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1

ULAS, MACIEJ. "A NOTE ON HIGHER TWISTS OF ELLIPTIC CURVES." Glasgow Mathematical Journal 52, no. 2 (2010): 371–81. http://dx.doi.org/10.1017/s0017089510000066.

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AbstractWe show that for any pair of elliptic curves E1, E2 over ℚ with j-invariant equal to 0, we can find a polynomial D ∈ ℤ[u, v] such that the cubic twists of the curves E1, E2 by D(u, v) have positive rank over ℚ(u, v). We also prove that for any quadruple of pairwise distinct elliptic curves Ei, i = 1, 2, 3, 4, with j-invariant j = 0, there exists a polynomial D ∈ ℤ[u] such that the sextic twists of Ei, i = 1, 2, 3, 4, by D(u) have positive rank. A similar result is proved for quadruplets of elliptic curves with j-invariant j = 1, 728.
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2

ULAS, MACIEJ. "VARIATIONS ON HIGHER TWISTS OF PAIRS OF ELLIPTIC CURVES." International Journal of Number Theory 06, no. 05 (2010): 1183–89. http://dx.doi.org/10.1142/s1793042110003472.

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In this note we show that for any pair of elliptic curves E1, E2 over ℚ with j-invariant equal to 0, we can find a polynomial D ∈ ℤ[u, v, w, t] such that the sextic twists of the curves E1, E2 by D(u, v, w, t) have rank ≥ 2 over the field ℚ(u, v, w, t). A similar result is proved for simultaneous quartic twists of pairs of elliptic curves with j-invariant 1728.
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3

Tchernov, Vladimir. "ARNOLD-TYPE INVARIANTS OF CURVES ON SURFACES." Journal of Knot Theory and Its Ramifications 08, no. 01 (1999): 71–97. http://dx.doi.org/10.1142/s0218216599000079.

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Recently V. Arnold introduced Strangeness and J± invariants of generic immersions of an oriented circle to ℝ2. Here these invariants are generalized to the case of generic immersions of an oriented circle to an arbitrary surface F. We explicitly describe all the invariants satisfying axioms, which naturally generalize the axioms used by V. Arnold.
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4

Venegas, José G., R. Scott Harris, and Brett A. Simon. "A comprehensive equation for the pulmonary pressure-volume curve." Journal of Applied Physiology 84, no. 1 (1998): 389–95. http://dx.doi.org/10.1152/jappl.1998.84.1.389.

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Venegas, José G., R. Scott Harris, and Brett A. Simon.A comprehensive equation for the pulmonary pressure-volume curve. J. Appl. Physiol. 84(1): 389–395, 1998.—Quantification of pulmonary pressure-volume (P-V) curves is often limited to calculation of specific compliance at a given pressure or the recoil pressure (P) at a given volume (V). These parameters can be substantially different depending on the arbitrary pressure or volume used in the comparison and may lead to erroneous conclusions. We evaluated a sigmoidal equation of the form, V = a + b[1 +[Formula: see text]]−1, for its ability to
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5

Sonander, Hans-G. "Letters to the Editor." Journal of Applied Physiology 85, no. 5 (1998): 1998–2000. http://dx.doi.org/10.1152/jappl.1998.85.5.1998.

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The following is the abstract of the article discussed in the subsequent letter: Venegas, José G., R. Scott Harris, and Brett A. Simon. A comprehensive equation for the pulmonary pressure-volume curve. J. Appl. Physiol. 84(1): 389–395, 1998.—Quantification of pulmonary pressure-volume (P-V) curves is often limited to calculation of specific compliance at a given pressure or the recoil pressure (P) at a given volume (V). These parameters can be substantially different depending on the arbitrary pressure or volume used in the comparison and may lead to erroneous conclusions. We evaluated a sigmo
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6

Baik, Jihye, Junbum Park, Gyeongjun Lee, Sungchul Kim, and Jungho Kim. "Effects of Incoherent Front Cover Glass on Current-Voltage Characteristics of Cu(In,Ga)Se2 Solar Cells: Investigation into Calculation Accuracy for Cover Glass Modeled as Optically Coherent or Incoherent." Applied Sciences 10, no. 9 (2020): 3312. http://dx.doi.org/10.3390/app10093312.

