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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

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