European Radio Interferometry School Dwingeloo (October 2017)

2 TUTORIAL - ALMA B5 I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

3 How we will proceed in this Tutorial There are three scripts and one measurement set provided: scriptforcalibration.py Standard calibration. scriptforpolcalibration.py Polarization calibration. ERIS2017 helper.py Some helper functions for plotting, hacking tables, etc. ERIS 2017.Polarization Tutorial.DATA.ms ALMA Band 5 (commissioning full-pol) observations of VY CMa. The script is almost ready to go. Just a few lines have to be uncommented (after discussion). The steps will be performed one by one. Results after each step will be discussed. Freedom to choose among different options (e.g., bandpass, reference antenna, etc.) and to play with (i.e., hack) the calibration tables. The script to obtain the final image of the target will be fully written by you! I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

4 ALMA Band 5 PART I: Standard Calibration Look at the schedule. Understand the observations. Putting a model to the primary flux calibrator. Check model column. Bandpass calibration Fast phase calibration (i.e., optimize coherence). Bandpass calibration. Does it vary with time? Gain calibration Fast phase & slow amplitude Absolute flux-density scaling Slow phase (for phase referencing) Check X/Y cross-phases. What happens to the ref. antenna? I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

5 ALMA Band 5 PART I: Standard Calibration Look at the schedule. Understand the observations. Putting a model to the primary flux calibrator. Check model column. Bandpass calibration Fast phase calibration (i.e., optimize coherence). Bandpass calibration. Does it vary with time? Gain calibration Fast phase & slow amplitude Absolute flux-density scaling Slow phase (for phase referencing) Check X/Y cross-phases. What happens to the ref. antenna? I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

6 ALMA Band 5: Understand I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

7 ALMA Band 5: Understand I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

8 ALMA Band 5 PART I: Standard Calibration Look at the schedule. Understand the observations. Putting a model to the primary flux calibrator. Check model column. Bandpass calibration Fast phase calibration (i.e., optimize coherence). Bandpass calibration. Does it vary with time? Gain calibration Fast phase & slow amplitude Absolute flux-density scaling Slow phase (for phase referencing) Check X/Y cross-phases. What happens to the ref. antenna? I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

9 ALMA Band 5: Flux Cal. I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

10 ALMA Band 5: Flux Cal. I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

11 ALMA Band 5 PART I: Standard Calibration Look at the schedule. Understand the observations. Putting a model to the primary flux calibrator. Check model column. Bandpass calibration Fast phase calibration (i.e., optimize coherence). Bandpass calibration. Does it vary with time? Gain calibration Fast phase & slow amplitude Absolute flux-density scaling Slow phase (for phase referencing) Check X/Y cross-phases. What happens to the ref. antenna? I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

12 ALMA Band 5: Bandpass I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

13 ALMA Band 5: Bandpass I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

14 ALMA Band 5: Bandpass I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

15 ALMA Band 5 PART I: Standard Calibration Look at the schedule. Understand the observations. Putting a model to the primary flux calibrator. Check model column. Bandpass calibration Fast phase calibration (i.e., optimize coherence). Bandpass calibration. Does it vary with time? Gain calibration Fast phase & slow amplitude Absolute flux-density scaling Slow phase (for phase referencing) Check X/Y cross-phases. What happens to the ref. antenna? I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

16 ALMA Band 5: Gain Cal. I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

17 ALMA Band 5: Gain Cal. I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

18 ALMA Band 5: Gain Cal. PART I: Standard Calibration Look at the schedule. Understand the observations. Putting a model to the primary flux calibrator. Check model column. Bandpass calibration Fast phase calibration (i.e., optimize coherence). Bandpass calibration. Does it vary with time? Gain calibration Fast phase & slow amplitude Absolute flux-density scaling Slow phase (for phase referencing) Check X/Y cross-phases. What happens to the ref. antenna? I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

19 ALMA Band 5: Gain Cal. I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

20 ALMA Band 5: Gain Cal. I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

21 ALMA Band 5 PART II: Polarization Calibration X/Y gain ratio for the Pol. calibrator (Q effect on XX/YY). Cross-delay calibration (take a look at the data) Cross-phase calibration (look at the estimated Stokes) Cross-phase calibration ambiguity Polarization leakage Amplitude cross-polarization ratios I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

22 ALMA Band 5 PART II: Polarization Calibration X/Y gain ratio for the Pol. calibrator (Q effect on XX/YY). Cross-delay calibration (take a look at the data) Cross-phase calibration (look at the estimated Stokes) Cross-phase calibration ambiguity Polarization leakage Amplitude cross-polarization ratios I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

23 ALMA Band 5: Q/U from Gain Remember the brightness matrix in linear-polarization basis: ( ) I + Qant U ant + j V S = U ant j V I Q ant where Q ant = Q sky cos 2ψ + U sky sin 2ψ I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

24 ALMA Band 5: Q/U from Gain Remember the brightness matrix in linear-polarization basis: ( ) I + Qant U ant + j V S = U ant j V I Q ant where Q ant = Q sky cos 2ψ + U sky sin 2ψ So: G x G y I + Q ant I Q ant = f (ψ). I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

25 ALMA Band 5: Q/U from Gain We estimate Q sky and U sky from G x G y vs. ψ I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

26 ALMA Band 5: Q/U from Gain We estimate Q sky and U sky from G x G y vs. ψ I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

27 ALMA Band 5 PART II: Polarization Calibration X/Y gain ratio for the Pol. calibrator (Q effect on XX/YY). Cross-delay calibration (take a look at the data) Cross-phase calibration (look at the estimated Stokes) Cross-phase calibration ambiguity Polarization leakage Amplitude cross-polarization ratios I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

28 ALMA Band 5: X-Y Delay I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

29 ALMA Band 5: X-Y Delay I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

30 ALMA Band 5 PART II: Polarization Calibration X/Y gain ratio for the Pol. calibrator (Q effect on XX/YY). Cross-delay calibration (take a look at the data) Cross-phase calibration (look at the estimated Stokes) Cross-phase calibration ambiguity Polarization leakage Amplitude cross-polarization ratios I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

31 ALMA Band 5: X-Y Phase Let s add a cross-polarization phase to the brightness matrix: S = ( I + Q ant (U ant + j V )e j ) (U ant j V )e +j I Q ant where G x = 1 and G y = e +j at all antennas. I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

32 ALMA Band 5: X-Y Phase Let s add a cross-polarization phase to the brightness matrix: S = ( I + Q ant (U ant + j V )e j ) (U ant j V )e +j I Q ant where G x = 1 and G y = e +j at all antennas. So the cross-polarization visibilities are: XY = (U sky cos 2ψ Q sky sin 2ψ + jv )e j. I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

