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1

YANG, Z. H., X. M. CHEN, Y. P. ZHANG, et al. "X-RAYS EMISSION OF HYDROGEN-LIKE AND HELIUM-LIKE ARGON IN INTERACTION WITH Mo METALLIC SURFACE." International Journal of Modern Physics B 19, no. 15n17 (2005): 2433–37. http://dx.doi.org/10.1142/s0217979205031109.

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14-GHz electron cyclotron resonance ion source (ECRIS) at the Heavy Ion Research Facility National Laboratory in Lanzhou has been used to investigate the radiative deexcitation of highly charged Ar 17+ and Ar 16+ ions as they interact with a molybdenum surface. The interaction of Ar 17+ and Ar 16+ ions above Mo Metallic Surface has been studied by looking at the X-rays with a Si ( Li ) detector. ECRIS is used in our work for the first time. As the experimental results, the X-ray spectra of Ar 17+ and Ar 16+ ions interacting with a Mo metal target have been given. The capture of many electrons
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2

Nikitović, Ž., V. Stojanović, and Z. Raspopović. "Rate Coefficients of Ar+ Ions in Ar/CF4 Mixtures." Acta Physica Polonica A 134, no. 6 (2018): 1134–36. http://dx.doi.org/10.12693/aphyspola.134.1134.

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3

Tawara, H., and P. Richard. "Ar K X-ray production in slow, highly charged Ar q+(q = 8–18) + Ar collisions." Canadian Journal of Physics 80, no. 12 (2002): 1579–89. http://dx.doi.org/10.1139/p02-077.

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In the present work, mechanisms of Ar K X-ray production have been investigated under low-energy Arq+ + Ar collisions in a wide range of the ion-charge states. Ar K X-rays have been observed as a function of the collision energy over (0.75–3.75)q keV/u and of the charge state over q = 8–16 of projectile Arq+ ions. If the L-shell vacancies become available (q = 9), Ar K X-ray yields are found to be enhanced roughly three orders of magnitude, compared with Ar8+ ions with no L-shell vacancy; to show some threshold; and to tend to quickly saturate at higher collision energies. The present analysis
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4

Kang, Chul, Gyuseok Lee, Woo-Jung Lee, et al. "Terahertz Emission and Ultrafast Carrier Dynamics of Ar-Ion Implanted Cu(In,Ga)Se2 Thin Films." Crystals 11, no. 4 (2021): 411. http://dx.doi.org/10.3390/cryst11040411.

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We investigated THz emission from Ar-ion-implanted Cu(In,Ga)Se2 (CIGS) films. THz radiation from the CIGS films increases as the density of implanted Ar ions increases. This is because Ar ions contribute to an increase in the surface surge current density. The effect of Ar-ion implantation on the carrier dynamics of CIGS films was also investigated using optical pump THz probe spectroscopy. The fitted results imply that implanted Ar ions increase the charge transition of intra-and carrier–carrier scattering lifetimes and decrease the bandgap transition lifetime.
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5

Nagata, Takashi. "Photodissociation Dynamics of Arn+ Cluster Ions." Laser Chemistry 14, no. 1-3 (1994): 15–29. http://dx.doi.org/10.1155/1994/98627.

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The time-of-flight (TOF) spectra of Ar+ and Ar fragments produced in the photodissociation of Arn+ (3 ≦ n ≧ 24) were measured at wavelength around 540 nm. The kinetic-energy and angular distributions of the neutral photofragments were obtained for n = 3, 9 and 24 by a simulation analysis of the measured TOF spectral profiles. The overall aspect of the photodissociation process of Arn+ is deduced from these distributions within the context of trimer ion core model; a linear Ar3+ core is solvated by neutral Ar atoms. For Arn+ with 4 ≦ n ≲ 14, direct dissociation of the Ar3+ chromophoric core giv
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6

Kaya, Yunus, Yalçin Kalkan, and Rob Veenhof. "Noble gas cluster ions." EPJ Web of Conferences 174 (2018): 06003. http://dx.doi.org/10.1051/epjconf/201817406003.

