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Table 1

Summary of the Gaussian fits to the [C i] and the CO transitions.

Name z quoted ν ref Ref. Trans Δv FWHM z fitted ΔF/F

SMM J123549+6215 2.202 T06 CO 3 → 2
2.202 W11 [C i]
SDSS J102434.56 2.2854 105.220 D95 CO 3 → 2 −69 ± 9 197 ± 24 2.28565 ± 0.00010 10 ± 4
   +470909.5 2.2854 149.8024 W05a [C i] −6.9 ± 2.7 157 ± 31 2.28532 ± 0.00003 ...
SMM J2135–0102 2.32591 138.563* D11 CO 4 → 3 0 ± 13 550 ± 30 2.32730 ± 0.00014 −10 ± 10
2.326 147.901* D11 [C i] 0 ± 16 515 ± 39 2.32764 ± 0.00018 ...
SMM J163658+4105 2.452 T06 CO 3 → 2
2.452 W11 [C i]
SMM J16359+6612 2.51732 131.074 W05 CO 4 → 3 −6 ± 21 410 ± 110 2.51733 ± 0.00025 −10 ± 12
2.517 139.9229 W11 [C i] 27 ± 15 430 ± 90 2.51769 ± 0.00018 ...
H 1413+117 2.55784 97.191 W03 CO 3 → 2 −14 ± 2 421 ± 5 2.55774 ± 0.00002 −4 ± 8
    (Cloverleaf) 2.5578 138.3313 W05a [C i] 4 ± 22 329 ± 52 2.55789 ± 0.00026 ...
SMM  J14011+0252 2.5653 96.9975 F99 CO 3 → 2 27 ± 7 189 ± 16 2.56532 ± 0.00008 −14 ± 8
2.5653 138.0457 W05a [C i] 51 ± 18 251 ± 40 2.56581 ± 0.00021 ...
RX J0911+0551 2.796 91.088 H04 CO 3 → 2
2.796 W11 [C i]
SMM J02399–0136 2.8076 90.81 G03 CO 3 → 2
2.808 W11 [C i]
APM 08279+5255 3.9114 93.867 D99 CO 4 → 3 −20 ± 12 571 ± 28 3.91131 ± 0.00019 −36 ± 9
3.913 100.216 W06 [C i] 128 ± 17 414 ± 49 3.91309 ± 0.00027 ...
MM 18423+5938 3.92960 93.5249 L10 CO 4 → 3 −30 ± 5 162 ± 12 3.92911 ± 0.00009 18 ± 4
3.930 99.8378 L10 [C i] −83 ± 6 230 ± 14 3.92825 ± 0.00010 ...
PSS 2322+1944 4.1199 90.048 C02 CO 4 → 3 3 ± 17 361 ± 42 4.11999 ± 0.00029 17 ± 13
4.1199 96.127 P04 [C i] −46 ± 22 277 ± 59 4.11911 ± 0.00037 ...
SDSS J1148+5251 6.4189 93.204 B03 CO 6 → 5
6.419 R09 [C i]

Notes. We list all of the sources in which a [C i] detection is claimed by Walter et al. (2011), although spectra are currently available for only eight (Fig. 1). These are in order of increasing redshift (zquoted, which is derived from the centroid frequencies quoted in the reference). νref [GHz] is the frequency given in the reference from which the velocity offset, Δv [km  s-1], and fitted redshift, zfitted, are determined. FWHM [km  s-1] gives the full-width half maximum of the line as determined from the Gaussian fit (all single fits except SMM J16359+6612 for which two Gaussians were used and Δv is the mean of the two fits). The final column gives ΔF/F, in units of 10-5, derived from the two values of zfitted.

*

The absolute frequency and

the centroid frequency of the line from a spectral scan.

D95 – Downes et al. (1995), D99 – Downes et al. (1999), F99 – Frayer et al. (1999), C02 – Cox et al. (2002), G03 – Genzel et al. (2003), B03 – Bertoldi et al. (2003), W03 – Weiß et al. (2003), H04 – Hainline et al. (2004), P04 – Pety et al. (2004), W05a – Weiß et al. (2005a), W05b – Weiß et al. (2005b), T06 – Tacconi et al. (2006), W06 – Wagg et al. (2006), R09 – Riechers et al. (2009) [according to Walter et al. 2011], L10 – Lestrade et al. (2010), D11 – Danielson et al. (2011), W11 – Walter et al. (2011).

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