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1

Jacksier, Tracey, and Ramon M. Barnes. "Atomic Emission Spectra of Xenon, Krypton, and Neon: Spectra from 200 to 900 nm by Sealed Inductively Coupled Plasma/Atomic Emission Spectroscopy." Applied Spectroscopy 48, no. 1 (1994): 65–71. http://dx.doi.org/10.1366/0003702944027543.

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The emission spectra of pure xenon, krypton, and neon are reported over the spectral range of 200 to 900 nm from an enclosed inductively coupled plasma discharge operated at atmospheric pressure and 350 W.
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2

El-Machtoub, G. "Contributions of high-n dielectronic satellites to krypton K-shell emission spectra." Canadian Journal of Physics 81, no. 10 (2003): 1177–83. http://dx.doi.org/10.1139/p03-097.

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We report here on the calculation of dielectronic recombination resonance strengths for high-lying K-shell resonance states of He-, Li-, and Be-like krypton ions. For proper analysis of spectral data explicit calculations of satellite intensity factors are carried out for all possible intermediate resonance states with n = 2–10. Our calculations successfully predict the details of X-ray emission spectra of highly charged krypton ions interacting with electron beams.PACS Nos.: 32.30.Rj, 32.70.Cs, 32.80.Rm, 34.79.+e
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3

PERERA, R. C. C., M. C. HETTRICK, and D. W. LINDLE. "HIGH RESOLUTION KRYPTON M4.5X-RAY EMISSION SPECTRA." Le Journal de Physique Colloques 48, no. C9 (1987): C9–645—C9–648. http://dx.doi.org/10.1051/jphyscol:19879110.

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4

Wang, Q., C. Zhou, and Z. Ma. "VUV spectra from the krypton-fluoride ionic excimer." Applied Physics B Lasers and Optics 61, no. 3 (1995): 301–4. http://dx.doi.org/10.1007/bf01082050.

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5

Gryzlova, Elena V., Maksim D. Kiselev, Maria M. Popova, Anton A. Zubekhin, Giuseppe Sansone, and Alexei N. Grum-Grzhimailo. "Multiple Sequential Ionization of Valence n = 4 Shell of Krypton by Intense Femtosecond XUV Pulses." Atoms 8, no. 4 (2020): 80. http://dx.doi.org/10.3390/atoms8040080.

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Sequential photoionization of krypton by intense extreme ultraviolet femtosecond pulses is studied theoretically for the photon energies below the 3d excitation threshold. This regime with energetically forbidden Auger decay is characterized by special features, such as time scaling of the level population. The model is based on the solution of rate equations with photoionization cross sections of krypton in different charge and multiplet states determined using R-matrix calculations. Predictions of the ion yields and photoelectron spectra for various photon fluence are presented and discussed.
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6

Kukla, K. W., A. E. Livingston, C. M. Vogel Vogt, et al. "Extreme-ultraviolet wavelength and lifetime measurements in highly ionized krypton." Canadian Journal of Physics 83, no. 11 (2005): 1127–39. http://dx.doi.org/10.1139/p05-066.

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We have studied the spectrum of highly ionized krypton in the extreme-ultraviolet wavelength region (50–300 Å), using beam-foil excitation of fast krypton ions at the Argonne ATLAS accelerator facility. We report measurements of transition wavelengths and excited-state lifetimes for n = 2 states in the lithiumlike, berylliumlike, and boronlike ions, Kr31+,32+,33+. Excited state lifetimes ranging from 10 ps to 3 ns were measured by acquiring time-of-flight-delayed spectra with a position-sensitive multichannel detector.PACS Nos.: 32.70.Cs, 32.30.Jc, 34.50.Fa
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7

Kochur, A. G., V. L. Sukhorukov, and Ye B. Mitkina. "Cascade-affected emission spectra of argon, krypton and xenon." Journal of Physics B: Atomic, Molecular and Optical Physics 33, no. 16 (2000): 2949–53. http://dx.doi.org/10.1088/0953-4075/33/16/301.

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8

van Herpen, W. M., W. Leo Meerts, and A. Dymanus. "Rotationally Resolved Spectroscopy of Tetracene and its Van Der Waals Complexes With Inert Gas Atoms." Laser Chemistry 6, no. 1 (1986): 37–46. http://dx.doi.org/10.1155/lc.6.37.

