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Chen, Yi-Ping Supervisor: Hirano, Naomi 12 CO J=2-1 Observation Of M51 With SMA Physical Department of Tamkang University August,27, 2002 Summer Student.

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Presentation on theme: "Chen, Yi-Ping Supervisor: Hirano, Naomi 12 CO J=2-1 Observation Of M51 With SMA Physical Department of Tamkang University August,27, 2002 Summer Student."— Presentation transcript:

1 Chen, Yi-Ping Supervisor: Hirano, Naomi 12 CO J=2-1 Observation Of M51 With SMA Physical Department of Tamkang University August,27, 2002 Summer Student Program,Institute of Astronomy and Astrophysics, Academia Sinica

2 Introduction Galaxy M51 SMA C 12 O Emission J=2-1 Data Reduction Analysis Data

3 Galaxy M51 Position (J2000): R.A. 13h 29m 52.37s Dec. +47°11' 40.8" Constellation: Canes Venatici Distance:About 9.6 Mpc Visual Magnitude:8.4 http://oposite.stsci.edu/pubinfo/PR/2001/10/index.html 3arcmin 9.3 kpc 1acrmin 50 arcsec (Field of view)

4 Sub-Millimeter Array Antenna: 5 Diameter:6-meter Covering bands :230 - 350 GHz Position: Summit of Mauna Kea, Hawaii http://www.asiaa.sinica.edu.tw/Research/SMART/index.html

5 OC Because of CO molecule has a permanent dipole moment,the binary molecule with a simples ladder of rotational level spaced such that the lowest transition are in the millimeter wavelength. 12 CO Emission J=2-1

6 J is the quantum number of total angular momentum correspond to the rotational level. Frequency : 230.538 GHz Energy : 16.6 Κ (upper level above ground) J=0 J=1 J=2 h ν= E 2 -E 1 h ν =E 1 -E 0

7 Observation Observation date : 2002 Feb 17,18 Telescope : SMA 6m(diameter)×5(antenna) 10 baseline Field of view : 50’’ @230 GH Z Bandwidth : 320 MH Z ~ 417.39 km/s((82 MH Z ~106.7 km/s)× 4) Spectral resolution : 812.5 KH Z ~1.06 km/s Gain calibrator : 1310 + 323 Band pass calibrator : Jupiter

8 Data Reduction Why using the Gain Calibration? Phase Amplitude t t Due to the instrument instability and atmosphere variation, it is necessary to do the gain calibration, and the better calibrator is quasar because it’s has a simple visibility function. V(u,v)=∫ ∞ - ∞ ∫ ∞ - ∞ A(x,y) I(x,y)e i2(ux+vy) dxdy 0 0 constant

9 I. Gain Calibraiton Before Gain Calibration Blue *-- (1310+323) Red *-- NGC5194 Row data

10 Blue--NGC5194 Red-- Cailbrator (1310+323) Set amplitude—1Jy

11 After Gain Calibration After calibration the phase is becoming zero(blue)&M51 drift like function.

12 II.Band Pass Calibration In the SMA Aarry each channel have four chunks Before band Pass Calibration

13 1chunk=82MHZ ≒ 106.7 km/s 1channel =4×chunk ≒ 320MHZ ≒ 417.39 Calibrator : Jupiter This calibrator must be strong enough that can clear display each of the chuck’s pattern. After Calibration Jupiter’s Spectra Spectra

14 After band Pass Calibration

15 Analysis Data -- Make Maps UV Coverage Beam Map Dirty Map(obtained from the inversion visibility function) Obtained by convolving the δ-function Clean Map UV plane FFT XY plane (Visibility function)

16 UV Coverage Beam map UV coverage

17 Dirty Map(Feb 18,chunk 2) Clean Map(Feb 18,chunk 2) Major axis = 4.584 +/- 0.4904 asec Minor axis = 3.651 +/- 0.3906 asec Position angle = 93.787 +/- 18.892 degrees Synthesize beam Beam map

18 Combine Map Total integration intensity V LSR =374.57~574.34 km/s V LSR = 479.2~574.3 km/s V LSR =374~480.7 km/s

19 Contour Map Due to the sigh of phase is flipped the map must rotate 180°

20 12 CO J=1-0 HCN J=1-0 ©The Astrophysical Journal,461:L29-L32,1996 April 10

21 Compare 12 CO J=2-1 & 12 CO J=1-0

22 Compare HCN J=1-0 &C 12 O J=2-1


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