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Artykuły w czasopismach na temat „Excited atoms”

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Autor: Grafiati

Data publikacji: 4 czerwca 2021

Data aktualizacji: 19 lutego 2022

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1

Adamatzky, Andrew. "On discovering functions in actin filament automata". Royal Society Open Science 6, nr 1 (styczeń 2019): 181198. http://dx.doi.org/10.1098/rsos.181198.

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We simulate an actin filament as an automaton network. Every atom takes two or three states and updates its state, in discrete time, depending on a ratio of its neighbours in some selected state. All atoms/automata simultaneously update their states by the same rule. Two state transition rules are considered. In semi-totalistic Game of Life like actin filament automaton atoms take binary states ‘0’ and ‘1’ and update their states depending on a ratio of neighbours in the state ‘1’. In excitable actin filament automaton atoms take three states: resting, excited and refractory. A resting atom excites if a ratio of its excited neighbours belong to some specified interval; transitions from excited state to refractory state and from refractory state to resting state are unconditional. In computational experiments, we implement mappings of an 8-bit input string to an 8-bit output string via dynamics of perturbation/excitation on actin filament automata. We assign eight domains in an actin filament as I/O ports. To write True to a port, we perturb/excite a certain percentage of the nodes in the domain corresponding to the port. We read outputs at the ports after some time interval. A port is considered to be in a state True if a number of excited nodes in the port's domain exceed a certain threshold. A range of eight-argument Boolean functions is uncovered in a series of computational trials when all possible configurations of eight-elements binary strings were mapped onto excitation outputs of the I/O domains.

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2

Friedrich, H. "Highly Excited Atoms". Zeitschrift für Physikalische Chemie 213, Part_1 (styczeń 1999): 110–11. http://dx.doi.org/10.1524/zpch.1999.213.part_1.110.

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3

Inagaki, Makoto, Kazuhiko Ninomiya, Akihiro Nambu, Takuto Kudo, Kentaro Terada, Akira Sato, Yoshitaka Kawashima, Dai Tomono i Atsushi Shinohara. "Chemical effect on muonic atom formation through muon transfer reaction in benzene and cyclohexane samples". Radiochimica Acta 109, nr 4 (11.02.2021): 319–26. http://dx.doi.org/10.1515/ract-2020-0112.

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Abstract To investigate the chemical effect on the muon capture process through a muon transfer reaction from a muonic hydrogen atom, the formation rate of muonic carbon atoms is measured for benzene and cyclohexane molecules in liquid samples. The muon transfer rate to carbon atoms of the benzene molecule is higher than that to the carbon atoms of the cyclohexane molecule. Such a deviation has never been observed among those molecules for gas samples. This may be because the transfers occur from the excited states of muonic hydrogen atoms in the liquid system, whereas in the gas system, all the transfers occur from the 1s (ground) state of muon hydrogen atoms. The muonic hydrogen atoms in the excited states have a larger radius than those in the 1s state and are therefore considered to be affected by the steric hindrance of the molecular structure. This indicates that the excited states of muonic hydrogen atoms contribute significantly to the chemical effects on the muon transfer reaction.

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4

LI, ZHIBING, i CHENGGUANG BAO. "SPINOR BEC IN THE LARGE-N LIMIT". International Journal of Modern Physics B 21, nr 23n24 (30.09.2007): 4248–55. http://dx.doi.org/10.1142/s0217979207045487.

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The superfine structure of Bose-Einstein condensate of alkali atoms due to the spin coupling have been investigated in the mean field approximation. In the limit of large number of atoms, we obtained the analytical solution for the fully condensed states and the states with one-atom excited. It was found that the energy of the one-atom excited state could be smaller than the energy of the fully condensed state, even two states have similar total spin.

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5

GORDILLO-VÁZQUEZ, F. J. "An approach to the ejection mechanisms of Li atoms from pulsed excimer laser ablation of a LiNbO3 target". Laser and Particle Beams 20, nr 2 (kwiecień 2002): 227–31. http://dx.doi.org/10.1017/s0263034602202116.

