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Artículos de revistas sobre el tema "H-111"

Autor: Grafiati

Publicado: 26 de julio de 2024

Última modificación: 31 de julio de 2025

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1

ALIPOOR, ZAHRA, ZOHREH GHOLAMZADEH, MAHDI SADEGHI, SOLALEH SEYYEDI, and MORTEZA AREF. "DATA EVALUATION ACQUIRED TALYS 1.0 CODE TO PRODUCE 111In FROM VARIOUS ACCELERATOR-BASED REACTIONS." International Journal of Modern Physics E 20, no. 05 (2011): 1307–24. http://dx.doi.org/10.1142/s0218301311018332.

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The Indium-111 physical-decay parameters as a β-emitter radionuclide show some potential for radiodiagnostic and radiotherapeutic purposes. Medical investigators have shown that 111 In is an important radionuclide for locating and imaging certain tumors, visualization of the lymphatic system and thousands of labeling reactions have been suggested. The TALYS 1.0 code was used here to calculate excitation functions of 112/114–118 Sn+p , 110 Cd +3 He , 109 Ag +3 He , 111–114 Cd+p , 110/111 Cd+d , 109 Ag +α to produce 111 In using low and medium energy accelerators. Calculations were performed up

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2

LU, HUNG-CHIEH, and LOU-SING KAN. "CADMIUM AND PROTON NMR STUDY ON [Cd2(BIS(2-PYRIDYL)FORMAMINE)3]." Biophysical Reviews and Letters 03, no. 04 (2008): 491–500. http://dx.doi.org/10.1142/s1793048008000861.

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The structure of a bi - Cd organic complex [ Cd 2(bis(2-pyridyl)formamine)3 or 1], is analyzed thoroughly by 1 H and 113/111 Cd NMR in solution. Only one representative set of pyridyl proton resonance of a total of six pyridines in 1 was observed. The resonance of protons in pyridine ring can be assigned by both 2D COSY and 2D NOESY. Similarly, only one Cd (either 113 Cd or 111 Cd NMR signal was observed too. This indicates that the two Cd atoms in 1 are chemically equivalent. The Cd signal is split by its three neighboring equivalent protons on the bridged carbon atoms ( C a H )3, resulting i

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3

Pan, Guyue, Yongsheng Zhang, Yonggang Li, Chuanguo Zhang, Zhe Zhao, and Zhi Zeng. "Orientation-dependent behaviors of H dissolution and diffusion near W surfaces: A first-principles study." International Journal of Modern Physics C 28, no. 07 (2017): 1750090. http://dx.doi.org/10.1142/s0129183117500905.

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The dissolution and diffusion behaviors of H in the four low-Miller-index W surfaces ((110), (112), (100) and (111)) are systematically studied by the density functional theory approach to understand the orientation dependence of the H bubble distribution on surface. The results show that H accumulation on surface is influenced by H diffusion barrier as well as vacancy and H formation. The barriers of diffusion towards surfaces are larger than that in bulk. It indicates that H is prone to diffuse into the deep in bulk once H dissolves in surface. H is preferred to accumulate on the W(111) surf

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4

Chorniy, R. "Guilt in compositions of crimes against bases of national safety of Ukraine: problem questions of theory and fixing in a law on criminal responsibility." Herald of criminal justice, no. 3 (2019): 136–50. http://dx.doi.org/10.17721/2413-5372.2019.3/136-150.

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The article is devoted to the investigation of forms and types of guilt in the composition of crimes against the basics of national security of Ukraine. The presence of a number of unresolved issues at the theoretical and legal level on this issue actualizes the need for its scientific elaboration and formulation of proposals to improve the provisions of the law on criminal liability. The purpose of the article is to investigate the problematic issues of forms and types of guilt in crimes against the bases of national security of Ukraine, ways of fixing them in the articles of Section I of the

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5

Melkozerova, J. A., and I. K. Gainullin. "Theoretical study of resonant charge exchange between H−ion and adsorbate-covered metal surface Cu(111)/Cu(110) with adsorbates Li+/Na+." Seriya 3: Fizika, Astronomiya, no. 4_2023 (September 20, 2023): 2340504–1. http://dx.doi.org/10.55959/msu0579-9392.78.2340504.

