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Relevant bibliographies by topics / Krypton

Academic literature on the topic 'Krypton'

Author: Grafiati

Published: 4 June 2021

Last updated: 31 July 2024

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Journal articles on the topic "Krypton"

1

Mitroy, Jim. "The Momentum Transfer Cross Section for Krypton." Australian Journal of Physics 43, no. 1 (1990): 19. http://dx.doi.org/10.1071/ph900019.

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A form of modified effective range theory (MERT) has been used to analyse drift velocity data for both pure krypton and molecular hydrogen-krypton mixtures. The present momentum transfer cross section reproduces the data to within 4% for pure krypton and to within 1 �0% for the H2-Kr mixtures.

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Kharlamov, G. V. "Simulating diffusion in the conditions of vapor-liquid phase transition by the molecular dynamics method." Journal of Physics: Conference Series 2057, no. 1 (October 1, 2021): 012114. http://dx.doi.org/10.1088/1742-6596/2057/1/012114.

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Abstract The molecular dynamics calculations of diffusion coefficients in binary Lennard-Jones systems have been carried out. The parameters of Lennard-Jones potentials correspond to argon and krypton atoms. The universal dependence of the reduced diffusion coefficient of krypton atoms on density for the homogeneous systems of low and middle densities is found. The deviations of the diffusion coefficients from the universal function are observed for the systems in the vapor – liquid phase transition region. The simulations have shown that almost all krypton atoms have situated inside the liquid phase of argon. Special numerical experiments have shown that the nanodroplets of argon are formed as a result of homogeneous nucleation and then the krypton atoms are captured by these droplets. This phenomenon decreases the diffusion coefficient of krypton atoms greatly.

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Clapp, J. T., R. C. Mancini, E. C. Harding, M. A. Schaeuble, and A. J. Harvey-Thompson. "Observation and diagnostic application of Kr K-shell emission in magnetized liner inertial fusion experiments at Z." Review of Scientific Instruments 93, no. 10 (October 1, 2022): 103532. http://dx.doi.org/10.1063/5.0101860.

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In a series of Magnetized Liner Inertial Fusion (MagLIF) experiments performed at the Z pulsed power accelerator of Sandia National Laboratories, beryllium liners filled with deuterium gas pressures in the 4–8 atm range and a tracer amount of krypton were imploded. At the collapse of the cylindrical implosion, temperatures in the 1–3 keV range and atom number densities of ∼1023 cm−3 were expected. The plasma was magnetized with a 10 T axial magnetic field. Krypton was added to the fuel for diagnosing implosion plasma conditions. Krypton K-shell line emission was recorded with the CRITR time-integrated transmission crystal x-ray spectrometer. The observation shows n = 2 to n = 1 line emissions in B-, Be-, Li-, and He-like Kr ions and is characteristic of the highest electron temperatures achieved in the thermonuclear plasma. Detailed modeling of the krypton atomic kinetics and radiation physics permits us to interpret the composite spectral feature, and it demonstrates that the spectrum is temperature sensitive. We discuss temperatures extracted from the krypton data analysis for experiments performed with several filling pressures.

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Campeanu, R. I., R. P. McEachran, and A. D. Stauffer. "Positron impact ionization of krypton and xenon." Canadian Journal of Physics 77, no. 10 (February 15, 2000): 769–74. http://dx.doi.org/10.1139/p99-066.

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Several distorted-wave models for positron ionization of krypton and xenon are investigated. Our previous CPE (Coulomb plus Plane waves -- full Energy range) model produces reliable cross sections for krypton. For xenon, at high positron energies, the CPE results fall below experiment. We have proposed an alternate model DCPE4 that works well for both krypton and xenon. A common feature of both of these models is that the free electron and positron are treated differently.PACS No.: 34.90.+q

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Skorek, Richard, Serge Maillard, Amélie Michel, Gaëlle Carlot, Eric Gilabert, and Thomas Jourdan. "Modelling Fission Gas Bubble Distribution in UO₂." Defect and Diffusion Forum 323-325 (April 2012): 209–14. http://dx.doi.org/10.4028/www.scientific.net/ddf.323-325.209.

