2022A&A...668A..88N


Query : 2022A&A...668A..88N

2022A&A...668A..88N - Astronomy and Astrophysics, volume 668A88 (2022/12-1)

The Galactic chemical evolution of phosphorus observed with IGRINS.

NANDAKUMAR G., RYDE N., MONTELIUS M., THORSBRO B., JONSSON H. and MACE G.

Abstract (from CDS):

Context. Phosphorus (P) is considered to be one of the key elements for life, making it an important element to look for in the abundance analysis of spectra of stellar systems. Yet, only a select number of spectroscopic studies exist to estimate the phosphorus abundances and investigate its trend across a range of metallicities. This is due to the lack of good phosphorus lines in the optical wavelength region and the requirement of careful manual analysis of the blended phosphorus lines in near-infrared H-band spectra obtained with individual observations and surveys such as the Apache Point Observatory Galactic Evolution Experiment (APOGEE). Aims. Based on a consistent and systematic analysis of high-resolution, near-infrared Immersion GRating INfrared Spectrograph (IGRINS) spectra of 38 K giant stars in the Solar neighborhood, we present and investigate the phosphorus abundance trend in the metallicity range of -1.2 dex < [Fe/H] < 0.4 dex. Furthermore, we compare this trend with the available chemical evolution models to shed some light on the origin and evolution of phosphorus. Methods. We have observed full H- and K-band spectra at a spectral resolving power of R = 45 000 with IGRINS mounted on the Gemini South telescope, the Discovery Channel Telescope, and the Harlan J Smith Telescope at McDonald Observatory. Abundances were determined from spectral lines by modeling the synthetic spectrum that best matches the observed spectrum by χ2 minimization. For this task, we used the Spectroscopy Made Easy (SME) tool in combination with one-dimensional (1D) Model Atmospheres in a Radiative and Convective Scheme (MARCS) stellar atmosphere models. The investigated sample of stars have reliable stellar parameters estimated using optical FIber-fed Echelle Spectrograph (FIES) spectra obtained in a previous study of a set of stars called Giants in the Local Disk (GILD). In order to determine the phosphorus abundances from the 16482.92 Å phosphorus line, we needed to take special care blending the CO(v = 7-4) line. With the stellar parameters known, we thus determined the C, N, and O abundances from atomic carbon and a range of nonblended molecular lines (CO, CN, and OH) which are plentiful in the H-band region of K giant stars, assuring an appropriate modeling of the blending CO(v = 7-4) line. Results. We present the [P/Fe] versus [Fe/H] trend for K giant stars in the metallicity range of -1.2 dex < [Fe/H] < 0.4 dex and enhanced phosphorus abundances for two metal-poor s-rich stars. We find that our trend matches well with the compiled literature sample of prominently dwarf stars and the limited number of giant stars. Our trend is found to be higher by ∼0.05-0.1 dex compared to the theoretical chemical evolution trend resulting from the core collapse supernova (type II) of massive stars with the phosphorus yields arbitrarily increased by a factor of 2.75. Thus the enhancement factor might need to be ∼0.05-0.1 dex higher to match our trend. We also find an empirically determined primary behavior for phosphorus. Furthermore, the phosphorus abundance is found to be elevated by ∼0.6-0.9 dex in the two s-enriched stars compared to the theoretical chemical evolution trend.

Abstract Copyright: © G. Nandakumar et al. 2022

Journal keyword(s): stars: abundances - stars: late-type - Galaxy: evolution - Galaxy: disk - infrared: stars