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We numerically investigate the effects of an incoherent front cover glass on the current–voltage (J–V) characteristics of a Cu(In,Ga)Se2 (CIGS) solar cell using an integrated optoelectronic model. A 3-mm cover glass—the thickness of which was larger than the coherence length of sunlight—was incoherently modeled based on the equispaced thickness averaging method, where coherent simulation results of the wave equation were averaged over a set of equispaced phase thicknesses. The changes in optical power dissipation, absorptivity and electron–hole pair generation rate were calculated depending on
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7

Liu, Yueli, Qiao Chen, Aohan Mei, Bin Hu, Zifan Yang, and Wen Chen. "Bandgap aligned Cu12Sb4S13 quantum dots as efficient inorganic hole transport materials in planar perovskite solar cells with enhanced stability." Sustainable Energy & Fuels 3, no. 3 (2019): 831–40. http://dx.doi.org/10.1039/c9se00003h.

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8

Lu, Honglin, Jia Zhuang, Zhu Ma, et al. "Crystal recombination control by using Ce doped in mesoporous TiO2 for efficient perovskite solar cells." RSC Advances 9, no. 2 (2019): 1075–83. http://dx.doi.org/10.1039/c8ra07800a.

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9

Luo, Paifeng, Zhaofan Liu, Wei Xia, Chenchen Yuan, Jigui Cheng, and Yingwei Lu. "A simple in situ tubular chemical vapor deposition processing of large-scale efficient perovskite solar cells and the research on their novel roll-over phenomenon in J–V curves." Journal of Materials Chemistry A 3, no. 23 (2015): 12443–51. http://dx.doi.org/10.1039/c5ta02306h.

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10

Zeng, Yuheng, Zetao Ding, Zunke Liu, et al. "Efficiency-loss analysis of monolithic perovskite/silicon tandem solar cells by identifying the patterns of a dual two-diode model’s current-voltage curves." Journal of Semiconductors 44, no. 8 (2023): 082702. http://dx.doi.org/10.1088/1674-4926/44/8/082702.

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Abstract In this work, we developed a simple and direct circuit model with a dual two-diode model that can be solved by a SPICE numerical simulation to comprehensively describe the monolithic perovskite/crystalline silicon (PVS/c-Si) tandem solar cells. We are able to reveal the effects of different efficiency-loss mechanisms based on the illuminated current density-voltage (J-V), semi-log dark J-V, and local ideality factor (m-V) curves. The effects of the individual efficiency-loss mechanism on the tandem cell’s efficiency are discussed, including the exp(V/V T) and exp(V/2V T) recombination
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11

Zhou, Zheng, Jia Xu, Li Xiao, et al. "Efficient planar perovskite solar cells prepared via a low-pressure vapor-assisted solution process with fullerene/TiO2 as an electron collection bilayer." RSC Advances 6, no. 82 (2016): 78585–94. http://dx.doi.org/10.1039/c6ra14372e.

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12

Wang, Jian, Fujun Zhang, Qiaoshi An, Qianqian Sun, Jian Zhang, and Bin Hu. "Unique insight into phase separation in polymer solar cells from their electric characteristics." Physical Chemistry Chemical Physics 17, no. 44 (2015): 29671–78. http://dx.doi.org/10.1039/c5cp05471k.

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13

Pedersen, O. F., H. J. L. Brackel, J. M. Bogaard, and K. F. Kerrebijn. "Wave-speed-determined flow limitation at peak flow in normal and asthmatic subjects." Journal of Applied Physiology 83, no. 5 (1997): 1721–32. http://dx.doi.org/10.1152/jappl.1997.83.5.1721.