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Rovibronic spectra of tetracene (C18H12) and its Van der Waals complexes with argon and krypton have been resolved by using a well collimated molecular beam in combination with a single frequency dye laser. The rotational constants of tetracene have been deduced in the S0 and S1 electronic state. The rovibronic spectra of the Van der Waals complexes show an enhanced intersystem crossing.
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9

IBUKI, T., K. OKADA, K. KAMIMORI, et al. "RESONANT AUGER SPECTRA OF Kr NEAR THE L3 THRESHOLD." Surface Review and Letters 09, no. 01 (2002): 85–88. http://dx.doi.org/10.1142/s0218625x02001987.

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Auger electron spectra were studied by scanning the photon energy near the L 3 threshold of krypton. Two resonant transitions were observed in the photon energy region 1673–1678 eV for the first time. They were identified to be the resonant 3d -2 5s and 3d -2 4d states originating in the 2p 3/2-1 5s and 2p 3/2-1 4d excitations, respectively.
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10

Picconi, David, and Irene Burghardt. "Time-resolved spectra of I2 in a krypton crystal by G-MCTDH simulations: nonadiabatic dynamics, dissipation and environment driven decoherence." Faraday Discussions 221 (2020): 30–58. http://dx.doi.org/10.1039/c9fd00065h.

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Time- and frequency-resolved pump-probe spectra of I<sub>2</sub> in a krypton crystal are calculated and analyzed using high-dimensional multi-state quantum dynamics by the Gaussian-based multi-configuration time-dependent Hartree (G-MCTDH) method.
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11

Lewis, E. Neil, Patrick J. Treado, and Ira W. Levin. "A Miniaturized, No-Moving-Parts Raman Spectrometer." Applied Spectroscopy 47, no. 5 (1993): 539–43. http://dx.doi.org/10.1366/0003702934067144.

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A solid-state acousto-optic tunable filter (AOTF) is combined with krypton laser excitation (647 nm), holographic Raman filters, and photon-counting silicon avalanche photodiode (APD) detection to construct a miniaturized Raman spectrometer with no moving parts. The physically compact AOTF and the highly integrated APD provide a rugged, digitally controlled spectrometer of moderate spectral resolution and with a footprint comparable in size to a laboratory notebook. Instrument design details are considered and representative spectra are reported. Potential areas of application for this prototype Raman spectrometer are also discussed.
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12

ERIKSSON, B., S. SVENSSON, N. MÅRTENSSON, and U. GELIUS. "THE HIGH ENERGY EXCITED SHAKE-UP ELECTRON SPECTRA OF KRYPTON." Le Journal de Physique Colloques 48, no. C9 (1987): C9–531—C9–534. http://dx.doi.org/10.1051/jphyscol:1987987.

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13

Bitter, M., H. Hsuan, C. Bush, et al. "Spectra of heliumlike krypton from Tokamak Fusion Test Reactor plasmas." Physical Review Letters 71, no. 7 (1993): 1007–10. http://dx.doi.org/10.1103/physrevlett.71.1007.

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14

Piracha, N. K., K. Nesbett, S. Moten, and P. Moeller. "On the Time-Resolved Optogalvanic Spectra of Neon and Krypton." Contributions to Plasma Physics 47, no. 6 (2007): 435–44. http://dx.doi.org/10.1002/ctpp.200710056.

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15

Hirabayashi, Shinichi, and Koichi M. T. Yamada. "Infrared spectra of water clusters in krypton and xenon matrices." Journal of Chemical Physics 122, no. 24 (2005): 244501. http://dx.doi.org/10.1063/1.1943948.

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16

Seely, J. F., C. A. Back, C. Constantin, et al. "Krypton K-shell X-ray spectra recorded by the HENEX spectrometer." Journal of Quantitative Spectroscopy and Radiative Transfer 99, no. 1-3 (2006): 572–83. http://dx.doi.org/10.1016/j.jqsrt.2005.05.046.

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17

Yi-Zhi, Qu, and Peng Yong-Lun. "Relativistic Multichannel Treatment of Krypton Spectra across the First Ionization Threshold." Chinese Physics Letters 22, no. 8 (2005): 1884–86. http://dx.doi.org/10.1088/0256-307x/22/8/017.

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18

Hall, R. I., L. Avaldi, G. Dawber, M. Zubek, and G. C. King. "Observation of the krypton and xenon photoelectron satellite spectra near threshold." Journal of Physics B: Atomic, Molecular and Optical Physics 23, no. 24 (1990): 4469–85. http://dx.doi.org/10.1088/0953-4075/23/24/008.