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The Cluster Dynamics method is assessed for the investigation of fission gas behaviour in a krypton-implanted and annealed UO2sample. The simulation results are then compared to Thermal Desorption Spectroscopy (TDS) data. A release mechanism is proposed: the initial burst is related to krypton migration via an interstitial mechanism, while the second stage of the release process can be accounted for by the diffusion of krypton in a substitutional position. This latter mechanism is compatible with a diffusion coefficient of 4.10-21m²/s.

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Kurzyna, Jacek, Maciej Jakubczak, Agnieszka Szelecka, and Käthe Dannenmayer. "Performance tests of IPPLM's krypton Hall thruster." Laser and Particle Beams 36, no. 1 (February 27, 2018): 105–14. http://dx.doi.org/10.1017/s0263034618000046.

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AbstractThe Institute of Plasma Physics and Laser Microfusion's (IPPLM) Hall effect thruster (Krypton Large IMpulse Thruster, KLIMT) is a 500 W class plasma engine with a mean diameter of discharge channel of 42 mm. KLIMT was developed within ESA/PECS project aiming to provide relatively small thruster for satellites that would be able to effectively operate with krypton propellant. Being several times less expensive than xenon, which is regarded as a propellant of choice for electric propulsion of electrostatic type, krypton since years has been suggested as an attractive alternative. In this paper, a design as well as performance tests of the laboratory model of KLIMT are discussed. It is shown that precise adjustment of magnetic field topography results in the stable operation of the thruster in wide range of operating conditions providing similar thrust and specific impulse production for both propellants. Maximum thrust produced with the use of xenon and krypton reached about 16–17 mN for mass flow rate of 1.15–1.2 mg/s resulting in specific impulse in the range of 1300–1500 s (13–15 km/s). However, for krypton the anode efficiency drops by ~10% in comparison with xenon. For krypton plasma beam divergence as measured by an average half-angle with respect to the beam axis was found to remain within the range of 19–23° for the whole set of the examined operating conditions. The reported characteristics are reasonable for Hall thruster of the discussed size and power.

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Goharshadi, Elaheh K., Mina JamiAlahmadi, and Bijan Najafi. "Determination of potential energy functions of argon, krypton, and xenon via the inversion of reduced-viscosity collision integrals at zero pressure." Canadian Journal of Chemistry 81, no. 7 (July 1, 2003): 866–71. http://dx.doi.org/10.1139/v03-095.

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The pair potential energy functions of argon, krypton, and xenon have been determined via the inversion of reduced-viscosity collision integrals at zero pressure. A comparison of the potentials with the previously determined potentials are included. The viscosity and thermal conductivity of argon, krypton, and xenon at different temperatures and pressures have been calculated and compared with experimental values. The present potentials for argon, krypton, and xenon provide a good overall account of the experimental properties of these compounds, considering the stated uncertainty in the measurements.Key words: potential energy function, collision integral, viscosity, thermal conductivity.

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Zhou, Bo, Rui Yan, Xiaohan Yu, Yang Zou, Shihe Yu, Pu Yang, and Yafen Liu. "Study on Kinetic Characteristics of Krypton and Xenon radioactive source term in molten salt reactor." EPJ Web of Conferences 239 (2020): 22005. http://dx.doi.org/10.1051/epjconf/202023922005.

