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The creation of positron and electron pairs through photon-photon collision, named Breit-Wheeler process, has been well understood in the theories of quantum electrodynamics for nearly 100 years. The photon-photon collision, which is one of the most basic processes of matter generation in the universe, has not been observed yet. The study on photon-photon collision can promote the development of two-photon physics, quantum electrodynamics theories and high energy physics. To observe photon-photon collision in the laboratory, one needs to collimate a huge number of energetic γ-ray photons into a very small spot. Recently, the development of highly collomated source generated by 10 PW laser makes photon-photon collider much more possible than before. In photon-photon collider, the study of numerical simulation plays a critical role since no experiment has achieved such a process. In this paper, a new numerical method is developed to handle the two-photon Breit-Wheeler process. This method is based on the exact two-photon collision dynamic principle, including energy threshold condition, cross-section condition, Lorentz transformation, etc. In the method, the photons are divided into quantitative photon blocks based on the spatial coordinates. Firstly, one needs to find the collision blocks according to the spatial motion law. Secondly, the ergodic method is used to look up the photons that satisfy the energy threshold condition and the cross-section condition from the blocks. Then, one can calculate the electron yield of the photon collision, and the kinetic parameters of the positrons and electrons. This method rigorously follows the physical principle so it has high precision. On the other hand, this method determines the collision of the block in advance, which can reduce the computational requirement a lot. A series of tests is carried out to confirm the accuracy and feasibility of this numerical method by calculating the collision between mono-energetic photon beams. In the tests, the collision angle is assumed to 180° and 60° separately, the results of pair momentum distribution are discussed. We also simulate the collision of the γ-ray beams generated through the interaction between ultra-intense laser and narrow tube targets. In the simulations, the collision angle is changed from 170° to 30° to see its effect on pair production. It is found that the yield of electron-positron pairs decreases with collision angle increasing, which has also been reported in previous work. Therefore, this numerical method can be efficiently used for modeling photon-photon collider, and provide theoretical reference and suggestion to the future experimental design of γ-ray collision.
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Keywords:
- photon collider /
- electron-positron pairs /
- Breit-Wheeler process /
- threshold energy
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[10] Yu J Q, Hu R H, Gong Z, Ting A, Najmudin Z, Wu D, Lu H Y, Ma W J, Yan X Q 2018 Appl. Phys. Lett. 112 204103Google Scholar
[11] Yu T P, Pukhov A, Sheng Z M, Liu F, Shvets G 2013 Phys. Rev. Lett. 110 045001Google Scholar
[12] Stark D J, Toncian T, Arefiev A V 2016 Phys. Rev. Lett. 116 185003Google Scholar
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[35] Huang T, Zhou C, Zhang H, Wu S, Qiao B, He X, Ruan S 2017 Appl. Phys. Lett. 110 021102Google Scholar
[36] Shen B, Bu Z, Xu J, Xu T, Ji L, Li R, Xu Z 2018 Plasma Phys. Controlled Fuison 60 044002Google Scholar
[37] Ribeyre X, d’Humi`eres E, Jansen O, Jequier S, Tikhonchuk V T, Lobet M 2016 Phys. Rev. E 93 013201Google Scholar
[38] Jansen O, d’Humi`eres E, Ribeyre X, Jequier S, Tikhonchuk V T 2018 J. Comput. Phys. 355 582
[39] Pike O J, Mackenroth F, Hill E G, Rose S J 2014 Nat. Photonics 8 434Google Scholar
[40] Ribeyre X, d’Humi`eres E, Jansen O, Jequier S, Tikhonchuk V T 2017 Plasma Phys. Controlled Fusion 59 014024Google Scholar
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[1] Marklund M, Shukla P K 2006 Rev. Mod. Phys. 78 591Google Scholar
[2] Ehlotzky F, Krajewska K, Kamiński J 2009 Rep. Prog. Phys. 72 046401Google Scholar
