Project supported by the National Natural Science Foundation of China (Grant Nos. 11574105, and 61475054) and the Fundamental Research Funds for the Central Universities, China (Grant No. 2017KFYXJJ029).
Project supported by the National Natural Science Foundation of China (Grant Nos. 11574105, and 61475054) and the Fundamental Research Funds for the Central Universities, China (Grant No. 2017KFYXJJ029).
† Corresponding author. E-mail:
Project supported by the National Natural Science Foundation of China (Grant Nos. 11574105, and 61475054) and the Fundamental Research Funds for the Central Universities, China (Grant No. 2017KFYXJJ029).
The mechanism of terahertz (THz) pulse generation with a static magnetic field imposed on a gas plasma is theoretically investigated. The investigation demonstrates that the static magnetic field alters the electron motion during the optical field ionization of gas, leading to a two-dimensional asymmetric acceleration process of the ionized electrons. Simulation results reveal that elliptically or circularly polarized broadband THz radiation can be generated with an external static magnetic field imposed along the propagation direction of the two-color laser. The polarization of the THz radiation can be tuned by the strength of the external static magnetic field.
In 1993, Hamster firstly observed sub-picosecond (ps) terahertz (THz) pulses from gas-plasma produced by single-color femtosecond (fs) laser.[1] Since then, more plasma-based THz generation schemes, such as external DC-bias, two-color fields and few-cycle pulses, have been reported.[2–4] Thanks to the development of laser pulses with higher power and shorter pulse-width, the THz peak electric field strength has exceeded few MV/cm and the bandwidth has reached up to 200 THz.[5,6] Thus gas plasma-based THz generation schemes are widely used in the laboratory today, and even commercial products have appeared.
Among these mentioned methods, the two-color experimental scheme, firstly reported by Cook et al. in 2000,[7] i.e., using a superposition of both fundamental and second-harmonic (SH) pulse fields to generate the plasma, has attracted the most research interest.[8–10] Its physical mechanism was initially treated as a four-wave mixing process. However, subsequent measured results overturned this intuitive explanation.[3,11] Using the so-called transient photocurrent model, Kim et al. pointed out that coherent THz waves originate from a net electron current surge generated by an asymmetric two-color laser field,[9,11] which is now widely accepted. Thus, based on this explanation, researchers have dedicated their efforts to finding various asymmetric ultrashort laser fields, in some cases with additional static electric or magnetic fields, to manipulate the emitted THz fields. For example, multiple-color fs-lasers can boost the THz conversion efficiency significantly to obtain higher intensity THz pulses.[12,13] Kim et al. demonstrated that the polarization of the THz wave is affected by successive polarization rotation of the local THz plasma sources and the velocity mismatch between the pump laser and the generated THz wave.[14] Appling a helical electric field along a plasma region, Lu et al. obtained an elliptically polarized THz wave.[15] Furthermore, the latest research suggests that polarization of the THz wave can be tuned by adjusting the time delays or intensity ratio in the input three-pulse configuration.[16] In 2015, Wang et al. reported that the magnetic plasma offers an approach to emit circularly or elliptically polarized THz radiation.[17] However, the results of their two-dimensional (2D) PIC simulations demonstrated that the generated circularly or elliptically polarized THz radiation is narrowband.
In this paper, we utilize the transient photocurrent (PC) model to theoretically investigate the mechanism of polarized THz pulse generation when a static magnetic field is imposed on the gas plasma along the propagation direction of the two-color laser. The simulation results demonstrate that the linearly polarized THz radiation under weak external B-field will be gradually turned to an elliptically or circularly polarized one when the magnetic field strength B is higher than 10 T. Moreover, the generated elliptically or circularly polarized THz wave is broadband rather than narrowband in Ref. [17], and its intensity can be enhanced. The physical mechanism is attributed to that the asymmetric acceleration process of the ionized electrons is changed from one-dimensional to two-dimensional due to the presence of the magnetic field.
