J/MNRAS/480/1563       Properties of UWISH2 PNe candidates        (Jones+, 2018)

The excitation mechanisms and evolutionary stages of UWISH2 planetary nebula candidates. Jones A.M., Gledhill T.M., Froebrich D., Smith M.D. <Mon. Not. R. Astron. Soc., 480, 1563-1579 (2018)> =2018MNRAS.480.1563J 2018MNRAS.480.1563J (SIMBAD/NED BibCode)
ADC_Keywords: Planetary nebulae ; Interstellar medium ; Infrared ; Line Profiles Keywords: ISM: lines and bands - planetary nebulae: general - infrared: ISM Abstract: We present medium-resolution K-band long-slit spectroscopy of 29 true, likely, possible, and candidate Galactic Plane planetary nebulae (PNe) from the UWISH2 survey, many of which have only been recently discovered. These objects are bright in molecular hydrogen (H2) emission, and many have bipolar morphologies. Through the detection of the Brγ emission line, which traces ionized hydrogen, we find that the majority of the candidate PNe are indeed likely to be PNe, while 2 of the targets are more likely young stellar objects (YSOs) or pre-planetary nebulae (pPNe). We detect Brγ in 13 objects which have no detection in IPHAS or SHS Hα surveys. This implies that they are potential members of the little-known optically obscured PN population, hidden from wide-field optical surveys. We use the spatial extent of the H2 1-0S(1) and Brγ lines to estimate the evolutionary stage of our targets, and find that W-BPNe (bipolar PNe with pinched waist morphologies) are likely to be younger objects, while R-BPNe (bipolar PNe with large ring structures) are more evolved. We use line ratios to trace the excitation mechanism of the H2, and find the 1-0S(1)/2-1S(1) and 1-0S(1)/Brγ ratios are higher for R-BPNe, implying the H2 is thermally excited. However, in W-BPNe, these ratios are lower, and so UV-fluorescence may be contributing to the excitation of H2. Description: In this work, we present K-band long-slit spectra of a sample of PNe and candidate PNe taken from the recent UWISH2 imaging survey (UKIRT Widefield Infrared Survey for H2) (Froebrich et al. 2011MNRAS.413..480F 2011MNRAS.413..480F). We focus on the mechanisms governing the excitation of H2, and how these relate to the evolutionary stages and morphologies of the targets. Along with spectra, we make use of near-IR H2 and optical Hα imaging, and mid-IR colours where available. UWISH2 was an unbiased Galactic Plane survey, focused on the H2 1-0S(1) line at 2.1218µm. Our sample for spectroscopic follow-up consisted of 29 targets, selected mainly due to their bright H2 fluxes. Observations were obtained on 2016 July 22-24, using the Long-slit Intermediate Resolution Infrared Spectrograph (LIRIS; Acosta Pulido et al. 2003; Manchado et al. 2003) on the William Herschel Telescope, located at the Observatorio del Roque de los Muchachos on La Palma, Canary Islands. LIRIS uses a 1024x1024 HAWAII detector, with a pixel scale of 0.25 arcsec pixel-1, yielding a field of view of 4.27arcminx4.27arcmin. Table 1 gives observational details for each target, table 2 contains the key line flux ratios and table C1 lists all detected emission line fluxes for each PNe candidate. File Summary: -------------------------------------------------------------------------------- FileName Lrecl Records Explanations -------------------------------------------------------------------------------- ReadMe 80 . This file table1.dat 96 29 Observation log and additional information for the 29 targets table2.dat 61 49 Key line flux ratios and errors, uncorrected for extinction tablec1.dat 126 49 Continuum-subtracted line fluxes and errors for K-band emission lines -------------------------------------------------------------------------------- Byte-by-byte Description of file: table1.