VizieR on-line data: <Available at CDS (J/A+A/668/A88): table2.dat>

Simbad objects: 41

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Number of rows : 41
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 NGC 752 OpC 01 56 53.7 +37 45 06           ~ 712 0
2 * bet Gem PM* 07 45 18.94987 +28 01 34.3160 3.00 2.14 1.14 0.39 -0.11 K0IIIb 1150 2
3 HD 76445 RG* 08 56 45.9896726544 +17 28 52.866611580   8.59 7.64     G5 39 0
4 * mu. Leo PM* 09 52 45.8170136628 +26 00 25.024269924 6.50 5.10 3.88 2.97 2.39 K2IIIbCN1Ca1 479 0
5 * gam Leo ** 10 19 58.35056 +19 50 29.3468           K1-III+G7IIIb 94 0
6 * ksi Hya ** 11 33 00.1149306166 -31 51 27.447975478 5.17 4.47 3.54 2.84 2.36 G7IIIb 269 0
7 HD 102328 * 11 46 55.6222860288 +55 37 41.480416020   6.528 5.254     K2.5IIIbCN1 169 0
8 * 9 Dra RG* 12 59 55.0715577048 +66 35 50.167972104   6.657 5.368     K0III 90 0
9 * eps Vir PM* 13 02 10.5970152536 +10 57 32.935398266 4.45 3.71 2.79 2.16 1.71 G8III-IIIb 574 0
10 * alf Boo RG* 14 15 39.67207 +19 10 56.6730 2.46 1.18 -0.05 -1.03 -1.68 K1.5IIIFe-0.5 2417 1
11 HD 129846 * 14 43 44.4335937840 +40 27 33.310334808 8.75 7.12 5.73     K4III 45 0
12 TYC 2046-759-1 RG* 16 11 33.6027851544 +24 36 52.439123556   12.59 11.14     ~ 14 0
13 TYC 3094-1605-1 RG* 17 21 56.6755406352 +43 01 40.723330908   11.57 10.40     ~ 16 0
14 * 42 Dra PM* 18 25 59.1369601368 +65 33 48.531343788   6.005 4.823     K1.5IIIFe-1 190 1
15 TYC 3126-1431-1 HB* 18 43 38.9518734024 +42 35 29.434301124   11.00 9.96 9.70   ~ 36 0
16 TYC 3531-194-1 HB* 18 44 49.1975925552 +47 17 43.461125916   12.44 11.50     K0III 34 0
17 TYC 3126-801-1 RG* 18 46 43.1010145152 +42 23 14.348294124   12.27 11.47     G6V 40 0
18 NGC 6705 1423 HB* 18 50 55.8201141624 -06 18 14.788090512   13.041 11.414     KIII: 40 0
19 NGC 6705 1184 HB* 18 51 02.0070991104 -06 17 26.535767388   13.030 11.426     ~ 42 0
20 NGC 6705 184 * 18 51 39.0194051784 -06 13 07.086497232   15.62 13.85     ~ 3 0
21 HD 175541 PM* 18 55 40.8841512864 +04 15 55.165056048   8.90 8.00     G6/8IV 129 1
22 TYC 3549-1225-1 HB* 19 01 43.8090729528 +49 23 06.255443004   12.53 11.65     K1.5III 45 0
23 TYC 3124-1301-1 HB* 19 02 17.2026542376 +41 07 23.756055276   12.01 10.55     K4IIIp 39 0
24 HD 176981 SB* 19 02 21.5664954360 +08 22 24.735527256   7.882 6.271     K3III 35 0
25 TYC 3120-835-1 HB* 19 02 39.3556695792 +39 05 59.225938296   12.33 10.88     ~ 40 0
26 TYC 3550-346-1 RG* 19 11 00.6314850072 +49 06 52.754050476   11.40 10.14     K3III 43 0
27 TYC 3125-2626-1 RG* 19 12 34.2821760048 +41 05 25.595544156   12.18 11.10     K1.5III 35 0
28 TYC 3134-31-1 RG* 19 27 26.7774736968 +39 00 45.630205236   12.06 10.81     K3III 41 0
29 BD+38 3601 HB* 19 27 28.7821391736 +38 48 09.640461816   10.03 8.86     K2III 22 0
30 HD 184293 PM* 19 31 19.3307715408 +50 18 24.138385416   6.814 5.540     K1III 48 0
31 TYC 3139-1534-1 HB* 19 32 18.5549620728 +40 58 21.851476896   11.03 9.90     G8III 38 0
32 TYC 3139-1785-1 RG* 19 32 40.5523321416 +39 46 33.871436004   11.48 10.20     K3III 38 0
33 TYC 3140-2350-1 RG* 19 41 34.3948190103 +40 17 48.192852940   12.96 11.37     K4III 59 0
34 2MASS J19421943+4016074 RG* 19 42 19.4577416640 +40 16 07.328613900           K2IIIb 37 0
35 TYC 3565-1299-1 HB* 19 46 43.8823081656 +49 34 20.946621360   12.88 11.57     G6V 41 0
36 HD 226210 RG* 19 51 24.0442483392 +41 49 28.469355492   11.29 10.34     ~ 35 0
37 HD 226247 HB* 19 51 51.3753033552 +41 06 37.705627764   9.885 8.68     K2 23 0
38 TYC 3562-764-1 RG* 19 53 05.9141004888 +48 33 17.944737840   12.46 11.13     ~ 26 0
39 NGC 6940 OpC 20 34 28.4 +28 17 07           ~ 215 0
40 * eps Cyg ** 20 46 12.6722768426 +33 58 13.182037125 4.370 3.520 2.480 1.73 1.19 K0III 519 0
41 HD 206610 * 21 43 24.9001051368 -07 24 29.710256004   9.38 8.35   8.76 K0III 51 1

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