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Pedersen, O. F., H. J. L. Brackel, J. M. Bogaard, and K. F. Kerrebijn. Wave-speed-determined flow limitation at peak flow in normal and asthmatic subjects. J. Appl. Physiol. 83(5): 1721–1732, 1997.—The purpose of this study was to examine whether peak expiratory flow is determined by the wave-speed flow-limiting mechanism. We examined 17 healthy subjects and 11 subjects with stable asthma, the latter treated with inhaled bronchodilators and corticosteroids. We used an esophageal balloon and a Pitot-static probe positioned at five locations between the right lower lobe and midtrachea to obtain
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14

Indow, T. "Chromatic Response Curves of Surface Colours." Perception 26, no. 1_suppl (1997): 184. http://dx.doi.org/10.1068/v970054.

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Basic data in colour vision such as chromatic response curves were obtained with aperture colours. It is not possible to apply the cancellation technique to define redness or yellowness components etc in a surface colour. A method was developed to obtain such information (Indow, 1987 Die Farbe34 253 – 260), which was based on the expanded form of multidimensional scaling. The results by an improved method are presented. First, it is shown how multiattribute perceptual differences between two Munsell colours, P j, P k, are predicted by distances ^ djk in the current Munsell solid. Colour differ
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15

Jiang, Huirong, Xingyu Liu, Nianyao Chai, et al. "Alleviate the J–V hysteresis of carbon-based perovskite solar cells via introducing additional methylammonium chloride into MAPbI3 precursor." RSC Advances 8, no. 61 (2018): 35157–61. http://dx.doi.org/10.1039/c8ra04347g.

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The hysteretic phenomenon commonly exists in the J–V curves of perovskite solar cells with different structures, especially for carbon-based mesoscopic perovskite solar cells without hole-conductor (carbon-based PSCs).
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16

Hindsley, Robert, and R. A. Bell. "An Adjustment to Cepheid Distances Calculated Using Model Atmospheres." International Astronomical Union Colloquium 139 (1993): 94. http://dx.doi.org/10.1017/s0252921100116987.

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Hindsley and Bell (1989, Ap. J., 341, 1004) determined distances for 23 Cepheids using the surface brightness method. The color V – IC on the Cousins system or V – RJ on the Johnson system was used to measure visual surface brightness. Combined with the observed visual magnitudes, angular diameters were then calculated. Comparison of angular diameters with radius differences in linear units, obtained by integrating the radial velocity curve, yielded each Cepheid's distance.Hindsley and Bell calibrated the relationship between color and surface brightness using model atmospheres. The zero point
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17

Liu, Tie, Pengyu Su, Li Liu, et al. "An ionic compensation strategy for high-performance mesoporous perovskite solar cells: healing defects with tri-iodide ions in a solvent vapor annealing process." Journal of Materials Chemistry A 7, no. 1 (2019): 353–62. http://dx.doi.org/10.1039/c8ta10094b.

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18

Gao, Jinhua, Qiaoshi An, Miao Zhang, et al. "One key issue in characterization of organic solar cells with solution processed interfacial layers." Physical Chemistry Chemical Physics 21, no. 10 (2019): 5790–95. http://dx.doi.org/10.1039/c9cp00181f.

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Solution processed PDIN interfacial layers may have some effect on the performance of OSCs; an appropriate shadow mask is necessary to measure the J–V curves of OSCs with solution processed interfacial layers.
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19

Yamamoto, Natasha A. D., Deize C. Grodniski, Lucimara S. Roman, Marlus Koehler, and Marcos G. E. da Luz. "Space-Charge-Limited Bipolar Currents at High Fields in Polymer/C60 Diodes: A Simple Model Description." Advanced Materials Research 747 (August 2013): 591–94. http://dx.doi.org/10.4028/www.scientific.net/amr.747.591.

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We investigate the dark transport properties of organic photovoltaic devices formed by a heterojunction of a semiconducting co-polymer and the fullerene (C60) [. The copolymers are composed of thiophene, phenylene and fluorene units, where the thiophene content was kept constant while the fluorene/phenylene ratio was varied. Measurements show that for low voltage, the current versus voltage (j x V) characteristics presents an exponential increasing, typical of a diode behavior. On the other hand, the j x V curves are space-charge limited at high voltages. This latter response follows the theor
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20

Wang, J. C., X. C. Ren, S. Q. Shi, C. W. Leung, and Paddy K. L. Chan. "Charge accumulation induced S-shape J–V curves in bilayer heterojunction organic solar cells." Organic Electronics 12, no. 6 (2011): 880–85. http://dx.doi.org/10.1016/j.orgel.2011.02.016.

