10 - H1 - Desy
10 - H1 - Desy
10 - H1 - Desy
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8.3 Error matrix evaluation 111<br />
expansion series:<br />
U i,j = ∑ k,l<br />
∣<br />
∂η i ∂η j<br />
Vk,l ∂θ k ∂θ l<br />
∣∣∣∣ˆθ<br />
θ (8.24)<br />
with ˆθ being the estimator of θ and V θ k,l = cov|θ k, θ l |. In the case of this analysis ⃗η = ⃗x true ,<br />
while m × n A i,j elements of migration matrix A (m×n) are used as variables θ. In such a<br />
case, using the equation 8.11 one can calculate derivatives:<br />
∂η i<br />
∂θ k<br />
≡ ∂xi true<br />
∂A p,q<br />
= (E u ) i,p × (V(⃗y obs − A⃗x true )) q − (E u A T V) i,q × (⃗x true ) p , (8.25)<br />
where indices i and p run over unfolding output bins and q runs over input bins.<br />
The covariance matrix U takes then the form:<br />
U i,j = ∑ p,q<br />
∑<br />
r,s<br />
∣<br />
∂x i true ∂x j ∣∣∣∣Â<br />
true<br />
V(p,q),(r,s) A ∂A p,q ∂A , (8.26)<br />
r,s<br />
where indices i, j, p and r run over unfolding output bins, while q and s are input bin<br />
indices.<br />
8.3.1 MC statistics error propagation<br />
The migration matrix as used in this analysis needs to be sufficiently populated to avoid<br />
large statistical fluctuations in the determination of the matrix itself. Special care was<br />
taken to include the MC statistical fluctuations in the final errors. The error originating<br />
from the limited statistics of the MC is calculated with each migration matrix element<br />
treated as independent source of uncorrelated error. In such a case the covariance matrix<br />
V A (p,q),(r,s) takes the form V A (p,q),(r,s) = {<br />
0 if (p, q) ≠ (r, s)<br />
σ 2 p,q if (p, q) = (r, s)<br />
(8.27)<br />
where σ 2 p,q is the statistical error of the element A p,q . The equation 8.26 simplifies to<br />
U i,j = ∑ p,q<br />
∂η i<br />
∂A p,q<br />
∣<br />
∂η ∣∣∣∣Â<br />
j<br />
σp,q 2 ≡ E mc (8.28)<br />
∂A p,q<br />
In practice, since migration matrix is normalised, two errors are propagated. One coming<br />
from the matrix binomial error and the second, originating from the limited statistics of<br />
the normalisation factor.<br />
The MC statistical error contributes to at most <strong>10</strong>% of the final error in the low η γ -high<br />
E γ T<br />
region. Typically it is consistently below 5% of the final error and thus considered to<br />
be reduced to negligible level over the whole studied phase space.