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Author: Grafiati

Published: 14 March 2023

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1

Jacques, Claude. "Les inscriptions du Phnom Kbal Spãn (K 1011, 1012, 1015 et 1016)." Bulletin de l'Ecole française d'Extrême-Orient 86, no. 1 (1999): 357–74. http://dx.doi.org/10.3406/befeo.1999.3417.

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2

Leszka, Mirosław Jerzy. "Gabriel Radomir (1014–1015) i Jan Władysław (1015–1018), władcy państwa bułgarskiego w źródłach bizantyńskich." Balcanica Posnaniensia Acta et studia 25 (February 15, 2019): 43–51. http://dx.doi.org/10.14746/bp.2018.25.2.

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Artykuł poświęcony jest wizerunkowi carów bułgarskich: Gabriela Radomira i Jana Władysława, którzy przez ponad trzy lata po śmierci cara Samuela stawiali opór cesarzowi Bazylemu II. Według autora nie wzbudzili on specjalnego zainteresowania bizantyńskich historiografów. Z jednej strony wynikało to z krótkotrwałości ich rządów, z drugiej zaś, być może, z przekonania, że losy zmagań cesarstwa z Bułgarią Komitopulów rozstrzygnęły się już wcześniej – w krwawych bojach z Samuelem, który dla Bizantyńczyków był z pewnością postacią zdecydowanie większego formatu niż jego następcy.

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3

Li, Hong C., Emily Y. Li, Lisa Neumeier, Laura Conforti, and Manoocher Soleimani. "Identification of a novel signal in the cytoplasmic tail of the Na+:HCO3− cotransporter NBC1 that mediates basolateral targeting." American Journal of Physiology-Renal Physiology 292, no. 4 (April 2007): F1245—F1255. http://dx.doi.org/10.1152/ajprenal.00410.2006.

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The Na+:HCO3− cotransporter NBC1 (SLC4A4, variant A, kidney specific) is located exclusively on the basolateral membrane of epithelial cells, implying that this molecule has acquired specific signals for targeting to the basolateral membrane. A motif with the sequence QQPFLS (positions 1010–1015) in the cytoplasmic tail of NBC1 was recently demonstrated to mediate targeting of NBC1 to the basolateral membrane. Here, we demonstrate that mutating the amino acid F (phenylalanine) or L (leucine) at positions 1013 or 1014 to alanine, respectively, resulted in the retargeting of NBC1 to the apical membrane. Furthermore, mutation of the FL motif to FF showed similar properties as the wild-type; however, mutation of the FL motif to LL showed significant intracellular retention of NBC1. Mutating the amino acids Q-Q-P and S (positions 1010-1011-1012 and 1015) to A-A-A and A, respectively, did not affect the membrane targeting of NBC1. Functional studies in oocytes with microelectrode demonstrated that the apically targeted mutants, as well as basolaterally targeted mutants, are all functional. We propose that the FL motif in the COOH-terminal tail of NBC1 is essential for the targeting of NBC1 to the basolateral membrane but is distinct from the membrane-targeting di-leucine motif identified in other membrane proteins.

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4

Campos‐Enriquez, J. O., H. F. Morales‐Rodrguez, F. Domnguez‐Mendez, and F. S. Birch. "Gauss’s theorem, mass deficiency at Chicxulub crater (Yucatan, Mexico), and the extinction of the dinosaurs." GEOPHYSICS 63, no. 5 (September 1998): 1585–94. http://dx.doi.org/10.1190/1.1444455.

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Using Gauss’s theorem, we estimated the mass deficiencies of the Chicxulub impact structure (Yucatan, Mexico) from its gravity anomaly. The mass deficiency obtained from the residual gravity anomaly map ranges between 1.06 × 1016 and 1.67 × 1016 kg. Because the gravity anomaly has approximately radial symmetry, we also estimated the mass deficiency from selected profiles. In this way, we obtained slightly lower mass deficiency (6.16 × 1015 to 1.35 × 1016 kg). The central gravity high, which is supposed to be associated with the central structural high, has a mean excess mass of 1.93 × 1014 kg. By assuming a mean density contrast of 100 kg/m3 between the country rock and the sedimentary and brecciated rocks, we estimated the equivalent total mass (1.60 × 1017 to 4.34 × 1017 kg) and volume (6.16 × 1013 to 1.67 × 1014 m3) of breccias and sedimentary rocks responsible for the gravity anomaly. These figures represent lower bounds on the mass and volume ejected from the impact crater. They represent estimates made from geophysical principles and data, and compare well with independent estimates based on other principles such as scaling relations. According to actual estimations of the sulfur dioxide mass generated by the Cretaceous‐Tertiary impact and our results, only a small fraction (about 1%) of the anhydrite in the target strata was vaporized.