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A numerical simulation program for the dynamic distribution of krypton and xenon with flow and on-line removal function was established for primary loop system of molten salt reactor(MSR) Based on Mathe-matica7.0.The simulation results of the static burnup was compared with ORIGEN-S program, and the deviation is less than 10%, which is in good agreement.The distribution and dynamic characteristics of krypton and xenon in the primary loop system were analyzed under the flow regionalization and online removal model.The results show that,the static burnup model underestimates the total 135Xe activity about 6.61% in the system, and the total activity of krypton and xenon in the system is underestimated by about 1.46%.Under the maximum removal fraction, the total activity of krypton and xenon in the exhaust gas system is 1.84×1016Bq, of which 83mKr, 85mKr, 87Kr, 88Kr, 133Xe, 135Xe and 138Xe account for about 95.6%.The total activity of krypton and xenon in the primary loop system is 2.64×1014Bq, of which 138Xe, 135mXe, 134mXe, 87Kr and 83mKr account for about 93.6%.The numerical simulation method and the conclusion consistent with the actual physical laws.Dynamic distribution, evolution and migration characteristics of krypton, xenon and these precursor in the primary loop in the molten salt can be simulated more accurately compared to static burnup model.The analysis results can provide a theoretical basis for the management scheme of airborne source termsthe cooling design of the radioactive exhaust system and the source term analysis in accident conditions for the molten salt reactor.

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Ordookhanians, Allen, Xin Li, Supun Nakandala, and Arun Kumar. "Demonstration of Krypton." Proceedings of the VLDB Endowment 12, no. 12 (August 2019): 1894–97. http://dx.doi.org/10.14778/3352063.3352093.

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Akimov, D. Yu, A. I. Bolozdynya, D. L. Churakov, A. V. Koutchenkov, V. F. Kuzichev, V. N. Lebendenko, I. A. Rogovsky, M. Chen, V. Yu Chepel, and V. V. Sushkov. "Condensed krypton scintillators." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 327, no. 1 (March 1993): 155–58. http://dx.doi.org/10.1016/0168-9002(93)91433-n.

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Dissertations / Theses on the topic "Krypton"

1

Firmann, Markus. "Dendritic solidification of krypton /." [S.l.] : [s.n.], 1987. http://e-collection.ethbib.ethz.ch/show?type=diss&nr=8346.

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Savard, Guy. "Saturation spectroscopy of krypton." Thesis, McGill University, 1985. http://digitool.Library.McGill.CA:80/R/?func=dbin-jump-full&object_id=63379.

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Ham, Hamphrey. "Etudes méthodologiques des applications médicales du krypton-81M." Doctoral thesis, Universite Libre de Bruxelles, 1986. http://hdl.handle.net/2013/ULB-DIPOT:oai:dipot.ulb.ac.be:2013/241287.

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Audet, Daniel. "Spectroscopie de polarisation : isotopes du krypton." Thesis, McGill University, 1985. http://digitool.Library.McGill.CA:80/R/?func=dbin-jump-full&object_id=63319.

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Petch, Jason Charles. "Resonant four-wave mixing in krypton." Thesis, Imperial College London, 1996. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.243502.

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King, Sean J. "Electron impact excitation of krypton atoms." Thesis, Queen's University Belfast, 1987. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.317100.

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KERDOUSSI, ABDERRAZAK. "Excitation multiphonique du krypton (#3p#1) et du xenon (5d) : spectroscopie dans l'ultraviolet lointain : cinetique du krypton." Toulouse 3, 1989. http://www.theses.fr/1989TOU30076.

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Creation selective par absorption multiphotonique, de differents etats du krypton et du xenon dans les domaines de pression variable 10##1 a 800 torr. Aux fortes pressions, l'etat 1#u(#3p#1) est cree par absorption de trois photons laser et/ou par un photon provenant de la generation d'harmoniwue 3 du faisceau laser. Determination des constantes de disparition par choc a deux et trois corps de l'etat resonnant #3p#1, mise en evidence de la participation de l'etat metastable #3p#1 a la formation de l'etat moleculaire 1#u(#3p#2). Pour le xenon, excitation par absorption a trois photons des etats 5d(5/2)#0#j#=#3 et 5d (7/2)#0#j#=#3

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Kisand, Vambola. "Creation of free excitons in solid krypton investigated by time resolved luminescence spectroscopy." [S.l. : s.n.], 2001. http://deposit.ddb.de/cgi-bin/dokserv?idn=961700092.

