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2. OBSERVATION SETUP

2.1. Survey design

The details of the observations are presented in Table 1. The observations in C-band (central frequency 6.000 GHz) cover a bandwidth of 2 GHz (4.979 – 7.021 GHz), in 16 spectral windows and 1024 spectral channels (64 in each spectral window). The L-band (central frequency 1.575 GHz) observations cover a bandwidth of 512 MHz (1.247 – 1.503 GHz, 1.647 – 1.903 GHz), in 32 spectral windows, and 2048 spectral channels. In L-band, we placed the two base bands, of 16 spectral windows each, 144 MHz apart in order to avoid a region of particularly strong and contaminating radio frequency interference (RFI). Note that due to flagging during the reductions, the final central frequencies shown in Tables 4 and 5 for each galaxy are adjusted from the values given here.

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Table 1. Observations

Galaxy aRA Dec Distance b (Mpc) Band Date (yymmdd) SB ID prim. cal c zero. pol. cal. c sec. cal.

N 660 01h43m02.s40 +13d38m42.s2 12.3 C 111209 5804098 3C48 3C84 J0204+1514
C 111218 5805266 3C48 3C84 J0204+1514
L 111219 6621021 3C48 3C84 J0204+1514
L 130317 6619959 3C48 3C84 J0204+1514
N 891* 02h22m33.s41 +42d20m56.s9 9.1* C 111209 5804098 3C48 3C84 J0230+4032
C 111218 5805266 3C48 3C84 J0230+4032
L 111219 6621021 3C48 3C84 J0314+4314
L 130317 6619959 3C48 3C84 J0314+4314
N 2613 08h33m22.s84 -22d58m25.s2 23.4 C 111213 4806011 3C286 OQ208 J0837-1951
L 130317 6619959 3C48 3C84 J0853-2047
L 111221 4807896 3C286 OQ208 J0853-2047
N 2683 08h52m41.s35 +33d25m18.s5 6.27 C 111213 4806011 3C286 OQ208 J0837+2454
L 111221 4807896 3C286 OQ208 J0909+4253
N 2820 09h21m45.s58 +64d15m28.s6 26.5 C 111217 4809751 3C286 OQ208 J0921+6215
L 111218 4812474 3C286 OQ208 J0949+6614
N 2992 09h45m42.s00 -14d19m35.s0 34 C 111213 4806011 3C286 OQ208 J0943-0819
L 111221 4807896 3C286 OQ208 J0943-0819
N 3003 09h48m36.s05 +33d25m17.s4 25.4 C 111213 4806011 3C286 OQ208 J0958+3224
L 111221 4807896 3C286 OQ208 J0958+3224
N 3044 09h53m40.s88 +01d34m46.s7 20.3 C 111213 4806011 3C286 OQ208 J0925+0019
L 111221 4807896 3C286 OQ208 J1007-0207
N 3079 10h01m57.s80 +55d40m47.s3 20.6 C 111217 4809751 3C286 OQ208 J1035+5628
L 111218 4812474 3C286 OQ208 J1035+5628
N 3432 10h52m31.s13 +36d37m07.s6 9.42 C 111217 4809751 3C286 OQ208 J1104+3812
L 111218 4812474 3C286 OQ208 J1006+3454
N 3448 10h54m39.s24 +54d18m18.s8 24.5 C 111217 4809751 3C286 OQ208 J1035+5628
L 111218 4812474 3C286 OQ208 J1035+5628
N 3556 11h11m30.s97 +55d40m26.s8 14.09 C 111217 4809751 3C286 OQ208 J1035+5628
L 111218 4812474 3C286 OQ208 J1035+5628
N 3628* 11h20m17.s01 +13d35m22.s9 8.5 C 111213 4806011 3C286 OQ208 J1120+1420
L 111221 4807896 3C286 OQ208 J1120+1420
N 3735 11h35m57.s30 +70d32m08.s1 42 C 111217 4809751 3C286 OQ208 J1056+7011
