Survey
* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
Two-color excitation of highly charged ions with keV X-ray radiation: a look from current experimental and theoretical RCE studies to XFEL perspectives V.V.Balashov, A.A.Sokolik, A.V.Stysin D.V.Skobeltsyn Institute of Nuclear Physics, M.V.Lomonosov Moscow State University, Moscow 119991, Russia Parameters of X-ray radiation from RCE and XFEL devices in keV energy range Channeled 423 MeV/u ions Fe24+ in [220] plane of Si crystal [*,**] The European XFEL Technical Design Report Wavelengths Photon energy, keV Coherence Polarization SASE 1 SASE 2 0.1 nm 12.4 yes linear 0.1-0.4 nm 3.1 –1 2.4 yes linear SASE 3 0.4-1.6 nm 0.8 - 3.1 yes circular, linear 0.07 – 0.46 nm 2.7 – 16.8 yes circular, linear [*] T.Azuma , Y.Takabayashi, C.Kondo, T.Muranaka et al. PRL 97 (2006) 145502 [**] V.V.Balashov, A.A.Sokolik, V.K.Dolinov, A.V.Stysin, JETP 107 (2008) 133; JETP Letters 89 (2009) 399. X rays < 100 > The Okorokov resonance condition ion trajectory θγ < 001 > q channe zion er l cent 1s2p : 1P1 < 010 > 6700.41 eV 1s2p : 3P1 ~ 4.5 eV X-ray RCE 1s2 : 1S0 V.V.Balashov, A.A.Sokolik, A.V.Stysin, JETP 107 (2008) 133 Fe24+ φγ < 100 > X rays ion trajectory θγ < 001 > q channe zion er l cent 1s2p : 1P1 < 010 > 6700.41 eV 1s2p : 3P1 X-ray RCE 1s2 : 1S0 Fe24+ From spectral and geometrical properties of the resonating electric field of the crystal to Stokes parameters of the characteristic X-ray radiation The elliptic character of the resonating in-crystal electric field in the rest frame of the trajectory defined propagating ion under planar channeling is the origin of variability of polarization properties of the produced X-ray radiation. But channeling is not a pre-requisite for resonant coherent excitation ! 1965 – 2006 : RCE exclusively with channeled ions – V.V.Okorokov, Yad. Fiz. 2 (1965) 1009; Pis’ma Zh. Eksp. Teor.Fiz 2 (1965) 175 S.Datz, C.D.Moak et al., PRL 40 (1978) 843; NIM 170 (1980) 15 K.Komaki, T.Azuma et al., NIM B 146 (1998) 19, and many other. Since 2006: RCE measurements with (a) channeled ions and (b) without channeling at all Present-day portrait of the RCE process (the Okorokov effect) from Tokyo RCE measurements of 2006-2009: Anisotropic X-ray emission from helium-like Fe24+ ions aligned by RCE with a periodic crystal potential – T.Azuma et al., PRL 97 (2006) 145502; Three-dimensional RCE of nonchanneling ions in a crystal – C.Kondo et al., PRL 97 (2006) 135503; Trajectory dependent RCE of planar-channeled ions in a thin Si crystal – C.Kondo et al. NIM B 256 (2007) 157; Doubly-resonant coherent excitation of HCI planar channeling in a Si crystal – Y.Nakano et al., J.Phys. Conf.Series 58 (2007) 359; Dressed atoms in flight through a periodic crystal field: X-UVU double resonances – Y.Nakai et al., PRL 101 (2008) 113201; RCE of lithium-like Li15+ ions in a thin Si crystal – Y.Nakano et al., J.Phys. Conf.Series 163 (2009) 012094; Polarization control in three-dimensional RCE – Y.Nakano et al., PRL 102 (2009) 085502; A unified concept for theoretical analysis of RCE data and suggestions for new measurements (Moscow State University; 1998-2009) Characteristic X-ray production in the RCE process V.V. Balashov, I.V. Bodrenko -- Phys.Lett. A 352 (2006) 129 Metastable ion production in the RCE process V.V. Balashov, I.V. Bodrenko -- NIM B 245 (2006) 52 Resonant coherent excitation of Ar17+ ions in planar channel of a silicon crystal V.V. Balashov, A.A. Sokolik -- Optics and Spectroscopy 103 (2007) 761 Angular anisotropy of characteristic X-radiation and Auger electrons during the resonance coherent excitation of relativistic ions under planar channeling V.V.Balashov, A.A.Sokolik, A.V.Stysin -- JETP 107 (2008) 133. Characteristic X-ray radiation and Auger electrons from resonant