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In this work, a reaction mechanism of formation of noble gas (Ng) cluster ions has been theoretically investigated in detail. The kinetic studies of formation of Xe+Xe cluster in Xe, Ar+Ar cluster ions in Ar, and Ne+Ne cluster ions in Ne have been made as theoretically. The optimized structures in the ground state were calculated using the density functional theory (DFT) by the B3LYP method combined with the Stuttgart/Dresden effective core potential basis set (SDD). In addition, we calculated the rate constants of all cluster formations. The results are 1.15 × 10−31, 3.58 × 10−31, 0.23 × 10−3
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7

Nagata, Takashi, Jun Hirokawa, and Tamotsu Kondow. "Photodissociation of Ar+n cluster ions." Chemical Physics Letters 176, no. 6 (1991): 526–30. http://dx.doi.org/10.1016/0009-2614(91)90249-9.

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8

Zhao, Xin-Qian, Ying-Shuang Liang, and Yuan-Yuan Guo. "Investigation on charged particles in inductively coupled Ar/O2 plasmas: The role of Ar proportion." Physics of Plasmas 29, no. 11 (2022): 113511. http://dx.doi.org/10.1063/5.0098152.

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In this paper, a 2D fluid model is built to reveal the inductively coupled Ar/O2 plasma behavior at 300 W, 30 mTorr, in the gas mixture of 95% Ar −5% O2 and 10% Ar −90% O2. The reliability of the model is first verified by comparing the calculated results with the experimental data, and the consistent results are obtained. Then, the spatial distributions of the charged species densities are investigated. As Ar fraction decreases, the maximum densities of charged particles shift toward the coil significantly, and the O2+ becomes the dominant positive ion at higher O2 fractions. The main reactio
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9

Kim, Yong-Hyun, Jong-Sik Kim, Dae-Chul Kim, et al. "Ion and Radical Characteristics (Mass/Energy Distribution) of a Capacitively Coupled Plasma Source Using Plasma Process Gases (CxFy)." Coatings 11, no. 8 (2021): 993. http://dx.doi.org/10.3390/coatings11080993.

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We constructed a capacitively coupled plasma (CCP) source and installed various diagnostic tools to perform process diagnosis using a plasma process gas (CxFy). We obtained the energy and mass distributions of the ions and radicals from Ar, C4F8/Ar, and C4F6/Ar plasmas. The energy distribution of the ions incident on the substrate was controlled using the self-bias voltage, and the ion energy was found to be inversely proportional to the mass. The measured species and density of the ions and radicals can help understand plasma process results as they provide information about the ions and radi
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10

Nikitovic, Zeljka, and Zoran Raspopovic. "Cross sections set and transport coefficients for Ar+ ions in Ar gas." Science of Sintering, no. 00 (2025): 30. https://doi.org/10.2298/sos250428030n.

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In this work we present a complete cross sections dataset and transport coefficients of Ar+ ions in Ar gas. These data are needed for modeling in numerous applications of technological importance. A Monte Carlo simulation method is applied to accurately calculate transport parameters in hydrodynamic regime. We discuss new data for Ar+ ions in Ar gas where the drift velocity, characteristic energy, flux and bulk values of reduced mobility, rate coefficients, diffusion coefficients and other transport parameters are given as a function of low, moderate and high reduced electric fields E/N (E-ele
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11

Lagutin, B. M., Ph V. Demekhin, I. D. Petrov, et al. "Photoionization of Ar and Ar-like ions near the 3s-threshold." Journal of Physics B: Atomic, Molecular and Optical Physics 32, no. 8 (1999): 1795–807. http://dx.doi.org/10.1088/0953-4075/32/8/303.