33 ALMA Band 5: X-Y Phase Let s add a cross-polarization phase to the brightness matrix: S = ( I + Q ant (U ant + j V )e j ) (U ant j V )e +j I Q ant where G x = 1 and G y = e +j at all antennas. So the cross-polarization visibilities are: XY = (U sky cos 2ψ Q sky sin 2ψ + jv )e j. Real vs. Imag: Re(XY ) = (U sky cos 2ψ Q sky sin 2ψ) cos V sin Im(XY ) = (U sky cos 2ψ Q sky sin 2ψ) sin + V sin I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

34 ALMA Band 5: X-Y Phase Let s add a cross-polarization phase to the brightness matrix: S = ( I + Q ant (U ant + j V )e j ) (U ant j V )e +j I Q ant where G x = 1 and G y = e +j at all antennas. So the cross-polarization visibilities are: XY = (U sky cos 2ψ Q sky sin 2ψ + jv )e j. Real vs. Imag: Re(XY ) = (U sky cos 2ψ Q sky sin 2ψ) cos V sin Im(XY ) = (U sky cos 2ψ Q sky sin 2ψ) sin + V sin If we plot Re(XY ) vs. Im(XY ), we will see a straight line (as long as V is negligible) with a slope proportional to tan ( ). I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

35 ALMA Band 5: X-Y Phase I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

36 ALMA Band 5: X-Y Phase I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

37 ALMA Band 5: X-Y Phase Ambiguity We fit for Q sky, U sky, and using XY and XY as data. I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

38 ALMA Band 5: X-Y Phase Ambiguity We fit for Q sky, U sky, and using XY and XY as data. BUT notice that XY = (U sky cos 2ψ Q sky sin 2ψ + jv )e j has an ambiguity. (Q sky, U sky, ) ( Q sky, U sky, + π) I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

39 ALMA Band 5: X-Y Phase Ambiguity I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

40 ALMA Band 5 PART II: Polarization Calibration X/Y gain ratio for the Pol. calibrator (Q effect on XX/YY). Cross-delay calibration (take a look at the data) Cross-phase calibration (look at the estimated Stokes) Cross-phase calibration ambiguity Polarization leakage Amplitude cross-polarization ratios I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

41 ALMA Band 5: Leakage Effect of the Dterms on the XY cross-correlations: XY XY + D a x YY + (D b y ) XX I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

42 ALMA Band 5: Leakage Effect of the Dterms on the XY cross-correlations: XY XY + D a x YY + (D b y ) XX In terms of the brightness matrix (i.e., assuming a point source): XY U ant + jv + D a x (I Q ant ) + (D b y ) (I + Q ant ) I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

43 ALMA Band 5: Leakage Effect of the Dterms on the XY cross-correlations: XY XY + D a x YY + (D b y ) XX In terms of the brightness matrix (i.e., assuming a point source): XY U ant + jv + D a x (I Q ant ) + (D b y ) (I + Q ant ) Re-arranging terms: XY U ant + Q ant ((D b y ) D a x ) + jv + I (D a x + (D b y ) ) I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

44 ALMA Band 5: Leakage By knowing U ant and Q ant, we can solve for D x and D y for all antennas. I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

45 ALMA Band 5 PART II: Polarization Calibration X/Y gain ratio for the Pol. calibrator (Q effect on XX/YY). Cross-delay calibration (take a look at the data) Cross-phase calibration (look at the estimated Stokes) Cross-phase calibration ambiguity Polarization leakage Amplitude cross-polarization ratios I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

46 ALMA Band 5: X-Y Amp. Ratio Let s add a cross-polarization amplitude ratio to the brightness matrix: ( ) I + Qant (U ant + j V )ρ b F[V ab ] (U ant j V )ρ a (I Q ant )ρ a ρ b where G i x = 1 and G i y = ρ i. Changes in the amplitudes vs. ψ allow us to solve for ρ i. I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

47 ALMA Band 5: X-Y Amp. Ratio I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

48 FINISHED! I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

49 FINISHED! LET S PLAY NOW! I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

50 ALMA Band 5: Pol. Calib. Image I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

51 ALMA Band 5: Hacking Tables! The function finetune G allows you to change any calibration table in many different ways. Make a backup of your tables, run finetune G and repeat steps 9, 11, and 12 of the polarization calibration script. You can load the different images with the plotpolimage function to compare! Some ideas: Add an offset to the imaginary parts of the Dterms (different sign for each polarization). Same as above, but add it to the real parts. Repeat both previous items by using the same signs for both polarizations. Add an offset to the X-Y cross-polarization phase. Add a ratio to the X-Y amplitude-ratio gains. Add a cross-polarization delay. Any combination of the above. I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

52 BONUS: Leakage calibration on circular polarizers Calibrate R/L phase offset using pol. calibrator. I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

53 BONUS: Leakage calibration on circular polarizers Calibrate R/L phase offset using pol. calibrator. ( ) ( D L) V obs = D a X Vab true X H Db H a ; X = ; D a = 0 e jα Da R 1 V obs RL = ((D R a + (D L b ) ) I + P) e jα + O(D 2 ) V obs LR = ((D L a + (D R b ) ) I + P ) e jα + O(D 2 ) I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

54 BONUS: Leakage calibration on circular polarizers Calibrate R/L phase offset using pol. calibrator. ( ) ( D L) V obs = D a X Vab true X H Db H a ; X = ; D a = 0 e jα Da R 1 V obs RL = ((D R a + (D L b ) ) I + P) e jα + O(D 2 ) V obs LR = ((D L a + (D R b ) ) I + P ) e jα + O(D 2 ) Unpolarized calibrator: (D L a, D R a, e jα ) (D L a e j + jk, D R a e j + jk, e j(α ) ) Polarized calibrator: (D L a, D R a, e jα ) (D L a + jk, D R a + jk, e j(α) ) I. Martí-Vidal (Onsala Space Observatory) Interferometric Polarimetry ERIS / 31

Polarization calibration of the Phased ALMA for mm VLBI

Polarization calibration of the Phased ALMA for mm VLBI Polarization calibration of the Phased ALMA for mm VLBI Algorithms for calibration and test simulations Ivan Martí-Vidal Nordic Node of the European ALMA Regional Center Onsala Space Observatory (Sweden)

More information

Dual differential polarimetry. A technique to recover polarimetric information from dual-polarization observations

