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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.

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