It is noted that magnetic fields with tens of tesla, in the form of ms-pulsed field can be easily obtained.[18,19] Applying destructive methods, even hundreds of tesla, ns-pulsed and thousands of tesla, ns-pulsed B-fields are already available.[20–22] Compared with two-color fs-lasers and ps-THz pulses, these magnetic fields can be treated as static fields. Besides these traditional methods, Santos et al. proposed an enlightening method to generate kilo-tesla, ns-pulsed quasi-static B-fields by employing intense laser-driven capacitor-coil targets.[23,24] According to their reports, the B-field strength can be tuned by the laser energy and the B-field direction is perpendicular to the cross section of the hollow coil. By using this method, an all-optic scheme can be proposed that focuses the two-color laser on the coil center to generate a magnetized gas plasma.
As shown in Fig.
![]() | Fig. 1. (color online) Schematic diagram of THz generation in a photoinduced plasma using two-color laser with a static magnetic field imposed on the plasma. |
Based on the PC model, the radiation field from plasma is proportional to the rate of change of such asymmetric ionization current, written as[9]
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![](cpb_27_5_058701/cpb_27_5_058701_ieqn1.gif)
![](cpb_27_5_058701/cpb_27_5_058701_ieqn2.gif)
In our simulation, the fundamental laser has a Gaussian formation, center wavelength λ = 800 nm, full width at half maximum (FWHM) TFWHM = 50 fs, and focal beam radius w0 = 10 μm. According to the experimental scheme, a 0.1 mm thick type-I β barium borate (BBO) crystal is used to generate the second harmonic (SH) field. The peak intensities of the fundamental and the SH laser pulses after the BBO crystal are Iω = 1.29 × 1014 W/cm2 and I2ω = 0.45 × 1014 W/cm2, respectively. We assume that the fundamental and the SH laser pulses have the same polarization direction, which can be precisely controlled by a dual-band waveplate. The gas is nitrogen and its density is assumed to be 2.4 × 1019 cm−3. The strength of the magnetic field B ∈ [0,1000 T].
Firstly, we obtain the THz E-field amplitudes along the x and y directions as the functions of time and magnetic field B, as depicted in Figs.
We plot the radiation spectra along two directions in the THz gap in Figs.
Figures
Next we plot the peak values of Ex and Ey versus B-field in Fig.
To further investigate the polarized properties of the THz radiation, we plot the three-dimensional THz electric field at B = 325 T and decompose it into three mutually orthogonal components with their polarization perpendicular to each other, as shown in Fig.
As mentioned above, the asymmetric ionization of bound electrons and the asymmetric electron acceleration play crucial roles in the whole process of THz generation. With an external B-field imposed on the gas plasma, these asymmetry processes could be more complex. By analyzing the force acting on the ionized electron motion, we will discuss our results. As the direction of the B-field is along the propagation direction of the two-color laser, the freed electrons will be deviated from the polarization direction of the laser due to the Lorentz force. After neglecting an attenuation item caused by the electron–ion collision, the freed electrons subjected to the laser field and static B-field accelerate as
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We decompose the electron velocity and forces in the x and y directions at two different time, as shown in Figs.
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The electron velocities along the x and y directions are plotted in Figs.
By using the transient PC model, we systematically investigate the THz pulse generation when a static magnetic field is imposed on gas plasma along the propagation direction of the two-color laser. The influence of the static magnetic field is analyzed from the point of view of ionized electron motion. It is found that the static magnetic field introduces a y-component of electron motion, changing the THz radiation from the linearly polarized one to an elliptically or circularly polarized one. Our simulations demonstrate that the polarization of the THz radiation can be tuned by changing the magnetic field strength. If the magnetic field strength is less than 10 T, the THz radiation is still nearly linearly polarized. When the magnetic field strength increases, the generated THz radiation gradually turns to be elliptically or even nearly broadband circularly polarized. Consequently, this scheme offers an extremely significant way to obtain tunable polarized broadband THz radiation.
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