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21

Xu, Xinfeng, Jian Shi, and Yuanjing Zhao. "Experimental Study on Plastic Deformation of EH690 Steel with the V-Notch during Falling Weight Impact Based on DIC." Processes 12, no. 4 (2024): 751. http://dx.doi.org/10.3390/pr12040751.

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In this study, a falling weight impact test was conducted on EH690 steel specimens with V-notches using Digital Imaging Correlation (DIC). In conjunction with scanning electron microscopy (SEM), the plastic deformation and crack initiation processes were examined at the notch of the specimen under different impact energies (90 J, 120 J, 135 J and 150 J). ABAQUS was used to simulate the plastic deformation of an EH690 specimen. The results show that the strain at the notch tip experienced some elasticity and yielding as the load increased under different impact energies. The load remains unchan
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22

Nguyen Thi Thu, Hang, Son Nguyen Thanh, and Truong Vu Van. "A SECOND MAIN THEOREM FOR ENTIRE CURVES IN A PROJECTIVE VARIETY WHOSE DERIVATIVES VANISH ON INVERSE IMAGE OF HYPERSURFACE TARGETS." Journal of Science Natural Science 65, no. 6 (2020): 31–40. http://dx.doi.org/10.18173/2354-1059.2020-0026.

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We establish a second main theorem for algebraically nondegenerate entire curves f in a projective variety V ⊂ P n(C) and a hypersurface target {D1, D2, . . . , Dq} satisfying f∗,z = 0 for all z ∈ ∪q j=1f−1(Dj).
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23

Luo, Shanglin, Mingfang Huo, Qin Xue, and Guohua Xie. "Numerical Simulation of S-Shaped Current–Voltage Curves Induced by Electron Traps in Inverted Organic Photovoltaics." International Journal of Molecular Sciences 23, no. 4 (2022): 2039. http://dx.doi.org/10.3390/ijms23042039.

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Organic photovoltaics (OPVs) differ from their inorganic counterparts because of inevitable electronic disorders and structural heterogeneity. Charge carrier traps are inevitable in organic semiconductors. A common failure mechanism of OPVs is the development of an S-shaped current density–voltage characteristic (J-V curve). Herein, we focus on investigating the underlying physical mechanism of S-shaped deformation of J-V curve of the inverted organic photovoltaic devices with bulk-heterojunction, proven by experiments with the n-doped electron extraction layer and numerical simulations assumi
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24

CHENG, CHIEN-MIN, MING-CHANG KUAN, KAI-HUNAG CHEN, and JEN-HWAN TSAI. "IMPROVEMENT ON CHARACTERISTICS OF FERROELECTRIC THIN FILMS USING SUPERCRITICAL CARBON DIOXIDE FLUID TREATMENT." International Journal of Modern Physics: Conference Series 06 (January 2012): 104–8. http://dx.doi.org/10.1142/s2010194512003017.

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Electrical and physical properties of as-deposited Bi 3.9 La 0.1 Ti 2.9 V 0.1 O 12 (BLTV) ferroelectric thin films on SiO 2/ Si (100) substrates were improved by low temperature supercritical carbon dioxide fluid (SCF) process treatment. The as-deposited BLTV ferroelectric thin films were treated by SCF process which mixed with propyl alcohol and pure water. The memory windows increased in C-V curves, and the oxygen vacancy and defect in leakage current density curves were obtained after SCF process treatment. Finally, the improvement properties of as-deposited BLTV thin films after SCF proces
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25

Zamora, Pedro, Belkacem Kouskoussa, Zouhair El Jouad, et al. "New electron donor in planar heterojunction: optimization of the cells efficiency through the choice of the hole-extracting layer." European Physical Journal Applied Physics 89, no. 2 (2020): 20201. http://dx.doi.org/10.1051/epjap/2020190346.