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The influence of the surface type on resonant charge exchange between H−ion with a metal surfaces Cu(111) and Cu(110) covered by adsorbate Li+/Na+has been studied. A model static problem was considered. For modeling, athree-dimensional realization of the wave-packet propagation method was used. The Cu(110) andCu(111) surfaces were described by a pseudopotential, derived from a density functional theory (DFT).An occupation of H− ion, an electron density dynamics and an ion level width were analyzed. As aresult, we obtained that an electron oscillates more in case of the surface Cu(111). Further

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6

Wang, Runnan, Qingyan Xu, Xiufang Gong, Xianglin Su, and Baicheng Liu. "Experimental and Numerical Studies on Recrystallization Behavior of Single-Crystal Ni-Base Superalloy." Materials 11, no. 7 (2018): 1242. http://dx.doi.org/10.3390/ma11071242.

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The recrystallization (RX) behavior of superalloy during standard solution heat treatment (SSHT) varies significantly with deformation temperature. Single-crystal (SX) samples of Ni-base superalloy were compressed to 5% plastic deformation at room temperature (RT) and 980 °C, and the deformed samples were then subjected to SSHT process which consists of 1290 °C/1 h, 1300 °C/2 h, and 1315 °C/4 h, air cooling. RT-deformed samples showed almost no RX grains until the annealing temperature was elevated to 1315 °C, while 980 °C-deformed samples showed a large number of RX grains in the initial stag

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7

OSHIMA, C., N. TANAKA, A. ITOH, E. ROKUTA, K. YAMASHITA, and T. SAKURAI. "A HETEROEPITAXIAL MULTI-ATOMIC-LAYER SYSTEM OF GRAPHENE AND h-BN." Surface Review and Letters 07, no. 05n06 (2000): 521–25. http://dx.doi.org/10.1142/s0218625x00000683.

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Multi-atomic-layer systems stacked with monolayer graphene/monolayer h-BN/Ni(111) have been grown in an epitaxial manner. The graphene overlayer formation changes drastically the interfacial interaction between the h-BN layer and Ni(111). As a result, a peculiar property of the monolayer h-BN on Ni(111) changes to a bulklike one. The π–d orbital hybridization at the interface disappears. Accordingly, a metallic character of monolayer h-BN disappears, the soft TO⊥ phonon returns to the bulk one, and the reduced lattice constant of h-BN on Ni(111) also returns to the bulk one. In contrast, the h

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8

Myerscough, Megan, Wes Chapple, William T. Meteer, and Daniel W. Shike. "22 Effects of Housing Cow-calf Pairs on Drylots vs Pasture on Calf Performance and Behavior Through Weaning." Journal of Animal Science 99, Supplement_1 (2021): 24. http://dx.doi.org/10.1093/jas/skab054.042.

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Abstract The objectives were to analyze the effects of housing cow-calf pairs in drylots or pasture on calf performance and behavior through weaning. Simmental × Angus (2 yr; 108/yr; 81 ± 15.3 d postpartum) spring-calving cows were stratified by age, BW, BCS, and calf sex and allotted to six groups/yr. Groups were randomly allotted to 1 of 2 treatments: drylot (DL) or pasture (PAST). Calves in the drylot had ad libitum access to a diet consisting of corn silage, dried distillers grain, corn stalks, dry rolled corn, and soybean hulls. Calves on PAST received creep feed three weeks prior to wean

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9

Editor, The. "Abstracts from current literature Vol 38(2)." Dhaka Shishu (Children) Hospital Journal 38, no. 2 (2023): 111–12. http://dx.doi.org/10.3329/dshj.v38i2.70597.

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10

Bauschlicher, Charles W., and Marzio Rosi. "Differentiating between H and F or H and CN on C(111) or Si(111) Surfaces." Journal of Physical Chemistry B 102, no. 13 (1998): 2403–5. http://dx.doi.org/10.1021/jp9734742.

