Kazuhisa Nakajima- Towards a table-top free-electron laser

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  • 8/3/2019 Kazuhisa Nakajima- Towards a table-top free-electron laser

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    NEWS & VIEWS

    92 nature physics| VOL 4 | FEBRUARY 2008 |www.nature.com/naturephysics

    COMPACT X-RAY SOURCES

    Towards a table-top free-electron laser

    Kazuhisa Nakajimais at the High Energy Accelerator Research

    Organization, 1-1 Oho, Tsukuba, Ibaraki

    305-0081, Japan.

    e-mail: [email protected]

    S

    ynchrotron radiation sources havebecome an indispensable tool in a

    wide range o disciplines, includingphysics, biology, materials science,chemistry and medicine. Te reasonthey are so useul is the high intensityo X-rays they produce generatedwhen the path o a beam o electronsmoving at relativistic speeds is bent by aperiodic magnetic eld in comparisonwith other X-ray sources. Such utility isexpected to grow still urther with thedevelopment o X-ray ree-electron lasers(FELs) devices that operate on a similarprinciple to synchrotrons but whichproduce X-rays in intense, coherent,

    emtosecond bursts, enabling thedynamics o chemical reactions, materialsand biomolecular systems to be studiedwith unprecedented spatial and temporalresolution1. Several X-ray FEL acilitiesare currently under construction24, ata cost o the order o US$1 billion each;the particle accelerators that produce themulti-GeV electron beams on which theiroperation relies span many kilometresin length. But on page 130 o this issue 5,Schlenvoigt and colleagues describe anapproach that could substantially reduceboth the size and cost o synchrotron and

    FEL X-ray sources, through the use oelectron beams produced by a laser-drivenparticle accelerator6.

    Although still in their inancy,great progress has been made in thedevelopment o so-called laser-wakeieldparticle accelerators. hese devices usethe immense electric ields producedat the ocus o modern ultra-high-intensity lasers to accelerate electrons,protons and ions over distances o justcentimetres thousands o times shorterthan a conventional particle accelerator.In their set-up, Schlenvoigt et al. ocusthe light rom a 5-W laser pulse into

    a 2-mm-wide gas jet. he interaction othe laser with the jet produces a beam oelectrons with a peak energy o between5575 MeV. Directing this beam into a1-m-long undulator which consists o

    a series o alternating magnets causesits electrons to wiggle back and orth,transverse to the beam direction,producing light at the red end o thevisible spectrum (with wavelength inthe range o 950550 nm). he authorsthereore provide the irst demonstrationo the production o resonant-likesynchrotron radiation rom a laser-generated electron beam. he results oseveral runs o their experiment showthat the emission wavelength scales withbeam energy just as theory predicts,suggesting that the generation o muchshorter wavelengths by this approach

    should be relatively straightorward. Byextending the length o the undulator to3 m, and eeding it with a more energeticbeam such as the 1-GeV, 30-pCbeams recently demonstrated in a 3-cm

    capillary laser-plasma accelerator7

    (seeFig. 1a) it should soon be possible toreach 3 nm in the sot-X-ray range, ata peak brilliance comparable to that oeven the largest modern synchrotronradiation sources.

    Once the easibility o a laser-drivensot-X-ray source is achieved, the nextstep will be to extend this approach tothe more ambitious task o constructingan FEL. X-ray FELs rely on a sel-ampliication o spontaneous emission(SASE)8, where coherent radiationbuilds up in a single pass through theinteraction o spontaneously emitted

    Synchrotron radiation generated using an electron beam rom a laser-driven accelerator

    opens the possibility o building an X-ray ree-electron laser hundreds o times smaller than

    conventional acilities currently under construction.

    102

    Peakbrilliance[Phot./(sec.mrad2.

    mm2.

    0.1

    %b

    andw.)

    ]

    1019

    1021

    1023

    1025

    1027

    1029

    1031

    1033

    1035

    103 104 105 106

    Photon energy (eV)

    Large-scale

    X-ray FELS

    FEL

    1-GeV beam

    3-m undulatorRadiation source

    Large-scale synchrotron

    radiation source

    40 TW, 30 fs

    laser pulse

    Focusing

    magnets

    Coherent X-ray

    radiation

    3 m

    1GeV

    electron

    beam

    Undulator

    magnet

    3-cm capillary

    plasma

    accelerator

    Figure 1 The path to X-rays on a table top. a, By combining the ability to produce 1-GeV electron beams rom a

    3-cm-long capillary laser wakefeld accelerator recently demonstrated by Leemans et al.7 with the synchrotron

    radiation scheme demonstrated by Schlenvoigt et al.5, a compact, high-brilliance source o coherent X-rays couldsoon become a reality. b, Peak brilliance o undulator synchrotron radiation sources as a unction o photon energy.

    Data rom re. 3. Taking the beam parameters reported by Leemans et al. (energy o 1 GeV, and an electron bunch

    length and charge o 10 s and 30 pC), a high-brilliance source comparable to existing large-scale synchrotron

    radiation should be readily achievable. In the FEL regime, such radiation could be amplifed by many orders o

    magnitude, to levels o brilliance similar to kilometre-scale FELs24 currently under construction.

    http://www.nature.com/naturephysicsmailto:[email protected]:[email protected]://www.nature.com/naturephysics
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