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Christoph Florian Schaller - FU Berlin, FB MI

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<strong>Christoph</strong> <strong>Schaller</strong> - STORMicroscopy 26<br />

Here M rot is an arbitrary rotation matrix and as already mentioned −→ x n does not denote the<br />

localization of a spot in frame n, but a mean localization of the surrounding frames. Now every<br />

assigned pair ( −→ x n , x<br />

−−→<br />

n+1 ) provides two equations to estimate the six parameters<br />

−→ v =<br />

(<br />

)<br />

v 1<br />

v 2<br />

and M rot =<br />

(<br />

)<br />

m 1 m 2<br />

.<br />

m 3 m 4<br />

of the drift −−→ x n+1 − −→ x n . Hence we need to locate at least three beads in the surrounding frames. In case<br />

of more localizations we calculate the linear least squares t since the drift is no longer parameterdependant<br />

in a non-linear way.<br />

At this point we only have to describe how to obtain such a t. Assume i ∈ N equations<br />

a i,1 λ 1 + a i,2 λ 2 + ... + a i,k λ k = b i<br />

for known right hand sides b i and factors a i,k are given and we want to estimate the k ∈ N unknowns<br />

λ k ∈ R. This can be accomplished by minimizing the error in the Euclidean norm, i.e.<br />

||b − Aλ|| 2 ≤ ||b − Av|| 2 ∀v ∈ R k .<br />

Now according to [18], Theorem 2.14, λ ∈ R k is a minimizer, if and only if<br />

A T Aλ = A T b (5.2)<br />

Furthermore it is unique if A is injective.<br />

In our case the right hand sides are the occuring drifts, the unknowns are the free parameters and<br />

the respective factors follow from (5.1):<br />

(<br />

) (<br />

b 2i<br />

:=<br />

b 2i+1<br />

) (<br />

x n+1,i<br />

−<br />

y n+1,i<br />

λ := (v 1 , v 2 , m 1 , m 2 , m 3 , m 4 ),<br />

a 2i := (1, 0, x n,i , y n,i , 0, 0) and<br />

a 2i+1 := (0, 1, 0, 0, x n,i , y n,i ).<br />

)<br />

x n,i<br />

,<br />

y n,i<br />

As we will not locate two spots in the exact same place A is obviously injective and thus a unique<br />

minimizer is given by (5.2), which can be evaluated using basic linear algebra.

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