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19

Raineri, M., M. Gallardo, J. Reyna Almandos, A. G. Trigueiros, and C. J. B. Pagan. "New Transition and Energy Levels of Three-Times Ionized Krypton (Kr IV)." Atoms 9, no. 3 (2021): 48. http://dx.doi.org/10.3390/atoms9030048.

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A capillary pulsed-discharge and a theta-pinch were used to record Kr spectra in the region of 330–4800 Å. A set of 168 transitions of these spectra were classified for the first time. We extended the analysis to twenty-five new energy levels belonging to 3s23p24d, 3s23p25d even configurations. We calculated weighted transition probabilities (gA) for all of the experimentally observed lines and lifetimes for new energy levels using a relativistic Hartree–Fock method, including core-polarization effects.
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20

OGURTSOV, A. N., E. V. SAVCHENKO, E. GMINDER, S. VIELHAUER, and G. ZIMMERER. "PHOTON YIELD FROM SOLID KRYPTON AND XENON AT THE EDGE OF EXCITON ABSORPTION." Surface Review and Letters 09, no. 01 (2002): 45–49. http://dx.doi.org/10.1142/s0218625x02001938.

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The spectra of photon yield from solid Xe and Kr were measured in the energy range of absorption of Γ(3/2) n = 1 excitons. Using combination of time-resolved spectroscopy with selective photoexcitation by synchrotron radiation, the creation of free excitons was experimentally separated from direct population of molecular emitting centers. For the first time the threshold of photon absorption by molecular trapped centers is observed in excitation spectra of free exciton luminescence.
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21

Frankowski, Marcin, Alice M. Smith-Gicklhorn, and Vladimir E. Bondybey. "Spectroscopy of the XeC2 molecule in xenon, argon, and krypton matrices." Canadian Journal of Chemistry 82, no. 6 (2004): 837–47. http://dx.doi.org/10.1139/v04-054.

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A self-igniting DC-electric discharge of C2H2 in Xe (matrix gas) or C2H2 and Xe in Ar or Kr (matrix gas) is used to produce and study the XeC2 molecule in these various rare gases at 12 K. Unlike in Ar and Kr, the well-known electronic spectra of C2 is completely absent in a Xe matrix. This together with annealing experiments in Ar matrices indicate that ground state Xe and C2 react uniquely and without a barrier to form the XeC2 molecule. The IR-active C-C stretch of this compound is found to be close to the C-C stretching frequency of the C2 anion, in excellent agreement with our density functional theoretical (DFT) calculations, which yield a XeCC singlet species bent by 148.6° and with substantial charge separation approaching Xe+C2– and a notably short (2.107 Å) Xe—C bond. The spectra of the Xe–13C–12C, Xe–12C–13C, and Xe–13C–13C species are also obtained and the isotopic shifts are in excellent agreement with the DFT predictions, although not sufficient to distinguish a bent from a linear structure. Numerous broad absorptions centered near 423 nm (in Xe) are observed, which are clearly due to the XeC2 molecule. Laser-induced fluorescence studies reveal a near-IR emission likely due to XeC2 but not yet understood. Infrared spectra in the Xe matrix reveal also formation of the HXeCCH molecule.Key words: matrix-isolation spectroscopy, rare gas compounds, charge transfer compounds, xenon–carbon bonds.
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22

Khasenov, M. U. "Emission spectra of noble gases and their mixtures under ion beam excitation." Laser and Particle Beams 34, no. 4 (2016): 655–62. http://dx.doi.org/10.1017/s0263034616000616.

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AbstractThe luminescence spectra of noble gases and their binary mixtures were measured using heavy ion beam excitation from a DC-60 accelerator. Spectra were measured in the range of 200–975 nm; the gas spectra were dominated by lines ofp–sandd–patomic transitions; in neon and argon, lines from atomic oxygen, N2, N2+, and OH radical bands were also observed. The ultraviolet region of the spectra was represented by a “third continuum” of noble gases. In krypton, the band of the KrO excimer molecule with a maximum at 557 nm was also observed. The maxima of the heteronuclear ionic molecules bands were located at wavelengths of 329 and 506 nm (Ar–Xe), 491 nm (Kr–Xe), and 642 nm (Ar–Kr). The relative intensities of the 2p–1stransitions of the noble gases atoms were measured and are discussed.
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23

Reininger, R., V. Saile, and A. M. Kohler. "Photoionisation yield spectra below the atomic ionisation energy in argon and krypton." Journal of Physics B: Atomic and Molecular Physics 20, no. 10 (1987): 2239–45. http://dx.doi.org/10.1088/0022-3700/20/10/016.

