• Matter and Radiation at Extremes
  • Vol. 4, Issue 2, 24201 (2019)
O. Renner1、* and F. B. Rosmej2、3
Author Affiliations
  • 1Institute of Physics and ELI-Beamlines Project, Academy of Sciences of the Czech Republic, Na Slovance 2, 18221 Prague, Czech Republic
  • 2Sorbonne University, Faculty of Science and Engineering, UMR7605, Case 128, 4 Place Jussieu, F-75252 Paris Cedex 05, France
  • 3LULI, Ecole Polytechnique, CEA, CNRS, Physique Atomique dans les Plasmas Denses PAPD, Route de Saclay, F-91128 Palaiseau, France
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    DOI: 10.1063/1.5086344 Cite this Article
    O. Renner, F. B. Rosmej. Challenges of x-ray spectroscopy in investigations of matter under extreme conditions[J]. Matter and Radiation at Extremes, 2019, 4(2): 24201 Copy Citation Text show less

    Abstract

    Advanced X-ray spectroscopic methods provide unique and critical data to study matter under extreme environmental conditions induced by high-intensity and high-energy lasers. The aim of this paper is to contribute to a contemporary discussion of the role of X-ray spectroscopy in the investigation of radiative properties of strongly coupled, highly correlated, and frequently weakly emissive plasma systems formed in matter irradiated by sub-petawatt and petawatt class lasers. After reviewing the properties of different X-ray crystal spectrometers, high-resolution X-ray diagnostic methods are surveyed with respect to their potential to study plasma-induced and externally induced radiation fields, suprathermal electrons, and strong electromagnetic field effects. Atomic physics in dense plasmas is reviewed with emphasis on non-Maxwellian non-LTE atomic kinetics, quasi-stationary and highly-transient conditions, hollow ion X-ray emission, and field-perturbed atoms and ions. Finally, we discuss the role of X-ray free electron lasers with respect to supplementary investigations of matter under extreme conditions via the use of controlled high-intensity radiation fields.
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    λ=λ0cosφ,(2)

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    1/p+1/q = 1/fh,v,(3)

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    p=RvRhsinθ2Rhsin2θRvq,(4)

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    K2L8M18N1+ehotK1L8M18N1+2e,(5)

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    K1L8M18N1K2L7M18N1+ωKα1,2.(6)

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    fhot=ne,hotne,hot+ne,bulk,(7)

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    neτplasma=1D+R+I+neT,(8)

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    neτplasma3×1011cm3 s(9)

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    K0LNK1LN1+ωhollow.(10)

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    N˜0=IFEL,δE,τ4cerf2(ln2)EFEL3.6108IFEL,δE,τ(W/cm2)EFEL(eV)[cm3],(11)

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    Ephoto=EXFELEcore,(12)

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    EE1E2=Ei.(13)

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    τji=1Aji+Cji+Cij+kΓjk1kΓjk110 fs.(14)

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    K2LN+ωXFELK1LN+e,(15)

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    K1LN+ωXFELK0LN+e,(16)

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    K0LNK1LN1+ωhollow–K0(17)

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    K2LN+ωXFELK1LN+ephoto,1,(18)

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    K1LN+ωXFELK0LN+1,(19)

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    K0LN+1K1LN+ωhollow.(20)

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    O. Renner, F. B. Rosmej. Challenges of x-ray spectroscopy in investigations of matter under extreme conditions[J]. Matter and Radiation at Extremes, 2019, 4(2): 24201
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