Dual differential polarimetry. A technique to recover polarimetric information from dual-polarization observations A&A 593, A61 (216) DOI: 1.151/4-6361/21628225 c ESO 216 Astronomy & Astrophysics Dual differential polarimetry. A technique to recover polarimetric information from dual-polarization observations I. Martí-Vidal,

More information

1mm VLBI Call for Proposals: Cycle 4

1mm VLBI Call for Proposals: Cycle 4 1mm VLBI Call for Proposals: Cycle 4 22 March 2016 Introduction The National Radio Astronomy Observatory (NRAO) invites proposals for 1mm Very Long Baseline Interferometry (VLBI) using the phased output

More information

Description. Polarization can be described several other ways

Description. Polarization can be described several other ways Polarization If there are magnetic fields ( Synchrotron, Cyclotron...) involved we can get a preferred direction of radiation - polarization We normally use Stokes parameters to show thes (I,Q,U,V) -total

More information

arxiv: v1 [astro-ph.im] 20 Jun 2017

arxiv: v1 [astro-ph.im] 20 Jun 2017 Draft version July 21, 2018 Typeset using L A TEX preprint style in AASTeX61 CALIBRATION ERRORS IN INTERFEROMETRIC RADIO POLARIMETRY Christopher A. Hales1, 2, arxiv:1706.06612v1 [astro-ph.im] 20 Jun 2017

More information

Polarization in Interferometry. Ramprasad Rao (ASIAA)

Polarization in Interferometry. Ramprasad Rao (ASIAA) Polarization in Interferometry Ramprasad Rao (ASIAA) W M A Q We Must Ask Questions Outline Polarization in Astronomical Sources Polarization Physics & Mathematics Antenna Response Interferometer Response

More information

Solar System Objects. Bryan Butler National Radio Astronomy Observatory

Solar System Objects. Bryan Butler National Radio Astronomy Observatory Solar System Objects Bryan Butler National Radio Astronomy Observatory Atacama Large Millimeter/submillimeter Array Expanded Very Large Array Robert C. Byrd Green Bank Telescope Very Long Baseline Array

More information

A strong magnetic field in the jet base of a supermassive black hole

A strong magnetic field in the jet base of a supermassive black hole A strong magnetic field in the jet base of a supermassive black hole arxiv:1604.01898v1 [astro-ph.he] 7 Apr 2016 Ivan Martí-Vidal, 1 Sébastien Muller, 1 Wouter Vlemmings, 1 Cathy Horellou, 1 Susanne Aalto

More information

Polarization in Interferometry

Polarization in Interferometry Polarization in Interferometry Rick Perley (NRAO-Socorro) Fourth INPE Advanced Course on Astrophysics: Radio Astronomy in the 21 st Century My Apologies, Up Front This lecture contains some difficult material.

More information

Polarimetry. Dave McConnell, CASS Radio Astronomy School, Narrabri 30 September kpc. 8.5 GHz B-vectors Perley & Carilli (1996)

Polarimetry. Dave McConnell, CASS Radio Astronomy School, Narrabri 30 September kpc. 8.5 GHz B-vectors Perley & Carilli (1996) VLA @ 8.5 GHz B-vectors Perley & Carilli (1996) 10 kpc Polarimetry Dave McConnell, CASS Radio Astronomy School, Narrabri 30 September 2010 1 Electro-magnetic waves are polarized E H S = c/4π (E H) S E/M

More information

On Calibration of ALMA s Solar Observations

On Calibration of ALMA s Solar Observations On Calibration of ALMA s Solar Observations M.A. Holdaway National Radio Astronomy Observatory 949 N. Cherry Ave. Tucson, AZ 85721-0655 email: mholdawa@nrao.edu January 4, 2007 Abstract 1 Introduction

More information

EVLA Memo 177 Polarimetric calibration and dynamic range issues

EVLA Memo 177 Polarimetric calibration and dynamic range issues EVLA Memo 177 Polarimetric calibration and dynamic range issues R.J. Sault, Rick Perley April 3, 2014 Introduction This memo considers some dynamic range issues resulting from limitations in the polarimetric

More information

Understanding radio polarimetry. III. Interpreting the IAU/IEEE definitions of the Stokes parameters

Understanding radio polarimetry. III. Interpreting the IAU/IEEE definitions of the Stokes parameters ASTRONOMY & ASTROPHYSICS MAY II 1996, PAGE 161 SUPPLEMENT SERIES Astron. Astrophys. Suppl. Ser. 117, 161-165 (1996) Understanding radio polarimetry. III. Interpreting the IAU/IEEE definitions of the Stokes

More information

Continuum and Line ALMA band 5: the supergiant VY CMa

Continuum and Line ALMA band 5: the supergiant VY CMa Continuum and Line Polarisation @ ALMA band 5: the supergiant VY CMa Wouter Vlemmings, Chalmers Univ. of Technology w. Theo Khouri, Daniel Tafoya, Ivan Marti-Vidal, Liz Humphreys, Anita Richards, Eamon

More information

Pseudocontinuum Polarimetry with the GBT Brian S. Mason v.1 31may07 v.2 03sep07. Abstract

Pseudocontinuum Polarimetry with the GBT Brian S. Mason v.1 31may07 v.2 03sep07. Abstract Pseudocontinuum Polarimetry with the GBT Brian S. Mason v.1 31may07 v.2 03sep07 Abstract We outline a simple method for calibrating correlation polarimetric data from the GBT spectrometer, and describe

More information

What is this radio interferometry business anyway? Basics of interferometry Calibration Imaging principles Detectability Using simulations

What is this radio interferometry business anyway? Basics of interferometry Calibration Imaging principles Detectability Using simulations What is this radio interferometry business anyway? Basics of interferometry Calibration Imaging principles Detectability Using simulations Interferometry Antenna locations Earth rotation aperture synthesis

More information

Polarimetry with Phased-Array Feeds

Polarimetry with Phased-Array Feeds Polarimetry with Phased-Array Feeds Bruce Veidt Dominion Radio Astrophysical Observatory Herzberg Institute of Astrophysics National Research Council of Canada Penticton, British Columbia, Canada Provo,

More information

Synthesis Polarimetry Fundamentals for ALMA. George Moellenbrock (NRAO) 2013 June 25 ALMA Italian ARC Node

Synthesis Polarimetry Fundamentals for ALMA. George Moellenbrock (NRAO) 2013 June 25 ALMA Italian ARC Node Synthesis Polarimetry Fundamentals for ALMA George Moellenbrock (NRAO) 2013 June 25 ALMA Italian ARC Node References Synthesis Imaging in Radio Astronomy II (1998 NRAO Summer School Book) Thompson, Moran,

More information

La vraie faute est celle qu on ne corrige pas Confucius

La vraie faute est celle qu on ne corrige pas Confucius La vraie faute est celle qu on ne corrige pas Confucius An introduction to optical/ir interferometry Brief summary of main results obtained during the last lecture: V = γ (0,u, v) = 12 S I '(ζ,η)exp{ i2π(

More information

Non-Closing Offsets on the VLA. R. C. Walker National Radio Astronomy Observatory Charlottesville VA.

