2021RAA....21...92S


Query : 2021RAA....21...92S

2021RAA....21...92S - Research in Astron. and astroph., 21, 92-92 (2021/April-0)

Precision of the Chinese Space Station Telescope (CSST) stellar radial velocities.

SUN Y., DENG D.-S. and YUAN H.-B.

Abstract (from CDS):

The Chinese Space Station Telescope (CSST) spectroscopic survey plans to deliver high-quality low-resolution (R > 200) slitless spectra for hundreds of millions of targets down to a limiting magnitude of about 21 mag, covering a large survey area (17 500 deg2) and a wide wavelength range (255-1000 nm by three bands GU, GV, and GI). In this work, we use empirical spectra of the Next Generation Spectral Library to simulate the CSST stellar spectra at R = 250, and investigate their capabilities in measuring radial velocities. We find that velocity uncertainties depend strongly on effective temperature, weakly on metallicity for only FGK stars, and hardly on surface gravity. It is possible to deliver stellar radial velocities to a precision of about 3 km s–1 for AFGKM stars, and about 10 km s–1 for OB stars, at signal-to-noise ratio (SNR) of 100. Velocity uncertainties using single GU/GV/GI band spectra are also explored. Given the same SNR, the GU band performs best, the GV band the second best, and then the GI band. The effects of spectral normalization and the imperfect template on velocity measurements are investigated and found to be very weak. The uncertainties caused by wavelength calibration are considered and found to be moderate. Given the possible precision of radial velocities, the CSST spectroscopic survey can enable interesting science such as searching for hyper-velocity stars. Limitations of our results are also discussed.

Abstract Copyright: © 2021 National Astronomical Observatories

Journal keyword(s): methods: data analysis - methods: statistical - stars: fundamental parameters - stars: kinematics and dynamics

Simbad objects: 17

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Number of rows : 17
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 HD 3793 PM* 00 40 27.8152609200 -14 03 40.201680348   9.89 9.40     F6V 5 0
2 HD 5256 PM* 01 05 41.5471334541 +87 19 08.356123039       8.3   G5 49 0
3 HD 8737 PM* 01 26 41.0979503064 +27 32 59.142229008   9.21 8.12     K0 4 0
4 G 272-61B PM* 01 39 01.6377185550 -17 57 01.001240728           M6V 892 0
5 HD 12146 PM* 01 58 29.5298561472 -33 25 09.867058140   9.91 9.28     G3V 14 0
6 V* VX Ari PM* 02 44 15.5097410539 +25 31 24.114854200 13.363 12.141 10.563 9.49 8.115 dM3 249 0
7 HD 20137 * 03 14 46.0617736128 +18 01 42.967343532   9.28 8.94     F 12 0
8 * 10 Tau PM* 03 36 52.3837044168 +00 24 05.992097829 5.23 5.15 4.30 4.09 3.77 F9IV-V 595 0
9 * tau CMa SB* 07 18 42.4849951654 -24 57 15.700749738 3.26 4.25 4.40 4.44 4.62 O9II 439 0
10 HD 95241 SB* 11 00 20.6841801504 +42 54 42.127624548       5.7   F9V 114 0
11 CD-69 1618 * 17 12 32.8978719504 -70 05 08.573209944 8.4 9.19 9.32     B2p 60 0
12 G 260-36 PM* 19 52 10.3011468144 +67 25 33.548812140       10.6   K2 28 0
13 HD 188262 * 19 53 45.9324220680 +16 46 41.152840500   8.51 7.73     G8II 47 0
14 HD 190073 Ae* 20 03 02.5098474264 +05 44 16.660712904 7.91 7.86 7.73   7.65 A2IVe 274 0
15 Wolf 1130 PM* 20 05 02.1950576493 +54 26 03.234326252   11.970 13.883     sdM1 153 0
16 * bet01 Cap SB* 20 21 00.6665981712 -14 46 53.067367488 4.14 3.87 3.08 2.53 2.03 G9II:+B8p:Si: 192 0
17 HD 196218 PM* 20 35 42.8713738392 +03 18 10.434787956   7.90 7.42     F7V 48 0

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