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11

Greuter, F., I. Strathy, E. W. Plummer, and W. Eberhardt. "Photoemission from H adsorbed on Ni(111) and Pd(111) surfaces." Physical Review B 33, no. 2 (1986): 736–46. http://dx.doi.org/10.1103/physrevb.33.736.

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12

Hammer, L., H. Landskron, W. Nichtl-Pecher, A. Fricke, K. Heinz, and K. Müller. "Hydrogen-induced restructuring of close-packed metal surfaces: H/Ni(111) and H/Fe(110)." Physical Review B 47, no. 23 (1993): 15969–72. http://dx.doi.org/10.1103/physrevb.47.15969.

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13

Svensson, Ann-Marie, Marko Modiano, Angela Karstadt, et al. "Reviews and notices." Moderna Språk 94, no. 1 (2000): 101–19. http://dx.doi.org/10.58221/mosp.v94i1.9661.

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Includes the following reviews: p. 101. Ann-Marie Svensson. Lightfoot, D., The Development of Language, Acquisition, Change, and Evolution. p. 101-103. Marko Modiano. Ronowicz, E. & Yallop, C. (eds), English: One Language, Different Cultures. p. 103-105. Angela Karstadt. Klintborg, S., The Transience of American English. p. 105-106. Mats Mobärg. Pinker, S., Words and Rules. The Ingredients of Language. p. 106-107. Åke Persson. Cartmell, D. & Whelehan, I. (eds), Adaptations: From Text to Screen, Screen to Text. p. 108. Monica Armini. Rivkin, J. &

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14

Seth, Michael, and Peter Schwerdtfeger. "A comparison of relativistic and electron correlation effects for (111)F, (111)H and (111)Li." Chemical Physics Letters 318, no. 4-5 (2000): 314–18. http://dx.doi.org/10.1016/s0009-2614(00)00034-8.

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15

Liu, Na, Xue-Ye Wang, and Ya-Li Wan. "First principle calculations of hydrogen sulfide adsorption and dissociation on pure Pd (111) and Au (111), and alloy Pd/Au (111) and Au/Pd (111) surfaces." Journal of Theoretical and Computational Chemistry 13, no. 08 (2014): 1450065. http://dx.doi.org/10.1142/s0219633614500655.

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The hydrogen sulfide adsorption and dissociation on pure Pd (111) and Au (111), alloy Pd / Au (111) and Au / Pd (111) surfaces have been investigated using the pseudo-potential plane wave method within the generalized-gradient approximation density functional theory (GGA+DFT). The results show that H 2 S tends to be adsorbed on top site, HS prefers to locate on bridge site, and the S and H locate on fcc site on various surfaces. Compared the adsorption of sulfur-containing species and hydrogen on pure and alloy metal surfaces, a similar trend of adsorption energies on the metal surfaces ( Pd /

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16

NOBUHARA, Kunihiro, Hideaki KASAI, Hiroshi NAKANISHI, and Wilson Agerico DIÑO. "H/Pd(111) Absorption and Desorption Dynamics." SHINKU 46, no. 3 (2003): 177–80. http://dx.doi.org/10.3131/jvsj.46.177.

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17

Bodlaki, D., and E. Borguet. "Photoreactivity of Si(111)−H in Ambient." Journal of Physical Chemistry C 111, no. 1 (2007): 234–39. http://dx.doi.org/10.1021/jp0639546.

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18

KAWASAKI, TOYOSEI, TAKASHI ICHIMURA, HIROSHI KISHIMOTO, ADE ASNEIL AKBAR, TAKASHI OGAWA, and CHUHEI OSHIMA. "DOUBLE ATOMIC LAYERS OF GRAPHENE/MONOLAYER h-BN ON Ni(111) STUDIED BY SCANNING TUNNELING MICROSCOPY AND SCANNING TUNNELING SPECTROSCOPY." Surface Review and Letters 09, no. 03n04 (2002): 1459–64. http://dx.doi.org/10.1142/s0218625x02003883.