Non-Closing Offsets on the VLA. R. C. Walker National Radio Astronomy Observatory Charlottesville VA. VLA SCIENTIFIC MEMORANDUM NO. 152 Non-Closing Offsets on the VLA R. C. Walker National Radio Astronomy Observatory Charlottesville VA. March 1984 Recent efforts to obtain very high dynamic range in VLA

More information

Interferometry of Solar System Objects

Interferometry of Solar System Objects Interferometry of Solar System Objects Bryan Butler National Radio Astronomy Observatory Atacama Large Millimeter/submillimeter Array Expanded Very Large Array Robert C. Byrd Green Bank Telescope Very

More information

The Source and Lens of B

The Source and Lens of B The Source and Lens of B0218+357 New Polarization Radio Data to Constrain the Source Structure and H 0 with LensCLEAN Olaf Wucknitz Astrophysics Seminar Potsdam University, Germany 5 July 2004 The source

More information

SKA polarimetry specication

SKA polarimetry specication specication Does the SKA really need to achieve its high polarimetric purity (and sensitivity) spec? Onsala Space Observatory Chalmers University, Sweden AAVP workshop, Cambridge, 8 Dec 2010 SKA Polarimetry

More information

J.-C. Zhang, Y.-Z. Yin, and J.-P. Ma National Laboratory of Antennas and Microwave Technology Xidian University Xi an, Shaanxi , P. R.

J.-C. Zhang, Y.-Z. Yin, and J.-P. Ma National Laboratory of Antennas and Microwave Technology Xidian University Xi an, Shaanxi , P. R. Progress In Electromagnetics Research Letters, Vol. 6, 55 60, 2009 MULTIFUNCTIONAL MEANDER LINE POLARIZER J.-C. Zhang, Y.-Z. Yin, and J.-P. Ma National Laboratory of Antennas and Microwave Technology Xidian

More information

Imaging the Sun with The Murchison Widefield Array

Imaging the Sun with The Murchison Widefield Array Imaging the Sun with The Murchison Widefield Array Divya Oberoi 1,2, Lynn D. Matthews 2, Leonid Benkevitch 2 and the MWA Collaboration 1 National Centre for Radio Astrophysics, Tata Institute for Fundamental

More information

Introduction to Interferometry

Introduction to Interferometry Introduction to Interferometry Ciro Pappalardo RadioNet has received funding from the European Union s Horizon 2020 research and innovation programme under grant agreement No 730562 Radioastronomy H.Hertz

More information

Atmospheric phase correction for ALMA with water-vapour radiometers

Atmospheric phase correction for ALMA with water-vapour radiometers Atmospheric phase correction for ALMA with water-vapour radiometers B. Nikolic Cavendish Laboratory, University of Cambridge January 29 NA URSI, Boulder, CO B. Nikolic (University of Cambridge) WVR phase

More information

Lecture 8: Polarimetry 2. Polarizers and Retarders. Polarimeters. Scattering Polarization. Zeeman Effect. Outline

Lecture 8: Polarimetry 2. Polarizers and Retarders. Polarimeters. Scattering Polarization. Zeeman Effect. Outline Lecture 8: Polarimetry 2 Outline 1 Polarizers and Retarders 2 Polarimeters 3 Scattering Polarization 4 Zeeman Effect Christoph U. Keller, Utrecht University, C.U.Keller@uu.nl Observational Astrophysics

More information

Deconvolving Primary Beam Patterns from SKA Images

Deconvolving Primary Beam Patterns from SKA Images SKA memo 103, 14 aug 2008 Deconvolving Primary Beam Patterns from SKA Images Melvyn Wright & Stuartt Corder University of California, Berkeley, & Caltech, Pasadena, CA. ABSTRACT In this memo we present

More information

Brewster Angle and Total Internal Reflection

Brewster Angle and Total Internal Reflection Lecture 5: Polarization Outline 1 Polarized Light in the Universe 2 Brewster Angle and Total Internal Reflection 3 Descriptions of Polarized Light 4 Polarizers 5 Retarders Christoph U. Keller, Leiden University,

More information

A Crash Course in Radio Astronomy and Interferometry: 2. Aperture Synthesis

A Crash Course in Radio Astronomy and Interferometry: 2. Aperture Synthesis A Crash Course in Radio Astronomy and Interferometry: 2. Aperture Synthesis James Di Francesco National Research Council of Canada North American ALMA Regional Center Victoria (thanks to S. Dougherty,

More information

Lecture 5: Polarization. Polarized Light in the Universe. Descriptions of Polarized Light. Polarizers. Retarders. Outline

Lecture 5: Polarization. Polarized Light in the Universe. Descriptions of Polarized Light. Polarizers. Retarders. Outline Lecture 5: Polarization Outline 1 Polarized Light in the Universe 2 Descriptions of Polarized Light 3 Polarizers 4 Retarders Christoph U. Keller, Leiden University, keller@strw.leidenuniv.nl ATI 2016,

More information

Two Posts to Fill On School Board

Two Posts to Fill On School Board Y Y 9 86 4 4 qz 86 x : ( ) z 7 854 Y x 4 z z x x 4 87 88 Y 5 x q x 8 Y 8 x x : 6 ; : 5 x ; 4 ( z ; ( ) ) x ; z 94 ; x 3 3 3 5 94 ; ; ; ; 3 x : 5 89 q ; ; x ; x ; ; x : ; ; ; ; ; ; 87 47% : () : / : 83

More information

Millimeter Antenna Calibration

Millimeter Antenna Calibration Millimeter Antenna Calibration 9 th IRAM Millimeter Interferometry School 10-14 October 2016 Michael Bremer, IRAM Grenoble The beam (or: where does an antenna look?) How and where to build a mm telescope

More information

Typical anisotropies introduced by geometry (not everything is spherically symmetric) temperature gradients magnetic fields electrical fields

Typical anisotropies introduced by geometry (not everything is spherically symmetric) temperature gradients magnetic fields electrical fields Lecture 6: Polarimetry 1 Outline 1 Polarized Light in the Universe 2 Fundamentals of Polarized Light 3 Descriptions of Polarized Light Polarized Light in the Universe Polarization indicates anisotropy

