• Title/Summary/Keyword: ultrashort pulse duration

Search Result 9, Processing Time 0.02 seconds

Reconstruction of the Electron Density Profile in O-mode Ultrashort Pulse Reflectometry using a Two-dimensional Finite Difference Time Domain

  • Roh, Young-Su
    • Journal of the Korean Institute of Illuminating and Electrical Installation Engineers
    • /
    • v.27 no.7
    • /
    • pp.52-58
    • /
    • 2013
  • The two-dimensional finite difference time domain algorithm is used to numerically reconstruct the electron density profile in O-mode ultrashort pulse reflectometry. A Gaussian pulse is employed as the source of a probing electromagnetic wave. The Gaussian pulse duration is chosen in such a manner as to have its frequency spectrum cover the whole range of the plasma frequency. By using a number of numerical band-pass filters, it is possible to compute the time delays of the frequency components of the reflected signal from the plasma. The electron density profile is reconstructed by substituting the time delays into the Abel integral equation. As a result of simulation, the reconstructed electron density profile agrees well with the assumed profile.

Effects of Temperature Coefficients for Dielectric Constants on Thermoreflectances and Thermal Responses of Metal Thin Films Exposed to Ultrashort Pulse Laser Beams

  • Seungho Park
    • International Journal of Air-Conditioning and Refrigeration
    • /
    • v.10 no.1
    • /
    • pp.1-9
    • /
    • 2002
  • Effects of temperature coefficients fur dielectric constants on transient reflectances and thermal responses have been investigated for a metal(gold) thin-film during ultrashort pulse laser heating. Heating processes are simulated using the conventional conduction model(parabolic one-step, POS), the parabolic tow-step model(PTS), the hyperbolic two-step model(HTS). Results fro the HTS model are very similar to those from the PTS model, since the laser heating time in this study is considerably greater than the electron relaxation time. PTS and HTS models, however, result in completely different temperature profiles from those obtained by the POS model due to slow electron-lattice interactions compared to laser pulse duration. Transient reflectances are directly estimated from the linear relationship between electron temperature and complex dielectric constants, while conventional approaches assume that the change in reflectances is proportional to that in temperatuer. Reflectances at the front surface vary considerably for various dielectric constants, while those at the rear surface remain unchanged relatively.

Ultrashort Pulse Reflectometry for the Measurement of Electron Density Profiles (전자 밀도 분포 측정을 위한 극단 펄스 레플렉토메터리)

  • 노영수
    • The Transactions of the Korean Institute of Electrical Engineers C
    • /
    • v.53 no.1
    • /
    • pp.8-14
    • /
    • 2004
  • An O-mode Ultrashort Pulse Reflectometry (USPR) system has been designed and developed for the measurement of electron density profiles on the Sustained Spheromak Physics Experiment (SSPX) spheromak. In the original design of SSPX, peak densities were envisioned to be in the range of 0.5-3${\times}$10$^{14}$ cm$^{-3}$ . The total duration of formation and sustained discharges is typically ∼2 msec. Moreover, diagnostic access on SSPX is severely restricted. Such high density and short duration plasmas coupled with stringent diagnostic access are quite challenging for conventional reflectometer systems. In USPR, the SSPX diagnostic requirements have been successfully satisfied by employing up-converting mixers and monostatic horn/waveguide configuration. As a result, the USPR system has proven its applicability for the density measurement of a future fusion device. In the density profile measurements, the USPR system is capable of routinely generating density profiles with a temporal resolution of 57 $\mu$s. This paper presents details regarding the USPR fundamental principles, associated subsystems and laboratory tests as well as the experimental results obtained on SSPX

High Power 1.83 GHz Femtosecond Yb-doped Fiber Laser Incorporating Repetition Rate Multipliers

  • In Chul Park;Eun Kyung Park;Ye Jin Oh;Hoon Jeong;Ji Won Kim;Jeong Sup Lee
    • Current Optics and Photonics
    • /
    • v.7 no.6
    • /
    • pp.732-737
    • /
    • 2023
  • A high-power Yb-doped femtosecond (fs) fiber laser at a repetition rate of 1.83 GHz is reported. By employing a 5-stage repetition rate multiplier, the repetition rate of the mode-locked master oscillator was multiplied from 57.1 MHz to 1.83 GHz. The ultrashort pulse output at 1.83 GHz was amplified in a two-stage Yb-doped fiber amplifier, leading to >100 W of fs laser output with a pulse duration of 290 fs. The theoretical pulse width along the fiber was simulated, showing that it was in good agreement with experimental results. Further improvement in power scaling is discussed.

