Abstract

We consider time delay for the Dirac equation. A new method to calculate the asymptotics of the expectation values of the operator ∫0∞eiH0tζ(∣x∣R)e−iH0tdt,\int\limits_{0} ^{\infty}e^{iH_{0}t}ζ\left( \frac{\left\vert x\right\vert }{R}\right) e^{-iH_{0}t}dt, as R→∞,R\rightarrow\infty, is presented. Here H0H_{0} is the free Dirac operator and ζ(t)ζ\left( t\right) is such that ζ(t)=1ζ\left( t\right) =1 for 0≤t≤10\leq t\leq1 and ζ(t)=0ζ\left( t\right) =0 for t>1.t>1. This approach allows us to obtain the time delay operator δT(f)δ\mathcal{T}\left( f\right) for initial states ff in H23/2+ε(R3;C4),\mathcal{H} _{2}^{3/2+\varepsilon}\left( \mathbb{R}^{3};\mathbb{C}^{4}\right) , ε>0,\varepsilon>0, the Sobolev space of order 3/2+ε3/2+\varepsilon and weight 2.2. The relation between the time delay operator δT(f)δ\mathcal{T}\left( f\right) and the Eisenbud-Wigner time delay operator is given. Also, the relation between the averaged time delay and the spectral shift function is presented.

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