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5

Амонов, М. З., Э. М. Ибрагимова, В. Н. Сандалов, М. М. Зиядуллаев, and Ш. Г. Саттарова. "НАНОФАЗЫ И ТЕРМОСТИМУЛИРОВАННЫЙ ПРИПОВЕРХНОСТНЫЙ ТОК В КРИСТАЛЛАХ LiF:(Cu, Br, Rb), ОБЛУЧЕННЫХ ЭЛЕКТРОНАМИ." «Узбекский физический журнал» 22, no. 3 (January 6, 2020): 174–81. http://dx.doi.org/10.52304/.v22i3.156.

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Исследованы фазовый состав и приповерхностный ток при 90−580 К в отработанных сцинтилляторах из легированных кристаллов LiF после облучения флюенсами 4 МэВ электронов 1013−1015 эл/см2 при >300 К и плотности тока пучка 100−400 нА/см2 . Установлены разные критические температуры, выше которых преобладает проводимость разных ионов (F при 1013 см-2, 370 К, Li+ при 465 К, при 1014 см-2, 480 К, Li+ , Н+ и O− при 1015 см−2 и 450 К). Показано, что рассчитанные величины энергии активации уменьшаются с набором флюенса от 1013 до 1015 эл/см2 . В отработанном сцинтилляторе обнаружена сложная фаза твердого раствора 2LiF-3B2O3, которая после флюенса 1015 эл/см2 преобразовалась в LiBH4 и LiH нанофазы. Появление В и Н возможно в результате ядерных реакций в LiF под пучком 4 МэВ электронов, их вклад следует учитывать в ионной проводимости термолюминесцентных дозиметров и детекторов.

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6

Kozlovskiy, Artem L., Mahambet Alin, and Daryn B. Borgekov. "Study of Polymorphic Transformation Processes and Their Influence in Polycrystalline ZrO2 Ceramics upon Irradiation with Heavy Ions." Ceramics 6, no. 1 (March 10, 2023): 686–706. http://dx.doi.org/10.3390/ceramics6010042.

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The aim of this work was to study the mechanisms of polymorphic transformations in ZrO2 ceramics under irradiation with heavy ions, as well as to determine the nature of structural distortions in the case of t-ZrO2 → c-ZrO2 type transformations and associated anisotropic deformations. The samples of ZrO2 ceramics were irradiated with Kr15+ heavy ions with an energy of 150 MeV and fluences of 1011–1016 ion/cm2. During evaluation of the structural changes depending on the irradiation fluence, it was found that at low irradiation fluences (1011–1012 ion/cm2), the main role is played by deformation distortions of the crystal lattice, which have a pronounced anisotropic character. Meanwhile, at fluences above 1013 ion/cm2, the main role is played by polymorphic transformations of the t-ZrO2 → c-ZrO2 type, followed by amorphization of the damaged layer at fluences above 1015 ion/cm2. It was established that the anisotropic distortion of the crystal lattice is more pronounced along the crystallographic a axis, as well as the (011) texture orientation, which is characteristic of t-ZrO2. The polymorphic transformation processes of the t-ZrO2 → c-ZrO2 type occur at irradiation fluences of 1013–1014 ions/cm2, which are characterized by the formation of an overlap of local areas of defects that appear along the trajectory of ions in the material. The dependences of changes in the strength and thermophysical properties of ZrO2 ceramics on the irradiation fluence were obtained. The mechanisms of influence of the structural disorder and polymorphic transformations on the decrease in strength and crack resistance were established.

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7

Shakoory, Bita, Negin Mohtasham, Richard Amdur, Matthew Mullen, Steven Opal, and Winn Chatham. "1015." Critical Care Medicine 43 (December 2015): 255. http://dx.doi.org/10.1097/01.ccm.0000474846.86153.d4.

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8

Kambhampati, Swetha, Saraswati Kache, Julie Williamson, Tracey Roberts, Solomon Messing, and Jason Arimura. "1015." Critical Care Medicine 40 (December 2012): 1–328. http://dx.doi.org/10.1097/01.ccm.0000425228.85185.60.

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9

Miller, Benjamin F. "1015." Medicine & Science in Sports & Exercise 41 (May 2009): 149. http://dx.doi.org/10.1249/01.mss.0000354099.94914.1c.

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10

McKeag, Douglas B. "1015." Medicine & Science in Sports & Exercise 39, Supplement (May 2007): S114. http://dx.doi.org/10.1249/01.mss.0000273374.54822.8a.

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11

Kowalchuk, John M. "1015." Medicine & Science in Sports & Exercise 40, Supplement (May 2008): S115. http://dx.doi.org/10.1249/01.mss.0000321950.29872.70.

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12

Leedahl, David, Heather Personett, Rahul Kashyap, Ognjen Gajic, and Garrett Schramm. "1015." Critical Care Medicine 41 (December 2013): A255. http://dx.doi.org/10.1097/01.ccm.0000440252.69363.5c.