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Using STM, we have directly confirmed the incommensurate stacking of double atomic layers of graphene and monolayer h-BN on Ni(111). The formation of a graphene layer weakens the interfacial interaction between monolayer h-BN and Ni(111), resulting in insulating h-BN layers, while a pristine monolayer h-BN on Ni(111) is metallic. The STS spectra of the double atomic layers showed a tunneling character with a band gap of 0.5 eV.

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19

Bártol, I., C. Moskát, Z. Karcza, T. Kisbenedek, and H. . "Great Reed Warblers Bury Artificial Objects, Not Only Cuckoo Eggs." Acta Zoologica Academiae Scientiarum Hungaricae 49, no. 2 (2003): 111–14. https://doi.org/10.5281/zenodo.12587125.

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20

Keck, Zhen-Yong, Vicky M. H. Sung, Susan Perkins, et al. "Human Monoclonal Antibody to Hepatitis C Virus E1 Glycoprotein That Blocks Virus Attachment and Viral Infectivity." Journal of Virology 78, no. 13 (2004): 7257–63. http://dx.doi.org/10.1128/jvi.78.13.7257-7263.2004.

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ABSTRACT Human antibodies elicited in response to hepatitis C virus (HCV) infection are anticipated to react with the native conformation of the viral envelope structure. Isolation of these antibodies as human monoclonal antibodies that block virus binding and entry will be useful in providing potential therapeutic reagents and for vaccine development. H-111, an antibody to HCV envelope 1 protein (E1) that maps to the YEVRNVSGVYH sequence and is located near the N terminus of E1 and is able to immunoprecipitate E1E2 heterodimers, is described. Binding of H-111 to HCV E1 genotypes 1a, 1b, 2b, a

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21

Dokhlikova, Nadezhda V., Andrey K. Gatin, Sergey Y. Sarvadii, Dinara Tastaibek, Vladislav G. Slutskii, and Maxim V. Grishin. "Surface Structure Effects on H and O Adsorption on Gold, Nickel and Platinum Nanoparticles." Materials 18, no. 3 (2025): 631. https://doi.org/10.3390/ma18030631.

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Using quantum chemical modelling, in this work, we considered the structure effects determining the adsorption of H and O atoms on (111), (100), (110) and (211) surfaces of gold, nickel and platinum nanoparticles. Surface deformation enhanced the adatom bonding to active sites with a large coordination number on flat (111) and (100) surfaces, while no distinct tendency was observed on kinked (110) and (211) surfaces. The effect of the neighboring atoms depends on the coupling matrix element Vad2. For metals with a considerable matrix element, the adsorption energy decreases with the rise in co

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22

SHUTTLEWORTH, I. G. "THE SATURATED (3 × 3)-H/Cu(111) SYSTEM: A STRUCTURAL STUDY USING MEDIUM-ENERGY ION SCATTERING AND HELIUM ATOM SCATTERING." Surface Review and Letters 14, no. 06 (2007): 1191–98. http://dx.doi.org/10.1142/s0218625x07010792.

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The adsorption of atomic hydrogen on Cu (111) has been studied using the techniques of helium atom scattering (HAS) and medium-energy ion scattering (MEIS). Ion scattering investigations of the saturated (3 × 3)- H / Cu (111) system indicate that no reconstruction of the Cu substrate exists along the high symmetry directions of the surface. The HAS hydrogen cross-section for H / Cu (111) has been determined to be (12.5 ± 2.5 Å2). The symmetry of the HAS diffraction pattern shows that the (3 × 3)- H / Cu (111) system is formed of a single domain structure.

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23

Buchan, Alastair M., Stan Z. Gertler, Hui Li, et al. "A Selective N-Type Ca2+-Channel Blocker Prevents CA1 Injury 24 h following Severe Forebrain Ischemia and Reduces Infarction following Focal Ischemia." Journal of Cerebral Blood Flow & Metabolism 14, no. 6 (1994): 903–10. http://dx.doi.org/10.1038/jcbfm.1994.121.