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Jabbour, Georges. "Etude des excimères de krypton et de xénon par TALIF : applications aux décharges à barrière diélectrique dans le krypton." Toulouse 3, 2009. http://thesesups.ups-tlse.fr/697/.

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Ce travail porte sur l'étude des mécanismes réactionnels de formation des excimères de krypton et la mesure de l'influence de la température sur la formation des excimères de krypton et de xénon. Ces études permettent de rendre compte des phénomènes mis en jeu dans un milieu plus complexe (micro-décharge). Les expériences les plus récentes sur les mécanismes de formation des excimères font appel à l'étude de la fluorescence induite par absorption de deux photons laser (TALIF). Cette technique d'excitation a permis de peupler sélectivement les deux premiers excités du krypton et du xénon à partir desquels sont créés les excimères émettant le rayonnement UVL. L'étude temporelle des émissions UVL du krypton a été réalisée après peuplement sélectif soit du premier état métastable Kr5s [3/2]o2 soit du premier état résonant Kr5s [3/2]o1. La contribution de chacun de ces états dans les émissions UVL en fonction de la pression a ainsi pu être déterminée. Les processus conduisant a la formation des excimères ont été identifiés. Les taux de réactions par collisions à trois corps de disparition des états résonant et métastable ont été mesurées tout comme la durée de vie radiative de l'excimères Kr2 (A1u). Un transfert efficace de l'état résonant vers l'état métastable a été mis en évidence. Cette étude sous excitation sélective s'est poursuivie par l'étude de l'influence de la température sur la formation des excimères de krypton et de xénon. Elle a conduit à la détermination des lois de variation des constantes de disparition à trois corps des premiers états métastables de ces gaz en fonction de la température. Elles montrent sans ambigüité que ces constantes de réaction varient fortement en fonction de la température. Il s'agit là de données de base nouvelles obtenues pour la première fois en excitation sélective. Les études spectroscopiques et temporelles conduites en excitation sélective dans le krypton ont permis d'interpréter les mesures effectuées dans une micro-décharge. Les mesures électriques sont comparées à celles effectuées dans d'autres gaz rares lors d'études antérieures. Les mesures spectroscopiques et temporelles ont été analysées à partir de celles réalisées par fluorescence induite par laser
This work deals about the study of reactionnal mechanisms of krypton excimers forming and the influence of the temperature on the formation of krypton and xenon excimers. These studies can account for the phenomena involved in a more complex (micro-discharges). The most recent experiments of the mechanisms of the formation of excimers (involve the study) of the fluorescence induced via the absorption of two (photons laser) (TALIF). This excitation technique permits to selectively populate the first two excited states of krypton and xenon from which are created the excimers emitting UVL radiation (excitation spectroscopy). The study of temporal LVU emissions of krypton was performed after selective settlement, either from the first metastable state Kr5s [3/2]o2 or from the first resonant state Kr5s [3/2]o1. The contribution of each of these statements in UVL emissions depending on pressure has been determined. The process leading to the formation of excimers was identified. The reaction rates of disappearance of resonant and metastable states caused by the collision of three body, was measured as the radiative lifetime of the excimer Kr2 (A1u). A transfer, from the resonant state towards the metastable state was highlighted. This enabled us to complete the kinetic patterns obtained in the group in previous studies. This study under selective excitation was followed by studying the influence of temperature on the formation of excimer krypton and xenon. It led to the determination of laws of constants variation of disappearance of the first metastable states of these gases depending on temperature. They show unambiguously that the reaction constants vary greatly depending on temperature. This is the basis of new data obtained for the first time in selective excitation. Spectroscopic and temporal studies conducted in selective excitation in krypton, permitted to interpret the measurements in a micro-discharge by the team. The electrical measurements are compared to those made in other rare gases in previous studies. The temporal and spectroscopic measurements were analyzed from those produced by laser-induced fluorescence

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Shrimpton, Neil Douglas. "Low temperature behavior of krypton monolayers on graphite." Thesis, University of British Columbia, 1987. http://hdl.handle.net/2429/27531.