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24

Gerasimov, G., R. Khallin, and B. Krylov. "VUV spectra of krypton-xenon mixtures in a cooled DC-excited discharge." Optics and Spectroscopy 88, no. 2 (2000): 176–81. http://dx.doi.org/10.1134/1.626774.

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25

Klots, T. D., T. Emilsson, R. S. Ruoff, and H. S. Gutowsky. "Microwave spectra of noble gas-pyridine dimers: argon-pyridine and krypton-pyridine." Journal of Physical Chemistry 93, no. 4 (1989): 1255–61. http://dx.doi.org/10.1021/j100341a017.

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26

Harrison, Jeremy J., and Bryce E. Williamson. "Magnetic Circular Dichroism and Absorption Spectra of Methylidyne in a Krypton Matrix." Journal of Physical Chemistry A 115, no. 31 (2011): 8643–49. http://dx.doi.org/10.1021/jp2048986.

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27

Loginov, A. V., and V. I. Tuchkin. "Radiative constants in the spectra of ions of the krypton isoelectronic sequence." Optics and Spectroscopy 91, no. 2 (2001): 165–76. http://dx.doi.org/10.1134/1.1397835.

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28

Dmitriev, Yu A. "Peculiarities of EPR spectra of methyl radicals in quench-condensed krypton films." Low Temperature Physics 34, no. 1 (2008): 75–77. http://dx.doi.org/10.1063/1.2832359.

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29

Kovalík, A., V. M. Gorozhankin, A. F. Novgorodov, A. Minkova, M. A. Mahmoud, and M. Ryšavý. "The K and LMX Auguer spectra of krypton from the 83Rb decay." Journal of Electron Spectroscopy and Related Phenomena 58, no. 1-2 (1992): 49–66. http://dx.doi.org/10.1016/0368-2048(92)80006-t.

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30

Machtoub, G. El. "Channel-specific dielectronic recombination of Ge(XXXII), Se(XXXIV), and Kr(XXXVI)." Canadian Journal of Physics 82, no. 4 (2004): 277–89. http://dx.doi.org/10.1139/p04-011.

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We present explicit calculations of channel-specific dielectronic recombination cross sections for hydrogen-like germanium, Ge(XXXII); selenium, Se(XXXIV); and krypton, Kr(XXXVI). The convoluted cross sections characterize K-shell emission spectra over a wide energy range where contributions from high-n (n = 2–10), satellite lines are included. The high-n contributions presented are important for better diagnostics in the domain of high-temperature plasmas. PACS Nos.: 32.30.Rj, 32.70.Rm, 34.70.te
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31

Holtz, Janet S. W., Richard W. Bormett, Zhenhuan Chi, et al. "Applications of a New 206.5-nm Continuous-Wave Laser Source: UV Raman Determination of Protein Secondary Structure and CVD Diamond Material Properties." Applied Spectroscopy 50, no. 11 (1996): 1459–68. http://dx.doi.org/10.1366/0003702963904683.

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We demonstrate the utility of a new 206.5-nm continuous-wave UV laser excitation source for spectroscopic studies of proteins and CVD diamond. Excitation at 206.5 nm is obtained by intracavity frequency doubling the 413-nm line of a krypton-ion laser. We use this excitation to excite resonance Raman spectra within the π → π amide transition of the protein peptide backbone. The 206.5-nm excitation resonance enhances the protein amide vibrational modes. We use these high signal-to-noise spectral data to determine protein secondary structure. We also demonstrate the utility of this source to excite CVD and gem-quality diamond within its electronic bandgap. The diamond Raman spectra have very high signal-to-noise ratios and show no interfering broad-band luminescence. Excitation within the diamond bandgap also gives rise to narrow photoluminescence peaks from diamond defects. These features have previously been observed only by cathodoluminescence measurements. This new continuous-wave UV source is superior to the previous pulsed sources, because it avoids nonlinear optical phenomena and thermal sample damage; Photoluminescence.
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32

Et al., N. A. Nurmatov. "“EXPERIMENTAL STUDY OF PHOTOELECTRONIC SPECTRA OF NIOBIUM-HAFNIUM-ZIRCONIUM ALLOY”." Psychology and Education Journal 58, no. 1 (2021): 5581–85. http://dx.doi.org/10.17762/pae.v58i1.1956.