More information

Introduction to Radio Interferometry Jim Braatz (NRAO)

Introduction to Radio Interferometry Jim Braatz (NRAO) Introduction to Radio Interferometry Jim Braatz (NRAO) Atacama Large Millimeter/submillimeter Array Expanded Very Large Array Robert C. Byrd Green Bank Telescope Very Long Baseline Array Radio Astronomy

More information

CROSSCORRELATION SPECTROPOLARIMETRY IN SINGLE-DISH RADIO ASTRONOMY

CROSSCORRELATION SPECTROPOLARIMETRY IN SINGLE-DISH RADIO ASTRONOMY CROSSCORRELATION SPECTROPOLARIMETRY IN SINGLE-DISH RADIO ASTRONOMY Carl Heiles Astronomy Department, University of California, Berkeley, CA 94720-3411; cheiles@astron.berkeley.edu ABSTRACT Modern digital

More information

ALMA Memo 599. The ALMA Calibrator Database I: Measurements taken during the commissioning phase of ALMA

ALMA Memo 599. The ALMA Calibrator Database I: Measurements taken during the commissioning phase of ALMA ALMA Memo 599 The ALMA Calibrator Database I: Measurements taken during the commissioning phase of ALMA T.A. van Kempen 1,2, R. Kneissl 1, N. Marcelino 3, E.B. Fomalont 3,1, D. Barkats 1, S.A. Corder 1,3,

More information

Solar Observation using ALMA

Solar Observation using ALMA Solar Observation using ALMA Sujin Kim ALMA EA Korean Node, KASI Content Science Target Cycle4 selection statistics: Sun Capability for Cycle5 Science Verification(SV) data - Single-dish observation -

More information

Radio Astronomy Project. VLA and VLBA Observations of AGN

Radio Astronomy Project. VLA and VLBA Observations of AGN Astronomy-423: Radio Astronomy Professor: Greg Taylor Spring 2006 Radio Astronomy Project VLA and VLBA Observations of AGN Adam Johnson Cristina Rodríguez Introduction It is important to observe radio

More information

ASKAP. and phased array feeds in astronomy. David McConnell CASS: ASKAP Commissioning and Early Science 16 November 2017

ASKAP. and phased array feeds in astronomy. David McConnell CASS: ASKAP Commissioning and Early Science 16 November 2017 ASKAP and phased array feeds in astronomy David McConnell CASS: ASKAP Commissioning and Early Science 16 November 2017 Image credit: Alex Cherney / terrastro.com 1 Credits ASKAP Commissioning & Early Science

More information

The data model. Panos Labropoulos. Kapteyn Instituut

The data model. Panos Labropoulos. Kapteyn Instituut The data model Panos Labropoulos " Challenges The actual 21-cm signal is several times weaker than the foregrounds and sits below the telescope noise Foregrounds: galactic and extragalactic (polarization?)

More information

Radio Interferometry and Aperture Synthesis

Radio Interferometry and Aperture Synthesis Radio Interferometry and Aperture Synthesis Phil gave a detailed picture of homodyne interferometry Have to combine the light beams physically for interference Imposes many stringent conditions on the

More information

17. Jones Matrices & Mueller Matrices

17. Jones Matrices & Mueller Matrices 7. Jones Matrices & Mueller Matrices Jones Matrices Rotation of coordinates - the rotation matrix Stokes Parameters and unpolarized light Mueller Matrices R. Clark Jones (96-24) Sir George G. Stokes (89-93)

More information

EHT data set validation and characterization of errors

EHT data set validation and characterization of errors Event Horizon Telescope Memo Series EHT Memo 219-CE-2 Calibration & Error Analysis WG EHT data set validation and characterization of errors M. Wielgus 1,2,, L. Blackburn 1, S. Issaoun 3, M. Janssen 3,

More information

On the Calibration of Full-polarization 86 GHz Global VLBI Observations

On the Calibration of Full-polarization 86 GHz Global VLBI Observations Astronomy & Astrophysics manuscript no. paper-gmva-v12 c ESO 212 October 16, 212 On the Calibration of Full-polarization 86 GHz Global VLBI Observations I. Martí-Vidal 1,2, T.P. Krichbaum 1, A. Marscher

More information

Radio Interferometry Fundamentals. John Conway Onsala Space Obs and Nordic ALMA ARC-node

Radio Interferometry Fundamentals. John Conway Onsala Space Obs and Nordic ALMA ARC-node Radio Interferometry Fundamentals John Conway Onsala Space Obs and Nordic ALMA ARC-node So far discussed only single dish radio/mm obs Resolution λ/d, for D=20m, is 30 at mm-wavelengths and 30 (diameter

More information

HERA Memo 51: System Noise from LST Di erencing March 17, 2017

HERA Memo 51: System Noise from LST Di erencing March 17, 2017 HERA Memo 51: System Noise from LST Di erencing March 17, 2017 C.L. Carilli 1,2 ccarilli@aoc.nrao.edu ABSTRACT I derive the visibility noise values (in Jy), and the system temperature for HERA, using di

More information

Behaviour of synchronous machine during a short-circuit (a simple example of electromagnetic transients)

Behaviour of synchronous machine during a short-circuit (a simple example of electromagnetic transients) ELEC0047 - Power system dynamics, control and stability (a simple example of electromagnetic transients) Thierry Van Cutsem t.vancutsem@ulg.ac.be www.montefiore.ulg.ac.be/~vct October 2018 1 / 25 Objectives

More information

OWELL WEEKLY JOURNAL

OWELL WEEKLY JOURNAL Y \»< - } Y Y Y & #»»» q ] q»»»>) & - - - } ) x ( - { Y» & ( x - (» & )< - Y X - & Q Q» 3 - x Q Y 6 \Y > Y Y X 3 3-9 33 x - - / - -»- --

More information

ALMA Memo 330 The overlap of the astronomical and WVR beams

ALMA Memo 330 The overlap of the astronomical and WVR beams ALMA Memo 330 The overlap of the astronomical and WVR beams A.G. Gibb and A.I. Harris Department of Astronomy, University of Maryland (agg@astro.umd.edu, harris@astro.umd.edu) October 24, 2000 Abstract

More information

Polarimetry in the E-ELT era. Polarized Light in the Universe. Descriptions of Polarized Light. Polarizers. Retarders. Fundamentals of Polarized Light