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The low temperature behaviour of a system of incommensurate krypton monolayers on graphite was analysed. The free energy was calculated for a variety of monolayer configurations and the misfit and orientation of the minimum energy configuration determined as a function of the temperature and chemical potential of the system. The free energy did not vary significantly over the temperature range from 0 K to 4 K. The zero point energy contributes significantly to the free energy and could not be neglected. The lowest energy vibrational modes were determined; these modes correspond to motion of the domain walls. For configurations with clearly separated domain walls the vibrational modes separated into groups of three (triads). In the lowest energy triad, the lowest energy mode was a compressional mode. The second and third lowest modes were shearing modes. These three modes describe the fundamental forms of domain wall motion. The modes of the higher energy triads are more energetic forms of the lowest energy triad.
Science, Faculty of
Physics and Astronomy, Department of
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Books on the topic "Krypton"

1

Levy, Janey. Krypton. New York: Rosen Pub. Group, 2008.

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2

Robinson, James Dale. Superman: New Krypton. New York: DC Comics, 2010.

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Bertzeletou, Tina. Krypton, neon, xenon. Athēna: Diattōn, 1993.

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Patterson, Michael J. Krypton ion thruster performance. [Washington, DC: National Aeronautics and Space Administration, 1992.

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Joe, Casey, and McGuinness Ed, eds. Superman: Return to Krypton. New York: DC Comics, 2004.

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Robinson, James Dale. Superman: New Krypton, volume three. New York: DC Comics, 2009.

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Anderson, Kevin J. The last days of Krypton. New York: HarperEntertainment, 2007.

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Sterling, Gates, Robinson James 1972-, and Johns Geoff 1973-, eds. Superman: New Krypton, volume two. New York: DC Comics, 2009.

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Sterling, Gates, Robinson James 1972-, and Johns Geoff 1973-, eds. Superman: New Krypton, volume two. New York: DC Comics, 2009.

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Pierman, Carol J. The age of krypton: Poems. Pittsburgh: Carnegie Mellon University Press, 1989.

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Book chapters on the topic "Krypton"

1

Holland, Greg. "Krypton." In Encyclopedia of Earth Sciences Series, 1–4. Cham: Springer International Publishing, 2017. http://dx.doi.org/10.1007/978-3-319-39193-9_198-1.

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Holland, Greg. "Krypton." In Encyclopedia of Earth Sciences Series, 784–87. Cham: Springer International Publishing, 2018. http://dx.doi.org/10.1007/978-3-319-39312-4_198.

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Arndt, T. "Krypton." In Lexikon der Medizinischen Laboratoriumsdiagnostik, 1. Berlin, Heidelberg: Springer Berlin Heidelberg, 2017. http://dx.doi.org/10.1007/978-3-662-49054-9_1788-1.

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Arndt, T. "Krypton." In Springer Reference Medizin, 1410–11. Berlin, Heidelberg: Springer Berlin Heidelberg, 2019. http://dx.doi.org/10.1007/978-3-662-48986-4_1788.

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W. Leachman, Jacob, Richard T Jacobsen, Eric W. Lemmon, and Steven G. Penoncello. "Krypton." In Thermodynamic Properties of Cryogenic Fluids, 199–210. Cham: Springer International Publishing, 2017. http://dx.doi.org/10.1007/978-3-319-57835-4_14.

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Šmalc, Andrej, Karel Lutar, Boris Žemva, and Scott A. Kinkead. "Krypton Difluoride." In Inorganic Syntheses, 11–15. Hoboken, NJ, USA: John Wiley & Sons, Inc., 2007. http://dx.doi.org/10.1002/9780470132609.ch6.

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Winkelmann, J. "Diffusion of krypton." In Gases in Gases, Liquids and their Mixtures, 137–43. Berlin, Heidelberg: Springer Berlin Heidelberg, 2007. http://dx.doi.org/10.1007/978-3-540-49718-9_32.