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SNX-111 (NEUREX Corporation, Menlo Park, CA, U.S.A.) an ω-conopeptide, was tested for cytoprotection following normothermic ischemia using both a four-vessel occlusion model of severe forebrain ischemia and a model of transient middle cerebral artery occlusion focal ischemia. Adult male Wistar rats were subjected to 10 min of forebrain ischemia followed by 7 days of reperfusion. A single dose of SNX-111 (5 mg/kg) was injected intravenously following delays of either 6 or 24 h after reperfusion. For 11 rats treated with saline, there was 78 ± 13% CA1 neuronal injury (mean ± SD); for 11 given SN

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24

SHUTTLEWORTH, I. G., and W. ALLISON. "THE ADSORPTION AND DESORPTION PROCESSES ACCOMPANYING THE CHEMICAL VAPOUR DEPOSITION OF SILANE ON Cu(111) AND Ni(111)." Surface Review and Letters 08, no. 06 (2001): 613–20. http://dx.doi.org/10.1142/s0218625x01001567.

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The adsorption and desorption processes accompanying the deposition of silane on Cu(111) and Ni(111) have been investigated using work function change (Δϕ), Auger electron spectroscopy (AES) and thermal desorption spectroscopy (TDS). In the early stages of deposition (0–2 L), at 130 K, on the Cu(111) surface, a predominantly hydrogenic phase forms. Heating the saturated surface to Ts>400 K produces a two-phase system: Cu 2 Si alloy and clean Cu(111). The regenerated Cu(111) phase extends across (16 ± 1)% of the total surface area and this process of clean surface generation can be repeated

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25

Giordano, L., L. Di Piazza, M. I. Trioni, and F. Montalenti. "Theoretical evidence for fast H-divacancy rotation on H/Pd(111)." Chemical Physics Letters 400, no. 1-3 (2004): 163–68. http://dx.doi.org/10.1016/j.cplett.2004.10.085.

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26

Nobuhara, K., H. Nakanishi, H. Kasai, and A. Okiji. "Quantum mechanical behavior of an H atom on Cu(111) and Pt(111)." Journal of Applied Physics 91, no. 4 (2002): 1855–59. http://dx.doi.org/10.1063/1.1432480.

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27

Prod’homme, P., F. Maroun, R. Cortès, and P. Allongue. "Electrochemical growth of ultraflat Au(111) epitaxial buffer layers on H–Si(111)." Applied Physics Letters 93, no. 17 (2008): 171901. http://dx.doi.org/10.1063/1.3006064.

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28

Vasquez, Natividad, and R. J. Madix. "Reactivity of Unsaturated Linear C6Hydrocarbons on Pd(111) and H(D)/Pd(111)." Journal of Catalysis 178, no. 1 (1998): 234–52. http://dx.doi.org/10.1006/jcat.1998.2133.

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29

Wu, Ling-Nan, Zhen-Yu Tian, and Wu Qin. "A Density Functional Theory and Microkinetic Study of Acetylene Partial Oxidation on the Perfect and Defective Cu2O (111) Surface Models." Molecules 27, no. 19 (2022): 6748. http://dx.doi.org/10.3390/molecules27196748.

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The catalytic removal of C2H2 by Cu2O was studied by investigating the adsorption and partial oxidation mechanism of C2H2 on both perfect (stoichiometric) and CuCUS-defective Cu2O (111) surface models using density functional theory calculations. The chemisorption of C2H2 on perfect and defective surface models needs to overcome the energy barrier of 0.70 and 0.81 eV at 0 K. The direct decomposition of C2H2 on both surface models is energy demanding with the energy barrier of 1.92 and 1.62 eV for the perfect and defective surface models, respectively. The H-abstractions of the chemisorbed C2H2

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30

Gui, Qingzhong, Zhen Wang, Chunmin Cheng, et al. "Theoretical study of the interface engineering for H-diamond field effect transistors with h-BN gate dielectric and graphite gate." Applied Physics Letters 121, no. 21 (2022): 211601. http://dx.doi.org/10.1063/5.0117263.