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Crystals of niobium and its alloys obtained by low-energy implantation of hafnium and zirconium ions have been studied in a multifunctional experimental setup. Distribution profiles of implanted hafnium and zirconium atoms, energy distributions of photoelectrons N (E), and spectral dependences of the quantum yield of photoelectron emission before and before and after heating of the niobium-hafnium-zirconium alloy have been investigated. The contribution of surface states and bands formed by hafnium and zirconium atoms to photoelectron emission in the photon energy range of 8–10 eV is analyzed. The experimental results are discussed on the basis of theoretical calculations of the surface, photoelectron emission in which the dominant factors are indirect optical transitions. The experiments were carried out under ultrahigh vacuum conditions using photoelectron and Auger electron spectroscopy. Krypton and xenon resonance lamps were used as radiation sources.&#x0D;
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33

Hirabayashi, Shinichi, and Koichi M. T. Yamada. "Infrared spectra and structure of water clusters trapped in argon and krypton matrices." Journal of Molecular Structure 795, no. 1-3 (2006): 78–83. http://dx.doi.org/10.1016/j.molstruc.2006.02.019.

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34

Durig, James R., Chao Zheng, Mohammad A. Qtaitat, Shiping Deng, and Gamil A. Guirgis. "Conformational stability from variable temperature infrared spectra of krypton solutions of 1,3-dichloropropane." Journal of Molecular Structure 657, no. 1-3 (2003): 357–73. http://dx.doi.org/10.1016/s0022-2860(03)00454-x.

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35

Date, H., K. Kondo, and H. Tagashira. "Transport coefficients defined by arrival time spectra of electron swarms in krypton gas." Journal of Physics D: Applied Physics 23, no. 11 (1990): 1384–89. http://dx.doi.org/10.1088/0022-3727/23/11/006.

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36

Verkhovtseva, E. T., E. A. Bondarenka, and yu s. Doronin. "Cluster size effects in vuv radiation spectra of argon and krypton supersonic jets." Chemical Physics Letters 140, no. 2 (1987): 181–88. http://dx.doi.org/10.1016/0009-2614(87)80811-4.

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37

Fritzsche, S., and G. Zschornack. "Effects of final-state interactions on the L-MM auger spectra of krypton." Zeitschrift f�r Physik D Atoms, Molecules and Clusters 21, S1 (1991): S155—S156. http://dx.doi.org/10.1007/bf01426271.

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38

Dawid, A., D. Wojcieszyk, and Z. Gburski. "Collision-induced light scattering spectra of krypton layer confined between graphite slabs – MD simulation." Journal of Molecular Structure 1126 (December 2016): 103–9. http://dx.doi.org/10.1016/j.molstruc.2016.01.063.

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39

Loginov, A. V. "Simulation of emission spectra of the gas-discharge plasma of a krypton-xenon mixture." Optics and Spectroscopy 109, no. 5 (2010): 655–61. http://dx.doi.org/10.1134/s0030400x10110020.

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40

Kochur, A. G. "Final-ion-charge spectra produced by cascading decay of hollow argon and krypton atoms." Journal of Electron Spectroscopy and Related Phenomena 114-116 (March 2001): 81–84. http://dx.doi.org/10.1016/s0368-2048(00)00240-1.

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41

Stewart, R. E., R. Dukart, D. D. Dietrich, and R. J. Fortner. "Soft-x-ray spectra of krypton xxiv–xxvii in gas puff Z-pinch plasmas." Journal of the Optical Society of America B 4, no. 3 (1987): 396. http://dx.doi.org/10.1364/josab.4.000396.

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42

Wyart, J. F., and TFR Group. "Identification of Krypton Kr XVIII to Kr XXIX Spectra Excited in TFR Tokamak Plasmas." Physica Scripta 31, no. 6 (1985): 539–44. http://dx.doi.org/10.1088/0031-8949/31/6/014.

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43

Nagels, V., C. Chenais-Popovics, V. Malka, J.-C. Gauthier, A. Bachelier, and J.-F. Wyart. "Spectra of Laser Irradiated Xenon and Krypton in the Wavelength Range 0.5–1.0 nm." Physica Scripta 68, no. 4 (2003): 233–43. http://dx.doi.org/10.1238/physica.regular.068a00233.