Polarimetry in the E-ELT era. Polarized Light in the Universe. Descriptions of Polarized Light. Polarizers. Retarders. Fundamentals of Polarized Light Polarimetry in the E-ELT era Fundamentals of Polarized Light 1 Polarized Light in the Universe 2 Descriptions of Polarized Light 3 Polarizers 4 Retarders Christoph U. Keller, Leiden University, keller@strw.leidenuniv.nl

More information

(A) (B) (C) (D) (E) (F) Figure 1: Graphs of functions from Question 1. Answer Positive: C, D; zero: B, E; negative: A, F. :)

(A) (B) (C) (D) (E) (F) Figure 1: Graphs of functions from Question 1. Answer Positive: C, D; zero: B, E; negative: A, F. :) Question ( marks) Each of the six diagrams in Figure represents the graph of some function of two variables whose second partial derivatives are continuous on R. Diagrams show the graphs in a neighbourhood

More information

PROOF-OF-CONCEPT DEMONSTRATION OF A MILLIMETRE WAVE IMAGING SOUNDER FOR GEOSTATIONARY EARTH ORBIT

PROOF-OF-CONCEPT DEMONSTRATION OF A MILLIMETRE WAVE IMAGING SOUNDER FOR GEOSTATIONARY EARTH ORBIT PROOF-OF-CONCEPT DEMONSTRATION OF A MILLIMETRE WAVE IMAGING SOUNDER FOR GEOSTATIONARY EARTH ORBIT Anders Carlström 1, Jacob Christensen 1, Anders Emrich 2, Johan Embretsén 2, Karl-Erik Kempe 2, and Peter

More information

14.7: Maxima and Minima

14.7: Maxima and Minima 14.7: Maxima and Minima Marius Ionescu October 29, 2012 Marius Ionescu () 14.7: Maxima and Minima October 29, 2012 1 / 13 Local Maximum and Local Minimum Denition Marius Ionescu () 14.7: Maxima and Minima

More information

Non-Imaging Data Analysis

Non-Imaging Data Analysis Outline 2 Non-Imaging Data Analysis Greg Taylor Based on the original lecture by T.J. Pearson Introduction Inspecting visibility data Model fitting Some applications Superluminal motion Gamma-ray bursts

More information

County Council Named for Kent

County Council Named for Kent \ Y Y 8 9 69 6» > 69 ««] 6 : 8 «V z 9 8 x 9 8 8 8?? 9 V q» :: q;; 8 x () «; 8 x ( z x 9 7 ; x >«\ 8 8 ; 7 z x [ q z «z : > ; ; ; ( 76 x ; x z «7 8 z ; 89 9 z > q _ x 9 : ; 6? ; ( 9 [ ) 89 _ ;»» «; x V

More information

Recap Lecture + Thomson Scattering. Thermal radiation Blackbody radiation Bremsstrahlung radiation

Recap Lecture + Thomson Scattering. Thermal radiation Blackbody radiation Bremsstrahlung radiation Recap Lecture + Thomson Scattering Thermal radiation Blackbody radiation Bremsstrahlung radiation LECTURE 1: Constancy of Brightness in Free Space We use now energy conservation: de=i ν 1 da1 d Ω1 dt d

More information

arxiv: v1 [astro-ph.co] 4 Dec 2010

arxiv: v1 [astro-ph.co] 4 Dec 2010 Spectropolarimetry with the Allen Telescope Array: Faraday Rotation toward Bright Polarized Radio Galaxies arxiv:1012.0945v1 [astro-ph.co] 4 Dec 2010 C. J. Law 1, B. M. Gaensler 2, G. C. Bower 1, D. C.

More information

Multi-frequency polarimetry of a complete sample of faint PACO sources. INAF-IRA (Bologna)

Multi-frequency polarimetry of a complete sample of faint PACO sources. INAF-IRA (Bologna) Multi-frequency polarimetry of a complete sample of faint PACO sources. Vincenzo Galluzzi Marcella Massardi DiFA (University of Bologna) INAF-IRA (Bologna) INAF-IRA & Italian ARC The state-of-the-art The

More information

Tracking Solar Eruptions to Their Impact on Earth Carl Luetzelschwab K9LA September 2016 Bonus

Tracking Solar Eruptions to Their Impact on Earth Carl Luetzelschwab K9LA September 2016 Bonus Tracking Solar Eruptions to Their Impact on Earth Carl Luetzelschwab K9LA September 2016 Bonus In June 2015, the Sun emitted several M-Class flares over a 2-day period. These flares were concurrent with

More information

Brewster Angle and Total Internal Reflection

Brewster Angle and Total Internal Reflection Lecture 4: Polarization Outline 1 Polarized Light in the Universe 2 Brewster Angle and Total Internal Reflection 3 Descriptions of Polarized Light 4 Polarizers 5 Retarders Christoph U. Keller, Utrecht

More information

LONG-TERM TRENDS IN THE AMOUNT OF ATMOSPHERIC WATER VAPOUR DERIVED FROM SPACE GEODETIC AND REMOTE SENSING TECHNIQUES

LONG-TERM TRENDS IN THE AMOUNT OF ATMOSPHERIC WATER VAPOUR DERIVED FROM SPACE GEODETIC AND REMOTE SENSING TECHNIQUES LONG-TERM TRENDS IN THE AMOUNT OF ATMOSPHERIC WATER VAPOUR DERIVED FROM SPACE GEODETIC AND REMOTE SENSING TECHNIQUES Rüdiger Haas, Tong Ning, and Gunnar Elgered Chalmers University of Technology, Onsala

More information

Outline. Mm-Wave Interferometry. Why do we care about mm/submm? Star-forming galaxies in the early universe. Dust emission in our Galaxy

Outline. Mm-Wave Interferometry. Why do we care about mm/submm? Star-forming galaxies in the early universe. Dust emission in our Galaxy Outline 2 Mm-Wave Interferometry Debra Shepherd & Claire Chandler Why a special lecture on mm interferometry? Everything about interferometry is more difficult at high frequencies Some problems are unique

More information

ANALYSIS OF LIMB BRIGHTENING ON THE QUIET SUN AT 21 CM USING A THREE-ELEMENT INTERFEROMETER

ANALYSIS OF LIMB BRIGHTENING ON THE QUIET SUN AT 21 CM USING A THREE-ELEMENT INTERFEROMETER ANALYSIS OF LIMB BRIGHTENING ON THE QUIET SUN AT 21 CM USING A THREE-ELEMENT INTERFEROMETER Jonathon Oiler Alan E.E. Rogers MIT Haystack Observatory ABSTRACT During the summer, three small radio telescopes

More information

Probing into the shadow of the galactic center black hole with sub-millimeter VLBI