coherently excited highly charged ions under channeling V.V.Balashov, A.A.Sokolik, A.V.Stysin -- NIM B 267 (2009) 903. Kinetics of double resonant coherent excitation of relativistic multicharged ions in crystals beyond the channeling conditions V.V.Balashov, A.A.Sokolik, A.V.Stysin -- JETP 108 (2009) 1010. Angular anisotropy of the RCE X-rays under planar channeling as manifestation of geometrical properties of the in-crystal electric field V.V.Balashov, A.A.Sokolik, A.V.Stysin -- NIM B 267 (2009) 1772. Polarization of photons emitted in the process of resonant coherent excitation of relativistic ions under planar channeling V.V.Balashov, V.K.Dolinov, A.A.Sokolik -- JETP Letters 89 (2009) 399. Density matrix description of resonant coherent excitations of swift highly charged ions in oriented crystals V.V.Balashov, I.V.Bodrenko, V.K.Dolinov, A.A.Sokolik, A.V.Stysin – J.Phys.Conf.Ser. 163 (2009) 012087. Polarization and correlation aspects of resonant coherent excitation of fast highly charged ions in crystals V V Balashov -- J. Phys.: Conf. Ser. 212 (2010) 012028 2D RCE versus 3D RCE ? Conceptually, 2D- and 3D- measurements complement each other in current RCE studies, e.g.: a) exciting harmonic separation – clear advantage for 3D RCE; here, contrary to the 2D RCE case, each resonating harmonic is characterized not only by its frequency ω klmbut also by its well defined wave vector Kklm with |Kkl|m| not equal, generally, to ωklm; a) sensitivity to other, besides the oscillating electric field, intrinsic properties of the matter of ion propagation, – clear advantage for 2D RCE; the profile and splitting of the resonances are here under influence of the collective Lindhard potential of the crystal lattice (take an example of RCE of ionic autoionizing states). Common experimental difficulties and theoretical problems in both cases of 2D RCE and 3D RCE studies: a) in the experiment – tuning to resonance harmonic; b) in the theory - unified description of both coherent and incoherent (relaxation) ion-crystal interactions. From single to double (two-color) resonant coherent excitation Y.Nakano et al., J.Phys. Conf.Series 58 (2007) 359; A remarkable variety of combinations of frequency ranges in double 2D or 3D resonant coherent excitations – an important aspect in the parallel to be drawn between current RCE and possible XFEL studies (see below). From single to double (two-color) resonant coherent excitation Y.Nakano et al., J.Phys. Conf.Series 58 (2007) 359; A remarkable variety of combinations of frequency ranges in double 2D or 3D resonant coherent excitations – an important aspect in the parallel to be drawn between current RCE and possible XFEL studies (see below). Conceptually, 2D- and 3D- measurements complement each other in current RCE studies, e.g.: a) exciting harmonic separation – clear advantage for 3D RCE; here, contrary to the 2D RCE case, each resonating harmonic is characterized not only by its frequency ω klmbut also by its well defined wave vector Kklm with |Kkl|m| not equal, generally, to ωklm; a) sensitivity to other, besides the oscillating electric field, intrinsic properties of the matter of ion propagation, – clear advantage for 2D RCE; the profile and splitting of the resonances are here under influence of the collective Lindhard potential of the crystal lattice (take an example of RCE of ionic autoionizing states). Common experimental difficulties and theoretical problems in both cases of 2D RCE and 3D RCE studies: a) in the experiment – tuning to resonance harmonic; b) in the theory - unified description of both coherent and incoherent (relaxation) ion-crystal interactions. Swift ion in matter is an open quantum system; key point of the density-matrix RCE approach is in the unified time-dependent description of both coherent and incoherent ion-crystal interactions very small for relativistic ions ! Ionization and spontaneous de-excitation probabilities (1013 s-1) for Ar16+ and Fe 24+ ions in Si crystal in non-channeling condition calculated at average target density 4.99 x 1022 cm –3. 