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12

Vasylyev, M. A., S. I. Sidorenko, S. M. Voloshko, V. S. Filatova, and P. A. Gurin. "Antibacterial Treatment of the Titanium with Ar$^+$ Ions." METALLOFIZIKA I NOVEISHIE TEKHNOLOGII 42, no. 2 (2020): 215–36. http://dx.doi.org/10.15407/mfint.42.02.0215.

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13

Сычева, А. А. "Влияние кривизны поверхности на процессы физического распыления кремния ионами Ar низкой энергии". Журнал технической физики 46, № 23 (2020): 29. http://dx.doi.org/10.21883/pjtf.2020.23.50345.18423.

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In this paper molecular dynamics simulations of the irradiation of silicon nanoparticles with 200 eV Ar ions were performed. The detailed analysis of the results obtained demonstrates special features of the interaction between incident low-energy Ar ions and silicon targets with different surface curvature.
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14

Seong, Inho, Sijun Kim, Minsu Choi, et al. "Enhancement of Ar Ion Flux on the Substrate by Heterogeneous Charge Transfer Collision of Ar Atom with He Ion in an Inductively Coupled Ar/He Plasma." Materials 16, no. 17 (2023): 5746. http://dx.doi.org/10.3390/ma16175746.

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The understanding of ion dynamics in plasma applications has received significant attention. In this study, we examined these effects between He and Ar species, focusing on the Ar ion flux on the substrate. To control heterogeneous collisions, we varied the He addition rate at fixed chamber pressure and the chamber pressure at fixed Ar/He ratio in an inductively coupled Ar/He plasma source. Throughout the experiments, we maintained an electron density in the bulk plasma and plasma potential as a constant value by adjusting the RF power and applying an additional DC bias to eliminate any distur
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15

Chung, Sang-Young, Takashi Kagawa, Kengo Moribayashi, and Dong Eon Kim. "Auger transition rates for Ar-like ions." Atomic Data and Nuclear Data Tables 95, no. 2 (2009): 141–54. http://dx.doi.org/10.1016/j.adt.2008.10.002.

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16

Likonen, J., and M. Hautala. "Sputtering of Cu atoms by Ar ions." Applied Physics A: Solids and Surface 45, no. 2 (1988): 137–50. http://dx.doi.org/10.1007/bf02565201.

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17

Fujimura, Yushi, Kouki Iwahara, and Yushi Kato. "Enhanced Production of Multicharged Ions by Mixing Low Z Gas and Emittance Measurement on Electron Cyclotron Resonance Ion Source." Journal of Physics: Conference Series 2743, no. 1 (2024): 012072. http://dx.doi.org/10.1088/1742-6596/2743/1/012072.

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Abstract We have studied to enhance efficiency of producing multicharged ions in an electron cyclotron resonance ion source (ECRIS). The gas mixing method is known as an empirical method for highly efficient production of multicharged ions. This method is to mix low Z gas into the multicharged ions plasma. There are various explanations for the gas mixing effect. One of them is the ion cooling effect. It is necessary to obtain parameters related to the ion temperature in order to experimentally confirm the effect. We measured emittances for ion beams by using a wire probe and a multi-slit. He
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18

Tosi, Paolo, Raffaele Correale, Wenyun Lu, and Davide Bassi. "Production of ArN+ ions in the reactions Ar++N2 and N2++Ar." Journal of Chemical Physics 110, no. 9 (1999): 4276–79. http://dx.doi.org/10.1063/1.478311.

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19

ZHU, PINPIN, JIANSHENG LIU, and ZHIZHAN XU. "Theoretical investigation of high-energy ions produced from laser-cluster interactions." Laser and Particle Beams 21, no. 4 (2003): 593–97. http://dx.doi.org/10.1017/s026303460321418x.