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13

Rampa, Sankeerth, Ashima Das, Veerasathpurush Allareddy, David Speicher, Veerajalandhar Allareddy, and Alexandre Rotta. "1015." Critical Care Medicine 42 (December 2014): A1604. http://dx.doi.org/10.1097/01.ccm.0000458512.13584.dd.

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14

Puckett, Yana, Ariel Santos, Robyn Richmond, Catherine Ronaghan, John Griswold, Michelle Estrada, and Virginia Tran. "1015." Critical Care Medicine 47 (January 2019): 486. http://dx.doi.org/10.1097/01.ccm.0000551763.44632.0a.

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15

Trudinger, B. "1015." Ultrasound in Medicine & Biology 32, no. 5 (May 2006): P6. http://dx.doi.org/10.1016/j.ultrasmedbio.2006.02.019.

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16

Tang, J. I., M. F. Back, R. Mukherjee, K. Lee, J. Lu, L. Wong, and T. Shakespeare. "1015." International Journal of Radiation Oncology*Biology*Physics 66, no. 3 (November 2006): S137. http://dx.doi.org/10.1016/j.ijrobp.2006.07.279.

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17

Bassett, David R. "1015." Medicine & Science in Sports & Exercise 38, Supplement (May 2006): S101. http://dx.doi.org/10.1249/00005768-200605001-01349.

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18

Zdorovets, Maxim V., Dmitriy I. Shlimas, Artem L. Kozlovskiy, and Daryn B. Borgekov. "Effect of Irradiation with Low-Energy He2+ Ions on Degradation of Structural, Strength and Heat-Conducting Properties of BeO Ceramics." Crystals 12, no. 1 (January 5, 2022): 69. http://dx.doi.org/10.3390/cryst12010069.

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The paper is devoted to the study of radiation-induced damage kinetics in beryllium oxide ceramics under irradiation with low-energy helium ions with fluences of 1015–1018 ion/cm2. It was revealed that at irradiation fluences above 1017 ion/cm2, a decrease in radiation-induced damage formation and accumulation rate is observed, which indicates the saturation effect. At the same time, the main mechanisms of structural changes caused by irradiation at these fluences are amorphization processes and dislocation density increase, while at fluences of 1015–1016 ion/cm2, the main mechanisms of structural changes are due to the reorientation of crystallites and a change in texture, with a small contribution of crystal lattice distorting factors. It was discovered that the radiation-induced damage accumulation as well as an implanted helium concentration increase leads to the surface layer destruction, which is expressed in the ceramic surface hardness and wear resistance deterioration. It was determined that with irradiation fluences of 1015–1016 ion/cm2, the decrease in thermal conductivity is minimal and is within the measurement error, while an increase in the irradiation fluence above 1017 ion/cm2 leads to an increase in heat losses by more than 10%.

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19

Жуков, И. "Вислая печать ростовского князя Бориса Владимировича (1010-1015 гг.)." Нумізматика і фалеристика, no. 3 (55) (2010): 10–11.

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20

He, C., and C. H. Becker. "Surface Analysis with 1014-1015 W cm2 Laser Intensities." Surface and Interface Analysis 24, no. 2 (February 1996): 79–85. http://dx.doi.org/10.1002/(sici)1096-9918(199602)24:2<79::aid-sia91>3.0.co;2-8.

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21

Guthe, Stefan, and Daniel Thuerck. "Algorithm 1015." ACM Transactions on Mathematical Software 47, no. 2 (April 2021): 1–27. http://dx.doi.org/10.1145/3442348.

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We present a new algorithm for solving the dense linear (sum) assignment problem and an efficient, parallel implementation that is based on the successive shortest path algorithm. More specifically, we introduce the well-known epsilon scaling approach used in the Auction algorithm to approximate the dual variables of the successive shortest path algorithm prior to solving the assignment problem to limit the complexity of the path search. This improves the runtime by several orders of magnitude for hard-to-solve real-world problems, making the runtime virtually independent of how hard the assignment is to find. In addition, our approach allows for using accelerators and/or external compute resources to calculate individual rows of the cost matrix. This enables us to solve problems that are larger than what has been reported in the past, including the ability to efficiently solve problems whose cost matrix exceeds the available systems memory. To our knowledge, this is the first implementation that is able to solve problems with more than one trillion arcs in less than 100 hours on a single machine.

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22

Mazur, P. "C-1015." Cryobiology 69, no. 3 (December 2014): 515. http://dx.doi.org/10.1016/j.cryobiol.2014.09.344.

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23

Zweifel, J. E., M. Christianson, A. S. Jaeger, N. Fost, D. Olive, and S. R. Lindheim. "P-1015." Fertility and Sterility 86, no. 3 (September 2006): S510—S511. http://dx.doi.org/10.1016/j.fertnstert.2006.07.1415.

