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Attosecond Control and Measurement: Lightwave Electronics

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1 . 3 AT T O S E C O N D A N D H I G H - F I E L D P H Y S I C S D I V I S I O N<br />

Figure 13: Gigaelectronvolt-scale laser wake field accelerator at MPQ. G: GRENOUILLE pulse diagnostics, C1-C5:<br />

cameras; D1, D2: diodes; L1, L2: scintillating screens; S: spectrometer; W: wedge; OAP: off-axis parabola; CAP:<br />

capillary waveguide. The inset shows the incoming laser focus at the capillary entrance.<br />

relativistic plasma, which shortens its duration into the<br />

required domain. Longer-than-optimal driver pulses<br />

compromise efficiency as well as reproducibility, <strong>and</strong><br />

result in copious amounts of low-energy electrons<br />

accompanying the mono-energetic emission with an<br />

exponentially-decaying spectrum, forming a “thermal”<br />

background. By using the multi-terawatt, sub-10-fs<br />

pulses from LWS-10, Karl Schmid, Laszlo Veisz <strong>and</strong><br />

coworkers, in close cooperation with Ulrich Schramm,<br />

Dieter Habs <strong>and</strong> collaborators from the Univ. Düsseldorf<br />

have recently demonstrated the first electron accelerator<br />

based on high-density plasma waves driven with<br />

laser pulses that fit in one half of the plasma period<br />

(Figure 11) [14]. Direct “impulsive” excitation of the<br />

plasma wave permits mono-energetic electron<br />

acceleration virtually free from a thermal background<br />

for the first time. In our experiments, 5-terawatt, 8femtosecond<br />

laser pulses yield electron bunches up to<br />

energies of 25 MeV (Figure 12). The flux of low-energy<br />

electrons dramatically reduced as compared to earlier<br />

experiments also manifests itself in a strongly-reduced<br />

secondary radiation emerging from the accelerator <strong>and</strong><br />

offers the potential for enhancing efficiency <strong>and</strong> stability<br />

with more intense driver pulses.<br />

The electron energy can be further boosted by laser-driven<br />

plasma-wake-field acceleration (LWFA) in a discharge<br />

capillary to the gigaelectronvolt range, as demonstrated<br />

by Wim Leemans <strong>and</strong> coworkers at Berkeley in 2006.<br />

Jens Osterhoff, Antonia Popp, Zsuzsanna Major, Stefan<br />

Karsch <strong>and</strong> coworkers, in close co-operation with Dieter<br />

Habs <strong>and</strong> his group, have recently also demonstrated<br />

LWFA to the GeV frontier from a discharge capillary<br />

waveguide provided by Simon Hooker from Oxford<br />

University by driving the accelerator with 0.75 J, 40fs,<br />

800-nm pulses from ATLAS, MPQ’s multiterawatt<br />

Ti:Sa laser, see Figure 13 [12].<br />

Quasi-monoenergetic electron beams with energies as<br />

high as 500 MeV have been detected, with features<br />

reaching up to 1 GeV, albeit with large shot-to-shot<br />

fluctuations. The beam divergence <strong>and</strong> the pointing<br />

stability in this case are around or below 1 mrad <strong>and</strong><br />

8 mrad, respectively. These shot-to-shot electron-bunch<br />

parameter variations are greatly suppressed by utilizing<br />

the capillary as a gas-vessel without pre-ionization by an<br />

external electrical discharge. In this regime of operation<br />

quasi-monoenergetic electron beams of up to ~200<br />

MeV in energy have been observed (Figure 14). These<br />

beams emitted within a low-divergence cone of mrad<br />

FWHM display unprecedented shot-to-shot stability<br />

in energy (2.5% RMS), pointing (1.4 mrad RMS) <strong>and</strong><br />

charge (16% RMS) owing to a highly reproducible gasdensity<br />

profile within the interaction volume (Figure15)<br />

[13]. The excellent stability of bunch parameters affords<br />

promise for the potential ability of laser-accelerated<br />

electron bunches to meet the stringent criteria for<br />

seeding free electron lasers.<br />

INTENSE ATTOSECOND XUV/SXR PUlSES<br />

might allow triggering as well as probing ultrafast<br />

electron dynamics with attosecond pulses, i.e.<br />

attosecond XUV-pump/XUV-probe spectroscopy,<br />

which has not been possible so far. Relativistic laserplasma<br />

interactions have been identified as a promising<br />

approach to achieving this goal. Recent experiments<br />

confirmed that relativistically-driven overdense plasmas<br />

are able to convert infrared laser light into harmonic<br />

XUV radiation with unparalleled efficiency <strong>and</strong> that the<br />

generation technique is scalable towards hard X-rays.<br />

In a recent experiment (Figure 15) Yutaka Nomura,<br />

Rainer Hörlein, Sergey Rykovanov, George Tsakiris <strong>and</strong><br />

coworkers, in collaboration with the teams of Matt Zepf<br />

from Belfast <strong>and</strong> Dimitris Charalambidis from Heraklion,<br />

have recently succeeded in obtaining conclusive<br />

experimental evidence for the phases of the XUV<br />

harmonics emanating from the interaction that they are<br />

144 Max-Planck-Institut für Quantenoptik • Progress Report 2007/2008

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