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Predel, B. "Au-Kr (Gold - Krypton)." In Ac-Ag ... Au-Zr, 1. Berlin, Heidelberg: Springer Berlin Heidelberg, 2006. http://dx.doi.org/10.1007/10793176_231.

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Wohlfarth, Ch. "Surface tension of krypton." In Supplement to IV/16, 22. Berlin, Heidelberg: Springer Berlin Heidelberg, 2008. http://dx.doi.org/10.1007/978-3-540-75508-1_5.

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Remme, Willem J. "Myocardial perfusion and krypton-81m." In Developments in Cardiovascular Medicine, 49–68. Dordrecht: Springer Netherlands, 1992. http://dx.doi.org/10.1007/978-94-011-2456-0_5.

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Conference papers on the topic "Krypton"

1

PATTERSON, MICHAEL, and GEORGE WILLIAMS, JR. "Krypton ion thruster performance." In 28th Joint Propulsion Conference and Exhibit. Reston, Virigina: American Institute of Aeronautics and Astronautics, 1992. http://dx.doi.org/10.2514/6.1992-3144.

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Cannon, B. D. "Hyperfine spectroscopy of krypton-81." In OSA Annual Meeting. Washington, D.C.: Optica Publishing Group, 1990. http://dx.doi.org/10.1364/oam.1990.tuy33.

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The hyperfine constants of krypton-81 and its isotope shifts relative to the stable krypton isotopes were measured for several transitions from the 5s [3/2] J = 2 metastable state. These measurements used continuous-wave single-frequency lasers for Doppler-free two-photon and saturated absorption spectroscopy. These measurements and the implications of the measured splittings for proposed ultratrace detection of krypton-81 for dating ancient ground water and glaciers will be discussed.

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Hill, K. D. "The triple point of krypton." In TEMPERATURE: ITS MEASUREMENT AND CONTROL IN SCIENCE AND INDUSTRY, VOLUME 8: Proceedings of the Ninth International Temperature Symposium. AIP, 2013. http://dx.doi.org/10.1063/1.4819539.

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Perry, Michael D., O. L. Landen, E. M. Campbell, and A. Szoke. "Resonant multiphoton ionization of krypton." In OSA Annual Meeting. Washington, D.C.: Optica Publishing Group, 1987. http://dx.doi.org/10.1364/oam.1987.tus4.

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The multiphoton ionization of krypton via a three-photon intermediate resonance is investigated using the second harmonic output of a short pulse dye laser system. The laser was tuned over the range λ = 2860 to 3000 Å in order to investigate the influence of the 4p → 5d and 4p → 6s intermediate resonances on the ionization rate. Enhancements of more than an order of magnitude over the nonresonant four-photon ionization were observed at intensities as high as 8 × 1012 W/cm2.

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5

Kramer, S. D., G. S. Hurst, C. H. Chen, M. G. Payne, S. L. Allman, R. C. Phillips, B. E. Lehmann, et al. "Analysis of 81Kr in groundwater using laser resonance ionization spectroscopy." In OSA Annual Meeting. Washington, D.C.: Optica Publishing Group, 1985. http://dx.doi.org/10.1364/oam.1985.tha3.

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A new analytical technique based on resonant ionization of krypton with a vacuum ultraviolet (VUV) laser source was used to determine low-level 81Kr concentrations in groundwater. The long half-life (210,000 yr) and low concentration (1.3 × 103 81Kr atoms/liter of modern water) make the detection of 81Kr by radioactive counting techniques extremely difficult. In this method, krypton gas was removed from water taken from an underground Swiss aquifer using standard cryogenic and chromatographic techniques. Stable krypton isotopes were then reduced by a factor of 107 by a two-stage isotopic enrichment cycle using commercial mass spectrometers. The enriched gas containing ~108 stable krypton atoms and ~103 atoms of 81Kr was implanted into a silicon disk. This disk was then placed in the high vacuum final counting chamber and the krypton released by laser annealing. This chamber contained a quadruple mass spectrometer which used a pulsed VUV laser source as the ionizer.1,2 The measured signal indicated that the sample contained 1200 (±300) atoms of 81Kr.