High-power SESAM Mode-locked Yb:KGW Laser with Different Group-velocity Dispersions

  • Park, Byeong-Jun;Song, Ji-Yeon;Lee, Seong-Yeon;Yee, Ki-Ju
    • Current Optics and Photonics
    • /
    • v.6 no.4
    • /
    • pp.407-412
    • /
    • 2022
  • We report on a diode-laser-pumped mode-locked Yb:KGW laser system, which delivers ultrashort pulses down to 89 fs at a repetition rate of 63 MHz, with an average power of up to 5.6 W. A fiber-coupled diode laser at 981 nm, operated with a compact driver, is used to optically pump the gain crystal via an off-axis parabolic mirror. A semiconductor saturable-absorber mirror is used to initiate the pulsed operation. Laser characteristics such as the pulse duration, spectrum bandwidth, and output power are investigated by varying the intracavity dispersions via changing the number of bounces between negative-dispersive mirrors within the cavity. Short pulses with a duration of 89 fs, a center wavelength of 1,027 nm, and 3.6 W of output power are produced at a group-velocity dispersion (GVD) of -3,300 fs2. As the negative GVD increases, the pulse duration lengthens but the output power at the single-pulse condition can be enhanced, reaching 5.6 W at a GVD of -6,600 fs2. Because of pulse broadening at high negative GVDs, the highest peak intensity is achievable at a moderate GVD with our system.

The Real-Time Temporal and Spatial Diagnostics of Ultrashort High-Power Laser Pulses using an All-Reflective Single-Shot Autocorrelator

  • Kim, Ha-Na;Park, Seong Hee;Kim, Kyung Nam;Han, Byungheon;Shin, Jae Sung;Lee, Kitae;Cha, Yong-Ho;Jang, Kyu-Ha;Jeon, Min Yong;Miginsky, Sergei V.;Jeong, Young Uk;Vinokurov, Nikolay A.
    • Journal of the Optical Society of Korea
    • /
    • v.18 no.4
    • /
    • pp.382-387
    • /
    • 2014
  • An all-reflective, simple noncollinear second harmonic (SH) autocorrelator is described for monitoring the shot-to-shot behavior of ultrashort high-power laser pulses. Two mirrors are used for the dispersion-free splitting of a pulse into two halves. One of the mirrors is able to adjust the delay time and angle between two halves of the laser pulse in a nonlinear crystal. We present the possibility of real-time measurement of the pulse duration, peak intensity (or energy), and the pointing jitters of a laser pulse, by analyzing the spatial profile of the SH autocorrelation signal measured by a CCD camera. The measurement of the shot-to-shot variation of those parameters will be important for the detailed characterization of laser accelerated electrons or protons.

Technology Of Application Of Multifrequency Signals To Create An Electromagnetic Field

  • Strembitska, Oksana;Tymoshenko, Roman;Mozhaiev, Mykhailo;Buslov, Pavlo;Kashyna, Ganna;Baranenko, Roman V.;Makiievskyi, Oleksii
    • International Journal of Computer Science & Network Security
    • /
    • v.21 no.2
    • /
    • pp.40-43
    • /
    • 2021
  • In the article of instability on the peak power level, duration and repetition period of a multifrequency space-time signal, we calculated the maximum values of the errors of the parameters of the laws of spatial-phase-frequency control. Requirements for the accuracy of the location of the phase centers of the emitters in a cylindrical phased array antenna with pyramidal horns; it is advisable to calculate the radiation field using single-stage and multi-stage distribution laws. The phase centers of individual radiation sources of a cylindrical phased array antenna have been studied; they have almost no effect on the duration and period of recurrence.

Simulation of an X-ray Fresnel Zone Plate with Nonideal Factors

  • Chen, Jie;Fan, Quanping;Wang, Junhua;Yuan, Dengpeng;Wei, Lai;Zhang, Qiangqiang;Liao, Junsheng;Xu, Min
    • Current Optics and Photonics
    • /
    • v.4 no.1
    • /
    • pp.9-15
    • /
    • 2020
  • Fresnel zone plates have been widely used in many applications, such as x-ray telescopes, microfluorescence, and microimaging. To obtain an x-ray Fresnel zone plate, many fabrication methods, such as electron-beam etching, ion-beam etching and chemical etching, have been developed. Fresnel zone plates fabricated by these methods will inevitably lead to some nonideal factors, which have an impact on the focusing characteristics of the zone plate. In this paper, the influences of these nonideal factors on the focusing characteristics of the zone plate are studied systematically, by numerical simulations based on scalar diffraction theory. The influence of the thickness of a Fresnel zone plate on the absolute focusing efficiency is calculated for a given incident x-ray's wavelength. The diffraction efficiency and size of the focal spot are calculated for different incline angles of the groove. The simulations of zone plates without struts, with regular struts, and with random struts are carried out, to study the effects of struts on the focusing characteristics of a zone plate. When a Fresnel zone plate is used to focus an ultrashort x-ray pulse, the effect of zone-plate structure on the final pulse duration is also discussed.