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Diamond has compelling advantages in power devices as an ultrawide-bandgap semiconductor. Using first-principles calculations, we systematically investigate the structural and electronic properties of hydrogen-terminated diamond (H-diamond) (111) van der Waals (vdW) heterostructures with graphite and hexagonal boron nitride (h-BN) layers. The graphite/H-diamond heterostructure forms a p-type ohmic contact and the p-type Schottky barrier decreases as the number of graphite layers increases. In contrast, the h-BN/H-diamond heterostructure exhibits semiconducting properties and a tunable type-II

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31

马腾飞, 朱松林, 宋佳璐, 虞游 та 田晓峰. "第一性原理研究单个水分子在PuO<sub>2</sub>（111）和（110）表面吸附行为". Acta Physica Sinica 74, № 15 (2025): 0. https://doi.org/10.7498/aps.74.20250082.

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Plutonium dioxide, as one of the primary materials for nuclear fuel, serves as a critical component in fast neutron reactor fuel and mixed oxide (MOX) fuel due to its distinctive physical and chemical properties. This significantly enhances the utilization efficiency of uranium and diminishes the demand for natural uranium resources. Moreover, plutonium dioxide constitutes an essential component of spent nuclear fuel. However, during long-term storage, oxygen vacancies on its surface can facilitate hydrogen release under the influence of water molecules, thereby posing potential risks to nucle

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32

Tanaka, T., A. Ito, A. Tajima, E. Rokuta, and C. Oshima. "Heteroepitaxial Film of Monolayer Graphene/Monolayer h-BN onNi(111)." Surface Review and Letters 10, no. 05 (2003): 721–26. http://dx.doi.org/10.1142/s0218625x03005529.

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Heteroepitaxial multilayers, consisting of graphene/hexagonal boron nitride (h-BN) films on Ni (111), have been investigated by means of vibrational spectroscopy, low energy electron diffraction and Auger electron spectroscopy. Vibrational spectra of the heteroepitaxial film show the appearance of transverse optical ( TO⊥) modes with out-of-plane polarization at 100 meV of the monolayer h-BN, in contrast to the softening phonon at 90 meV on the pristine system of monolayer h-BN on Ni (111). The findings strongly suggest that the interfacial bonds between h-BN and Ni (111) weaken due to the for

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33

Kluckert, Ehrenfried, and Adolf Schahl. "Rezension von: Schahl, Adolf, Dominikus Hermenegild Herberger." Schwäbische Heimat 32, no. 1 (2025): 66–67. https://doi.org/10.53458/sh.v32i1.16517.

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Adolf Schahl: Dominikus Hermenegild Herberger 1694-1760. Ein Bildhauer des Rokoko in Oberschwaben und am Bodensee. Aufnahmen von Traute Uhland-Clauss. Anton H. Konrad Verlag Weißenhorn 1980. 111 Seiten, 113 Schwarzweiß- und 12 Farbaufnahmen. Leinen DM 48,-

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34

Huang, Jianmei, Qiang Wang, Pengfei Liu, Guang-hui Chen, and Yanhui Yang. "Tuning adlayer-substrate interactions of graphene/h-BN heterostructures on Cu(111)–Ni and Ni(111)–Cu surface alloys." RSC Advances 11, no. 4 (2021): 1916–27. http://dx.doi.org/10.1039/d0ra08622c.

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The evolution of the interface and interaction of h-BN and graphene/h-BN (Gr/h-BN) on Cu(111)–Ni and Ni(111)–Cu surface alloys versus the Ni/Cu atomic percentage on the alloy surface were comparatively studied by DFT-D2, including critical long-range van der Waals forces.

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35

Luo, Wenhua, Lei Wan, Gan Li, and Tao Gao. "Adsorption and dissociation behavior of H2 on PuH2 (100), (110) and (111) surfaces: a density functional theory+U study." RSC Advances 10, no. 33 (2020): 19576–86. http://dx.doi.org/10.1039/d0ra01621g.

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The density functional theory (DFT) and DFT plus correction for on-site Coulomb interaction (DFT+U) method were performed to investigate the adsorption and dissociation of H<sub>2</sub> on PuH<sub>2</sub> (100), (110) and (111) surfaces.