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Thornhill, Joseph W., John P. Apruzese, Jack Davis, and Robert W. Clark, Jr. "Photoresonant neonlike krypton x-ray lasers." In San Diego, '91, San Diego, CA, edited by Szymon Suckewer. SPIE, 1992. http://dx.doi.org/10.1117/12.134831.

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Clément, E. "Shape Coexistence In Light Krypton Isotopes." In NUCLEI AT THE LIMITS. AIP, 2005. http://dx.doi.org/10.1063/1.1905291.

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Görgen, A. "Shape Coexistence in Light Krypton Isotopes." In EXOTIC NUCLEAR SYSTEMS: International Symposium on Exotic Nuclear Systems ENS'05. AIP, 2005. http://dx.doi.org/10.1063/1.2140666.

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Sandstrom, R. L., R. P. Akins, U. K. Sengupta, C. Reiser, D. G. Larson, and S. L. Anderson. "Krypton Fluoride Excimer Laser for Microlithography." In 1989 Microlithography Conferences, edited by Burn J. Lin. SPIE, 1989. http://dx.doi.org/10.1117/12.953169.

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Jaenisch, Holger M. "Krypton Processing Of Argon-Ion Lasers." In 1988 Los Angeles Symposium--O-E/LASE '88, edited by Peter P. Chenausky, Roland A. Sauerbrey, and James H. Tillotson. SPIE, 1988. http://dx.doi.org/10.1117/12.944409.

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Reports on the topic "Krypton"

1

Knecht, D. A. Design documentation: Krypton encapsulation preconceptual design. Office of Scientific and Technical Information (OSTI), October 1994. http://dx.doi.org/10.2172/147730.

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2

Oliver, Brian M., Greg C. Eiden, and Nathan E. Ballou. Implantation and Release of Krypton with Copper Foils. Office of Scientific and Technical Information (OSTI), September 2001. http://dx.doi.org/10.2172/786814.

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3

Oliver, Brian M., Greg C. C. Eiden, and Nathan E. Ballou. Implantation and Release of Krypton with Copper Foils. Office of Scientific and Technical Information (OSTI), September 2001. http://dx.doi.org/10.2172/15003484.

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4

Turkevich, A., L. Winsberg, H. Flotow, and R. M. Adams. The radioactivity of atmospheric krypton in 1949--1950. Office of Scientific and Technical Information (OSTI), August 1997. http://dx.doi.org/10.2172/510355.

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5

Hohorst, F. A., and M. A. Sherlock. Partitioning of krypton-85 in liquid scintillation cocktail. Office of Scientific and Technical Information (OSTI), December 1994. http://dx.doi.org/10.2172/10116930.

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6

Whitehead, C. A., B. D. Cannon, and J. F. Wacker. Krypton isotope analysis using near-resonant stimulated Raman spectroscopy. Office of Scientific and Technical Information (OSTI), December 1994. http://dx.doi.org/10.2172/10106570.

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7

Cannon, Bret D., and Robert F. Shannon. Experimental Investigation of Continuous-Wave Laser Ionization of Krypton. Office of Scientific and Technical Information (OSTI), October 2001. http://dx.doi.org/10.2172/789273.

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8

Sanner, R., and J. Satcher, Jr. Synthesis and characterization of krypton and xenon clathrate complexes. Office of Scientific and Technical Information (OSTI), September 1989. http://dx.doi.org/10.2172/5554172.

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9

Cannon, Bret D. Model Calculations of Continuous-Wave Laser Ionization of Krypton. Office of Scientific and Technical Information (OSTI), July 1999. http://dx.doi.org/10.2172/9150.

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10

Cannon, Bret D., and Robert F. Shannon. Experimental Investigation of Continuous-Wave Laser Ionization of Krypton. Office of Scientific and Technical Information (OSTI), October 2001. http://dx.doi.org/10.2172/965653.

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