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By using an effective dielectric constant to modify the nanoplasma model, the interactions of large Ar clusters with high-intensity femtosecond laser pulses have been studied. It is shown that the resonance absorption mechanism plays a predominant role in the production of highly energetic argon ions, and the calculated mean kinetic energy of Ar ions is in good agreement with our previous experimental results. The scaling of mean kinetic energy and charge states of Ar ions against cluster size and laser intensity has also been analyzed. The results indicate the existence of optimum cluster siz
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20

Воробьев, В. Л., П. В. Быков, В. Я. Баянкин та Ф. З. Гильмутдинов. "Формирование наноразмерных поверхностных слоев нержавеющей стали 03Х17Н12М2 имплантацией ионов N-=SUP=-+-=/SUP=-". Журнал технической физики 89, № 8 (2019): 1248. http://dx.doi.org/10.21883/jtf.2019.08.47899.2623.

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The accumulation of nitrogen to 14 at.% in the nanosized surface layers of samples of 03Х17Н12М2 stainless steel after implantation of N+ ions, the formation of metal nitrides, mainly CrN chromium nitride, and solid solution introduction has been established. It is shown that implantation of N+ ions using pretreatment by Ar+ and O+ ions leads to a decrease in the maximum nitrogen concentration by 2 or more times. It is assumed that this is due to segregation to the surface layers of iron atoms under irradiation by Ar+ ions and the formation of Cr2O3 chromium oxide and CrOOH chromium hydroxide
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21

Tsuda, K., W. Kubo, S. Harisaki, et al. "Low Z gas mixing effects of Ar and Xe multicharged ions in electron cyclotron resonance ion source." Journal of Physics: Conference Series 2244, no. 1 (2022): 012019. http://dx.doi.org/10.1088/1742-6596/2244/1/012019.

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Abstract An electron cyclotron resonance (ECR) ion source (ECRIS) has wide applications such as cancer therapy and material synthesis. We have constructed a single ECRIS capable of producing various ions with low to high mass/charge ratio, and have been conducting various experiments. We focus on the efficient production of multicharged ions and aim to increase the yield of multicharged ions by new effects of electromagnetic waves in ECRIS. We investigated the possibility of selective heating to low Z ions under low Z gas mixing. Therefore, as a preliminary step of these experiments, the low Z
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22

Tsuda, K., W. Kubo, S. Harisaki, et al. "Low Z gas mixing effects of Ar and Xe multicharged ions in electron cyclotron resonance ion source." Journal of Physics: Conference Series 2244, no. 1 (2022): 012019. http://dx.doi.org/10.1088/1742-6596/2244/1/012019.

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Abstract An electron cyclotron resonance (ECR) ion source (ECRIS) has wide applications such as cancer therapy and material synthesis. We have constructed a single ECRIS capable of producing various ions with low to high mass/charge ratio, and have been conducting various experiments. We focus on the efficient production of multicharged ions and aim to increase the yield of multicharged ions by new effects of electromagnetic waves in ECRIS. We investigated the possibility of selective heating to low Z ions under low Z gas mixing. Therefore, as a preliminary step of these experiments, the low Z
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23

Gard, Faramarz Sahra, та Elena Forlerer. "The effect of low-energy Ar+ irradiation on the surface of monocrystalline α-Al2O3 (0001)". European Physical Journal Applied Physics 85, № 2 (2019): 21302. http://dx.doi.org/10.1051/epjap/2019180241.

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Single crystals α-Al2O3 (0001) were exposed to the energetic Ar+-ions for two periods of 4 min with kinetic energy of 2 keV and 4 min of 5 keV at an incident angle of 45°. The samples were studied by X-ray photoemission spectroscopy (XPS) before and after Ar+-ion beam exposure. The average values of the bandgap energy before and after Ar+-ion beam treatment were measured to be (7.8 ± 0.2) eV and (6.3 ± 0.2) eV, respectively. The dynamic change in the XPS spectra of the valence band (VB) region before and after Ar+-ion beam treatment were explained using the theoretical calculation of the densi
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24

Insepov, Zeke, Ardak Ainabayev, Kumiszhan Dybyspayeva, et al. "Graphene, Graphene Oxide and Silicon Irradiation by Cluster Ions of Argon and Highly Charged Ions." MRS Advances 1, no. 20 (2016): 1417–22. http://dx.doi.org/10.1557/adv.2016.205.