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Due to their light weight, flexibility and semi-transparency the organic photovoltaic cells play an important role for solar conversion photovoltaic (OPV). To achieve good performances, both donor and acceptor materials in OPVs need to have good extinction coefficients, high stabilities and good film morphologies. Since the donor plays a critical role as the absorber to solar photon flux, donor materials require wide optical absorption to match the solar spectrum. In this work the couple ED/EA in planar heterojunction was Tetracyano 4,4'-bis(9Hcarbazol-9-yl) biphenyl (TCC)/fullerene (C60). Opt
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26

Ito, Shota. "Capacity Recovery Phenomenon Manifested in Lithium-Ion Batteries Due to over-Discharge." ECS Meeting Abstracts MA2024-02, no. 2 (2024): 239. https://doi.org/10.1149/ma2024-022239mtgabs.

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【Background】 The need for Lithium-ion batteries (LIBs) with longer life is growing with the popularization of their applications, but LIBs lose capacity with use. These reduction in capacity of LIBs is mainly due to three factors: namely, the reduction of a positive electrode capacity, the reduction of a negative electrode capacity, and the mutual “capacity slippage” between the capacity of a positive and a negative electrodes [1]. The reduction of a positive and a negative electrode capacity is caused by deactivation of active materials due to decrease in the conducting paths of electrons and
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27

Topulos, G. P., M. B. Reid, and D. E. Leith. "Pliometric activity of inspiratory muscles: maximal pressure-flow curves." Journal of Applied Physiology 62, no. 1 (1987): 322–27. http://dx.doi.org/10.1152/jappl.1987.62.1.322.

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We tested the hypothesis that inspiratory muscles, like other skeletal muscles, would exert greater force under pliometric conditions (being lengthened while active) than under isometric or miometric (active shortening) conditions. Maximal inspiratory pressure-flow curves of the respiratory system are analogous to the force-velocity curves for isolated muscle (Agostoni and Fenn, J. Appl. Physiol. 15:349–353, 1960). We measured esophageal pressure (Pes) and plethysmographic flow (V) at relaxation volume of the respiratory system in six trained subjects inspiring maximally through graded resisto
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28

WANG, L. G., H. W. ZHANG, X. L. TANG, and C. H. MU. "CALCULATION AND ANALYSIS OF ELECTRICAL BEHAVIOR IN DISORDERED SEMICONDUCTING POLYMERS BASED ON EXTENDED GAUSSIAN DISORDER MODEL." Modern Physics Letters B 24, no. 15 (2010): 1647–56. http://dx.doi.org/10.1142/s0217984910024043.

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We calculate and analyze some electrical properties of semiconducting polymers in detail based on the extended Gaussian disorder model.10 It is shown that the carrier density at the interface (the boundary carrier density) has an important influence on the current–voltage (J–V) characteristics. Too large or too small values of the boundary carrier density will lead to incorrect J–V characteristics. Additionally, we show that numerically calculated carrier density is a decreasing function of the distance from the interface, and the slope of curves decrease with the increasing boundary carrier d
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29

Martín-Gómez, José Javier, Diego Gutiérrez del Pozo, Mariano Ucchesu, et al. "Seed Morphology in the Vitaceae Based on Geometric Models." Agronomy 10, no. 5 (2020): 739. http://dx.doi.org/10.3390/agronomy10050739.

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Morphometric methods based on artificial vision algorithms provide measurements for magnitudes descriptive of seed images (i.e., the length, width, area, and surface circularity index). Nevertheless, their results frequently omit the resemblance of the images to geometric figures that may be used as models. A complementary method based on the comparison of seed images with geometric models is applied to seeds of Vitis spp. The J index gives the percentage of similarity between a seed image and the model. Seven new geometric models are described based on the heart-shaped and piriform curves. Se
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30

Chernomorskii, Alexandr I. "The Relation between the Depolarization and Electrode Potentials." ECS Meeting Abstracts MA2025-01, no. 50 (2025): 2523. https://doi.org/10.1149/ma2025-01502523mtgabs.