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24

Patel, Shalaka, Amy Wayland-Smith, and Bryan Ray. "1015-LB." Human Immunology 74, no. 5 (May 2013): 492. http://dx.doi.org/10.1016/j.humimm.2012.11.048.

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25

Roovers, Dick, Jeroen Adema, Michelle Bacelar, Nienke Westerink, Maarten Penning, Wietse Mulder, Erik Rozemuller, and Doug Bost. "1015-LBP." Human Immunology 75, no. 6 (June 2014): 486. http://dx.doi.org/10.1016/j.humimm.2014.01.027.

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26

Li, Chuanying, Peibing Du, Kuan Li, Yu Liu, Hao Jiang, and Zhe Quan. "Accurate Goertzel Algorithm: Error Analysis, Validations and Applications." Mathematics 10, no. 11 (May 24, 2022): 1788. http://dx.doi.org/10.3390/math10111788.

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The Horner and Goertzel algorithms are frequently used in polynomial evaluation. Each of them can be less expensive than the other in special cases. In this paper, we present a new compensated algorithm to improve the accuracy of the Goertzel algorithm by using error-free transformations. We derive the forward round-off error bound for our algorithm, which implies that our algorithm yields a full precision accuracy for polynomials that are not too ill-conditioned. A dynamic error estimate in our algorithm is also presented by running round-off error analysis. Moreover, we show the cases in which our algorithms are less expensive than the compensated Horner algorithm for evaluating polynomials. Numerical experiments indicate that our algorithms run faster than the compensated Horner algorithm in those cases while producing the same accurate results, and our algorithm is absolutely stable when the condition number is smaller than 1016. An application is given to illustrate that our algorithm is more accurate than MATLAB’s fft function. The results show that the relative error of our algorithm is from 1015 to 1017, and that of the fft was from 1012 to 1015.

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27

Munshi, Parthapratim, and T. N. Guru Row. "Electron density study of 2H-chromene-2-thione." Acta Crystallographica Section B Structural Science 59, no. 1 (January 28, 2003): 159. http://dx.doi.org/10.1107/s0108768103001666.

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Owing to a printers' error in the paper by Munshi & Guru Row [ Acta Cryst. (2002), B58, 1011–1017], Figs. 4(a) and 4(b) on page 1015 were transposed. Revised PDF versions of these pages are available in the online version of this erratum, which is available through Crystallography Journals Online.

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28

Moscatelli, Francesco, Andrea Scorzoni, Antonella Poggi, Mara Passini, Giulio Pizzocchero, and Roberta Nipoti. "Effects of Very High Neutron Fluence Irradiation on p⁺n Junction 4H-SiC Diodes." Materials Science Forum 556-557 (September 2007): 917–20. http://dx.doi.org/10.4028/www.scientific.net/msf.556-557.917.

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In this work we analyzed the radiation hardness of SiC p+n diodes after very high 1 MeV neutron fluence. The diode structure is based on a p+ emitter ion implanted in n-type epilayer with thickness equal to 5 %m and donor doping ND = 3×1015 cm-3. Before irradiation, the average leakage current density at 100 V reverse bias was of the order of 3 nA/cm2. These devices were irradiated at four different fluence values, logarithmically distributed in the range 1014-1016 (1 MeV) neutrons/cm2. After irradiation the epilayer material became more resistive, as indicated by the reduction of the forward and reverse current density at a given voltage. In particular, after a neutron fluence of 1×1014 n/cm2 the epilayer active doping concentration decreased to 1.5×1015 cm-3. After irradiation at 1016 n/cm2, i.e. the highest fluence value, the average leakage current density at 100 V reverse bias decreased to values of the order of 0.1 nA/cm2. This very low noise even after very high fluence is very important to obtain a high signal to noise ratio even at room temperature.

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29

Привалов, В. Е., and В. Г. Шеманин. "Лидарное зондирование смеси молекул сероводорода и метана в атмосфере с летающей платформы." Журнал технической физики 127, no. 12 (2019): 1046. http://dx.doi.org/10.21883/os.2019.12.48707.153-19.

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The back scattering Raman lidar equation for the gas mixture of the hydrogen sulfide and the methane molecules numerical solution results are presented at the hydrogen sulfide and methane molecules remote sensing in the atmospheric boundary layer with the concentration in the range of 1010 cm-3 … 1016 cm-3 from the flying platform at the heights up to 500 m in the synchronous photon counting lidar mode. It has been shown that the studied hydrogen sulfide molecules concentration at the level of 1,4 1011 cm-3 can be registered during measurement time duration of 10 s and the methane molecules concentration of 7,6 1015 cm-3 - during measurement time of 1 ms for such a lidar variant at the 405 nm laser radiation wavelength and the platform flight altitude up to 500 m.