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ABSTRACTDefect formation in the samples of graphene, graphene oxide and silicon irradiated with Ar cluster and highly-charged ion irradiations were studied. Ar cluster ions, with acceleration energy E = 30 kV (Exogenesis nAccel00, Boston, USA) and total Ar cluster ion fluences ranged from 1x109cm-2to 1x1013cm-2were directed toward various surfaces. Highly-charged ions (HCI) bombardment on surfaces with highly charged Xeq+(q= 22) was employed at Eurasian National University, Kazakhstan, using a DC-60 cyclotron accelerator. Multi-layer graphene oxide, single-layer graphene- (SLG), few-layer of g
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25

MEYER, M., A. MARQUETTE, A. GRUM-GRZHIMAILO, R. FLESCH, and E. RÜHL. "ALIGNMENT OF Ar+ IONS PRODUCED AFTER RESONANT AUGER DECAY OF Ar* 2p53d RESONANCES." Surface Review and Letters 09, no. 01 (2002): 141–46. http://dx.doi.org/10.1142/s0218625x02002063.

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Fluorescence spectra have been recorded in the wavelength region 300 nm ≤ λ(fluo) ≤ 500 nm after resonant 2p → 3d excitation of atomic Ar using monochromatic synchrotron light. The radiative emission is characterized by strong transitions from Ar + 3p 4 (1 S , 1 D , 3 P ) n ℓ ionic states. It is mainly assigned to processes of the type 3p 4 4d → 3p 4 4p and 3p 4 4p → 3p 4 4s . In addition, we have analyzed the degree of polarization of the fluorescence lines and we have determined the alignment of the Ar + ions, which are produced after the resonant Auger decay. In comparison to investigations
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26

Gushchina, N. V., K. V. Shalomov, V. V. Ovchinnikov, N. S. Bannikova, R. S. Zavornitsyn, and M. A. Milyaev. "A comparative study of the effect of ions of different atomic masses on the magnetoresistive properties of Co90Fe10/Cu superlattices." Journal of Physics: Conference Series 2144, no. 1 (2021): 012028. http://dx.doi.org/10.1088/1742-6596/2144/1/012028.

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Abstract The effect of inert gas ions with different atomic masses (Ar+, Xe+) on the magnetoresistance of Co90Fe10/Cu superlattices deposited on a silicon substrate has been investigated by comparison. The Ar+ ion irradiation has been found to decrease the magnetoresistance more significantly than Xe+ ion irradiation, which seems to be due to a larger average projective range for Ar+ (Rp = 5–6 nm) than that for Xe+ (Rp = 3.3–4.3 nm) and, accordingly, a greater depth of the atom mixing zone (∽(2–3)×Rp) when ions move from the top layers of the superlattice toward the substrate.
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27

Khromushin, Igor V., Taтiana I. Aksenova, Turgora Tuseyev, et al. "Modification of Barium Cerate by Heavy Ion Irradiation." Advanced Materials Research 781-784 (September 2013): 357–61. http://dx.doi.org/10.4028/www.scientific.net/amr.781-784.357.

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The effect of irradiation with heavy ions Ne, Ar, and Kr of various energies on the structure and properties of ceramic barium cerate doped with neodymium and annealed in air at 650°C for 7 hours is studied. It is noted that blistering was observed on cerate surface during its irradiation by low energy Ne ions, whereas it was not observed under low-energy Ar and Kr ions irradiation. Irradiation of the cerate with high energy ions caused partial amorphization of the irradiated surface of the material, while the structure of the non-irradiated surface did not change. In addition, the irradiated
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28

Koh, Seok-Keun, Won-Kook Choi, Jun-Sik Cho, Seok-Kyun Song, Young-Man Kim, and Hyung-Jin Jung. "Ar+ ion irradiation in oxygen environment for improving wettability of polymethylmethacrylate." Journal of Materials Research 11, no. 11 (1996): 2933–39. http://dx.doi.org/10.1557/jmr.1996.0371.

