| Hauptseite > Publikationsdatenbank > Tunable Circularly Polarized Terahertz Radiation from Magnetized Gas Plasma > print |
| 001 | 202644 | ||
| 005 | 20260127142650.0 | ||
| 024 | 7 | _ | |2 doi |a 10.1103/PhysRevLett.114.253901 |
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| 100 | 1 | _ | |0 P:(DE-Juel1)161531 |a Wang, W.-M. |b 0 |e Corresponding author |u fzj |
| 245 | _ | _ | |a Tunable Circularly Polarized Terahertz Radiation from Magnetized Gas Plasma |
| 260 | _ | _ | |a College Park, Md. |b APS |c 2015 |
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| 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 | _ | |0 P:(DE-HGF)0 |a Sheng, Z.-M. |b 2 |
| 700 | 1 | _ | |0 P:(DE-HGF)0 |a Li, Y.-T. |b 3 |
| 773 | _ | _ | |0 PERI:(DE-600)1472655-5 |a 10.1103/PhysRevLett.114.253901 |g Vol. 114, no. 25, p. 253901 |n 25 |p 253901 |t Physical review letters |v 114 |x 1079-7114 |y 2015 |
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