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30

NIEMELA, J. J., S. BABUIN, and K. R. SREENIVASAN. "Turbulent rotating convection at high Rayleigh and Taylor numbers." Journal of Fluid Mechanics 649 (April 13, 2010): 509–22. http://dx.doi.org/10.1017/s0022112009994101.

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We report heat transport measurements in a cylindrical convection apparatus rotating about the vertical axis. The aspect ratio was 1/2. The working fluid was cryogenic helium gas and the following parameter ranges applied: the Rayleigh number, Ra, varied in the range 1011 < Ra < 4.3 × 1015, the Taylor number, Ta, varied in the range 1011 < Ta < 3 × 1015, the convective Rossby number, Ro, varied in the range 0.4 < Ro < 1.6 and the Prandtl number, Pr, varied in the range 0.7 < Pr < 5.9. Boussinesq conditions applied quite closely. The heat transport for steady rotation, under all conditions of the present experiments, was smaller than that for the non-rotating case. When the rotation rate varied periodically in time, a sharp transition to a state of significantly enhanced heat transport was observed for modulation Taylor numbers Ta* ≳ 1014, where Ta* is based on the peak value of the modulation angular velocity.

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31

Fowe, Emmanuel Penka, and André Dieter Bandrauk. "Nonlinear time-dependent density functional theory studies of the ionization of CO2 by ultrashort intense laser pulses." Canadian Journal of Chemistry 87, no. 7 (July 2009): 1081–89. http://dx.doi.org/10.1139/v09-074.

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Time-dependent density functional theory (TDDFT) studies of the ionization of CO2 by intense laser pulses (3.50 × 1014, 1.40 × 1015, 2.99 × 1015, and 1.25 × 1016 W/cm2) at 800 nm (ω = 0.0584 au) are presented in the nonlinear nonpertubative regime. Special emphasis is placed on elucidating molecular orbital orientation and various peak-intensities effects on the ionization processes. The results reveal that molecular orbital ionizations are strongly sensitive to their symmetry and the laser intensities. Most notably, we found that with a proper choice of the laser intensity (3.5 × 1014 W/cm2), the sensitivity is strong enough such that the nature and symmetry of the highest occupied molecular orbital (HOMO) can be directly probed and visualized from the angular dependence of laser-induced ionization. At higher intensities, ionization is found to occur also from inner orbitals, thus complicating the imaging of simple orbitals. A time-dependent electron-localization function (TDELF) is used to get a visual insight on the time evolution process of the electron density.

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32

Shaulov, Sergey. "Exotic model of the cosmic ray spectrum." EPJ Web of Conferences 208 (2019): 02004. http://dx.doi.org/10.1051/epjconf/201920802004.

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A detailed study of the cores of extensive air showers (EAS) at mountain level (Tien-Shan 690 g/cm2) was carried out in the hybrid experiment HADRON. An analysis of the fine structure of the EAS spectrum in the energy region1015 - 1017 (knee) showed that there are two breaks in the spectrum. Along with the previously known break at an energy of 3 · 1015 eV, a change in the slope of the EAS spectrum is observed at an energy slightly below 1017 eV. In addition the use of a large X-ray emulsion chamber (XREC) as a detector of EAS cores allowed us to obtain several new results. An abnormal scaling violation in hadron spectra for Ne ~ 107 (E0 ~ 1016 eV) means the existence of a penetrating component of non-nuclear origin. The conclusion about the non-nuclear origin of the penetrating component in the primary radiation of CR is confirmed by the data about the excess of muons in the EAS containing hadrons of maximum energies. It is assumed that the mass composition of primary cosmic radiation varies sharply at energies of 1015 - 1016 eV, where quasi-nuclei (strangelets) appear instead of nuclei. A new model of the mass composition of cosmic rays in the region of ultrahigh energies is proposed on this basis .

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33

Shrestha, Neelu, Martyn H. Kibel, Patrick W. Leech, Anthony S. Holland, Geoffrey K. Reeves, Mark C. Ridgway, and Phillip Tanner. "Low Energy Ion Implantation and Annealing of Au/Ni/Ti Contacts to n-SiC." MRS Advances 2, no. 51 (2017): 2903–8. http://dx.doi.org/10.1557/adv.2017.314.

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ABSTRACTThe electrical characteristics of Au/Ni/Ti/ n-SiC contacts have been examined as a function of implant dose (1013-1014 ions/cm2) at 5 KeV and temperature of annealing (750-1000 °C). Measurements of specific contact resistance, ρc, were approximately constant at lower implant doses until increasing at 1 x 1015 ions/cm2 for both C and P ions. Annealing at a temperature of 1000 °C has reduced the value of ρc by an order of magnitude to ∼1 x 10-6 Ω.cm2 at implant doses of 1013-1014 ions/cm2. Auger Electron Spectroscopy (AES) has shown that annealing at 1000 °C resulted in a strong indiffusion of the metallization layers at the interface.