Probing into the shadow of the galactic center black hole with sub-millimeter VLBI Probing into the shadow of the galactic center black hole with sub-millimeter VLBI Zhi-Qiang Shen (Shanghai Astronomical Observatory) In collaboration with: L. Huang, M. Cai, F. Yuan, S.-M. Liu K. Y. Lo,

More information

BROWN UNIVERSITY PROBLEM SET 4 INSTRUCTOR: SAMUEL S. WATSON DUE: 6 OCTOBER 2017

BROWN UNIVERSITY PROBLEM SET 4 INSTRUCTOR: SAMUEL S. WATSON DUE: 6 OCTOBER 2017 BROWN UNIVERSITY PROBLEM SET 4 INSTRUCTOR: SAMUEL S. WATSON DUE: 6 OCTOBER 2017 Print out these pages, including the additional space at the end, and complete the problems by hand. Then use Gradescope

More information

Optical interferometry: problems and practice

Optical interferometry: problems and practice Outline Optical interferometry: problems and practice Chris Haniff Aims. What is an interferometer? Fundamental differences between optical and radio. Implementation at optical wavelengths. Conclusions.

More information

Circular polarization in comets: calibration of measurements

Circular polarization in comets: calibration of measurements Circular polarization in comets: calibration of measurements Vera Rosenbush, Nikolai Kiselev Main Astronomical Observatory of the National Academy of Sciences of Ukraine, rosevera@mao.kiev.ua Kyiv 1 Outline

More information

measuring polariza/on with CARMA (currently possible only in the 1mm band)

measuring polariza/on with CARMA (currently possible only in the 1mm band) measuring polariza/on with CARMA (currently possible only in the 1mm band) mode measure benefits correlator LL most flexible correlator setup RR NONE! (Tsys is slightly higher for RCP rcvrs)

More information

Planning an interferometer observation

Planning an interferometer observation 2nd ERIS, Bonn, September 2007 Planning an interferometer observation T. Venturi Istituto di Radioastronomia, Bologna, INAF tventuri@ira.inaf.it Outline I. Planning an experiment/preparing a proposal II.

More information

III. Spherical Waves and Radiation

III. Spherical Waves and Radiation III. Spherical Waves and Radiation Antennas radiate spherical waves into free space Receiving antennas, reciprocity, path gain and path loss Noise as a limit to reception Ray model for antennas above a

More information

Lecture 4: Polarimetry 2. Polarizers and Retarders. Polarimeters. Scattering Polarization. Zeeman Effect. Outline

Lecture 4: Polarimetry 2. Polarizers and Retarders. Polarimeters. Scattering Polarization. Zeeman Effect. Outline Lecture 4: Polarimetry 2 Outline 1 Polarizers and Retarders 2 Polarimeters 3 Scattering Polarization 4 Zeeman Effect Christoph U. Keller, Utrecht University, C.U.Keller@uu.nl Observational Astrophysics

More information

ALMA Memo 373 Relative Pointing Sensitivity at 30 and 90 GHz for the ALMA Test Interferometer M.A. Holdaway and Jeff Mangum National Radio Astronomy O

ALMA Memo 373 Relative Pointing Sensitivity at 30 and 90 GHz for the ALMA Test Interferometer M.A. Holdaway and Jeff Mangum National Radio Astronomy O ALMA Memo 373 Relative Pointing Sensitivity at 30 and 90 GHz for the ALMA Test Interferometer M.A. Holdaway and Jeff Mangum National Radio Astronomy Observatory 949 N. Cherry Ave. Tucson, AZ 85721-0655

More information

Massachusetts Institute of Technology Physics 8.03 Fall 2004 Final Exam Thursday, December 16, 2004

Massachusetts Institute of Technology Physics 8.03 Fall 2004 Final Exam Thursday, December 16, 2004 You have 3 hours Do all eight problems You may use calculators Massachusetts Institute of Technology Physics 8.03 Fall 004 Final Exam Thursday, December 16, 004 This is a closed-book exam; no notes are

More information

Properties of surfaces II: Second moment of area

Properties of surfaces II: Second moment of area Properties of surfaces II: Second moment of area Just as we have discussing first moment of an area and its relation with problems in mechanics, we will now describe second moment and product of area of

More information

ECE 6341 Spring 2016 HW 2

ECE 6341 Spring 2016 HW 2 ECE 6341 Spring 216 HW 2 Assigned problems: 1-6 9-11 13-15 1) Assume that a TEN models a layered structure where the direction (the direction perpendicular to the layers) is the direction that the transmission

More information

Multi-Frequency VLBI Telescopes & Synergy with ALMA Taehyun Jung

Multi-Frequency VLBI Telescopes & Synergy with ALMA Taehyun Jung Multi-Frequency VLBI Telescopes & Synergy with ALMA Taehyun Jung Korean VLBI Network (KVN) Korea Astronomy & Space Science Institute (KASI) Workshop on mm-vlbi with ALMA @ Istituto di Radioastronomia Bologna,

More information

ASKAP Commissioning Update #7 April-July Latest results from the BETA test array

ASKAP Commissioning Update #7 April-July Latest results from the BETA test array ASKAP Commissioning Update #7 April-July 2014 Welcome to the seventh edition of the ASKAP Commissioning Update. This includes all the latest results from commissioning of the six-antenna Boolardy Engineering

More information

Band 4 & 8 Imaging Verification Test Report: 30 May 2014

Band 4 & 8 Imaging Verification Test Report: 30 May 2014 Band 4 & 8 Imaging Verification Test Report: 30 May 2014 ALMA Technical Note Number: 3 Status: FINAL Prepared by: Organization: Date: Takahashi Satoko JAO/NAOJ 30 May 2014 Band 4 Imaging Verification Report

More information

SPACE TELESCOPE SCIENCE INSTITUTE. ACS Polarization Calibration: Introduction and Progress Report

SPACE TELESCOPE SCIENCE INSTITUTE. ACS Polarization Calibration: Introduction and Progress Report 1 ACS Polarization Calibration: Introduction and Progress Report J. Biretta, V. Platais, F. Boffi, W. Sparks, J. Walsh Introduction: Theory / ACS Polarizers / Supported Modes Potential Issues for ACS Polarization

More information

Keck Instrument Technical Note KITN: 0004 Page 1 of 9

Keck Instrument Technical Note KITN: 0004 Page 1 of 9 KITN: 0004 Page 1 of 9 LRIS: Polarimetry with the ADC The use of the ADC (Atmospheric Dispersion Compensator) with LRIS may have some effect on polarization measurements with the LRISp polarimetry module.