1s2 2p2 1s2p λionization λionization λX-ray λionization λX-ray λAuger Ar16+ (416 MeV/u) 13.6 28.3 10.5 52.2 12.4 34.5 Fe 24+ (433 MeV/u) 5.9 19.1 45.6 Swift ion in matter is an open quantum system; key point of the density-matrix RCE approach is in the unified time-dependent description of both coherent and incoherent ion-crystal interactions General scheme of our density-matrix approach As soon as the in-crystal electric field is known and wave functions of the free ion are chosen, one takes standard quantum mechanics to calculate matrix elements Vpq(t) . The incoherence parameters such as electron loss and collision induced level-to-level transition cross sections are calculated or taken from tables. The equations are solved numerically.Their solutions are transformed into RCE observables. When dealing with those related to polarization and angular correlation RCE phenomena, another aspect of the density matrix technique – statistical tensor calculations – is used throughout. Two-color excitation of highly charged ions with keV X-ray radiation: a look from current experimental and theoretical RCE studies to XFEL perspectives 4.8 eV to double RCE corrections from 2p -> 3s and 2p -> 3d excitations n=3 3934-3936 eV ~ 0.6 keV n=2 3318-3322 eV ~ 3.3 keV n=1 Ar17 Exp,: Tokyo Theory: Moscow The combined frequencies in current two-color RCE studies (n=1)→(n=2) and (n=2)→(n=3) double RCE of hydrogen-like ions Combined friequences REFs a) 3.3 keV; b) 0.6 keV C.Kondo et al., PRL 97 135503 (2006) V.V.Balashov, A.A.Sokolik, A.V.Stysin, JETP, 108 (2009) 1010 Auger electrons from double RCE The same without channeling Exp,: Tokyo Theory: Moscow, also strongly anisotropic angular distribution of the Auger electrons predicted The combined frequencies in current two-color RCE studies Combined friequences REFs (n=1)→(n=2) and (n=2)→(n=3) double RCE of hydrogen-like ions a) 3.3 keV; b) 0.6 keV C.Kondo et al., PRL 97 135503 (2006) V.V.Balashov, A.A.Sokolik, A.V.Stysin, JETP, 108 (2009) 1010 RCE of autoionizing states in helium-like ions; Ar16 a) 3.14 keV b) 3.28 keV Y.Nakano et al., J.Phys. Conf.Series 58 (2007) 359; V.V.Balashov, A.A.Sokolik, A.V.Stysin NIM B 267 (2009) 903. Autler-Townes effect in resonant coherent excitation of relativistic highly charged ions in crystals Autler-Townes doublet at resonant coherent excitation (RCE) of relativistic ions in crystals without channeling Ar 16+, 416 MeV/u t (Si) ~ 1 μm Tuning to coupling and probing resonances – by target rotation Autler-Townes doublet at resonant coherent excitation (RCE) of relativistic ions in crystals without channeling Ar 16+, 416 MeV/u t (Si) ~ 1 μm Both coupling and probing electric fields in the ion rest frame are strong! Pprobing = 7.2 x 1015 W/cm2 Ppumpong = 2.8 x 1015 W/cm2 Survival fraction measurements “Dressed atoms in flight through a periodic crystal field” –Y.Nakai, Y.Nakano, T.Azuma et al. Phys.Rev.Lett. 101, 113201 (2008) “Kinetics of double resonant coherent excitation of relativistic multicharged ions in crystals beyond channeling conditions” – V.V.Balashov, A.A.Sokolik, A.V.Stysin JETP 108 (2009) 1010 Red lines –calculation with 5x5 density matrix in basis 1s2:1S0; 1s2s:1S0; 1s2p:1P1(M=0;±1). No fitting parameters. Ω0 as a fitting parameter in the Autler-Townes formula = = 3.72 eV; Ω0 as calculated matrix element < 1s2p:1P1|V0,0,2|1s2s:1S0 > of the field = 3.55 eV Autler-Townes doublet in characteristic X-ray distribution X-ray radiation at double resonant coherent excitation