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001 | 202644 | ||
005 | 20220930130044.0 | ||
024 | 7 | _ | |a 10.1103/PhysRevLett.114.253901 |2 doi |
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024 | 7 | _ | |a 1079-7114 |2 ISSN |
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100 | 1 | _ | |a Wang, W.-M. |0 P:(DE-Juel1)161531 |b 0 |e Corresponding author |u fzj |
245 | _ | _ | |a Tunable Circularly Polarized Terahertz Radiation from Magnetized Gas Plasma |
260 | _ | _ | |a College Park, Md. |c 2015 |b APS |
336 | 7 | _ | |a Journal Article |b journal |m journal |0 PUB:(DE-HGF)16 |s 1436791605_20875 |2 PUB:(DE-HGF) |
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336 | 7 | _ | |a article |2 DRIVER |
520 | _ | _ | |a It is shown, by simulation and theory, that circularly orelliptically polarized terahertz radiation can be generated when astatic magnetic (B) field is imposed on a gas target along thepropagation direction of a two-color laser driver. The radiationfrequency is determined by $\sqrt{\omega_p^2+{\omega_c^2}/{4}} +{\omega_c}/{2}$, where $\omega_p$ is the plasma frequency and$\omega_c$ is the electron cyclotron frequency. With the increase ofthe B field, the radiation changes from a single-cycle broadbandwaveform to a continuous narrow-band emission. In high-B-fieldcases, the radiation strength is proportional to$\omega_p^2/\omega_c$. The B field provides a tunability in theradiation frequency, spectrum width, and field strength. |
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700 | 1 | _ | |a Gibbon, P. |0 P:(DE-Juel1)132115 |b 1 |u fzj |
700 | 1 | _ | |a Sheng, Z.-M. |0 P:(DE-HGF)0 |b 2 |
700 | 1 | _ | |a Li, Y.-T. |0 P:(DE-HGF)0 |b 3 |
773 | _ | _ | |a 10.1103/PhysRevLett.114.253901 |g Vol. 114, no. 25, p. 253901 |0 PERI:(DE-600)1472655-5 |n 25 |p 253901 |t Physical review letters |v 114 |y 2015 |x 1079-7114 |
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