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Depolarization (the interaction of the deposited metal with the electrode metal) significantly shifts the deposition potential to the positive side. For example, alkali metals are deposited on lead electrodes at potentials that are ~ 1.5 V more positive than their equilibrium potentials [1]. In principle, the Gibbs energy of depolarization ΔGdepol could compensate the Gibbs energy ΔGequil of the electrode half-reaction -interaction. The potential jump in the double - electric layer Δψequil = - ΔGequil / nF caused by the half-reaction could be compensated by ΔEdepol = - ΔGdepol / nF [2]. When t
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31

Jin, T. M., W. Rui, Z. Shu, et al. "ZnO:Polymer Composite Material to Eliminate Kink in J-V Curves of Inverted Polymer Solar Cells." ECS Solid State Letters 3, no. 3 (2014): Q9—Q12. http://dx.doi.org/10.1149/2.006403ssl.

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32

Kuan, Ming Chang, Kai Huang Chen, Wen Cheng Tzou, Chien Min Cheng, and Yi Jun Lin. "Low Temperature Method for Enhancing Ferroelectric Thin Films in Non-Volatile Random Access Memory Devices." Advanced Materials Research 239-242 (May 2011): 2628–31. http://dx.doi.org/10.4028/www.scientific.net/amr.239-242.2628.

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In this study, the electrical properties of as-deposited Sr0.4Ba0.6Nb2O6(SBN) ferroelectric thin films on SiO2/Si(100) substrates were improved by low temperature supercritical carbon dioxide fluid (SCF) process treatment. The as-deposited SBN ferroelectric thin films were treated by SCF process which mixed with pure H2O and propyl alcohol. After SCF process treatment, the memory windows increased in C-V curves, and the passivation of oxygen vacancy and defect in leakage current density curves were obtained. In addition, the improvement properties of as-deposited SBN thin films after SCF proce
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33

Soutiere, Shawn E., and Wayne Mitzner. "On defining total lung capacity in the mouse." Journal of Applied Physiology 96, no. 5 (2004): 1658–64. http://dx.doi.org/10.1152/japplphysiol.01098.2003.

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Maximal lung volume or total lung capacity in experimental animals is dependent on the pressure to which the lungs are inflated. Although 25-30 cmH2O are nominally used for such inflations, mouse pressure-volume (P-V) curves show little flattening on inflation to those pressures. In the present study, we examined P-V relations and mean alveolar chord length in three strains (C3H/HeJ, A/J, and C57BL/6J) at multiple inflation pressures. Mice were anesthetized, and their lungs were degassed in vivo by absorption of 100% O2. P-V curves were then recorded in situ with increasing peak inflation pres
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34

Brugallé, Erwan, Pierre-Vincent Koseleff, and Daniel Pecker. "On the lexicographic degree of two-bridge knots." Journal of Knot Theory and Its Ramifications 25, no. 07 (2016): 1650044. http://dx.doi.org/10.1142/s0218216516500449.

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We study the degree of polynomial representations of knots. We obtain the lexicographic degree for two-bridge torus knots and generalized twist knots. The proof uses the braid theoretical method developed by Orevkov to study real plane curves, combined with previous results from [Chebyshev diagrams for two-bridge knots, Geom. Dedicata 150 (2010) 405–425; E. Brugallé, P.-V. Koseleff, D. Pecker, Untangling trigonal diagrams, to appear in J. Knot Theory and its Ramifications]. We also give a sharp lower bound for the lexicographic degree of any knot, using real polynomial curves properties.
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35

Chaw, Chaw Su Nandar Hlaing, and Thiri Nwe. "Analysis on Band Layer Design and J-V characteristics of Zinc Oxide Based Junction Field Effect Transistor." Journal La Multiapp 1, no. 2 (2020): 14–21. http://dx.doi.org/10.37899/journallamultiapp.v1i2.108.