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A nonequilibrium kinetic model is used for predicting the time evolution of the Li atom concentrations (ground and excited states) in the plasma produced by excimer laser ablation of a LiNbO3 target. The model predicts a very high ionization degree (∼0.97) that agrees well with the one obtained experimentally (∼1). These results together with the prediction of high (and close to local thermodynamic equilibrium) population densities of the electronically excited Li upper energy levels provide an indirect support for an electronic rather than thermal ablation mechanism of Li atoms.

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6

Kweon, Gyeong-il, i N. M. Lawandy. "Dispersion interactions between excited atoms". Physical Review A 47, nr 5 (1.05.1993): 4513–16. http://dx.doi.org/10.1103/physreva.47.4513.

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7

Falcone, G., i F. Piperno. "Kinematics of sputtered excited atoms". Surface Science 365, nr 2 (wrzesień 1996): 511–16. http://dx.doi.org/10.1016/0039-6028(96)00715-7.

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8

Pogrebnyak, N. I., S. F. Dyubko, M. P. Perepechai i A. S. Kutsenko. "INVESTIGATION OF THE SPECTRUM OF ZN I ATOMS IN THE TRIPLET RYDBERG STATES". Radio physics and radio astronomy 26, nr 3 (14.09.2021): 256–69. http://dx.doi.org/10.15407/rpra26.03.256.

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Purpose: This work aims at investigating the zinc atoms in the triplet preionization – Rydberg states. The energy levels of atoms having two electrons outside the closed shell were studied mainly by the optical spectroscopy methods. However, just using the microwave spectroscopy to measure the frequency of transitions between the two Rydberg states allows to increase the accuracy of measurements in two or more orders of magnitude. Disign/methodology/approach:A line of three dye lasers is used to excite the zinc atoms into the triplet Rydberg states with a predetermined set of quantum numbers. The radiation of the first two of them is transformed into the second harmonic in nonlinear crystals. Dye lasers are excited by the radiation of the second harmonic of one YAG: ND3+ laser. All three radiations are reduced to the zone of interaction with the laser and the microwave radiation, which is located between the plates of the ionization cell, where the pulsed electric field is created. The excited Rydberg atoms are recorded with the field ionization procedure. The beam of neutral atoms is created by an effusion cell under the vacuum conditions, the residual pressure does not exceed 10-5 mm Hg. A pulsed electric field of some certain intensity results inionization of atoms excited by microwave radiation and in acceleration of electrons, which have appeared in the direction of the secondary electron multiplier, though being insufficient for ionization of atoms excited only by the laser radiation and which are initial for interaction with microwaves. By scanning the microwave radiation frequency with the given step and measuring the signal intensity of the secondary electron multiplier, the excitation spectrum of the atoms under study can be obtained. Findings: Using the created laser-microwave spectrometer, the frequencies of the F→D, F→F and F→G transitions between the triplet Rydberg states of zinc atoms were measured. From the analysis made of the transition frequencies, the quantum defect decomposition constants were obtained by the Ritz formula for the D, F, and G states of zinc atoms. Conclusions: The frequencies of the F→D, F→F and F→G transitions between the triplet Rydberg states of zinc atoms were measured that allowed obtaining the quantum defect decomposition constants according to the Ritz formula for the D, F and G states of zinc atoms, that in turn had allowed to calculate the energy of these terms and the transition frequencies at least in two orders of magnitude more accurately as against the similar measurements made by the optical spectroscopy. Key words: zinc atom, triplet states of atoms, Rydberg states, laser excitation, microwave radiation

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9

Mavroyannis, Constantine. "Adsorbate spectra of rare-gas atoms on metal surfaces". Canadian Journal of Chemistry 66, nr 4 (1.04.1988): 741–51. http://dx.doi.org/10.1139/v88-129.

