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Nonperturbative signatures of nonlinear Compton scattering

机译:非线性康普顿散射的非触发性签名

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The probabilities of various elementary laser-photon-electron/positron interactions display in selected phase space and parameter regions typical nonperturbative dependencies such as ∝ P exp { ? a E crit / E } , where P is a preexponential factor, E crit denotes the critical Sauter-Schwinger field strength, and E characterizes the (laser) field strength. While the Schwinger process with a = a S ≡ π and the nonlinear Breit-Wheeler process in the tunneling regime with a = a n ? BW ≡ 4 m / 3 ω ′ (with ω ′ the probe photon energy and m the electron/positron mass) are famous results, we point out here that also the nonlinear Compton scattering exhibits a similar behavior when focusing on high harmonics. Using a suitable cutoff c > 0 , the factor a becomes a = a n ? C ≡ 2 3 c m / ( p 0 + p 0 2 ? m 2 ) . This opens the avenue toward a new signature of the boiling point of the vacuum even for field strengths E below E crit by employing a high electron beam-energy p 0 to counter balance the large ratio E crit / E by a small factor a to achieve E / a → E crit . In the weak-field regime, the cutoff facilitates a threshold leading to multiphoton signatures showing up in the total cross section at subthreshold energies.
机译:在所选相位空间和参数区域中的各种基本激光 - 光子 - 电子/正电子相互作用的概率和参数区域典型的非实际依赖性,如αpexp {? e CRIT / E},其中P是PREEXPONENTION系数,E CRIT表示临界沙油施韦格的场强,E表征(激光)场强。虽然Schwinger用A = A =π和隧道制度中的非线性Breen-Wheeler工艺,而A = a n? BW≡4 m /3Ω'(仪表探头光子能量和m电子/正电子质量)是着名的结果,我们在此指出,非线性康普顿散射在聚焦高谐波时也表现出类似的行为。使用合适的截止C> 0,因子A变为= a n? C≥23 C m /(p 0 + p 02≤m2)。即使通过采用高电子束能量P 0通过使用高电子束 - 能量P 0通过小因子A来计数平衡,将开启真空沸点的新标记为真空沸点的新签名。 E / A→e CRIT。在弱场制度中,截止促进了导致亚阈值能量的总横截面中显示的多光子签名的阈值。

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