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34

Нікітенко, М. М. "Історична доля житія прп. Антонія Печерського крізь призму подій 1015 - 1019 рр." Лаврський альманах, Вип. 25 (2010): 18–30.

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35

Kalmykov, N. N., L. A. Kuzmichev, G. V. Kulikov, V. V. Prosin, V. P. Sulakov, and Yu A. Fomin. "Spectrum and composition of cosmic rays at energies of 1015–1018 eV." Moscow University Physics Bulletin 65, no. 4 (August 2010): 275–82. http://dx.doi.org/10.3103/s0027134910040065.

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36

Wang, Ke-Ming, Bo-Rong Shi, Pei-Jun Ding, Wei Wang, W. A. Lanford, Zhuang Zhuo, and Yao-Gang Liu. "Waveguide formation of KTiOPO4 by multienergy MeV He+ implantation." Journal of Materials Research 11, no. 6 (June 1996): 1333–35. http://dx.doi.org/10.1557/jmr.1996.0169.

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X-cut potassium titanyl phosphate (KTiOPO4 or KTP) was implanted by multienergy MeV He+ implantation with a total dose of 2 × 1016 ions/cm2 at liquid nitrogen temperature. The energy and dose used are as follows: 3.3 MeV and 2 × 1015 ions/cm2, 3.2 MeV and 4 × 1015 ions/cm2, 3.1 MeV and 4 × 1015 ions/cm2, and 3.0 MeV and 1.0 × 1016 ions/cm2 to reduce tunneling effect. The 22 dark modes were measured by the isosceles prism coupling method. The 15 bright modes were observed after 250 °C, 60 min annealing. The result shows that the waveguide formation of KTiOPO4 implanted by MeV He+ is not strongly dependent on the cut direction, which is different from the waveguide formation of KTiOPO4 by ion exchange process.

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37

Hind, Nicholas, Kit Strange, and Christabel King. "1015. INULA RHIZOCEPHALA: Compositae." Curtis's Botanical Magazine 39, no. 1 (January 21, 2022): 169–89. http://dx.doi.org/10.1111/curt.12437.

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38

. "1015 Jeugdzorg Wordt Volwassen." Zorg en Financiering 6, no. 8 (August 2007): 74–75. http://dx.doi.org/10.1007/bf03094307.

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39

GIUNTI, C., C. W. KIM, and U. W. LEE. "RUNNING COUPLING CONSTANTS AND GRAND UNIFICATION MODELS." Modern Physics Letters A 06, no. 19 (June 21, 1991): 1745–55. http://dx.doi.org/10.1142/s0217732391001883.

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The evolution of the gauge coupling constants in the SU (N) and SO (N) grand unification models is examined. It is shown that the three coupling constants αs, α2, α1 in the minimal SU(5) model do not merge into one at 99% confidence level when they are extrapolated from the values at the mass scale MZ, whereas in its supersymmetric version, the coupling constants do merge into one within one standard deviation. In the SU (N) (with N > 5) models with a two-step symmetry breaking the coupling constants can merge into one, but these models are ruled out by the constraint imposed on the unification mass scale from the absence of proton decay. The SO (N) models with N ≥ 10 are shown to be consistent with the proton decay constraint. In particular, the unification scale for the SO(10) model is shown to be 1015~1016 GeV and the intermediate energy scale is 1013~1014 GeV .

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40

Ashiev, A. R., М. V. Skulova, and K. N. Khabibullin. "Productivity and elements of its structure of the new pea lines." Grain Economy of Russia, no. 5 (November 9, 2018): 26–28. http://dx.doi.org/10.31367/2079-8725-2018-59-5-26-28.

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The studies were carried out in 2016–2018 in the competitive variety testing of peas on the crop rotation fields belonging to the laboratory of legume breeding and seed-growing of the FSBSI “Agricultural Research Center “Donskoy”, located in the part of the Rostov region with unstable humidity (Zernograd). During the years of research, the meteorological conditions of the pea vegetation were contrast that made it possible to objectively estimate the pea lines in the given weather and climate conditions. In the competitive variety testing, the 18 lines were studied according to economically valuable traits (seed productivity, productivity elements, adaptability to machine harvesting). As a result of the study, the 6 pea lines were identified: 2 lines of the mustache morphotype “G-1002”, “G-1003”; 4 leafy lines “G-1010”, “G-1011”, “G-1013” and “G-1015”. In the group of the mustache morphotype, 2 lines “G-1002” (on 0.30 t/ha), “G-1003” (on 0.39 t/ha) exceeded the grain productivity of the standard variety for 3 years of study on average. The productivity increase was from 12.4 to 16.1%. In the group of variety samples of the leafy morphotype, the line “G-1010” (on 0.31 t/ha) significantly exceeded grain productivity of the standard variety. All the selected lines were tolerant to their seed-shedding. The line “G-1010” (48.8 pc per plant) showed the highest seed yield per plant. The lines “G-1003” (222.1 g), “G-1011” (209.5 g) and “G-1013” (207.8 g) had the largest fineness of grain. The line “G-1010” (8.85 g/plant) demonstrated the highest productivity per plant. However, having a low coefficient of resistance to lodging (0.35), this line has the greatest loss of seeds during harvesting. The identified lines will be used in further breeding work according to a number of their economically valuable traits.