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The optical excitation spectra of neutral rare-gas atoms physisorbed on metal surfaces have been considered. Emphasis has been given to the dynamic effects of the surface plasmons on the lifetimes of the adsorbed atoms. At low coverage and when the damping of the surface plasmons is much greater than the effective radiative damping, the spectral functions of the symmetric and antisymmetric modes consist of asymmetric Lorentzian lines, whose asymmetry depends on the strength of the surface plasmons. At this limit the relative intensities of the symmetric and antisymmetric modes take positive and negative values describing the physical processes of absorption (attenuation) and stimulated emission (amplification), respectively. Hence, the occasional disappearance of the spectral lines of the optical absorption is due to a cancellation process, which takes place between the frequency profiles arising from two nearby excited states of the adsorbed atom. The red shifted peak of the symmetric mode of the higher excited state and the blue shifted peak of the antisymmetric mode of the lower excited state of the atom cancel each other out provided that their frequency profiles nearly coincide. This may be a possible explanation of the persistence-extinction phenomenon that has been observed for a number of rare-gas substrate systems in the low coverage limit, where it has been proposed that a charge-transfer instability exists. Numerical results indicate that the peaks of excited Xe on Al and excited Kr on Au vanish in the low coverage limit.

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10

Dagviikhorol, Naranchimeg, Munkhsaikhan Gonchigsuren, Lochin Khenmedekh, Namsrai Tsogbadrakh i Ochir Sukh. "Imaginary-Time Time-Dependent Density Functional Calculation of Excited States of Atoms Using CWDVR Approach". Solid State Phenomena 323 (30.08.2021): 14–20. http://dx.doi.org/10.4028/www.scientific.net/ssp.323.14.

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We have calculated the energies of excited states for the He, Li, and Be atoms by the time dependent self-consistent Kohn Sham equation using the Coulomb Wave Function Discrete Variable Representation CWDVR) approach. The CWDVR approach was used the uniform and optimal spatial grid discretization to the solution of the Kohn-Sham equation for the excited states of atoms. Our results suggest that the CWDVR approach is an efficient and precise solutions of excited-state energies of atoms. We have shown that the calculated electronic energies of excited states for the He, Li, and Be atoms agree with the other researcher values.

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11

Шафраньош, І. І. "Electron inelastic interaction with excited atoms". Scientific Herald of Uzhhorod University.Series Physics 20 (30.06.2007): 12–16. http://dx.doi.org/10.24144/2415-8038.2007.20.12-16.

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12

Molina, Quintín R. "Doubly excited ridge states of atoms". Physical Review A 47, nr 6 (1.06.1993): 4713–19. http://dx.doi.org/10.1103/physreva.47.4713.

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13

Kweon, Gyeong-il, i N. M. Lawandy. "Erratum: Dispersion interactions between excited atoms". Physical Review A 49, nr 3 (1.03.1994): 2205–6. http://dx.doi.org/10.1103/physreva.49.2205.

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14

González-Ureña, A., i R. Vetter. "Reactive collisions with excited-state atoms". J. Chem. Soc., Faraday Trans. 91, nr 3 (1995): 389–98. http://dx.doi.org/10.1039/ft9959100389.

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15

Sheludko, David V., Simon C. Bell, Edgar J. D. Vredenbregt i Robert E. Scholten. "Excited-state imaging of cold atoms". Journal of Physics: Conference Series 80 (1.09.2007): 012040. http://dx.doi.org/10.1088/1742-6596/80/1/012040.

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16

Peterson, I. "Exploring Gravity, Tides, and Excited Atoms". Science News 144, nr 2 (10.07.1993): 21. http://dx.doi.org/10.2307/3977516.

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17

Williams, Jim, i Dehong Yu. "Angular Momentum Effects in Excited Atoms". Journal of the Chinese Chemical Society 48, nr 3 (czerwiec 2001): 371–80. http://dx.doi.org/10.1002/jccs.200100056.

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18

Chéret, M., i L. Barbier. "COLLISIONAL IONISATION OF EXCITED RUBIDIUM ATOMS". Le Journal de Physique Colloques 46, nr C1 (styczeń 1985): C1–193—C1–197. http://dx.doi.org/10.1051/jphyscol:1985119.