L 111218 4812474 3C286 OQ208 J1206+6413
N 3877 11h46m07.s80 +47d29m41.s2 17.7 C 111227 5062561 3C286 OQ208 J1219+4829
L 111218 4812474 3C286 OQ208 J1219+4829
N 4013 11h58m31.s38 +43d56m47.s7 16 C 111227 5062561 3C286 OQ208 J1146+3958
L 111218 4812474 3C286 OQ208 J1146+3958
N 4096 12h06m01.s13 +47d28m42.s4 10.32 C 111227 5062561 3C286 OQ208 J1146+3958
L 111218 4812474 3C286 OQ208 J1146+3958
N 4157 12h11m04.s37 +50d29m04.s8 15.6 C 111227 5062561 3C286 OQ208 J1219+4829
L 111218 4812474 3C286 OQ208 J1219+4829
N 4192 12h13m48.s29 +14d54m01.s2 13.55V C 111229 4809749 3C286 OQ208 J1239+0730
L 111221 4807896 3C286 OQ208 J1254+1141
L 111230 4812476 3C286 OQ208 J1254+1141
N 4217 12h15m50.s90 +47d05m30.s4 20.6 C 111227 5062561 3C286 OQ208 J1219+4829
L 111218 4812474 3C286 OQ208 J1219+4829
N 4244* 12h17m29.s66 +37d48m25.s6 4.4* C 111217 4809751 3C286 OQ208 J1227+3635
L 111218 4812474 3C286 OQ208 J1227+3635
N 4302 12h21m42.s48 +14d35m53.s9 19.41V C 111219 5062559 3C286 OQ208 J1254+1141
L 111221 4807896 3C286 OQ208 J1254+1141
L 111230 4812476 3C286 OQ208 J1254+1141
N 4388 12h25m46.s75 +12d39m43.s5 16.6V C 111219 5062559 3C286 OQ208 J1254+1141
L 111221 4807896 3C286 OQ208 J1254+1141
L 111230 4812476 3C286 OQ208 J1254+1141
N 4438 12h27m45.s59 +13d00m31.s8 10.39V C 111219 5062559 3C286 OQ208 J1254+1141
L 111221 4807896 3C286 OQ208 J1254+1141
L 111230 4812476 3C286 OQ208 J1254+1141
N 4565* 12h36m20.s78 +25d59m15.s6 11.9* C 111229 4809749 3C286 OQ208 J1221+2813
L 111230 4812476 3C286 OQ208 J1221+2813
N 4594* 12h39m59.s43 -11d37m23.s0 12.7 C 111219 5062559 3C286 OQ208 J1246-0730
L 111230 4812476 3C286 OQ208 J1246-0730
N 4631* 12h42m08.s01 +32d32m29.s4 7.4* C 111229 4809749 3C286 OQ208 J1310+3220
L 111230 4812476 3C286 OQ208 J1221+2813
N 4666 12h45m08.s59 -00d27m42.s8 27.5 C 111219 5062559 3C286 OQ208 J1246-0730
L 111230 4812476 3C286 OQ208 J1246-0730
N 4845 12h58m01.s19 +01d34m33.s0 16.98V C 111219 5062559 3C286 OQ208 J1246-0730
L 111230 4812476 3C286 OQ208 J1246-0730
N 5084* 13h20m16.s92 -21d49m39.s3 23.4 C 111229 4809749 3C286 OQ208 J1248-1959
C 111213 4806011 3C286 OQ208 J1248-1959
C 111210 5062309 3C286 OQ208 J1248-1959
L 111230 4812476 3C286 OQ208 J1248-1959
N 5297 13h46m23.s68 +43d52m20.s5 40.4 C 111227 5062561 3C286 OQ208 J1327+4326
L 111218 4812474 3C286 OQ208 J1357+4353
N 5775 14h53m58.s00 +03d32m40.s1 28.9 C 111210 5062309 3C286 OQ208 J1445+0958
L 111230 4812476 3C286 OQ208 J1445+0958
N 5792 14h58m22.s71 -01d05m27.s9 31.7 C 111210 5062309 3C286 OQ208 J1505+0326
L 111230 4812476 3C286 OQ208 J1510-0543
N 5907* 15h15m53.s77 +56d19m43.s6 16.8* C 111227 5062561 3C286 OQ208 J1438+6211
L 111230 4812476 3C286 OQ208 J1438+6211
U 10288 16h14m24.s80 -00d12m27.s1 34.1 C 111210 5062309 3C286 OQ208 J1557-0001
L 111230 4812476 3C286 OQ208 J1557-0001