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41

Carlone, Cosmo, and Monia Buteau. "Studies of irradiated cadmium sulfide in a diamond anvil pressure cell." Canadian Journal of Physics 73, no. 5-6 (May 1, 1995): 324–29. http://dx.doi.org/10.1139/p95-045.

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Cadmium sulfide (CdS) was irradiated with 7 MeV electrons in the fluence range 1013–1017 cm−2. The samples were subsequently studied in a diamond anvil cell up to a pressure of 100 kbar (1 bar = 105 Pa). Samples irradiated up to 1015 cm−2 underwent the wurtzite (yellow) to rock-salt (black) change of phase at 27 ± 2 kbar. Samples irradiated at 1016, 3 × 1016, and 1017 cm−2 also underwent the wurtzite to rock-salt transformation at 27 ± 2 kbar, but at the critical pressure they changed to an orange form which colour persisted as the pressure was increased. As the pressure was decreased, the orange samples reverted to the rock-salt structure at 30 ± 2 kbar, and then to the orange form, which persisted to atmospheric pressure. Heating the recovered orange CdS to 500 ± 50 °C returned it to its wurtzite form. X-ray diffraction studies of the irradiated but not pressurized samples revealed two peaks that correspond to the distance between planes (d) of 1.40 and 1.26 Å (1 Å = 10−10 m). In the irradiated and pressurized samples, we observed peaks having d = 1.47, 1.40, 1.32, 1.27, 1.19, 1.16, 1.09, and 0.96 Å. We attribute the orange form of CdS to defects. Irradiation of CdS with 7 MeV electrons to a fluence of 1016 cm−2 tends to suppress the wurtzite to rock-salt change of phase.

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42

Shao, Jun Peng, Hui Tang, and Yan Qin Zhang. "Study on Computer Emulation of PTFE’s Wearability Improvement by Al³⁺ Ion Implantation." Materials Science Forum 575-578 (April 2008): 843–47. http://dx.doi.org/10.4028/www.scientific.net/msf.575-578.843.

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The surface material of Elastic-metal pads(EMP) is PTFE which has poor wearability . Ion implantation can improve the wearability of EMP surface .This paper investigated the wearability improvement of the EMP’s surface by Al2O3/PTFE film which generated by ion implantation. The accelerating voltage of the ion implantation apparatus is 40KV and the ion emitting energy of aluminum is 20KeV. The dosages of three kinds of Al3+ ion beams in the study are 1×1015 ions/cm2, 5×1015 ions/cm2 and 1×1016 ions/cm2 respectively. The aluminum ion’s density is 10uA/cm2. The vacuum pressure of the ion implantation is 3×10-3Pa. The experimental specimens modified by Al3+ ion implantation were tested by ESCA, XRD, AFM/FFM and nanometer probe , which got the chemical bond, phase structure and friction coefficient of the film. According to the experimental results, the mathematical model was built using the Fesow Geometric Model and the Halind Rang Theory. The computer simulation was made in which SRIM simulator program was employed. The ion implantation’s energy for the simulation is 20keV and the material density of PTFE is 2.56g/cm³. In addition, the dose is 5×1015 ions/cm², the time interval is 230 minutes and the velocity of Al3+ ion implantation is 2.15-2.20×1013 ions/minute. Finally the simulation curves of particle distribution, energy distribution and impairment etc. were plotted and discussed.

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Montoya, Aquiles. "¡Qué viva la democracia!" ECA: Estudios Centroamericanos 52, no. 588 (October 31, 1997): 1015–17. http://dx.doi.org/10.51378/eca.v52i588.6464.

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Cruz, José Miguel. "¿Nacidos para perder?" ECA: Estudios Centroamericanos 56, no. 636 (October 31, 2001): 1010–15. http://dx.doi.org/10.51378/eca.v56i636.5797.

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45

Marjunus, Roniyus, Yusril Al Fath, Yanti Yulianti, and Wahyu Widanarto. "Simulation of Pt80Au14Ti6 Work Function Change-Based Sensor of H2 Gas." Journal of Physical Science 33, no. 3 (November 30, 2022): 45–62. http://dx.doi.org/10.21315/jps2022.33.3.4.