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19

Grujić, P. V. "Multiply-excited atoms and line broadening". Journal of Applied Spectroscopy 63, nr 5 (wrzesień 1996): 704–8. http://dx.doi.org/10.1007/bf02606863.

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20

Dohrmann, Th, i B. Sonntag. "VUV-photoionization of laser-excited atoms". Journal of Electron Spectroscopy and Related Phenomena 79 (maj 1996): 263–68. http://dx.doi.org/10.1016/0368-2048(96)02850-2.

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21

Cherepkov, N. A., L. V. Chernysheva, V. V. Kuznetsov i S. K. Semenov. "Photoionization of polarized excited Li atoms". Journal of Electron Spectroscopy and Related Phenomena 79 (maj 1996): 275–78. http://dx.doi.org/10.1016/0368-2048(96)02852-6.

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22

Samson, James A. R., Y. Chung i E. M. Lee. "Autoionization of doubly excited Ne atoms into excited ionic states". Physical Review A 45, nr 1 (1.01.1992): 259–66. http://dx.doi.org/10.1103/physreva.45.259.

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23

Desfrancois, C., J. P. Astruc, R. Barbe, A. Lagreze i J. P. Schermann. "Electron Transfer Collisions of Excited Sodium Atoms and Oxygen Molecules". Laser Chemistry 6, nr 1 (1.01.1986): 1–14. http://dx.doi.org/10.1155/lc.6.1.

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The vibronic network model is here considered for excited sodium atoms and oxygen molecules collisions. Electronic to vibration transfer and reaction cross sections are computed with a single adjustable parameter : the ionic covalent matrix element. The comparison between the atom-molecule and the quasi-free electron models is presented.

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24

Yu, Hoon, Seung Jin Kim i Jung Bog Kim. "Optimal control for generating excited state expansion in ring potential". Open Physics 18, nr 1 (28.07.2020): 374–79. http://dx.doi.org/10.1515/phys-2020-0171.

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AbstractWe applied an optimal control algorithm to an ultra-cold atomic system for constructing an atomic Sagnac interferometer in a ring trap. We constructed a ring potential on an atom chip by using an RF-dressed potential. A field gradient along the radial direction in a ring trap known as the dimple-ring trap is generated by using an additional RF field. The position of the dimple is moved by changing the phase of the RF field [1]. For Sagnac interferometers, we suggest transferring Bose–Einstein condensates to a dimple-ring trap and shaking the dimple potential to excite atoms to the vibrational-excited state of the dimple-ring potential. The optimal control theory is used to find a way to shake the dimple-ring trap for an excitation. After excitation, atoms are released from the dimple-ring trap to a ring trap by adiabatically turning off the additional RF field, and this constructs a Sagnac interferometer when opposite momentum components are overlapped. We also describe the simulation to construct the interferometer.

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25

Ljepojevic, N. N., i A. A. Mihajlov. "Ionisation of atoms by collision with excited atoms at low energies". Journal of Physics B: Atomic, Molecular and Optical Physics 23, nr 9 (14.05.1990): L129—L132. http://dx.doi.org/10.1088/0953-4075/23/9/002.

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26

Karov, M., I. Rusinov i A. Blagoev. "Chemi-ionization of ground-state Hg atoms by excited Ar atoms". Journal of Physics B: Atomic, Molecular and Optical Physics 30, nr 5 (14.03.1997): 1361–68. http://dx.doi.org/10.1088/0953-4075/30/5/026.

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27

HAN, FENG, i YUN-JIE XIA. "PAIRWISE ENTANGLEMENT DYNAMICS OF A MULTIPARTITE SYSTEM IN THE TAVIS–CUMMINGS MODEL". International Journal of Quantum Information 07, nr 07 (październik 2009): 1337–48. http://dx.doi.org/10.1142/s0219749909005821.