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 14 A14 --- Name Planetary nebula name (PN GLLL.l+BB.b) 16- 40 A25 --- OtherName Other name associated to the source 42- 50 F9.5 deg RAdeg Right ascension (J2000) 52- 60 F9.5 deg DEdeg Declination (J2000) 62- 65 I4 s Int Integration time 67- 70 F4.2 --- Airmass Airmass 72- 75 A4 --- H2morph Morphology in H2 (1) 77- 83 A7 --- H2size Size in H2 (1) 85- 87 A3 --- Hamorph Morphology in Hα (1) 89- 94 A6 --- Hasize Size in Hα (1) 96 A1 --- PNstatus Planetary nebula status (2) -------------------------------------------------------------------------------- Note (1): Morphologies and sizes in H2 and Hα are taken from table A1 of Gledhill et al. (2018MNRAS.479.3759G 2018MNRAS.479.3759G). Where no Hα morphology is given, the object is not detected in Hα emission. Morphologies make use of the 'ERBIAS' classification system (Parker et al. 2006MNRAS.373...79P 2006MNRAS.373...79P), and sizes are the major and minor axis dimensions in arcsec. Note (2): PN status comes from the HASH PN database (Parker, Bojicic & Frew 2016JPhCS.728c2008P 2016JPhCS.728c2008P). Status as follows: T = true PNe L = likely to be PNe P = possible PNe C = candidate PNe -------------------------------------------------------------------------------- Byte-by-byte Description of file: table2.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 14 A14 --- Name Planetary nebula name (PN GLLL.l+BB.b) 16- 25 A10 --- Region Region of the source 27- 30 F4.1 --- nu1/nu2 ? Ratio of the 1-0S(1) (2.1218µm) and the 2-1S(1) (2.2477µm) H2 lines 32- 34 F3.1 --- e_nu1/nu2 ? Error on nu1/nu2 36- 37 I2 --- nu1/nu3 ?=- Ratio of the 1-0S(1) and the 3-2S(3) (2.2014µm) H2 lines 39- 40 I2 --- e_nu1/nu3 ?=- Error on nu1/nu3 42- 46 F5.2 --- nu1/Brg ? Ratio of the 1-0S(1) and the Brγ (2.1661µm) lines 48- 51 F4.2 --- e_nu1/Brg ? Error on nu1/Brg 53- 56 F4.2 --- HeI/Brg ? Ratio of the HeI (2.0587µm) and the Brγ line 58- 61 F4.2 --- e_HeI/Brg ? Error on HeI/Brg -------------------------------------------------------------------------------- Byte-by-byte Description of file: tablec1.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 14 A14 --- Name Planetary nebula name (PN GLLL.l+BB.b) 16- 25 A10 --- Region Region of the object 27- 32 F6.1 10-19W/m2 HeI1 ? Continuum-substracted HeI (2.0587µm) line flux 34- 37 F4.1 10-19W/m2 e_HeI1 ? Error on HeI1 39- 42 F4.1 10-19W/m2 2-1S(3) ? Continuum-substracted 2-1S(3) (2.0735µm) line flux 44- 47 F4.1 10-19W/m2 e_2-1S(3) ? Error on 2-1S(3) flux 49- 53 F5.1 10-19W/m2 HeI2 ? Continuum-substracted HeI (2.1127µm) line flux 55- 58 F4.1 10-19W/m2 e_HeI2 ? Error on HeI2 60- 62 I3 10-19W/m2 1-0S(1) Continuum-substracted 1-0S(1) (2.1218µm) line flux 64- 65 I2 10-19W/m2 e_1-0S(1) Error on 1-0S(1) flux 67- 68 I2 10-19W/m2 2-1S(2) ?=- Continuum-substracted 2-1S(2) (2.1542µm) line flux 70- 71 I2 10-19W/m2 e_2-1S(2) ?=- Error on 2-1S(2) flux 73- 78 F6.1 10-19W/m2 Brg ? Continuum-substracted Brγ (2.1661µm) line flux 80- 83 F4.1 10-19W/m2 e_Brg ? Error on Brg 85- 86 I2 10-19W/m2 HeII ?=- Continuum-substracted HeII (2.1891µm) line flux 88 I1 10-19W/m2 e_HeII ?=- Error on HeII 90- 93 F4.1 10-19W/m2 3-2S(3) ? Continuum-substracted 3-2S(3) (2.2014µm) line flux 95- 97 F3.1 10-19W/m2 e_3-2S(3) ? Error on 3-2S(3) flux 99-101 I3 10-19W/m2 1-0S(0) Continuum-substracted 1-0S(0) (2.2233µm) line flux 103-104 I2 10-19W/m2 e_1-0S(0) Error on 1-0S(0) flux 106-109 F4.1 10-19W/m2 2-1S(1) ? Continuum-substracted 2-1S(1) (2.2477µm) line flux 111-113 F3.1 10-19W/m2 e_2-1S(1) ? Error on 2-1S(1) flux 115-117 I3 10-19W/m2 3-2S(2) ?=- Continuum-substracted 3-2S(2) (2.2870µm) line flux 119 I1 10-19W/m2 e_3-2S(2) ?=- Error on 3-2S(2) flux 121-123 I3 10-19W/m2 1-0Q(1) Continuum-substracted 1-0Q(1) (2.4066µm) line flux 125-126 I2 10-19W/m2 e_1-0Q(1) Error on 1-0Q(1) flux -------------------------------------------------------------------------------- History: From electronic version of the journal
(End) Ana Fiallos [CDS] 17-May-2022
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