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Ion irradiation with various oxygen flow rates has been carried out to improve the wettability of polymethylmethacrylate (PMMA) to water and to enhance the adhesion between Al and the polymer. Ar+ ion and oxygen ion were irradiated on the polymer, and amounts of ions were changed from 5 × 1014 Ar+/cm2 to 5 × 1016 Ar+/cm2 by a broad ion beam source. Oxygen gas from 0 ml/min to 7 ml/min was flowed near the polymer surface during the ion irradiation, and the energy of ions was changed from 500 eV to 1500 eV. The wetting angle was reduced from 68° to 49° with the Ar+ ion irradiation only at 1 keV
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29

Hiraoka, Kenzo, and Toshiharu Mori. "Formation and stabilities of cluster ions Ar+n." Journal of Chemical Physics 90, no. 12 (1989): 7143–49. http://dx.doi.org/10.1063/1.456245.

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30

Scherbakov, I. P., and A. E. Chmel’. "Photoluminescence of Amorphous SiO2 with Implanted Ar+ Ions." Physics of the Solid State 61, no. 4 (2019): 592–95. http://dx.doi.org/10.1134/s1063783419040279.

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31

Lehnert, U., M. P. Stöckli, and C. L. Cocke. "X-ray emission for Ar ions impacting on." Journal of Physics B: Atomic, Molecular and Optical Physics 31, no. 23 (1998): 5117–22. http://dx.doi.org/10.1088/0953-4075/31/23/009.

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32

Covington, A. M., A. Aguilar, I. R. Covington та ін. "Valence-shell photoionization of Cℓ-like Ar+Ions". Journal of Physics: Conference Series 388, № 2 (2012): 022035. http://dx.doi.org/10.1088/1742-6596/388/2/022035.

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33

Albertoni, C. R., R. Kuhn, H. W. Sarkas, and A. W. Castleman. "Photodissociation of rare gas cluster ions: Ar+3." Journal of Chemical Physics 87, no. 8 (1987): 5043–44. http://dx.doi.org/10.1063/1.453709.

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34

Saied, Bashair Mohammed, and SaadNafea Yaqoob. "Interaction of (O,Ar)ions with Prostate tissue." Journal of Physics: Conference Series 1003 (May 2018): 012106. http://dx.doi.org/10.1088/1742-6596/1003/1/012106.

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35

Matsuo, Jiro, Noriaki Toyoda, Makoto Akizuki, and Isao Yamada. "Sputtering of elemental metals by Ar cluster ions." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 121, no. 1-4 (1997): 459–63. http://dx.doi.org/10.1016/s0168-583x(96)00541-1.

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36

Svorcík, V. "Amino acids grafting of Ar+ ions modified PE." Radiation Physics and Chemistry 60, no. 1-2 (2001): 89–93. http://dx.doi.org/10.1016/s0969-806x(00)00320-0.

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37

Nikolić, Dragan. "Photorecombination of Ar-like gallium and germanium ions." Journal of Quantitative Spectroscopy and Radiative Transfer 112, no. 1 (2011): 68–77. http://dx.doi.org/10.1016/j.jqsrt.2010.08.007.

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38

Nikitović, Ž., V. Stojanović, and Z. Raspopović. "Rate Coefficients of F-Ions in Ar/BF3Mixtures." Acta Physica Polonica A 127, no. 6 (2015): 1634–36. http://dx.doi.org/10.12693/aphyspola.127.1634.

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39

Duffy, Liam M., Thomas N. Feinberg, and Tomas Baer. "Infrared vibrational photodissociation spectra of Ar+2 ions." Journal of Chemical Physics 101, no. 4 (1994): 2793–99. http://dx.doi.org/10.1063/1.467594.