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The pairwise entanglement dynamics in a multipartite system consisting of three two-level atoms A, B, C and a single-mode cavity field a is studied via negativity. Three atoms are arranged in such a way that atoms BC are embedded in and locally interact with the cavity while atom A is located in a spatially separate place outside of the cavity. Initially, atom-pair AB is prepared in a Bell-like state while atom C in a superposition of ground and excited state, |gC〉 and |eC〉. It shall be shown that all the pairwise negativities of the total system including atoms and cavity undergo qualitatively different evolutions. The so-called entanglement sudden death is observed for atom-pair AB under certain conditions and the entanglement transfer among all the possible degrees of freedom of the whole system is also discussed.

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28

Bashkirov, E. K. "ENTANGLEMENT OF ATOMS SUCCESIVELY PASSING A CAVITY TAKING INTO ACCOUNT THE STARK SHIFT". Vestnik of Samara University. Natural Science Series 20, nr 7 (30.05.2017): 115–24. http://dx.doi.org/10.18287/2541-7525-2014-20-7-115-124.

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In the article we consider the influence of dynamical Stark shift on entanglement degree of two atoms with degenerate two-photon transitions successively passing an ideal one-mode cavity. We suppose that the field be prepared in vacuum state and the atoms be prepared in coherent superposition of excited and ground states. Thus it was also supposed that atoms fly by the cavity for identical time. On the basis of exact expression of evolution operator we carried out atom-atom entanglement for different values of two-atom coherence parameters and different values of cavity flight time. It is shown that Stark shift of energy levels can be used for effective control on a degree of atomic entanglement.

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29

Afanas'ev, V. P., B. M. Smirnov i D. A. Zhilyaev. "EXCITED ATOMS IN ARGON GAS DISCHARGE PLASMA". Журнал Экспериментальной и Теоретической Физики 146, nr 1 (2014): 160–68. http://dx.doi.org/10.7868/s0044451014070177.

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30

Zhao Jian-Dong i Xin Jie. "Coherence effect of high excited state atoms". Acta Physica Sinica 61, nr 19 (2012): 193302. http://dx.doi.org/10.7498/aps.61.193302.

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31

SHEN YI-FAN i LI WAN-XING. "COLLISIONAL ENERGY POOLING BETWEEN EXCITED SODIUM ATOMS". Acta Physica Sinica 45, nr 1 (1996): 29. http://dx.doi.org/10.7498/aps.45.29.

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32

Trajmar, S., I. Kanik, M. A. Khakoo, L. R. LeClair, I. Bray, D. Fursa i G. Csanak. "Elastic electron scattering by laser-excited atoms". Journal of Physics B: Atomic, Molecular and Optical Physics 31, nr 8 (28.04.1998): L393—L400. http://dx.doi.org/10.1088/0953-4075/31/8/010.

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33

Japha, Y., G. Kurizki i V. M. Akulin. "Localized decay of excited atoms in cavities". Optics Express 1, nr 6 (15.09.1997): 134. http://dx.doi.org/10.1364/oe.1.000134.

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34

Craig, B. I., J. P. Baxter, J. Singh, G. A. Schick, P. H. Kobrin, B. J. Garrison i N. Winograd. "Deexcitation Model for Sputtered Excited Neutral Atoms". Physical Review Letters 57, nr 11 (15.09.1986): 1351–54. http://dx.doi.org/10.1103/physrevlett.57.1351.

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35

Hart, Hugo W. van der, i Liang Feng. "Double photoionization of excited He-like atoms". Journal of Physics B: Atomic, Molecular and Optical Physics 34, nr 18 (12.09.2001): L601—L609. http://dx.doi.org/10.1088/0953-4075/34/18/103.

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36

Andreev, E. A., P. V. Kashtanov i B. M. Smirnov. "Resonant charge exchange involving highly excited atoms". Journal of Experimental and Theoretical Physics 102, nr 6 (czerwiec 2006): 871–81. http://dx.doi.org/10.1134/s106377610606001x.

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37

MEYER, M., T. PRESCHER, E. v. RAVEN, M. RICHTER, B. SONNTAG, B. R. MÜLLER, W. FIEDLER i P. ZIMMERMANN. "PHOTOELECTRON SPECTROSCOPY OF LASER EXCITED Ca ATOMS". Le Journal de Physique Colloques 48, nr C9 (grudzień 1987): C9–547—C9–550. http://dx.doi.org/10.1051/jphyscol:1987991.