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This paper presents the band gap design and J-V characteristic curve of Zinc Oxide (ZnO) based on Junction Field Effect Transistor (JFET). The physical properties for analysis of semiconductor field effect transistor play a vital role in semiconductor measurements to obtain the high-performance devices. The main objective of this research is to design and analyse the band diagram design of semiconductor materials which are used for high performance junction field effect transistor. In this paper, the fundamental theory of semiconductors, the electrical properties analysis and bandgap design of
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36

Jiang, Yunguo, Shao-Ming Hu, Xu Chen, Xi Shao та Qiu-Hong Huo. "Locations of optical and γ-ray emitting regions and variation phenomena of PMN J2345−1555". Monthly Notices of the Royal Astronomical Society 493, № 3 (2020): 3757–69. http://dx.doi.org/10.1093/mnras/staa475.

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ABSTRACT We collect the long-term γ-ray, optical, and radio 15 GHz light curves of quasar object PMN J2345−1555, and make correlation analyses between them. We find that different samplings can lead to different time delays, and the periodicity of light curves can produce signals that are beyond 3σ significance level. The optical V and R band and the infrared J band light curves lead the radio 15 GHz light curve by $49^{+15}_{-12}$ d. There is no lag between the optical and γ-ray light curves. We use the time lags to derive the core size and its uncertainty. We find that the core region of 15
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37

van der Kooij, A. M., and S. C. Luijendijk. "Longitudinal dispersion of gases measured in a model of the bronchial airways." Journal of Applied Physiology 59, no. 5 (1985): 1343–49. http://dx.doi.org/10.1152/jappl.1985.59.5.1343.

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We investigated the longitudinal dispersion of helium (He), methane, acetylene, butane, sulfur hexafluoride, and octafluorocyclobutane (C4F8) in a clear plastic model of the human bronchial airways. The dimensions of the seven airway generations (0–6) of the model were chosen to be equal to those given by Weibel's model A (Morphometry of the Human Lung; New York: Academic, 1963). Total volume of the model amounts to 52 ml. A small bolus of each of the tracer gases was injected within 1 ms into a constant airflow at the inlet of the model, and the bolus dispersion curve was measured at the outl
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38

Ahmmad, B., Y. Kusumoto, M. Abdulla-Al-Mamun, A. Mihata, and H. Yang. "Effect of Single Walled Carbon Nanotube as Counter Electrode on Laser-deposited Fe2O3 and TiO2 Films Solar Cells." Journal of Scientific Research 1, no. 3 (2009): 430–37. http://dx.doi.org/10.3329/jsr.v1i3.2631.

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Laser-deposited Fe2O3 films or dye-fixed TiO2 films were prepared for solar cells. For both the cells, a single walled carbon nanotube (SWNT) film or a Pt-loaded SWNT film, prepared by simply pasting over ITO glass, was used as a counter electrode. Stable current (I)-voltage (V) curves were found under UV-visible light irradiation using water containing KI and I2 as an electrolyte. A comparison of I-V curves was made for Pt alone and SWNT alone films used as a counter electrode. Almost similar efficiency was found by using both types of counter electrodes. However, enhanced efficiency was obta
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39

Osorio, Henrry Marcelo, Santiago Martín, María Carmen López, et al. "Electrical characterization of single molecule and Langmuir–Blodgett monomolecular films of a pyridine-terminated oligo(phenylene-ethynylene) derivative." Beilstein Journal of Nanotechnology 6 (May 11, 2015): 1145–57. http://dx.doi.org/10.3762/bjnano.6.116.

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Monolayer Langmuir–Blodgett (LB) films of 1,4-bis(pyridin-4-ylethynyl)benzene (1) together with the “STM touch-to-contact” method have been used to study the nature of metal–monolayer–metal junctions in which the pyridyl group provides the contact at both molecule–surface interfaces. Surface pressure vs area per molecule isotherms and Brewster angle microscopy images indicate that 1 forms true monolayers at the air–water interface. LB films of 1 were fabricated by deposition of the Langmuir films onto solid supports resulting in monolayers with surface coverage of 0.98 × 10−9 mol·cm−2. The mor
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40

Verbanck, S., D. Linnarsson, G. K. Prisk, and M. Paiva. "Specific ventilation distribution in microgravity." Journal of Applied Physiology 80, no. 5 (1996): 1458–65. http://dx.doi.org/10.1152/jappl.1996.80.5.1458.