More information

SMOS L1 Sun BT Valida0on against on-ground radio-telescope network

SMOS L1 Sun BT Valida0on against on-ground radio-telescope network SMOS L1 Sun BT Valida0on against on-ground radio-telescope network Daniele Casella 1, Raffaele Crapolicchio 1;2, Nicola Compare7 1, Christophe Marqué 3 1 Serco 2 ESA-ESRIN 3 Royal Observatory of Belgium

More information

SOLUTIONS FOR PROBLEMS 1-30

SOLUTIONS FOR PROBLEMS 1-30 . Answer: 5 Evaluate x x + 9 for x SOLUTIONS FOR PROBLEMS - 0 When substituting x in x be sure to do the exponent before the multiplication by to get (). + 9 5 + When multiplying ( ) so that ( 7) ( ).

More information

EVLA Memo 207 Implementing Polarimetry with the JVLA s Low-Band Receivers

EVLA Memo 207 Implementing Polarimetry with the JVLA s Low-Band Receivers EVLA Memo 27 Implementing Polarimetry with the JVLA s Low-Band Receivers Rick Perley and Eric Greisen National Radio Astronomy Observatory, Socorro, NM April 11, 219 Abstract The JVLA s low-frequency receivers

More information

Quadratic Equations 6 QUESTIONS. Relatively Easy: Questions 1 to 2 Moderately Difficult: Questions 3 to 4 Difficult: Questions 5 to 6

Quadratic Equations 6 QUESTIONS. Relatively Easy: Questions 1 to 2 Moderately Difficult: Questions 3 to 4 Difficult: Questions 5 to 6 Quadratic Equations 6 QUESTIONS Relatively Easy: Questions 1 to 2 Moderately Difficult: Questions 3 to 4 Difficult: Questions 5 to 6 Questions www.tutornext.com Page 2 of 11 Q1. The factors of 2x² - 7x

More information

arxiv: v2 [astro-ph.sr] 18 Apr 2015

arxiv: v2 [astro-ph.sr] 18 Apr 2015 Astronomy& Astrophysics manuscript no. Vlemmings_Mira c ESO 215 April 21, 215 Letter to the Editor Resolving the stellar activity of the Mira AB binary with ALMA W. H. T. Vlemmings 1,, S. Ramstedt 2, E.

More information

LOFAR Polarization Commissioning by the MKSP

LOFAR Polarization Commissioning by the MKSP LOFAR Polarization Commissioning by the MKSP James M Anderson anderson@mpifr-bonn.mpg.de On behalf of the LOFAR collaboration Surveys KSP Meeting, Leiden, 2010 March 11 James M Anderson 1/15 Timeline 2010

More information

Exam 3 November 19, 2012 Instructor: Timothy Martin

Exam 3 November 19, 2012 Instructor: Timothy Martin PHY 232 Exam 3 October 15, 2012 Exam 3 November 19, 2012 Instructor: Timothy Martin Student Information Name and section: UK Student ID: Seat #: Instructions Answer the questions in the space provided.

More information

Binary stars in loose associations: AB Dor B and HD

Binary stars in loose associations: AB Dor B and HD Highlights of Spanish Astrophysics VIII, Proceedings of the XI Scientific Meeting of the Spanish Astronomical Society held on September 8 12, 2014, in Teruel, Spain. A. J. Cenarro, F. Figueras, C. Hernández-

More information

Optical interferometry a gentle introduction to the theory

Optical interferometry a gentle introduction to the theory Optical interferometry a gentle introduction to the theory Chris Haniff Astrophysics Group, Cavendish Laboratory, Madingley Road, Cambridge, CB3 0HE, UK Motivation A Uninterested: I m here for the holiday.

More information

Introduction. Name: Basic Features of Sunspots. The Solar Rotational Period. Sunspot Numbers

Introduction. Name: Basic Features of Sunspots. The Solar Rotational Period. Sunspot Numbers PHYS-1050 Tracking Sunspots Spring 2013 Name: 1 Introduction Sunspots are regions on the solar surface that appear dark because they are cooler than the surrounding photosphere, typically by about 1500

More information

Model based forest height estimation with ALOS/PalSAR: A first study.

Model based forest height estimation with ALOS/PalSAR: A first study. Model based forest height estimation with ALOS/PalSAR: A first study. K.P. Papathanassiou*, I. Hajnsek*, T.Mette*, S.R. Cloude** and A. Moreira* * (DLR) (DLR-HR) Oberpfaffenhofen, Germany ** AEL Consultants

More information

Foregrounds for observations of the high redshift global 21 cm signal

Foregrounds for observations of the high redshift global 21 cm signal Foregrounds for observations of the high redshift global 21 cm signal Geraint Harker 28/10/2010 Fall Postdoc Symposium 1 The hydrogen 21cm line The hydrogen 21cm (1420MHz) transition is a forbidden transition

More information

' '-'in.-i 1 'iritt in \ rrivfi pr' 1 p. ru

' '-'in.-i 1 'iritt in \ rrivfi pr' 1 p. ru V X X Y Y 7 VY Y Y F # < F V 6 7»< V q q $ $» q & V 7» Q F Y Q 6 Q Y F & Q &» & V V» Y V Y [ & Y V» & VV & F > V } & F Q \ Q \» Y / 7 F F V 7 7 x» > QX < #» > X >» < F & V F» > > # < q V 6 & Y Y q < &

More information

An introduction to closure phases

An introduction to closure phases An introduction to closure phases Michelson Summer Workshop Frontiers of Interferometry: Stars, disks, terrestrial planets Pasadena, USA, July 24 th -28 th 2006 C.A.Haniff Astrophysics Group, Department

More information

A Data Exchange Standard for Optical (Visible/IR) Interferometry

A Data Exchange Standard for Optical (Visible/IR) Interferometry Release 5 (1 st production release) A Data Exchange Standard for Optical (Visible/IR) Interferometry Prepared by NPOI and COAST First Version: 10 January 2001 Last Update: 7 April 2003 1 Introduction Considering

More information

MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 6 C) - 12 (6x - 7)3

MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 6 C) - 12 (6x - 7)3 Part B- Pre-Test 2 for Cal (2.4, 2.5, 2.6) Test 2 will be on Oct 4th, chapter 2 (except 2.6) Name MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.

More information

The science of light. P. Ewart

The science of light. P. Ewart The science of light P. Ewart Oxford Physics: Second Year, Optics Parallel reflecting surfaces t images source Extended source path difference xcos 2t=x Fringes localized at infinity Circular fringe constant

More information