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38

Cheron, B., i S. Mosaddak. "Collisions between excited potassium and rubidium atoms". Journal of Physics B: Atomic and Molecular Physics 18, nr 15 (14.08.1985): 3197–202. http://dx.doi.org/10.1088/0022-3700/18/15/025.

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39

Werij, H. G. C., M. Harris, J. Cooper, A. Gallagher i J. F. Kelly. "Collisional energy transfer between excited Sr atoms". Physical Review A 43, nr 5 (1.03.1991): 2237–49. http://dx.doi.org/10.1103/physreva.43.2237.

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40

Бандурина, Л. О., i С. В. Гедеон. "Inelastic electron scattering from excited barium atoms". Scientific Herald of Uzhhorod University.Series Physics 43 (30.06.2018): 108–16. http://dx.doi.org/10.24144/2415-8038.2018.43.108-116.

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41

Afanas’ev, V. P., B. M. Smirnov i D. A. Zhilyaev. "Excited atoms in argon gas discharge plasma". Journal of Experimental and Theoretical Physics 119, nr 1 (lipiec 2014): 138–45. http://dx.doi.org/10.1134/s1063776114060089.

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42

Gavrilyuk, A. P., i N. Ya Shaparev. "Resonant laser discharge involving excited nitrogen atoms". Quantum Electronics 23, nr 9 (30.09.1993): 745–47. http://dx.doi.org/10.1070/qe1993v023n09abeh003161.

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43

Bartschat, K. "Electron scattering from laser-excited chromium atoms". Journal of Physics B: Atomic, Molecular and Optical Physics 28, nr 5 (14.03.1995): 879–84. http://dx.doi.org/10.1088/0953-4075/28/5/019.

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44

Barnett, Stephen M., Bruno Huttner, Rodney Loudon i Reza Matloob. "Decay of excited atoms in absorbing dielectrics". Journal of Physics B: Atomic, Molecular and Optical Physics 29, nr 16 (28.08.1996): 3763–81. http://dx.doi.org/10.1088/0953-4075/29/16/019.

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45

Jacka, M., M. D. Hoogerland, W. Lu, D. Milic, K. G. H. Baldwin, K. Bartschat i S. J. Buckman. "Electron scattering from laser-excited He atoms". Journal of Physics B: Atomic, Molecular and Optical Physics 29, nr 23 (14.12.1996): L825—L830. http://dx.doi.org/10.1088/0953-4075/29/23/003.

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46

Zetner, P. W., S. Trajmar, S. Wang, I. Kanik, G. Csanak, R. E. H. Clark, J. Abdallah i J. C. Nickel. "Inelastic electron scattering by laser-excited atoms". Journal of Physics B: Atomic, Molecular and Optical Physics 30, nr 22 (28.11.1997): 5317–39. http://dx.doi.org/10.1088/0953-4075/30/22/026.

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47

Bl�mel, R., i U. Smilansky. "Microwave ionization of highly excited hydrogen atoms". Zeitschrift f�r Physik D Atoms, Molecules and Clusters 6, nr 2 (czerwiec 1987): 83–105. http://dx.doi.org/10.1007/bf01384595.

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48

Nordlander, P., i J. C. Tully. "Lifetimes of excited atoms near metal surfaces". Surface Science 211-212 (kwiecień 1989): 207–17. http://dx.doi.org/10.1016/0039-6028(89)90772-3.

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49

Nordlander, P., i J. C. Tully. "Lifetimes of excited atoms near metal surfaces". Surface Science Letters 211-212 (kwiecień 1989): A113. http://dx.doi.org/10.1016/0167-2584(89)90320-4.

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Azizi, M., C. W�lker, W. Hink i W. Sandner. "Electron impact on laser excited barium atoms". Zeitschrift f�r Physik D Atoms, Molecules and Clusters 30, nr 2-3 (czerwiec 1994): 161–67. http://dx.doi.org/10.1007/bf01426066.

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