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40

Jin Yunfan, Xu Ronghui, Quan Jingming, et al. "1 GeV Ar ions induced amorphization in garnet." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 107, no. 1-4 (1996): 227–31. http://dx.doi.org/10.1016/0168-583x(95)00805-5.

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41

Gadea, F. X., and J. Durup. "Comment on “photodissociation of Ar+n cluster ions”." Chemical Physics Letters 181, no. 4 (1991): 378–79. http://dx.doi.org/10.1016/0009-2614(91)80088-f.

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42

Svorc�k, V., V. Rybka, V. Hnatowicz, et al. "Degradation of polyimide by implantation with Ar+ ions." Journal of Applied Polymer Science 64, no. 4 (1997): 723–28. http://dx.doi.org/10.1002/(sici)1097-4628(19970425)64:4<723::aid-app12>3.0.co;2-v.

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43

Xi, Yingxue, Jiwu Zhao, Jin Zhang, Changming Zhang, and Qi Wu. "The Influence of Ion Beam Bombardment on the Properties of High Laser-Induced Damage Threshold HfO2 Thin Films." Crystals 12, no. 1 (2022): 117. http://dx.doi.org/10.3390/cryst12010117.

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HfO2 thin films were deposited on BK-7 glass substrates using an electron beam evaporation deposition (EBD) technique and then post-treated with argon and oxygen ions at an ion energy ranging from 800 to 1200 eV. The optical properties, laser damage resistance, and surface morphology of the thin films exposed to Ar ions and O2 ions at various energies were studied. It was found that the two ion post-treatment methods after deposition were effective for improving the LIDT of HfO2 thin films, but the mechanism for the improvement differs. The dense thin films highly resistant to laser damage can
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44

Sun, S. X., Y. Z. Wu та H. Y. Mei. "Effect of H, He and Ar irradiation on β-Ga2O3 material". Digest Journal of Nanomaterials and Biostructures 18, № 2 (2023): 557–66. http://dx.doi.org/10.15251/djnb.2023.182.557.

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In this work, the projected range, the nuclear stopping power(Sn), electronic stopping power (Se), vacancies, replacement collisions, and total target damage of β-Ga2O3 by H, He and Ar ion bombardment are investigated by the Monte Carlo SRIM software. The ions were vertically incident on a 1-um β-Ga2O3 material, and their energies varied from 100 keV to 1 MeV. The results showed that the projected range increased for all three ions with increasing incident energies, with H ions having the largest projected range. The Sn for Se with incident energy of 0-1MeV in β-Ga2O3 is much greater than the
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45

BRANDELLI, ADRIANO, PATRICIA V. MIRANDA, and JORGE G. TEZÓN. "Voltage‐Dependent Calcium Channels and Gi Regulatory Protein Mediate the Human Sperm Acrosomal Exocytosis Induced by N‐Acetylglucosaminyl/Mannosyl Neoglycoproteins." Journal of Andrology 17, no. 5 (1996): 522–29. http://dx.doi.org/10.1002/j.1939-4640.1996.tb01829.x.

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ABSTRACT: Mammalian spermatozoa must undergo an exocytotic event during fertilization, the acrosome reaction (AR). In most species studied this process is induced by specific glycoproteins of the oocyte extracellular matrix, the zona pellucida (ZP), and it involves guanine nucleotide‐binding regulatory proteins (G‐proteins), resulting in an uptake of extracellular calcium by the sperm. In the bull, this event has been reported to be mediated by voltage‐dependent calcium channels (VDCC). Previous observations showed that neoglycoproteins (NGPs) with N‐acetylglucosamine or mannose (GlcNAc‐BSA or
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46

Sakaguchi, Isao, Tsubasa Nakagawa, Kenji Matsumoto, et al. "Redistributing Unintentional Defects Induced by Heavy Ion Implantation in ZnO Ceramics." Key Engineering Materials 421-422 (December 2009): 201–4. http://dx.doi.org/10.4028/www.scientific.net/kem.421-422.201.

