We show that the distribution in the J − W1 colour for spectroscopic quasars, stars and non-ids. At two different cuts, the distribution of the non-ids more closely follows that for quasars. As such, we infer that the greater part of the non-identified sources are quasars that are not positively identified by our spectroscopic observations.
. | QSO . | Stars . | Non-id . |
---|---|---|---|
. | (0.8 < z < 2.5) . | . | . |
J − W1 > 1.5 | 98 per cent (3583) | 22 per cent(126) | 92 per cent(1311) |
J − W1 < 1.5 | 2 per cent (2) | 78 per cent(460) | 8 per cent(111) |
J − W1 > 2 | 83 per cent | 13 per cent | 80 per cent |
J − W1 < 2 | 17 per cent | 87 per cent | 20 per cent |
. | QSO . | Stars . | Non-id . |
---|---|---|---|
. | (0.8 < z < 2.5) . | . | . |
J − W1 > 1.5 | 98 per cent (3583) | 22 per cent(126) | 92 per cent(1311) |
J − W1 < 1.5 | 2 per cent (2) | 78 per cent(460) | 8 per cent(111) |
J − W1 > 2 | 83 per cent | 13 per cent | 80 per cent |
J − W1 < 2 | 17 per cent | 87 per cent | 20 per cent |
We show that the distribution in the J − W1 colour for spectroscopic quasars, stars and non-ids. At two different cuts, the distribution of the non-ids more closely follows that for quasars. As such, we infer that the greater part of the non-identified sources are quasars that are not positively identified by our spectroscopic observations.
. | QSO . | Stars . | Non-id . |
---|---|---|---|
. | (0.8 < z < 2.5) . | . | . |
J − W1 > 1.5 | 98 per cent (3583) | 22 per cent(126) | 92 per cent(1311) |
J − W1 < 1.5 | 2 per cent (2) | 78 per cent(460) | 8 per cent(111) |
J − W1 > 2 | 83 per cent | 13 per cent | 80 per cent |
J − W1 < 2 | 17 per cent | 87 per cent | 20 per cent |
. | QSO . | Stars . | Non-id . |
---|---|---|---|
. | (0.8 < z < 2.5) . | . | . |
J − W1 > 1.5 | 98 per cent (3583) | 22 per cent(126) | 92 per cent(1311) |
J − W1 < 1.5 | 2 per cent (2) | 78 per cent(460) | 8 per cent(111) |
J − W1 > 2 | 83 per cent | 13 per cent | 80 per cent |
J − W1 < 2 | 17 per cent | 87 per cent | 20 per cent |
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