Abstract
We propose to investigate the THz emission using laser–plasma interaction, when two X-mode lasers beat and interact with inhomogeneous plasmas. Pulse steepness varies from slow rise and fall to the steep rise and steep fall in spatial electric field envelope as Gaussian pulse changes into non-Gaussian (triangular and round triangular) laser pulse. X-mode of Gaussian (G), round triangular (RT) and triangular (T) laser pulses are used to investigate the THz emission. THz amplitude varies with magnetic field, transverse distance and resonance frequency. THz radiation intensifies and attains peak value at resonance condition. For exact phase matching condition, THz efficiency of the order of \({10}^{-4}\) can be achieved for Gaussian pulses. X-mode lasers are more favourable to produce high-amplitude THz radiations in comparison with ordinary laser mode. Present study concludes that Gaussian and non-Gaussian laser pulses influence THz emission differently in ordinary and extraordinary laser modes.
Similar content being viewed by others
References
D Dragoman and M Dragoman Prog. Quantum Electron. 28 1 (2004)
B Ferguson and X C Zhang Nat. Mater. 1 26 (2002)
Z D Taylor et al IEEE Trans. THz Sci. Tech. 1 201 (2011)
R A Lewis J. Phys. D Appl. Phys. 47 374001 (2014)
M Nagai, E Matsubara and M Ashida IEEE Trans. THz Sci. Tech. 4 440 (2014)
H Hamster and A Sullivan IEEE Trans. Plasma Sci. Phys. Rev. E 49 671 (1994)
L Bhasin and V K Tripathi Phys. Plasmas 16 103105 (2009)
Z Wu et al Rev. Sci. Instrum. 84 2701 (2013)
A Houard, Y Liu, B Prade, V T Tikhonchuk and A Mysyrowicz Phys. Rev. Lett. 100 255006 (2008)
A G Stepanov Phys. Lett. 83 3000 (2003)
A G Stepanov Appl. Phys. B 81 23 (2005)
K Y Kim, A Taylor, J Glownia and G Rodriguez Nat. Photon. 2 605 (2008)
H Hamster, A Sullivan and S Gordon Phys. Rev. Lett. 71 2725 (1993)
Z M Sheng, K Mima, J Zhang and H Sanuki Phys. Rev. Lett. 94 095003 (2005)
Z M Sheng, K Mima and J Zhang Phys. Plasmas. 12 123103 (2005)
J Yoshii, C H Lai and T Katsouleas Phys. Rev. Lett. 79 4194 (1997)
G Brodin and J Lundberg Phys. Rev. E 57 7041 (1998)
M Singh and R P Sharma Contrib. Plasma Phys. 53 540 (2013)
P Varshney, A Upadhayay and K Madhubabu Laser Part. Beams 36 236 (2018)
D Singh and H K Malik Phys. Plasmas. 21 083105 (2014)
M H Cho, Y K Kim, H Suk, B Ersfeld, D A Jaroszynski and M.S Hur New J. Phys. 17 043045 (2015)
I Babushkin et al. Phys. Rev. Lett. 105 053903 (2010)
S Saxena, S Bagchi, B S Rao, P A Naik and J A Chakera IEEE Trans. Terahertz Sci. Technol. 8 528 (2018)
K Gopal, D N Gupta and H Suk IEEE Trans. Plasma Sci. 49 1152 (2021)
K Gopal, D N Gupta, A Jain, M H Hur and H Suk Current Appl. Phys. 25 82(2021)
G L Carr, M C Martin, W R McKinney, K Jordan, G R Neil and G P Williams Nature 420 153 (2002)
C Li et al Opt. Express 22 11797 (2014)
A Sagisaka et al Appl. Phys. B 90 373 (2008)
A Gopal et al Opt. Lett. 38 4705 (2013)
M C Gurjar, K Gopal, D N Gupta, V V Kulagin and H Suk IEEE Trans. Plasma Sci. 48 3727 (2020)
M C Gurjar, K Gopal, D N Gupta and V V Kulagin Euro Phys. Lett. 13314001(2021)
P Varshney, K Gopal and A Upadhyaay Laser Phys. Lett. 17 126002 (2020)
D N Gupta and A Jain Optik 227 165824 (2021)
C H Pai et al. Phys. Plasmas 12 070707 (2005)
R Gill and H K Malik Phys. Lett. A 383 2891 (2019)
K Gopal, M A Raja and D N Gupta Indian J. Phys. 92 919 (2018)
K Gopal, D N Gupta, Y K Kim, M S Hur, and H Suk J. Appl. Phys. 119 123101 (2016)
R K Singh, M Singh, S K Rajouria, and R P Sharma Phys. Plasmas 24 103103 (2017)
T M Antonsen Jr, J Palastra, H M Milchberg Phys. Plasmas 14 033107 (2007)
Author information
Authors and Affiliations
Corresponding author
Additional information
Publisher's Note
Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Rights and permissions
About this article
Cite this article
Pushplata, Varshney, P., Gopal, K. et al. THz emission with X-mode laser pulses. Indian J Phys 96, 3015–3022 (2022). https://doi.org/10.1007/s12648-021-02219-6
Received:
Accepted:
Published:
Issue Date:
DOI: https://doi.org/10.1007/s12648-021-02219-6