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36

Liu, Chunli, Ling Zhu, Xiaodong Wen, Yong Yang, Yong-Wang Li, and Haijun Jiao. "Exploring direct and hydrogen-assisted CO activation on iridium surfaces – surface dependent activity." Catalysis Science & Technology 10, no. 13 (2020): 4424–35. http://dx.doi.org/10.1039/c9cy02559f.

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To understand CO activation on iridium surfaces, direct dissociation, H-assisted activation and hydrogenation to methanol were computed on the flat Ir(111) and Ir(100), corrugated Ir(110) and Ir(210), and stepped Ir(311) and Ir(221) surfaces.

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37

Bitzer, T., M. Gruyters, H. J. Lewerenz, and K. Jacobi. "Electrochemically prepared Si(111) 1×1‐H surface." Applied Physics Letters 63, no. 3 (1993): 397–99. http://dx.doi.org/10.1063/1.110054.

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38

Hong-Nian, Li, Wang Xiao-Xiong, He Shao-Long, Zhang Han-Jie, Li Hai-Yang, and Bao Shi-Ning. "Electronic structure of Yb/H–Si (111) interface." Chinese Physics 13, no. 11 (2004): 1941–46. http://dx.doi.org/10.1088/1009-1963/13/11/032.

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39

Ćavar, E., R. Westerström, A. Mikkelsen, et al. "A single h-BN layer on Pt(111)." Surface Science 602, no. 9 (2008): 1722–26. http://dx.doi.org/10.1016/j.susc.2008.03.008.

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40

Bahrim, B., S. Yu, B. Makarenko, and J. W. Rabalais. "Electron dynamics in H−/Na/Cu(111) collisions." Surface Science 603, no. 4 (2009): 703–8. http://dx.doi.org/10.1016/j.susc.2009.01.009.

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41

Harten, U., J. P. Toennies, Ch Wöll, et al. "Surface phonons in Si(111) + H(1×1)." Physical Review B 38, no. 5 (1988): 3305–10. http://dx.doi.org/10.1103/physrevb.38.3305.

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42

Ziegler, J. C., A. Reitzle, O. Bunk, J. Zegenhagen, and D. M. Kolb. "Metal deposition on n-Si(111):H electrodes." Electrochimica Acta 45, no. 28 (2000): 4599–605. http://dx.doi.org/10.1016/s0013-4686(00)00611-3.

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43

Honke, R., P. Pavone, and U. Schröder. "Surface phonons of Si(111):H-(1 × 1) and Si(111):As-(1 × 1)." Surface Science 367, no. 1 (1996): 75–86. http://dx.doi.org/10.1016/s0039-6028(96)00836-9.

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44

Pistonesi, Carolina, Estela Pronsato, and Alfredo Juan. "A DFT study of H adsorption on Pt(111) and Pt–Ru(111) surfaces." Applied Surface Science 254, no. 18 (2008): 5827–30. http://dx.doi.org/10.1016/j.apsusc.2008.03.167.

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45

Bauer, Sondes, Berkin Nergis, Xiaowei Jin, et al. "Relevance of Platinum Underlayer Crystal Quality for the Microstructure and Magnetic Properties of the Heterostructures YbFeO3/Pt/YSZ(111)." Nanomaterials 14, no. 12 (2024): 1041. http://dx.doi.org/10.3390/nano14121041.

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The hexagonal ferrite h-YbFeO3 grown on YSZ(111) by pulsed laser deposition is foreseen as a promising single multiferroic candidate where ferroelectricity and antiferromagnetism coexist for future applications at low temperatures. We studied in detail the microstructure as well as the temperature dependence of the magnetic properties of the devices by comparing the heterostructures grown directly on YSZ(111) (i.e., YbPt_Th0nm) with h-YbFeO3 films deposited on substrates buffered with platinum Pt/YSZ(111) and in dependence on the Pt underlayer film thickness (i.e., YbPt_Th10nm, YbPt_Th40nm, Yb

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46

Schaal, Maximilian, Takumi Aihara, Marco Gruenewald, et al. "Hybridization vs decoupling: influence of an h-BN interlayer on the physical properties of a lander-type molecule on Ni(111)." Beilstein Journal of Nanotechnology 11 (August 4, 2020): 1168–77. http://dx.doi.org/10.3762/bjnano.11.101.

