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“k10031final” — 2009/4/6 — 12:30 — page 85 — #93
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4.4. ERRORS IN MEASUREMENTS 85
that give numerical estimates of θ
2
values in different applications).
Under these assumptions, the actual observations S
Pi
and S
Ni
have
variance σ
2
(1 + θ
2
) rather than σ
2
, and hence
AUC
=Φ
μ
P
−μ
N
[2σ
2
(1 + θ
2
)]
.
A confidence interval can thus be constructed in the usual way starting
from AUC
(e.g., by using the method of Owen et al., 1964), and this
interval has limits Φ(δ
L
), Φ(δ
U
)whereδ
L
,δ
U
are the lower and upper
confidence limits for μ
P
− μ
N
. Thus, to take measurement errors into
account, δ
L
and δ
U
must both be multiplied by
√
1+θ
2
, and the limits
for AUC altered according ...