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Table 3

WSRT H i properties.

HVC name AGC RA+Dec cz W50 θhf SHI NHI,peak
210′′ 210′′ 105′′ 60′′ 210′′ 105′′ 60′′
J2000 km s-1 km s-1 Jy km s-1 1019 atoms cm-2
(1) (2) (3) (4) (5) (6) (7) (8)

HVC214.78+42.45+47 198606 093002.8+163813 51 24 11.4 15.3 14.0 11.8 4.2 4.9 6.1
HVC204.88+44.86+147 198511 093017.2+241119 151 15 7.0 0.86 0.78 ... 0.59 0.98 ...
HVC205.83+45.14+173 198683 093212.8+233348 176 23 8.2 0.63 0.42 ... 0.46 1.2 ...
HVC217.77+58.67+96 208747 103710.0+203214 96 19 6.8 1.69 1.57 ... 1.1 1.6 ...
HVC212.68+62.39+64 208753 104931.8+235526 65 24 10.6 3.32 3.1 ... 0.93 1.4 ...
HVC230.27+71.10+76 219663 113422.1+201212 73 13 5.8 0.65 0.49 ... 0.68 1.1 ...
HVC235.38+74.79+195 219656 115123.7+203403 191 28 8.0 1.22 1.09 ... 0.67 1.2 ...
HVC271.57+79.03+248 229326 122735.5+173852 239 22 5.5 0.63 0.58 ... 0.63 1.0 ...
HVC276.53+79.84+255 229327 123223.6+175522 253 17 8.8 0.62 0.62 ... 0.38 0.88 ...
HVC028.09+71.87-142 249393 ... ... ... ... ... ... ... 0.34a ... ...
HVC011.76+67.89+60 249525 141752.7+173240 47 18 6.8 5.12 4.85 4.64 3.6 4.8 5.4
HVC015.96+63.90+44 249565 143556.3+170847 29 18 5.4 1.69 1.74 1.6 1.8 2.9 4.0

Notes. Table columns are as follows: Col. 1: the HVC name of the source as for Table 1; Col. 2: AGC number as in Table 1; Col. 3: equatorial coordinates of the H i centroid (epoch J2000) for the 210′′ WSRT data, derived using the task maxfit in Miriad; Col. 4: heliocentric recessional velocity, derived from Gaussian fitting to the WSRT 210′′ spectrum; Col. 5: full width at half maximum of the WSRT 210′′ spectrum, derived from Gaussian fitting; Col. 6: effective half-flux radius in arcminutes, derived as discussed in Sect. 2.2; Col. 7: integrated flux density for each angular resolution, calculated as discussed in Sect. 2.2. The uncertainty is taken to be 10%; Col. 8: peak NHI for each angular resolution in units of 1019 atoms cm-2.

(a)

This source is a non-detection; the peak column density value is based on the moment zero map of the dirty data.

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