Table 4.

Galaxies from the literature with PAH, IR, and/or CO emission.

NameRADec.Sample|$z$|log(L6.2/L)EW6.2log(L7.7/L)log(LIR/L)Linelog(⁠|$L^{\prime }_{\rm CO}$|/L)
[hh:mm:ss][dd:mm:ss][|$\mu$|m]
NGC 304909:54:49.59+09:16:18.1SINGS0.0067.81 ± 0.02a9.65 ± 0.02aCO(3–2)7.68 ± 0.21b
IRAS 10565 + 244810:59:18.12+24:32:34.5local ULIRGs0.0439.57 ± 0.0112.04 ± 0.02cCO(1–0)9.72 ± 0.03c
GN2612:36:34.51+62:12:40.9SMGs1.22310.48 ± 0.020.38 ± 0.0411.01 ± 0.1012.66 ± 0.17cCO(2–1)10.92 ± 0.12c
GN70.21112:37:10.60+62:22:34.5High-|$z$| SFGs1.52310.39 ± 0.1010.84 ± 0.1211.94 ± 0.17cCO(1–0)10.20 ± 0.12c
MIPS50617:11:38.59+58:38:38.6High-|$z$| SBs2.4700.30 ± 0.14d11.11 ± 0.1312.93 ± 0.09eCO(3–2)10.52 ± 0.09e
NameRADec.Sample|$z$|log(L6.2/L)EW6.2log(L7.7/L)log(LIR/L)Linelog(⁠|$L^{\prime }_{\rm CO}$|/L)
[hh:mm:ss][dd:mm:ss][|$\mu$|m]
NGC 304909:54:49.59+09:16:18.1SINGS0.0067.81 ± 0.02a9.65 ± 0.02aCO(3–2)7.68 ± 0.21b
IRAS 10565 + 244810:59:18.12+24:32:34.5local ULIRGs0.0439.57 ± 0.0112.04 ± 0.02cCO(1–0)9.72 ± 0.03c
GN2612:36:34.51+62:12:40.9SMGs1.22310.48 ± 0.020.38 ± 0.0411.01 ± 0.1012.66 ± 0.17cCO(2–1)10.92 ± 0.12c
GN70.21112:37:10.60+62:22:34.5High-|$z$| SFGs1.52310.39 ± 0.1010.84 ± 0.1211.94 ± 0.17cCO(1–0)10.20 ± 0.12c
MIPS50617:11:38.59+58:38:38.6High-|$z$| SBs2.4700.30 ± 0.14d11.11 ± 0.1312.93 ± 0.09eCO(3–2)10.52 ± 0.09e

Notes. Column (1): Source name; column (2): Right ascension in units of hours, minutes, and seconds; column (3): Declination in units of degrees, arcminutes, and arcseconds; column (4): Galaxy sample or selection; column (5): Redshift; column (6): PAH 6.2 |$\mu$|m luminosity; column (7): Equivalent width of the PAH 6.2 |$\mu$|m feature; column (8): Infrared luminosity (integrated from 8−1000 |$\mu$|m); column (9): Observed CO line; column (10): CO(1–0) luminosity.

aFrom Smith et al. (2007). IR luminosities are aperture corrected.

bFrom Wilson et al. (2012). Converted to CO(1-0) luminosities using r32/10 = 0.18 ± 0.02.

cFrom Pope et al. (2013). For the CO luminosities, we corrected higher J transitions using the conversion scheme listed in Bothwell et al. (2013): r21/10 = 0.84 ± 0.13, r32/10 = 0.52 ± 0.09, r43/10 = 0.41 ± 0.07.

dFrom Sajina et al. (2007).

eFrom Yan et al. (2010).

Table 4.

Galaxies from the literature with PAH, IR, and/or CO emission.

NameRADec.Sample|$z$|log(L6.2/L)EW6.2log(L7.7/L)log(LIR/L)Linelog(⁠|$L^{\prime }_{\rm CO}$|/L)
[hh:mm:ss][dd:mm:ss][|$\mu$|m]
NGC 304909:54:49.59+09:16:18.1SINGS0.0067.81 ± 0.02a9.65 ± 0.02aCO(3–2)7.68 ± 0.21b
IRAS 10565 + 244810:59:18.12+24:32:34.5local ULIRGs0.0439.57 ± 0.0112.04 ± 0.02cCO(1–0)9.72 ± 0.03c
GN2612:36:34.51+62:12:40.9SMGs1.22310.48 ± 0.020.38 ± 0.0411.01 ± 0.1012.66 ± 0.17cCO(2–1)10.92 ± 0.12c
GN70.21112:37:10.60+62:22:34.5High-|$z$| SFGs1.52310.39 ± 0.1010.84 ± 0.1211.94 ± 0.17cCO(1–0)10.20 ± 0.12c
MIPS50617:11:38.59+58:38:38.6High-|$z$| SBs2.4700.30 ± 0.14d11.11 ± 0.1312.93 ± 0.09eCO(3–2)10.52 ± 0.09e
NameRADec.Sample|$z$|log(L6.2/L)EW6.2log(L7.7/L)log(LIR/L)Linelog(⁠|$L^{\prime }_{\rm CO}$|/L)
[hh:mm:ss][dd:mm:ss][|$\mu$|m]
NGC 304909:54:49.59+09:16:18.1SINGS0.0067.81 ± 0.02a9.65 ± 0.02aCO(3–2)7.68 ± 0.21b
IRAS 10565 + 244810:59:18.12+24:32:34.5local ULIRGs0.0439.57 ± 0.0112.04 ± 0.02cCO(1–0)9.72 ± 0.03c
GN2612:36:34.51+62:12:40.9SMGs1.22310.48 ± 0.020.38 ± 0.0411.01 ± 0.1012.66 ± 0.17cCO(2–1)10.92 ± 0.12c
GN70.21112:37:10.60+62:22:34.5High-|$z$| SFGs1.52310.39 ± 0.1010.84 ± 0.1211.94 ± 0.17cCO(1–0)10.20 ± 0.12c
MIPS50617:11:38.59+58:38:38.6High-|$z$| SBs2.4700.30 ± 0.14d11.11 ± 0.1312.93 ± 0.09eCO(3–2)10.52 ± 0.09e

Notes. Column (1): Source name; column (2): Right ascension in units of hours, minutes, and seconds; column (3): Declination in units of degrees, arcminutes, and arcseconds; column (4): Galaxy sample or selection; column (5): Redshift; column (6): PAH 6.2 |$\mu$|m luminosity; column (7): Equivalent width of the PAH 6.2 |$\mu$|m feature; column (8): Infrared luminosity (integrated from 8−1000 |$\mu$|m); column (9): Observed CO line; column (10): CO(1–0) luminosity.

aFrom Smith et al. (2007). IR luminosities are aperture corrected.

bFrom Wilson et al. (2012). Converted to CO(1-0) luminosities using r32/10 = 0.18 ± 0.02.

cFrom Pope et al. (2013). For the CO luminosities, we corrected higher J transitions using the conversion scheme listed in Bothwell et al. (2013): r21/10 = 0.84 ± 0.13, r32/10 = 0.52 ± 0.09, r43/10 = 0.41 ± 0.07.

dFrom Sajina et al. (2007).

eFrom Yan et al. (2010).

Close
This Feature Is Available To Subscribers Only

Sign In or Create an Account

Close

This PDF is available to Subscribers Only

View Article Abstract & Purchase Options

For full access to this pdf, sign in to an existing account, or purchase an annual subscription.

Close