[1] J. S. Schwinger, “On gauge invariance and vacuum polarization,” Phys. Rev. 82, 664 (1951). DOI: 10.1103/PhysRev.82.664
[2] R. Sch¨utzhold, H. Gies, and G. Dunne, “Dynamically assisted Schwinger mechanism,” Phys. Rev. Lett. 101, 130404 (2008). DOI: 10.1103/PhysRevLett.101.130404
[3] C. K. Dumlu, “Quantum kinetic approach and the scattering approach to vacuum pair production,” Phys. Rev. D 179, 065027 (2009). DOI: 10.1103/PhysRevD.79.065027
[4] H. Gies and G. Torgrimsson, “Critical Schwinger pair production,” Phys. Rev. Lett. 116, 090406 (2016). DOI: 10.1103/PhysRevLett.116.090406
[5] C. Schneider and R. Sch¨utzhold, “Dynamically assisted Sauter-Schwinger effect in inhomogeneous electric fields,” JHEP 102, 164 (2016). DOI: 10.1007/JHEP02(2016)164
[6] A. Otto, D. Graeveling, and B. K¨ampfer, “Response of the QED(2) vacuum to a quench: Long-term oscillations of the electric field and the pair creation rate,” Plasma Phys. Control. Fusion 61, 074002 (2019). DOI: 10.1088/1361-6587/ab1a21
[7] I. A. Aleksandrov and C. Kohlf¨urst, “Pair production in temporally and spatially oscillating fields,” Phys. Rev. D 101, 096009 (2020). DOI: 10.1103/PhysRevD.101.096009
[8] J. Maldacena, “The Large N limit of superconformal field theories and supergravity”, Int. J. Theor. Phys. 38, 1113 (1999). DOI: 10.1023/A:1026654312961
[9] G. W. Semenoff and K. Zarembo, “Holographic Schwinger effect,” Phys. Rev. Lett. 107, 171601 (2011). DOI:10.1103/PhysRevLett.107.171601
[10] Y. Sato and K. Yoshida, “Potential analysis in holographic Schwinger effect,” JHEP 08, 002 (2013). DOI:10.1007/JHEP08(2013)002
[11] S. Bolognesi, F. Kiefer, and E. Rabinovici, “Comments on critical electric and magnetic fields from holography,” JHEP 01, 174 (2013). DOI: 10.1007/JHEP01(2013)174
[12] K. Hashimoto and T. Oka, “Vacuum instability in electric fields via AdS/CFT: Euler-Heisenberg Lagrangian and Planckian thermalization,” JHEP 10, 116 (2013). DOI:10.1007/JHEP10(2013)116
[13] Y. Sato and K. Yoshida, “Holographic Schwinger effect in confining phase,” JHEP 09, 134 (2013). DOI: 10.1007/JHEP09(2013)134
[14] J. Sadeghi, B. Pourhassan, S. Tahery, and F. Razavi, “Holographic Schwinger effect with a deformed AdS background,” Int. J. Mod. Phys. A 32, 1750045 (2017). DOI:10.1142/S0217751X17500452
[15] L. Shahkarami, M. Dehghani, and P. Dehghani, “Holographic Schwinger effect in a D-instanton background,” Phys. Rev. D 97, 046013 (2018). DOI: 10.1103/PhysRevD.97.046013
[16] L. Shahkarami and F. Charmchi, “Confining D-instanton background in an external electric field,” Eur. Phys. J. C 79, 343 (2019). DOI: 10.1140/epjc/s10052-019-6765-9
[17] Sw. Li, Sk. Luo, and Hq. Li, “Holographic Schwinger effect and electric instability with anisotropy,” JHEP 08, 206 (2022). DOI: 10.1007/JHEP08(2022)206
[18] K. Hashimoto, S. Kinoshita, K. Murata, and T. Oka, “Electric field quench in AdS/CFT,” JHEP 09, 126 (2014). DOI: 10.1007/JHEP09(2014)126
[19] S. Amiri-Sharifi, M. Ali-Akbari, and H. R. Sepangi, “Electric field quench, equilibration and universal behavior,” Phys. Rev. D 91, 126007 (2015). DOI: 10.1103/PhysRevD.91.126007
[20] M. Ali-Akbari, H. Ebrahim, and S. Heshmatian, “Thermal quench at finite t’Hooft coupling,” Nucl. Phys. B904, 527 (2016). DOI: 10.1016/j.nuclphysb.2016.02.003
[21] S. Amiri-Sharifi, M. Ali-Akbari, A. Kishani-Farahani, and N. Shafie, “Double relaxation via AdS/CFT,” Nucl. Phys. B909, 778 (2016). DOI: 10.1016/j.nuclphysb.2016.06.011
[22] M. Ali-Akbari and F. Charmchi, “Holographic equilibration under external dynamical electric field,” Phys. Lett. B 773, 271 (2017). DOI: 10.1016/j.physletb.2017.08.040
[23] L. Shahkarami and F. Charmchi, “Late time oscillations and universal behavior in pulsed electric fields,” [arXiv:2308.02218 [hep-th]]. DOI: 10.48550/arXiv.2308.02218
[24] T. Ishii, S. Kinoshita, K. Murata, and N. Tanahashi, “Dynamical meson melting in holography,” JHEP 04, 099 (2014). DOI: 10.1007/JHEP04(2014)099
[25] M. Ali-Akbari, F. Charmchi, A. Davody, H. Ebrahim, and L. Shahkarami, “Time-dependent meson melting in external magnetic field,” Phys. Rev. D 91, 106008 (2015). DOI: 10.1103/PhysRevD.91.106008
[26] T. Albash, V. G. Filev, C. V. Johnson, and A. Kundu, “Quarks in an external electric field in finite temperature large-N gauge theory,” JHEP 08, 092 (2008). DOI:10.1088/1126-6708/2008/08/092
[27] J. Erdmenger, R. Meyer, and J. P. Shock, “AdS/CFT with flavour in electric and magnetic Kalb-Ramond fields,” JHEP 12, 091 (2007). DOI: 10.1088/1126-6708/2007/12/091