NOTE. - Observations of the galaxies, with the date, scheduling block identification number and primary, secondary and zero polarization leakage calibrators
a Large galaxies denoted with an asterisk were observed in two pointings in C-band
b Updated distances (see Sec. 2.1.2) derived with TGRB are shown with an asterisk. Virgo cluster galaxies are indicated with a V
c Alternate names for primary and leakage calibrators: 3C84 = J0319+4130, 3C286 = J1331+305, 3C48 = OQ208 = QSO B1404+2841 or J1407+2827

2.1.1. Sensitivity

The theoretical noise level is approximately 6 µJy/beam in C-band (with confusion limit and flagging taken into account). Due to a high uncertainty in confusion, the theoretical estimate for L-band of 89 µJy/beam is substantially higher than the actual value we achieved, which is around 30-35 µJy/beam. However, due to variable noise in the L-band, we measured the noise in areas far from the source where it was more uniform (see Sec. 4.1). Additionally, a few galaxies exhibit higher values for reasons outlined later in this paper.

2.1.2. Distances

We have made a few modifications to the distances used in Table 1 of Paper I. Five galaxies have had their distances modified, whereas the rest remain the same as listed in Paper I.

The five galaxies with modified distances are: NGC 891, NGC 4244, NGC 4565, NGC 4631, and NGC 5907. These were adjusted because they have distances derived from the Tip of the Red Giant Branch (TRGB) (Radburn-Smith et al. 2011). Because of the reliability of the TRGB method, and that it likely provides the best distances for edge-on systems, we have adopted those distances here. The most significant distance change was for NGC 4565, which went from a Hubble Flow distance of 27.1 Mpc to a TRGB distance of 11.9 Mpc. For the other four galaxies the changes were minor (see Table 1).

Of the remaining galaxies, the distances of the five Virgo cluster galaxies (denoted with V in Table 1) were adopted from Solanes et al. (2002).

All other galaxy distances were taken from NED, using the "Hubble flow corrected for Virgo and the Great Attractor" (HF) distance, and a Hubble constant of 73 km/s/Mpc. Since a Hubble flow method may not always be accurate for nearby galaxies at low heliocentric velocities, we reviewed the galaxy distances for this paper. We compared the HF distance with the median of various Tully-Fisher (TF) derived distances. The latter are listed in NED as "red-shift independent" distance derivations. Note that we excluded the "Tully 1988" values listed in NED since those are Hubble Flow based. For the majority of the galaxies, the changes between the two methods were well within the uncertainties associated with either method. In particular, it is not uncommon to find a factor 2 difference in the various TF-method published distances. We therefore retained the distances used in Paper I for these 25 systems. The comparison showed that for 16 galaxies the agreement between the adopted HF distance and the median TF distances was better than 25%, for 9 galaxies the difference was larger than 25%. The galaxies with the largest distance uncertainty (> 35%) include NGC 2683, NGC 3432, NGC 4666, NGC 5775, and NGC 5792. See Table 1 for our current distance list.

2.2. Observations

Of the 405 hours which were awarded for the entire CHANG-ES project, 65 hours were set apart for the D-configuration observations in two frequency bands, L and C. The observations were divided up into 13 scheduling blocks, each of which contained scans of one primary gain and phase calibrator (hereafter referred to as the primary calibrator) and one zero polarization calibrator to calibrate polarization leakage from the instrumentation. Additionally, complex gain calibrations were performed using a source (hereafter the secondary calibrator) less than 10 degrees from the target galaxy. The secondary calibrator was observed before and after the galaxy scans, every 20-25 minutes. The bulk of the data was observed during December 2011. Two scheduling blocks were re-observed in March 2013. See Table 1 for observation specifics. One scheduling block observed in C-band, ID 5062559, suffered increased antenna system temperatures at times coinciding with bad weather (snow). Consequently, the rms noises for galaxies NGC 4302, NGC 4388, NGC 4438, NGC 4594, NGC 4666 and NGC 4845 increased to approximately twice the theoretical expectation at C-band.

2.2.1. Large galaxies

Eight galaxies in the sample are too large to fit inside the primary beam of 7.5' FWHM at C-band. We thus observed these in two pointings, separated by half the diameter of the primary beam at half maximum, i.e. one quarter beam from the galaxy centre along the disk on either side of the centre. The two-pointing galaxies are marked with an asterisk beside their names in Table 1. Table 2 lists the coordinates for the separate pointings. One single pointing was sufficient for all galaixes in L-band, where the diameter of the primary beam is 30'.

Table 2. Two pointings of large galaxies

Galaxy RA 1 Dec 1 RA 2 Dec 2
1 2 3 4 5

N891 02h 22m 37.21s 42d 22m 41.2s 02h 22m 29.61s 42d 19m 12.6s
N3628 11h 20m 24.50s 13d 34m 55.7s 11h 20m 9.52s 13d 35m 50.1s
N4244 12h 17m 36.71s 37d 49m 40.9s 12h 17m 22.61s 37d 47m 10.3s
N4565 12h 36m 26.58s 25d 57m 54.7s 12h 36m 14.98s 26d 00m 36.6s
N4631 12h 42m 16.88s 32d 32m 37.2s 12h 41m 59.14s 32d 32m 21.6s
N4594 12h 40m 07.09s - 11d 37m 23.0s 12h 39m 51.77s - 11d 37m 23.0s
N5084 13h 20m 24.88s - 21d 49m 19.8s 13h 20m 8.96s - 21d 49m 58.8s
N5907 15h 15m 59.49s 56d 18m 1.6s 15h 15m 48.05 56d 21m 25.5s

NOTE. - Column 1: Galaxy name; Column 2: Right Ascension of pointing 1; Column 3: Declination of pointing 1; Column 4: Right Ascension of pointing 2; Column 5: Declination of pointing 2.

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