2022ApJ...933..172J


Query : 2022ApJ...933..172J

2022ApJ...933..172J - Astrophys. J., 933, 172-172 (2022/July-2)

Cosmological Results from the RAISIN Survey: Using Type Ia Supernovae in the Near Infrared as a Novel Path to Measure the Dark Energy Equation of State.

JONES D.O., MANDEL K.S., KIRSHNER R.P., THORP S., CHALLIS P.M., AVELINO A., BROUT D., BURNS C., FOLEY R.J., PAN Y.-C., SCOLNIC D.M., SIEBERT M.R., CHORNOCK R., FREEDMAN W.L., FRIEDMAN A., FRIEMAN J., GALBANY L., HSIAO E., KELSEY L., MARION G.H., NICHOL R.C., NUGENT P.E., PHILLIPS M.M., REST A., RIESS A.G., SAKO M., SMITH M., WISEMAN P. and WOOD-VASEY W.M.

Abstract (from CDS):

Type Ia supernovae (SNe Ia) are more precise standardizable candles when measured in the near-infrared (NIR) than in the optical. With this motivation, from 2012 to 2017 we embarked on the RAISIN program with the Hubble Space Telescope (HST) to obtain rest-frame NIR light curves for a cosmologically distant sample of 37 SNe Ia (0.2 <= z <= 0.6) discovered by Pan-STARRS and the Dark Energy Survey. By comparing higher-z HST data with 42 SNe Ia at z < 0.1 observed in the NIR by the Carnegie Supernova Project, we construct a Hubble diagram from NIR observations (with only time of maximum light and some selection cuts from optical photometry) to pursue a unique avenue to constrain the dark energy equation-of-state parameter, w. We analyze the dependence of the full set of Hubble residuals on the SN Ia host galaxy mass and find Hubble residual steps of size ∼0.06-0.1 mag with 1.5σ-2.5σ significance depending on the method and step location used. Combining our NIR sample with cosmic microwave background constraints, we find 1 + w = -0.17 ± 0.12 (statistical + systematic errors). The largest systematic errors are the redshift-dependent SN selection biases and the properties of the NIR mass step. We also use these data to measure H0 = 75.9 ± 2.2 km s–1 Mpc–1 from stars with geometric distance calibration in the hosts of eight SNe Ia observed in the NIR versus H0 = 71.2 ± 3.8 km s–1 Mpc–1 using an inverse distance ladder approach tied to Planck. Using optical data, we find 1 + w = -0.10 ± 0.09, and with optical and NIR data combined, we find 1 + w = -0.06 ± 0.07; these shifts of up to ∼0.11 in w could point to inconsistency in the optical versus NIR SN models. There will be many opportunities to improve this NIR measurement and better understand systematic uncertainties through larger low-z samples, new light-curve models, calibration improvements, and eventually by building high-z samples from the Roman Space Telescope.

Abstract Copyright: © 2022. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Observational cosmology - Hubble constant - Type Ia supernovae

VizieR on-line data: <Available at CDS (J/ApJ/933/172): table5.dat table6.dat table7.dat>

