Laser particle acceleration

Optics InfoBase Conference Papers (2009)

Authors:

PA Norreys, APL Robinson, RMGM Trines

Abstract:

The production of highly energetic beams of both electrons and ions is a major part of the experimental programme at the Central Laser Facility (CLF), STFC Rutherford Appleton Laboratory. Every year sees a significant number of experiments done in both areas. This has been complemented by theoretical studies that have been carried out at the CLF and UK universities. In a recent consultation on plans to build a 10 PW upgrade to the VULCAN facility, laser-driven particle acceleration formed a very significant part of the science case that emerged from this consultation. In this talk, I will review the experimental progress that has been made in particle acceleration, and I will also examine what theoretical investigations suggest the future of this field will be. Experimental studies of laser-driven ion acceleration of the CLF using both the VULCAN and ASTRA systems have looked at a number of aspects including focussing and control of the ion beam, manipulation of the energy spectrum, energy scaling with laser and target parameters, and direct use of the proton beam in both isochoric heating of secondary targets and proton radiography. Recently there has been great interest in a number of theoretical studies which indicate that it should be possible to explore radiation-pressure driven ion acceleration for intensities above 1021 Wcm-2, which will be accessible with the ASTRA-GEMINI system. This very exciting prospect will also be discussed. Electron acceleration in laser wakefields is also a well established part of the CLF programme. Experimental studies of laser-driven electron acceleration using the ASTRA laser have explored electron acceleration in both supersonic gas jets and gas-filled capillaries. This has led to the production of electron bunches with up to 1 GeV energy and a few percent energy spread. The influence of tuneable parameters such as the evolution of the plasma channel inside a capillary or the position of the laser focus with respect to the gas jet is actively being investigated. These efforts are backed up by a matching numerical campaign. Recent experiments have also shown that electron bunches trapped on a downward density ramp can have a very small absolute energy spread, and the potential consequences of these results will also be discussed. © 2011 Optical Society of America.

Laser-driven soft-X-ray undulator source

Nature Physics 5:11 (2009) 826-829

Authors:

M Fuchs, R Weingartner, A Popp, Z Major, S Becker, J Osterhoff, I Cortrie, B Zeitler, R Hörlein, GD Tsakiris, U Schramm, TP Rowlands-Rees, SM Hooker, D Habs, F Krausz, S Karsch, F Grüner

Abstract:

Synchrotrons and free-electron lasers are the most powerful sources of X-ray radiation. They constitute invaluable tools for a broad range of research 1 ; however, their dependence on large-scale radiofrequency electron accelerators means that only a few of these sources exist worldwide. Laser-driven plasma-wave ccelerators 2-10 provide markedly increased accelerating fields and hence offer the potential to shrink the size and cost of these X-ray sources to the niversity-laboratory scale. Here, we demonstrate the generation of soft-X-ray undulator radiation with laser-plasma-accelerated electron beams. The well-collimated beams deliver soft-X-ray pulses with an expected pulse duration of ∼ 10 fs (inferred from plasma-accelerator physics). Our source draws on a 30-cm-long undulator and a 1.5-cm-long accelerator delivering stable electron beams with energies of ∼ 210 MeV. The spectrum of the generated undulator radiation typically consists of a main peak centred at a wavelength of ∼ 18 nm (fundamental), a second peak near ∼ 9 nm (second harmonic) and a high-energy cutoff at ∼ 7 nm. Magnetic quadrupole lenses ensure efficient electron-beam transport and demonstrate an enabling technology for reproducible generation of tunable undulator radiation. The source is scalable to shorter wavelengths by increasing the electron energy. Our results open the prospect of tunable, brilliant, ultrashort-pulsed X-ray sources for small-scale laboratories. © 2009 Macmillan Publishers Limited. All rights reserved.

Nuclear physics with intense lasers

Springer Series in Optical Sciences 134 (2009) 519-536

Authors:

R Singhal, P Norreys, H Habara

Perspective for high energy density studies using x-ray free electron lasers

IEEE International Conference on Plasma Science (2009)

Authors:

RW Lee, B Nagler, U Zastrau, R Fäustlin, S Vinko, T Whitcher, R Sobierajski, J Krzywinski, L Juha, A Nelson, S Bajt, T Bornath, T Burian, J Chalupsky, H Chapman, J Cihelka, T Döppner, T Dzelzainis, S Düsterer, M Fajardo, E Förster, C Fortmann, SH Glenzer, S Göde, G Gregori, V Hajkova, P Heimann, M Jurek, F Khattak, AR Khorsand, D Klinger, M Kozlova, T Laarmann, H Lee, K Meiwes-Broer, P Mercere, WJ Murphy, A Przystawik, R Redmer, H Reinholz, D Riley, G Röpke, K Saksl, R Thiele, J Tiggesbäumker, S Toleikis, T Tschentscher, I Uschmann, JS Wark

Turning solid aluminium transparent by intense soft X-ray photoionization

Nature Physics 5:9 (2009) 693-696

Authors:

B Nagler, U Zastrau, RR Fäustlin, SM Vinko, T Whitcher, AJ Nelson, R Sobierajski, J Krzywinski, J Chalupsky, E Abreu, S Bajt, T Bornath, T Burian, H Chapman, J Cihelka, T Döppner, S Düsterer, T Dzelzainis, M Fajardo, E Förster, C Fortmann, E Galtier, SH Glenzer, S Göde, G Gregori, V Hajkova, P Heimann, L Juha, M Jurek, FY Khattak, AR Khorsand, D Klinger, M Kozlova, T Laarmann, HJ Lee, RW Lee, KH Meiwes-Broer, P Mercere, WJ Murphy, A Przystawik, R Redmer, H Reinholz, D Riley, G Röpke, F Rosmej, K Saksl, R Schott, R Thiele, J Tiggesbäumker, S Toleikis, T Tschentscher, I Uschmann, HJ Vollmer, JS Wark

Abstract:

Saturable absorption is a phenomenon readily seen in the optical and infrared wavelengths. It has never been observed in core-electron transitions owing to the short lifetime of the excited states involved and the high intensities of the soft X-rays needed. We report saturable absorption of an L-shell transition in aluminium using record intensities over 10 16 W cm 2 at a photon energy of 92 eV. From a consideration of the relevant timescales, we infer that immediately after the X-rays have passed, the sample is in an exotic state where all of the aluminium atoms have an L-shell hole, and the valence band has approximately a 9 eV temperature, whereas the atoms are still on their crystallographic positions. Subsequently, Auger decay heats the material to the warm dense matter regime, at around 25 eV temperatures. The method is an ideal candidate to study homogeneous warm dense matter, highly relevant to planetary science, astrophysics and inertial confinement fusion. © 2009 Macmillan Publishers Limited. All rights reserved.