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Astron. Astrophys. 358, 835-840 (2000)
3. Results of statistical tests
Before presenting the results of the statistical tests, it is
immediately clear from Table 1 that radio-intermediate and
radio-loud BAL QSOs are not the most polarized objects. Among the five
radio-loud BAL QSOs from Brotherton et al. (1998), only one,
J1053-0058, which belongs to the LIBAL class, is significantly
polarized with . It is particularly
interesting to note that J1053-0058 has the smallest detachment index
among the radio-loud BAL QSOs, in good agreement with the
anticorrelation between and DI found
in
Paper I 2.
Since and
are often upper limits, the search
for possible correlations between
(or ) and other BAL QSO properties
must rely on survival analysis. We then use the standard survival
analysis tests available in the ASURV Rev. 1.3 package (LaValley
et al. 1992). Several sub-samples are considered: LIBAL QSOs, HIBAL
QSOs, and BAL QSOs with . The latter
limit corresponds to the redshift at which the
BAL starts to be detected in the
visible. Probabilities (P) that the observed statistics occur
by chance among indices uncorrelated with
are summarized in Table 3,
using the generalized Kendall and
Spearman rank order correlation
coefficients, and the Cox proportional hazard model (LaValley et al.
1992, Isobe et al. 1986). Results from Table 3 indicate that
is essentially uncorrelated with the
other quantities ( 0.05), except
within the LIBAL QSO sub-sample. The statistical analysis includes the
few radio-loud BAL QSOs. Indeed, these objects, although formally
radio-loud, are not powerful radio-sources and mostly in the
radio-quiet / radio-loud transition region. However, since the
original suggestion by Goodrich (1997) only includes formally
radio-intermediate objects, we have also considered the sample of BAL
QSOs with . In this case, the results
of Table 3 are basically unchanged, P being only slightly
higher for the weak correlations detected in the LIBAL QSO sub-sample.
Finally the same statistical analysis has been carried out considering
instead of
, with the result that
is totally uncorrelated with the
other quantities, whatever the sub-sample.
![[TABLE]](img51.gif)
Table 3. Analysis of correlation of various indices with .
Notes:
This table gives the probabilities that the observed statistics (Cox, Kendall, Spearman) occur by chance among uncorrelated quantities. n is the number of objects considered in the correlation analysis, and m the number of objects with upper limits. The sign of the correlation is also given, from the sign of the Spearman . The three less accurate values of are considered as detections, although the results are unchanged if they are not taken into account. The Cox model cannot be used to test correlations with , since is also left-censored. Some results, obtained with very few detections and given here for completeness, must be seen with caution
Within the LIBAL QSO sub-sample, the statistical tests suggest the
existence of a weakly significant anticorrelation between
and
( 0.05 for all tests), and a
marginally significant anticorrelation between
and
( 0.05 for only one test). We have
therefore plotted and
against
in Figs. 1 and 2. The
anticorrelations do not appear very convincing. And indeed, if we
delete only one object from the LIBAL QSO sub-sample (e.g. B2225-0534
in Fig. 1, and J1053-0058 in Fig. 2), the statistical tests indicate
that the correlations are not significant any longer. Further, if one
restricts the LIBAL QSO sub-sample to high-redshift objects
( ), the correlation between
and
disappears ( 0.35 with n/m = 15/9),
suggesting a possible bias. Note that due to the limited sample of
LIBAL QSOs, no distinction between LIBAL sub-types was made.
![[FIGURE]](img58.gif) |
Fig. 1. The BAL QSO polarization, , is plotted here against the radio-to-optical flux ratio, . Censored data points are indicated. Open squares represent HIBAL QSOs, filled squares LIBAL QSOs, and squares with a cross unclassified BAL QSOs
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![[FIGURE]](img66.gif) |
Fig. 2. The BAL maximum velocity, , is plotted here against the radio-to-optical flux ratio, . Censored data points are indicated. Open squares represent HIBAL QSOs, filled squares LIBAL QSOs, and squares with a cross unclassified BAL QSOs
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In view of the apparently different behavior of LIBAL QSOs, we have
also compared the distribution of
for the LIBAL and HIBAL QSO sub-samples, again using standard survival
analysis tests from the ASURV package. Tests include the Logrank test,
and the Gehan, Peto & Peto, and Peto & Prentice generalized
Wilcoxon tests (LaValley et al. 1992, Feigelson et al. 1985). The
probability that the two samples (25 HIBALs and 21 LIBALs) are drawn
from the same parent population is found to range from 0.06 to 0.09,
depending on the test. This means that no significant difference in
the distribution of is detected when
comparing the LIBAL and HIBAL QSO sub-samples.
© European Southern Observatory (ESO) 2000
Online publication: June 20, 2000
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