Arbitrary normalization for experimental data and results of the calculations Drastic change in both experiment and calculation [JETP 108 (2009) 1010] in profile of the Autler-Townes doublet for X-ray photons detected in the (2,-2,0) plane direction [horizontal] and perpendicular to this plane [vertical] -clear demonstration of the potential of the Autler-Townes scheme in X-ray measurements to control polarization characteristics of double excitation of highly charged ions. Here - indication to “fine structure” magnetic quantum number splitting of the Autler-Townes dublet 1s2s:!S0 -- 1s2p:!PM=0;±1. The combined frequencies in current two-color RCE studies Combined friequences REFs (n=1)→(n=2) and (n=2)→(n=3) double RCE of hydrogen-like ions a) 3.3 keV; b) 0.6 keV C.Kondo et al., PRL 97 135503 (2006) V.V.Balashov, A.A.Sokolik, A.V.Stysin, JETP, 108 (2009) 1010 RCE of autoionizing states in helium-like ions; Ar16 a) 3.14 keV b) 3.28 keV Y.Nakano et al., J.Phys. Conf.Series 58 (2007) 359; V.V.Balashov, A.A.Sokolik, A.V.Stysin NIM B 267 (2009) 903. Autler-Townes effect in double RCE of helium-like ions; Ar16 a) 3.14 keV b) 15.03 eV Y.Nakai et al., PRL, 101, 113201 (2008) V.V.Balashov, A.A.Sokolik, A.V.Stysin, JETP, 108 (2009) 1010 Parameters of X-ray radiation from RCE and XFEL devices in keV energy range Channeled 423 MeV/u ions Fe24+ in [220] plane of Si crystal [*,**] The European XFEL Technical Design Report Wavelengths Photon energy, keV Coherence Polarization SASE 1 SASE 2 0.1 nm 12.4 yes linear 0.1-0.4 nm 3.1 –1 2.4 yes linear SASE 3 0.4-1.6 nm 0.8 - 3.1 yes circular, linear 0.07 – 0.46 nm 2.7 – 16.8 yes circular, linear [*] T.Azuma , Y.Takabayashi, C.Kondo, T.Muranaka et al. PRL 97 (2006) 145502 [**] V.V.Balashov, A.A.Sokolik, V.K.Dolinov, A.V.Stysin, JETP 107 (2008) 133; JETP Letters 89 (2009) 399. Also – high intensity of the photon energy flux: ~ 0.5 x 1016 W/cm2 (in the rest frame of propagating ion) Conclusion 1. Made 45 years ago Okorokov’s prediction on resonant coherent excitation of fast ions in crystals, famous S.Datz’s experiments united RCE with physics of highly charged ions and, now, the breadth and irresistible appeal of current research in this area by the Tokyo RCE collaboration – all this shows the process of resonant coherent excitation of fast highly charged ions in crystals as a real model for future XFEL studies in the keV range. Its basic parameters in current experimental and theoretical works (the produced photon energy, intensity of the X-ray radiation energy flux in the ion rest frame) look close to those usually related to XFELs. Even of not less importance is the unique feature of RCE as a tunable source of polarized X-ray radiation. True, RCE will never compete with lasers in whole. But the wide experience gained in experimental and theoretical RCE studies, especially concerning polarization and angular correlation aspects of the dynamics of various multi-photon processes in keV energy region, will be a strong support among others for future XFEL experiments. 2. The variety of combinations of the frequency ranges between two partners in typical twocolor RCE processes – from almost equal to each other keV photons at two-step excitation of ionic autoionizing states to the opposite strongly asymmetric case of soft, of some eV, pumping radiation combined with probing X-ray radiation of several keV in the Autler-Townes RCE investigations – suggests a real landmark for theoretical, experimental and, perhaps primarily, engineering work in preparing concrete XFEL devices in the keV range. 3. On the other hand, a lot of studies must be done in the nearest future for further development of the RCE methods themselves, as concerns their both fundamental aspects and possible practical application. Thank you!