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2D materials such as hexagonal boron nitride (h-BN) are widely used to decouple organic molecules from metal substrates. Nevertheless, there are also indications in the literature for a significant hybridization, which results in a perturbation of the intrinsic molecular properties. In this work we study the electronic and optical properties as well as the lateral structure of tetraphenyldibenzoperiflanthene (DBP) on Ni(111) with and without an atomically thin h-BN interlayer to investigate its possible decoupling effect. To this end, we use in situ differential reflectance spectroscopy as an

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47

Вариков, Геннадий, Кирилл Дрозд та Виктор Жорник. "Оптимизация процесса газотермического напыления полимерных покрытий, модифицированных наноалмазами". Journal of Civil Protection 3, № 1 (2019): 23–31. http://dx.doi.org/10.33408/2519-237x.2019.3-1.23.

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С использованием метода многомерного проектного синтеза разработана экспериментально-статистическая математическая модель процесса газотермического напыления композиционного полимер-наноалмазного покрытия для различных видов наноразмерного модификатора (очищенные наноалмазы детонационного синтеза (НАДС) и алмазосодержащая шихта (ША)), в которой в качестве управляющих параметров приняты концентрация модификатора в исходной полимер-наноалмазной порошковой композиции (C), давление горючей смеси (Р), дистанция наплыления (l) и толщина покрытия (h), а критериями оптимизации являются адгезионная про

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48

Li, Yu-Jin, King-Ning Tu, and Chih Chen. "Tensile Properties and Thermal Stability of Unidirectionally <111>-Oriented Nanotwinned and <110>-Oriented Microtwinned Copper." Materials 13, no. 5 (2020): 1211. http://dx.doi.org/10.3390/ma13051211.

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Tensile tests on two kinds of electroplated copper foils with twins before and after annealing were performed. One electroplating parameter results in a microstructure of <110>-oriented microtwinned Cu (mt-Cu), and the other is <111>-oriented nanotwinned Cu (nt-Cu). The latter shows higher thermal stability than the former after annealing. Though the toughness for the two as-plated foils are quite close, the toughness for the <111> oriented nt-Cu increased from 34 to 74 MJ/m3 after annealing at 250 °C for 3 h. In comparison, the toughness of the <110>-oriented mt-Cu rem

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49

Herron, Jeffrey A., Yoshitada Morikawa, and Manos Mavrikakis. "Ab initio molecular dynamics of solvation effects on reactivity at electrified interfaces." Proceedings of the National Academy of Sciences 113, no. 34 (2016): E4937—E4945. http://dx.doi.org/10.1073/pnas.1604590113.

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Using ab initio molecular dynamics as implemented in periodic, self-consistent (generalized gradient approximation Perdew–Burke–Ernzerhof) density functional theory, we investigated the mechanism of methanol electrooxidation on Pt(111). We investigated the role of water solvation and electrode potential on the energetics of the first proton transfer step, methanol electrooxidation to methoxy (CH3O) or hydroxymethyl (CH2OH). The results show that solvation weakens the adsorption of methoxy to uncharged Pt(111), whereas the binding energies of methanol and hydroxymethyl are not significantly aff

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50

Korhonen, Hannu, and Paavo Niemelä. "Seasonal and circadian changes in activity rates of adult farm blue foxes." Agricultural and Food Science 7, no. 1 (1998): 21–29. http://dx.doi.org/10.23986/afsci.72852.

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The present paper reports systematic activity rates obtained from year-round video recordings of farmbred blue foxes (Alopex lagopus) housed singly in conventional wire-mesh cages (107 cm wide x 110 long x 70 cm high). Subjects were 9 males and 13 females. Mean whole-year activity rates were slightly higher in males (394 ± 116 min/24 h; mean ± SD) than females (349 ± 111 min/24 h). Significant (P

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