Simbad objects: 69

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Number of rows : 69
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 SN 2007A SN* 00 25 16.66 +12 53 12.5     16.0     SNIa 82 1
2 DES16E2rd SN* 00 32 21.32 -43 50 46.0           SNIa 2 0
3 DES15E2nlz SN* 00 35 51.337 -44 40 36.11           SNIa 8 0
4 DES16E1dcx SN* 00 35 52.43 -43 21 28.8           SNIa 4 0
5 DES16E2clk SN* 00 36 48.85 -44 08 23.1           SNIa 4 0
6 DES15E2uc SN* 00 37 53.408 -43 18 52.28           SNIa 7 0
7 DES16E2cqq SN* 00 39 50.07 -43 33 53.2           SNIa 4 0
8 DES16E2cxw SN* 00 40 42.70 -43 55 18.5           SNIa 4 0
9 DES15E2mhy SN* 00 41 17.094 -43 53 10.42           SNIa 7 0
10 SN 2006ot SN* 02 15 04.84 -20 45 58.2     17.4     SNIap 48 1
11 DES16X1cpf SN* 02 16 49.5120 -04 13 06.096           SNIa 1 0
12 DES15X2mey SN* 02 20 30.752 -06 26 47.30           SNIa 6 0
13 DES15X2kvt SN* 02 21 46.248 -05 38 23.45           SNIa 8 0
14 DES15X2nkz SN* 02 22 13.206 -05 52 18.15           SNIa 7 0
15 [JSR2018] psc560027 SN* 02 23 24.150 -03 05 02.20           SNIa 7 0
16 DES16X3cry SN* 02 24 10.5480 -03 49 51.996           SNIa 1 0
17 [JSR2018] psc450339 SN* 02 25 08.965 -03 21 12.20           SNIa 7 0
18 DES16X3zd SN* 02 26 56.45 -04 25 09.5           SNIa 2 0
19 [JSR2018] psc440236 SN* 02 28 24.444 -04 25 28.58           SNIa 7 0
20 DES16S2afz SN* 02 46 24.29 -01 13 31.0           SNIa 2 0
21 DES16S1bno SN* 02 50 03.8230 -00 01 17.724           SNIa 1 0
22 DES16S1agd SN* 02 52 20.02 -00 54 40.2           SNIa 2 0
23 DES16C3cmy SN* 03 27 13.4400 -27 29 20.724           SNIa 1 0
24 DES15C3odz SN* 03 27 54.955 -28 33 51.96           SNIa 8 0
25 [JSR2018] psc470110 SN* 03 28 16.936 -28 37 23.97           SNIa 7 0
26 [JSR2018] psc440005 SN* 03 31 57.421 -28 53 00.81           SNIa 7 0
27 UCAC3 125-8171 * 03 32 32.8728703992 -27 51 48.339287532 18.74 18.0893 16.64   17.0383 ~ 40 0
28 SN 2012fr SN* 03 33 35.99 -36 07 37.7           SNIa-norm 178 1
29 DES16C2cva SN* 03 34 44.0350 -29 19 02.028           SNIa 1 0
30 SN 2007on SN* 03 38 50.90 -35 34 30.0       14.9   SNIa 153 1
31 SN 2011iv SN* 03 38 51.4 -35 35 32           SNIa-norm 96 1
32 NGC 1404 rG 03 38 51.917 -35 35 39.81 11.53 10.69 10.00 9.03   ~ 787 1
33 DES15C1nhv SN* 03 39 00.937 -27 50 35.35           SNIa 8 0
34 DES16C1cim SN* 03 39 30.3620 -26 38 57.048           SNIa 1 0
35 SN 2009ab SN* 04 16 36.39 +02 45 51.0           SNIa 33 1
36 BD+52 913 WD* 05 05 30.6180977592 +52 49 51.919301604 10.25 11.44 11.69 11.93 12.108 DA.8 1153 0
37 GD 71 WD* 05 52 27.6198591816 +15 53 13.228887444 11.675 12.783 13.032 13.169 13.337 DA1.5 407 0
38 SN 2015F SN* 07 36 15.76 -69 30 23.0           SNIa 100 1
39 NAME JMK2022 PS1-470240 SN* 08 42 53.5080 +45 54 04.910           SNIa 1 0
40 [JSR2018] psc470041 SN* 08 45 21.004 +44 45 17.25           SNIa 7 0
41 [JSR2018] psc500100 SN* 08 46 33.246 +45 21 22.15           SNIa 7 0
42 [JSR2018] psc490521 SN* 09 55 27.641 +01 34 31.05           SNIa 6 0
43 [JSR2018] psc480794 SN* 09 58 10.025 +01 21 50.79           SNIa 2 0
44 [JSR2018] psc480464 SN* 09 59 12.104 +03 13 17.64           SNIa 7 0
45 [JSR2018] psc490037 SN* 09 59 49.727 +00 48 59.82           SNIa 7 0
46 SN 2012ht SN* 10 53 22.8 +16 46 35           SNIa-norm 84 1
47 SN 2007sr SN* 12 01 52.80 -18 58 21.7     12.79     SNIa 100 1
48 NAME JMK2022 PS1-520107 SN* 12 16 38.6310 +47 48 57.881           SNIa 1 0
49 [JSR2018] psc510457 SN* 12 25 33.318 +48 08 12.71           SNIa 7 0
50 SN 2006D SN* 12 52 33.87 -09 46 30.7           SNIa 107 1
51 GD 153 WD* 12 57 02.3224909560 +22 01 52.634778240 11.883 13.060 13.349 13.488 13.669 DA1.2 380 0
52 SN 2005al SN* 13 50 00.329 -30 34 34.21           SNIa 50 1
53 SN 2011fe SN* 14 03 05.711 +54 16 25.22   10.12 10.06     SNIa-norm 747 1
54 [JSR2018] psc520188 SN* 14 22 05.767 +52 32 40.70           SNIa 7 0
55 [JSR2018] psc500301 SN* 14 22 11.451 +52 37 54.64           SNIa 7 0
56 SN 2007af SN* 14 22 21.03 -00 23 37.6     15.4     SNIa 185 1
57 SN 2009Y SN* 14 42 23.68 -17 14 48.3           SNIa-norm 57 1
58 SN 2006bt SN* 15 56 33.81 +20 03 07.2     17.5     SNIap 114 1
59 [JSR2018] psc520062 SN* 16 17 48.328 +54 38 00.18           SNIa 7 0
60 GSC 02581-02323 * 16 31 33.8123836584 +30 08 46.397382324 13.576 12.972 12.917 12.564 12.212 G2V 106 0
61 * alf Lyr dS* 18 36 56.33635 +38 47 01.2802 0.03 0.03 0.03 0.07 0.10 A0V 2787 1
62 SN 2004ey SN* 21 49 07.81 +00 26 39.2     16.0     SNIa 78 1
63 BD+17 4708 SB* 22 11 31.3756832854 +18 05 34.177983548 9.73 9.91 9.46 9.03 8.70 sdF8 580 0
64 [JSR2018] psc530251 SN* 22 18 32.226 +01 06 53.61           SNIa 7 0
65 [JSR2018] psc540087 SN* 22 21 30.357 +00 07 46.34           SNIa 2 0
66 [JSR2018] psc550202 SN* 23 27 11.973 -00 46 58.53           SNIa 7 0
67 [JSR2018] psc540118 SN* 23 27 17.417 -00 02 53.05           SNIa 2 0
68 [JSR2018] psc560054 SN* 23 33 10.992 -00 20 11.06           SNIa 7 0
69 [JSR2018] psc450082 SN* 23 33 25.442 +00 18 37.77           SNIa 7 0

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