Raman Backscattering In Plasma Research Articles

Laser pulse cutoff at nonlinear reflection due to Raman backscattering in plasma.

A method for generating subrelativistic laser pulses with a sharp leading edge is proposed, which is based on Raman backscattering of an intense short pump pulse by a counter-propagating long low-frequency pulse propagating in a thin plasma layer. A thin plasma layer serves both to attenuate parasitic effects and to effectively reflect the central part of the pump pulse when the field amplitude exceeds the threshold value. A prepulse with a lower field amplitude passes through the plasma almost without scattering. This method works for subrelativistic laser pulses with durations up to 100 fs. The contrast of the leading edge of the laser pulse is determined by the seed pulse amplitude.

Stimulated Raman backscattering amplification with a low-intensity pump

The efficiency transfer from the pump to the seed of stimulated Raman backscattering in plasma was optimized at a pump intensity below 1014 W/cm2. Two ways were employed to obtain high-quality but low-intensity pump beams. First, the pump focus was moved away from the plasma entrance to optimize guiding the uniform part of the beam in the plasma channel. The seed was amplified from 50 μJ to 1.1 mJ after 2-mm interaction, with an effective Raman transfer efficiency over 4.7%. Second, an aperture was set to make the pump focus pass through the plasma channel. An output seed energy of 1.02 mJ was obtained when the pump energy decreased to 20 mJ, showing a transfer efficiency of 5.1%. The experimental results indicate that the transfer efficiency may be mainly suppressed by plasma heating but not spontaneous Raman scattering.

Chirped pulse Raman amplification in warm plasma: towards controlling saturation.

Stimulated Raman backscattering in plasma is potentially an efficient method of amplifying laser pulses to reach exawatt powers because plasma is fully broken down and withstands extremely high electric fields. Plasma also has unique nonlinear optical properties that allow simultaneous compression of optical pulses to ultra-short durations. However, current measured efficiencies are limited to several percent. Here we investigate Raman amplification of short duration seed pulses with different chirp rates using a chirped pump pulse in a preformed plasma waveguide. We identify electron trapping and wavebreaking as the main saturation mechanisms, which lead to spectral broadening and gain saturation when the seed reaches several millijoules for durations of 10’s – 100’s fs for 250 ps, 800 nm chirped pump pulses. We show that this prevents access to the nonlinear regime and limits the efficiency, and interpret the experimental results using slowly-varying-amplitude, current-averaged particle-in-cell simulations. We also propose methods for achieving higher efficiencies.

Stimulated Raman Backscattering in Plasma — a Promising Tool for the Generation of Ultra-High Power Laser Beams

In the last fifteen years stimulated Raman backscattering (SRBS) in plasma has been intensively elaborated as a promising tool on the way towards high intense lasers. There are several advantages of this technique in comparison to the world-wide used the CPA-Chirped Pulse Amplification technique for a laser amplification. We present the principle of the SRBS technique, the best results so far obtained in theory and experiment, and a possible SRBS project at the PALS Research Centre in Prague.

The role of absorption in Raman amplification in warm plasma

Raman backscattering in plasma is subject to—collisional and collisionless—absorption of the interacting waves. A model for studying its role over a wide parameter range is developed by coupling the envelope equations for pump, probe, and plasma waves with those describing heating of the plasma. The latter is treated as a warm fluid, making the model useful for moderate temperatures and field amplitudes. The main effect is the time-dependent Bohm–Gross shift of the Langmuir resonance frequency, which can either enhance or suppress amplification; this can be further controlled by varying the frequency of the pump. Anisotropy in the collisional processes for longitudinal and transverse waves leads to temperature anisotropy at high field amplitudes. Direct Landau damping of the plasma wave, as well as its contribution to the frequency shift, can be neglected due to rapid saturation.

Laser pulse compression and amplification via Raman backscattering in plasma

AbstractA simple theoretical model is proposed for the interaction between two counter-propagating laser pulses (a pump and a seed pulse) in unmagnetized plasma. Pulse compression and amplification are observed via numerical simulation. A one dimensional fluid model for stimulated Raman backscattering is proposed to investigate the pulse compression and pulse amplification mechanisms. To accomplish this, energy is transferred from the long pump pulse to a seed pulse, with a Langmuir plasma wave mediating the transfer. The study focuses on the intensity profile of the pump laser pulse. A Gaussian and a ring intensity profile are, separately, considered for the pump laser pulse.