[3] Piazza A D, Müller C, Hatsagortsyan K Z, Keitel C H 2012 Rev. Mod. Phys. 84 1177Google Scholar
[4] 黄金书, 罗鹏晖, 鲁公儒 2009 物理学报 58 12
Huang J S, Luo P H, Lu G R 2009 Acta Phys. Sin. 58 12
[5] Burke D L, Field R C, Smith G H, Spencer J E, Walz D 1997 Phys. Rev. Lett. 79 1626Google Scholar
[6] Breit G, Wheeler J A 1934 Phys. Rev. 46 1087Google Scholar
[7] Yu J Q, Lu H Y, Takahashi T, Hu R H, Gong Z, Ma W J, Huang Y S, Chen C E, Yan X Q 2019 Phys. Rev. Lett. 122 014802Google Scholar
[8] 周美林, 颜学庆 2015 物理 44 281Google Scholar
Zhou M L, Yan X Q 2015 Physics 44 281Google Scholar
[9] Brady C S, Ridgers C, Arber T, Bell A R 2013 Plasma. Phys. Controlled Fusion 55 124016Google Scholar
[10] Yu J Q, Hu R H, Gong Z, Ting A, Najmudin Z, Wu D, Lu H Y, Ma W J, Yan X Q 2018 Appl. Phys. Lett. 112 204103Google Scholar
[11] Yu T P, Pukhov A, Sheng Z M, Liu F, Shvets G 2013 Phys. Rev. Lett. 110 045001Google Scholar
[12] Stark D J, Toncian T, Arefiev A V 2016 Phys. Rev. Lett. 116 185003Google Scholar
[13] Capdessus R, Humi`eres E, Tikhonchuk V T 2013 Phys. Rev. Lett. 110 215003Google Scholar
[14] Brady C S, Ridgers C P, Arber T D, Bell A R, Kirk J G 2012 Phys. Rev. Lett. 109 245006Google Scholar
[15] Nakamura T, Koga J K, Esirkepov T Z, Kando M, Korn G, Bulanov S V 2012 Phys. Rev. Lett. 108 195001Google Scholar
[16] Yi L, Pukhov A, Thanh P L, Shen B 2016 Phys. Rev. Lett. 116 115001Google Scholar
[17] Ji L L, Snyder J, Pukhov A, Freeman R R, Akli K U 2016 Sci. Rep. 6 23256Google Scholar
[18] Zhu X L, Yu T P, Sheng Z M, Yin Y, Turcu I C E, Pukhov A 2016 Nat. Commun. 7 13686Google Scholar
[19] Liu J X, Ma Y Y, Yu T P, Zhao J, Yang X H, Zou D B, Zhang G B, Zhao Y, Yang J K, Li H Z, Zhuo H B, Shao F Q, Kawata S 2017 Chin. Phys. B 26 035202Google Scholar
[20] Geng P F, Lv W J, Li X L, Tang R A, Xue J K 2018 Chin. Phys. B 27 035201Google Scholar
[21] Zhang G B, Hafz N A M, Ma Y Y, Qian L J, Shao F Q, Sheng Z M 2016 Chin. Phys. Lett. 33 095202Google Scholar
[22] Zhu X L, Yin Y, Yu T P, Shao F Q, Ge Z Y, Wang W Q, Liu J J 2015 New J. Phys. 17 053039Google Scholar
[23] Liu J J, Yu T P, Yin Y, Zhu X L, Shao F Q 2016 Opt. Express 24 14
[24] Yu T P, Hu L X, Yin Y, Shao F Q, Zhuo H B, Ma Y Y, Yang X H, Luo W, Pukhov A 2014 Appl. Phys. Lett. 105 114101Google Scholar
[25] Luo W, Zhu Y B, Zhuo H B, Ma Y Y, Song Y M, Zhu Z C, Wang X D, Li X H, Turcu I, Chen M 2015 Phys. Plasmas 22 063112Google Scholar
[26] Luo W, Wu S D, Liu W Y, Ma Y Y, Li F Y, Yuan T, Yu J Y, Chen M, Sheng Z M 2018 Plasma Phys. Controlled Fusion 60 095006Google Scholar
[27] Chen L M, Yan W C, Li D Z, Hu Z D, Zhang L, Wang W M, Hafz N, Mao J Y, Huang K, Ma Y, Zhao J R, Ma J L, Li Y T, Lu X, Sheng Z M, Wei Z Y, Gao J, Zhang J 2013 Sci. Rep. 3 1912Google Scholar
[28] Wang W M, Sheng Z M, Gibbon P, Chen L M, Li Y T, Zhang J 2018 Proc. Natl. Acad. Sci. U.S.A. 115 9911Google Scholar
[29] Wang W M, Gibbon P, Sheng Z M, Li Y T, Zhang J 2017 Phys. Rev. E 96 013201Google Scholar
[30] Chen M, Luo J, Li F Y, Liu F, Sheng Z M, Zhang J 2016 Light-Sci. Appl. 5 e16015Google Scholar
[31] Liu J B, Yu J Q, Shou Y R, Wang D H, Hu R H, Tang Y H, Wang P J, Cao Z X, Mei Z S, Lin C, Lu H Y, Zhao Y Y, Zhu K, Yan X Q, Ma W J 2019 Phys. Plasmas 26 033109Google Scholar
[32] Gong Z, Hu R H, Lu H Y, Yu J Q, Wang D H, Fu E G, Chen C E, He X T, Yan X Q 2018 Plasma Phys. Controlled Fusion 60 044004Google Scholar
[33] H X Chang, B Qiao, Y X Zhang, Z Xu, W P Yao, C T Zhou, X T He 2017 Phys. Plasmas 24 043111Google Scholar
[34] Cristoforetti G, Londrillo P, Singh P K et al. 2017 Phys. Plasmas 7 1479Google Scholar
[35] Huang T, Zhou C, Zhang H, Wu S, Qiao B, He X, Ruan S 2017 Appl. Phys. Lett. 110 021102Google Scholar
[36] Shen B, Bu Z, Xu J, Xu T, Ji L, Li R, Xu Z 2018 Plasma Phys. Controlled Fuison 60 044002Google Scholar
[37] Ribeyre X, d’Humi`eres E, Jansen O, Jequier S, Tikhonchuk V T, Lobet M 2016 Phys. Rev. E 93 013201Google Scholar
[38] Jansen O, d’Humi`eres E, Ribeyre X, Jequier S, Tikhonchuk V T 2018 J. Comput. Phys. 355 582
[39] Pike O J, Mackenroth F, Hill E G, Rose S J 2014 Nat. Photonics 8 434Google Scholar
[40] Ribeyre X, d’Humi`eres E, Jansen O, Jequier S, Tikhonchuk V T 2017 Plasma Phys. Controlled Fusion 59 014024Google Scholar
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