On the Schwinger limit attainability with extreme power lasers
On the Schwinger limit attainability with extreme power lasers
On the Schwinger limit attainability with extreme power lasers
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The pairs are created in a small 4-volume near <strong>the</strong> electric field maximum<br />
(maximum of F ) <strong>with</strong> <strong>the</strong> characteristic size<br />
TM<br />
Here normalized <strong>Schwinger</strong> field is<br />
5 a <br />
16 aS 3/ 2 4<br />
2 0 0<br />
0 0 0 5<br />
r z ct<br />
2<br />
mc e 5.110 <br />
Integrating over <strong>the</strong> 4-volume <strong>the</strong> probability of <strong>the</strong> pair creation<br />
we obtain <strong>the</strong> number of pairs produced per wave period,<br />
a<br />
S<br />
0<br />
3/ 2<br />
5 4 a S<br />
N W<br />
dVdt a 3 0 exp<br />
e e e e<br />
<br />
4<br />
a<br />
The first pairs can be observed for an one-micron wavelength laser intensity of <strong>the</strong> order of<br />
27 2<br />
10 W/cm , which corresponds to a0 / aS0.05 , i.e. a characteristic size, 0 ,<br />
Is approximately equal to<br />
r<br />
0.04<br />
0<br />
5<br />
2<br />
F a<br />
TM /<br />
0 <br />
2<br />
z0<br />
r0