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Chemical reactions simulation in detecting hydrogen gas (H2) on Pt80Au14Ti6 sensor surface based on work function change (Δɸ) has been conducted. The simulation result is compared with laboratory results of detecting H2 gas. Three chemical reactions contained three coverages, H coverage (θH), O coverage (θO), and H2O coverage (θH2O). The simulation was run using MATLAB. This research can find the reaction parameter values such as the Arrhenius coefficient of H2O forming reaction on Pt (υf3Pt), H2O forming reaction on Au (υf3Au), i.e., H2O dissociation on Au (υf3Au ), O2 desorption on Ti (υd2Ti), H2O forming reaction on Ti (υf3Ti), and H2O dissociation on Ti (υf3Ti), i.e., 7.5×1014 s–1, 9.85×1015 s–1, 3.25×1015 s–1, 7.11×1015 s–1, 3.425×1015 s–1 and 2.725×1015 s–1, respectively. The simulation results also have the same trend as the laboratory results. However, the contact potential difference (CPD) simulation result, i.e., –240 mV, is not the same as the laboratory result, (–297± 9) mV. In addition, this simulation also obtained approximation coverage for atoms/molecules on PT80Au14Ti6 surface, i.e., θH = 0.665154 Mono Layer (ML); θO = 1.5621× 10–6 ML; and θH2O = 5.41676 ×10–5 ML.

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46

Yan, Fei, A. Espenlaub, Robert P. Devaty, Takeshi Ohshima, and Wolfgang J. Choyke. "Using Intrinsic Defect Spectra in 4H SiC as Imbedded Thermometers in the Temperature Range from 100°C to 1500°C." Materials Science Forum 679-680 (March 2011): 237–40. http://dx.doi.org/10.4028/www.scientific.net/msf.679-680.237.

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Low doped epitaxial films of 4H SiC irradiated at 1 MeV and electron fluences of 1×1015 cm-2, 3×1015 cm-2 and 1×1016 cm-2 have been used to measure temperatures in two temperature intervals: 580°C to 640°C and 1220°C to 1320°C. Possible accuracy of the temperature measurements is judged to be better than 10 degrees Centigrade. Similar measurements should be possible from 100°C to 1500°C.

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47

Roinishvili, N. N. "Inelastic interaction at 1015-1016eV." Journal of Physics G: Nuclear and Particle Physics 21, no. 11 (November 1, 1995): 1407–36. http://dx.doi.org/10.1088/0954-3899/21/11/002.

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48

Bourland, Fred, and Don Jones. "Registration of Arkot 1005, Arkot 1015, and Arkot 1019 cotton germplasm lines." Journal of Plant Registrations, November 16, 2022. http://dx.doi.org/10.1002/plr2.20262.

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49

Ager, Joel W., Sung Han, Ron S. Wagner, Lawrence S. Pan, D. R. Kania, and Stephen M. Lane. "Characterization of Cvd Diamond Films by Optical Spectroscopies." MRS Proceedings 302 (1993). http://dx.doi.org/10.1557/proc-302-275.

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ABSTRACTRaman and photoluminescence spectroscopy was used to investigate radiation damage by 5 MeV He+ ions at room temperature in prototype CVD-diamond detector material. Amorphization of the diamond is not observed at fluences up to 8×1015 cm-2. A threshold behavior is seen in the formation of the H3 vacancy-dinitrogen color center. The defect is not observed for fluences in the range 1.6×1012 to 1.6×1013 cm-2; a linear behavior increase in H3 intensity is observed over the range 1.6×1014 to 1.6×1015 cm-2. The formation mechanism of the H3 color center under He+ irradiation involves a self-annealing effect that allows vacancies to diffuse to, and complex with, nitrogen complexes.

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Nadella, R. K., J. Vellanki, and M. V. Rao. "High-Energy Elevated Temperature Si and Room Temperature B Implants in InP." MRS Proceedings 240 (1991). http://dx.doi.org/10.1557/proc-240-829.

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ABSTRACTHigh-energy (3 MeV) Si implantations were performed in InP:Fe at an elevated temperature of 200 °C for fluences 8×1014, 2×1015, and 5×1015 cm“2. For the 8×1014 cm−2 fluence, an activation of 82 %, carrier mobility of 1200 cm2/V-s, a peak carrier concentration of 9×1018 cm−3, and lattice quality comparable to that of virgin crystal were obtained. No amorphization takes place for any of the fluences used. Boron compensation implantations were performed in InP:Sn (n sime 2×1018 cm3) at room temperature in the energy range 1 to 5 MeV and fluence range 1011 to 1015 cm−2. After heat treatment, maximum resistivity of the order of 106 Ω-cm was obtained in B implanted InP.

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