Compression of powerful x-ray pulses to attosecond durations by stimulated Raman backscattering in plasmas

Backward Raman amplification (BRA) in plasmas holds the potential for longitudinal compression and focusing of powerful x-ray pulses. In principle, this method is capable of producing pulse intensities close to the vacuum breakdown threshold by manipulating the output of planned x-ray sources. The minimum wavelength limit of BRA applicability to compression of laser pulses in plasmas is found.

Raman laser amplification in preformed and ionizing plasmas

The recently proposed backward Raman laser amplification scheme utilizes the stimulated Raman backscattering in plasma of a long pumping laser pulse to amplify a short, and frequency downshifted seed pulse. The output intensity for this scheme is limited by the development of forward Raman scattering (FRS) or modulational instabilities of the highly amplified seed. Theoretically, focused output intensities as high as 1025 W/cm2, and pulse lengths of less than 100 fs, could be accessible by this technique for 1 μm lasers—an improvement of 104–105 in focused intensity over current techniques. Simulations with the particle-in-cell (PIC) code Zohar are presented, which investigate the effects of FRS and modulational instabilities, and of Langmuir wave breaking on the output intensity for Raman amplification. Using the intense seed pulse to photoionize the plasma simultaneous with its amplification (and hence avoid plasmas-based instabilities of the pump) is also investigated by PIC simulations. It is shown that both approaches can access focused intensities in the 1025 W/cm2 range.

Laser pulse amplification upon Raman backscattering in plasma produced in dielectric capillaries

Femtosecond-pulse amplification upon stimulated Raman scattering is experimentally demonstrated for the case of a counter-propagating femtosecond laser pulse and a frequency-modulated broadband pump pulse with the same carrier frequency in a dielectric capillary filled with gas plasma. A value of ∼103 obtained for the spectral intensity amplification and ∼102 for the output energy are the highest ever achieved for these quantities to date. Numerical simulation demonstrates good agreement with the experimental results. Based on the experimental data and the results of theoretical calculations, we propose a hydrodynamic mechanism for plasma-wave breaking as the mechanism playing an important role in the amplification restriction in the scheme considered.

Noise suppression and enhanced focusability in plasma Raman amplifier with multi-frequency pump

Laser pulse compression–amplification through Raman backscattering in plasmas can be facilitated by using multi-frequency pump laser beams. The efficiency of amplification is increased by suppressing the Raman instability of thermal fluctuations and seed precursors. Also the focusability of the amplified radiation is enhanced due to the suppression of large-scale longitudinal speckles in the pump wave structure.

Amplification of short laser pulses by Raman backscattering in capillary plasmas

Short laser pulses can be significantly amplified in the process of Raman backscattering in plasma inside an oversized dielectric capillary. A dielectric capillary allows obtaining high intensities of the output radiation by sustaining efficient amplification at large distances compared to the diffraction length. The efficiency of the interaction between the pump wave and the amplified pulse is shown not to be critically sensitive to the transverse structure of the wave fields. For a quasi-single-mode initial seed pulse and a low pump intensity, the amplified pulse tends to preserve its transverse structure due to nonlinear competition of the capillary eigen-modes. At a high power of the pump wave, multimode amplification always takes place but the growth of the front peak of the pulse still follows the one-dimensional model. The Raman backscattering instability of the pump wave resulting in the noise amplification can be suppressed in detuned interaction by chirping the pump wave or arranging an inhomogeneous plasma density profile along the trace of amplification. The efficiency of the desired pulse amplification does not significantly depend on detuning in the case of a smooth detuning profile. Density inhomogeneities are shown to exert less influence on the amplification within a capillary than in the one-dimensional problem. Parameters of a future experiment on the Raman amplification of a short laser pulse inside a capillary are proposed.

Storing, retrieving, and processing optical information by Raman backscattering in plasmas.

By employing stimulated Raman backscattering in a plasma, information carried by a laser pulse can be captured in the form of a very slowly propagating plasma wave that persists for a time long compared with the pulse duration. If the plasma is then probed with a short laser pulse, the information stored in the plasma wave can be retrieved in a second scattered electromagnetic wave. The recording and retrieving processes can conserve robustly the pulse shape, thus enabling the recording and retrieving with fidelity of information stored in optical signals.