Abstract:Strong terahertz (THz) electric and magnetic transients open up new horizons in science and applications. We review the most promising way of achieving sub-cycle THz pulses with extreme field strengths. During the nonlinear propagation of two-color mid-infrared and far-infrared ultrashort laser pulses, long, and thick plasma strings are produced, where strong photocurrents result in intense THz transients. The corresponding THz electric and magnetic field strengths can potentially reach the gigavolt per centim… Show more
“…As for the 1-D modulational profile, σ is the width of the packet with kσ 1, and v g the group velocity; we ignore packet dispersion. To implement the idea of superluminal carriers, we also consider a dispersion relation of the type ω = c 2 k 2 + ω 2 0 , where ω 2 0 incorporates the effects of the finite transverse dimensions of a wave guide, a possible diffractive geometry related to focused laser beams in vacuum (Esarey et al 1995;Steinhauer & Kimura 2003;Ralph et al 2009;Lemos et al 2018;Fedorov & Tzortzakis 2020) or the effects of a plasma medium (Elmore & Heald 1985). We note that TE 01 and TE 10 EM modes in a wave guide with rectangular cross-section produce a null in the axial magnetic field right at the cross-sectional midpoint.…”
In the present work we investigate the dynamics of electrons under the action of wave packets of high-frequency electromagnetic carrier waves. When the group velocities of the packets are subluminal, electrons can be efficiently accelerated. We show that the whole process can be described by an accurate ponderomotive canonical formalism that includes relevant extensions of the original ponderomotive approach applied to carriers moving at the speed of light. Single-particle simulations validate our analytical approach and show that extended canonical methods provide better agreement with numerics than previous investigations. In particular, we obtain a precise relationship between the wave amplitude and group velocity for optimum acceleration of initially stationary targets.
“…As for the 1-D modulational profile, σ is the width of the packet with kσ 1, and v g the group velocity; we ignore packet dispersion. To implement the idea of superluminal carriers, we also consider a dispersion relation of the type ω = c 2 k 2 + ω 2 0 , where ω 2 0 incorporates the effects of the finite transverse dimensions of a wave guide, a possible diffractive geometry related to focused laser beams in vacuum (Esarey et al 1995;Steinhauer & Kimura 2003;Ralph et al 2009;Lemos et al 2018;Fedorov & Tzortzakis 2020) or the effects of a plasma medium (Elmore & Heald 1985). We note that TE 01 and TE 10 EM modes in a wave guide with rectangular cross-section produce a null in the axial magnetic field right at the cross-sectional midpoint.…”
In the present work we investigate the dynamics of electrons under the action of wave packets of high-frequency electromagnetic carrier waves. When the group velocities of the packets are subluminal, electrons can be efficiently accelerated. We show that the whole process can be described by an accurate ponderomotive canonical formalism that includes relevant extensions of the original ponderomotive approach applied to carriers moving at the speed of light. Single-particle simulations validate our analytical approach and show that extended canonical methods provide better agreement with numerics than previous investigations. In particular, we obtain a precise relationship between the wave amplitude and group velocity for optimum acceleration of initially stationary targets.
“…6G communication frequencies worked at 0.12, 0.22, 0.28, and 0.42 THz are attracting more attention. However, high-performance detectors in large areas at room temperature are still an enormous challenge. − According to the effective detection area of detectors, the existing THz detectors can be recognized as the micro–nano detectors and the millimeter-scale detectors. The micro and nano detectors are mainly graphene-based nonlinear hall effect (NHE) detector, Bi 2 Se 3 -based electromagnetic induced well (EIW) detector, AlGaN/GaN and PtTe 2 field-effect transistor (FET) detector, PdTe 2 -based photogalvanic effects (PCE) detector, black phosphorus (BP)-based photo-thermoelectric effect (PTE) detector, and Bi 88 Sb 12 -based thermoelectric detector .…”
The 6G technology has defined 0.1–0.28 THz as
the communication
band. However, high-performance detectors in large areas at room temperature
are still an enormous challenge. To greatly improve the performance
of the THz detector, a room-temperature terahertz (THz) detector based
on PbS quantum dot (QD) microwheel arrays have been designed and fabricated.
The QD microwheel array was fabricated on a thin GaN/Si substrate
and with the engraved periodic wheel. In addition, the concave convergence
of the microwheel further improves the interaction between the terahertz
wave and the device. The detector has been tested under the 6G communication
frequencies of 0.14 and 0.28 THz and showed current responsivities
of 3.12 and 4.67 A/W. The detector based on the QD microwheel array
has shown a current responsivity up to 9 times higher compared with
the signal QD film. The noise equivalent power valuesof the devices
for 0.14 and 0.28 THz are 6.61 × 10–13 and
1.88 × 10–14 W/Hz1/2. The results
give a chance to develop the large-area, high-performance THz detector
based on QDs, which could provide a reliable alternative for 6G communication
equipment at room temperature.
“…The THz lies between microwave and far infrared regions. Until recently, there was no easy and direct process for generating THz sources whose strength are comparable to the powerful high‐energy lasers (Fedorov and Tzortzakis, 2020). The THz has a wide range of potential applications in areas related to imaging such as diagnostics, industrial quality control, security, food inspection, or artwork examination (Afsah‐Hejri et al, 2019; Cheng et al, 2021; Ohrstrom et al, 2015).…”
Terahertz (THz) radiation has a wide range of applications including use in medicine. However, effects of high‐power THz radiation have not been clearly elucidated. We used a 2.52 THz self‐made optically pumped gas THz laser, the low‐ and high‐energy group, to irradiate the backs of Hartley guinea pigs. RNA‐sequencing was done to explore global transcriptional responses in the irradiated skin. Gene Ontology analysis revealed that differentially expressed genes (DEGs) between the unexposed and low‐energy exposed groups were associated with skin development, skin barrier establishment, and multicellular organismal water homeostasis or water loss regulation via the skin. On the other hand, comparison between the unexposed and high‐energy exposed groups showed that the DEGs mediated monocarboxylic acid metabolism, blood vessel morphogenesis, establishment of skin barrier, blood vessel development, or angiogenesis. Our analyses demonstrate the potential effects of high‐power THz source on the skin and sets the basis for further studies on the safety and application of the high‐power THz in dermatology.
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.