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44

Nixon, A. P., T. E. Gallon, F. Yousif, and J. A. D. Matthew. "Argon and krypton Auger spectra induced by ion bombardment of aluminium and silicon surfaces." Journal of Physics: Condensed Matter 6, no. 14 (1994): 2681–88. http://dx.doi.org/10.1088/0953-8984/6/14/006.

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45

Volkova, G. A. "XUV emission spectra of pulsed discharges through a capillary in xenon, krypton, and argon." Journal of Applied Spectroscopy 44, no. 1 (1986): 1–4. http://dx.doi.org/10.1007/bf00658307.

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46

Herron, J. R., and R. B. Peterson. "Optical Determination of Stagnation Temperature Behind a Gas Sampling Orifice." Journal of Heat Transfer 112, no. 4 (1990): 1070–75. http://dx.doi.org/10.1115/1.2910480.

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A technique has been developed for measuring the temperature during a transient combustion event. It combines the features of atomic resonance absorption and direct sampling to produce a relatively simple, intrusive diagnostic technique to obtain time-resolved measurements. In this study, a propagating hydrogen/air flame was used to provide a rapid temperature increase. A small fraction of krypton was added to the reactants and the absorption of resonant radiation at 123.5 nm was recorded downstream of the sampling orifice within a flow tube. Conversion from absorption measurements to temperature values was performed using a computer model of the radiation source and the absorption by the sample. The model of the source was validated by comparing predicted and recorded spectra of hydrogen Lyman-α emissions, while the absorption model for the sampled gas was tested by comparing the temperatures predicted by krypton absorption measurements with those recorded at a range of known temperatures. The direct sampling atomic resonance technique minimizes time-history distortions inherent in other direct sampling techniques, and is capable of tracking local temperatures during the passage of a propagating flame front.
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47

Wachulak, Przemysław, Martin Duda, Tomasz Fok, et al. "Single-Shot near Edge X-ray Fine Structure (NEXAFS) Spectroscopy Using a Laboratory Laser-Plasma Light Source." Materials 11, no. 8 (2018): 1303. http://dx.doi.org/10.3390/ma11081303.

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We present a proof of principle experiment on single-shot near edge soft X-ray fine structure (NEXAFS) spectroscopy with the use of a laboratory laser-plasma light source. The source is based on a plasma created as a result of the interaction of a nanosecond laser pulse with a double stream gas puff target. The laser-plasma source was optimized for efficient soft X-ray (SXR) emission from the krypton/helium target in the wavelength range from 2 nm to 5 nm. This emission was used to acquire simultaneously emission and absorption spectra of soft X-ray light from the source and from the investigated sample using a grazing incidence grating spectrometer. NEXAFS measurements in a transmission mode revealed the spectral features near the carbon K-α absorption edge of thin polyethylene terephthalate (PET) film and L-ascorbic acid in a single-shot. From these features, the composition of the PET sample was successfully obtained. The NEXAFS spectrum of the L-ascorbic acid obtained in a single-shot exposure was also compared to the spectrum obtained a multi-shot exposure and to numerical simulations showing good agreement. In the paper, the detailed information about the source, the spectroscopy system, the absorption spectra measurements and the results of the studies are presented and discussed.
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48

Poklonski, N. A., N. I. Gorbachuk, S. V. Shpakovski, et al. "DLTS SPECTRA OF SILICON DIODES WITH P+—N–JUNCTION IRRADIATED WITH HIGH ENERGY KRYPTON IONS." Izvestiya Vysshikh Uchebnykh Zavedenii. Materialy Elektronnoi Tekhniki = Materials of Electronics Engineering, no. 1 (March 14, 2015): 42. http://dx.doi.org/10.17073/1609-3577-2014-1-42-46.

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Poklonski, Nikolai A., Nikolay I. Gorbachuk, Sergey V. Shpakovski, et al. "DLTS spectra of silicon diodes with p+-n-junction irradiated with high energy krypton ions." Modern Electronic Materials 2, no. 2 (2016): 48–50. http://dx.doi.org/10.1016/j.moem.2016.09.001.

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Kulbida, Anatoly, and Rui Fausto. "Conformers, vibrational spectra and infrared-induced rotamerization of dichloroacetic acid in argon and krypton matrices." Journal of the Chemical Society, Faraday Transactions 89, no. 24 (1993): 4257. http://dx.doi.org/10.1039/ft9938904257.

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