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The relationship between the defect structure and luminescence property of ZnO ceramics implanted with Ar of 2×1015 – 60×1015 ions/cm2 was studied. After annealing, the heavy dose-implanted sample (Ar ≥ 30×1015 ions/cm2) was characterized by a luminescence peak at the 730-nm wavelength. Defects in the implanted region formed voids during post-annealing. Oxygen tracer experiments indicated that grain boundary diffusion in the implanted region was enhanced significantly.
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47

Han, Je Hwan, Sung Nam Park, Bok Kyun Shin, et al. "Extraction experiments at the UNIST electron beam ion trap for highly charged ion studies." Journal of Physics: Conference Series 2743, no. 1 (2024): 012050. http://dx.doi.org/10.1088/1742-6596/2743/1/012050.

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Abstract Highly charged ions (HCIs) are currently utilized in numerous fundamental and applied sciences, including astrophysics, dark matter search, optical clocks, semiconductor lithography, and quantum dot fabrication, to name just a few examples. At Ulsan National Institute of Science and Technology (UNIST), a tabletop electron beam ion trap (EBIT) has been developed for creating and studying HCIs. The UNIST-EBIT compresses the electron beam by 72 permanent magnets (up to 0.84 T) and produces up to He-like Ar ions. The primary objective of the UNIST-EBIT is to obtain X-ray spectrum data ess
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48

Kagami, Keiichi, Yoko Abe, Yukari Shinonaga, et al. "Antibacterial and Antifungal Activities of PMMAs Implanted Fluorine and/or Silver Ions by Plasma-Based Ion Implantation with Argon." Materials 13, no. 20 (2020): 4525. http://dx.doi.org/10.3390/ma13204525.

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The purpose of this study was to examine the anti-oral microorganism effects of fluorine and/or silver ions implanted into acrylic resin (PMMA) using plasma-based ion implantation (PBII) with argon gas. The experimental PMMA specimens were implanted with F and Ag ions alone or simultaneously by the PBII method using Ar or Ar/F2 gases and Ag mesh. The surface characteristics were evaluated by X-ray photoelectron spectroscopy (XPS), contact angle measurements, and atomic force microscopy (AFM). Moreover, the antibacterial activity against Streptococcus mutans (S. mutans) and the antifungal activ
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NEKAB, M., A. PAPE, and Ch HEITZ. "MATRIX EFFECT ON S X-RAY PRODUCTION BY PROTONS AND Ar IONS." International Journal of PIXE 05, no. 01 (1995): 11–20. http://dx.doi.org/10.1142/s0129083595000034.

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Thick targets of Li2B4O7 containing different concentrations of S have been irradiated with 0.8 to 3.0 MeV protons and 1.0 to 5.0 MeV Ar ions and the K X-ray yields of the S and one projectile (Ar) measured. The K X-ray production cross sections deduced from the measured yields, show a strong dependence on the S concentration in the case of the Ar bombardments. This effect is interpreted as being a consequence of the double-scattering mechanism occurring in the Ar-S collision system.
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50

Khromushin, I. V., T. I. Aksenova, T. Tuseev, K. K. Munasbayeva, and A. Bolatbekuly. "Paticularities of radiation defect formation in ceramic barium cerate." Bulletin of Shakarim University. Technical Sciences 1, no. 4(12) (2023): 167–75. http://dx.doi.org/10.53360/2788-7995-2023-4(12)-21.

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The results of the investigations are presented on the effect of irradiation with electrons, ions of inert gases (Ne, Ar, Kr) and oxygen on the structure and properties of Nd-doped barium cerate by the methods of X-ray diffraction analysis, scanning electron and atomic force microscopy, thermal desorption spectroscopy. It is shown that the low-energy irradiation with Ne and Ar ions stimulates the blistering processes on the surface, whereas the high energy ion irradiation by Ne, Ar, Kr ions the cerate surface undergoes the following stages of the spherulite growth - nucleation, growth (view of
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