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We studied the contribution of inter- and intraregional inhomogeneities of specific ventilation (delta V/Vo) from the rebreathing inert gas trace in microgravity and on Earth. The rebreathing tests were carried out by four astronauts before, during, and after the 10-day Spacelab D-2 mission. Starting from functional residual capacity, the rebreathing maneuver consisted of eight reinspirations from a bag filled with 1.8-2.2 liters of test gas mixtures containing approximately 5% argon. The rate of argon equilibration in the rebreathing bag, termed RBeq, was quantified by determining the logarit
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41

Assi, Ahmed Ali, Wasan R. Saleh, and Ezzedin Mohajerani. "Effect of Deposit Au thin Layer Between Layers of Perovskite Solar Cell on Cell's Performance." Iraqi Journal of Physics (IJP) 19, no. 51 (2021): 23–32. http://dx.doi.org/10.30723/ijp.v19i51.696.

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The present work aims to fabricate n-i-p forward perovskite solar cell (PSC) withئ structure (FTO/ compact TiO2/ compact TiO2/ MAPbI3 Perovskite/ hole transport layer/ Au). P3HT, CuI and Spiro-OMeTAD were used as hole transport layers. A nano film of 25 nm gold layer was deposited once between the electron transport layer and the perovskite layer, then between the hole transport layer and the perovskite layer. The performance of the forward-perovskite solar cell was studied. Also, the role of each electron transport layer and the hole transport layer in the perovskite solar cell was presented.
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42

Zhong, Qian, Hong-Bang Liu, Kangfa Cheng, et al. "Polarization Evolution of Gamma-Ray Burst Prompt Emission with Bulk Acceleration." Astrophysical Journal 986, no. 1 (2025): 32. https://doi.org/10.3847/1538-4357/add0ac.

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Abstract During the prompt phase, Poynting-flux-dominated jets undergo acceleration accompanied by magnetic dissipation. By using an outward-propagating thin-shell model, where bulk Lorentz factors Γ increase with radius and the magnetic field strength decay is related to the acceleration and the energy conversion rate, this process can be investigated through time-resolved polarization analysis. Faster acceleration produces a greater flux, steeper light-curve growth followed by a sharper decline, and polarization degree decreases sharply. With a fixed acceleration index, lower energy conversi
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43

Han, Fang, Shyam Subramanian, Thomas E. Dick, Ismail A. Dreshaj, and Kingman P. Strohl. "Ventilatory behavior after hypoxia in C57BL/6J and A/J mice." Journal of Applied Physiology 91, no. 5 (2001): 1962–70. http://dx.doi.org/10.1152/jappl.2001.91.5.1962.

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Given the environmental forcing by extremes in hypoxia-reoxygenation, there might be no genetic effect on posthypoxic short-term potentiation of ventilation. Minute ventilation (V˙e), respiratory frequency (f), tidal volume (Vt), and the airway resistance during chemical loading were assessed in unanesthetized unrestrained C57BL/6J (B6) and A/J mice using whole body plethysmography. Static pressure-volume curves were also performed. In 12 males for each strain, after 5 min of 8% O2 exposure, B6 mice had a prominent decrease inV˙e on reoxygenation with either air (−11%) or 100% O2 (−20%), due t
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44

Zhang, Lin, Lin Yao, Yanfang Chu, et al. "Hydrogen Bonds in Precursor Solution: The Origin of the Anomalous J–V Curves in Perovskite Solar Cells." Crystals 12, no. 5 (2022): 610. http://dx.doi.org/10.3390/cryst12050610.

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Perovskite Solar Cells are a promising solar energy harvesting technology due to their low cost and high-power conversion efficiency. A high-quality perovskite layer is fundamental for a highly efficient perovskite Solar Cell. Utilizing a gas quenching process (GQP) can eliminate the need for toxic, flammable, and expensive anti-solvents in the preparation of perovskite layers. It is a promising candidate technology for large scale preparation of perovskite layers, as it can be easily integrated in a production line by coupling up-scalable techniques. The GQP removes the need for polar solvent
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45

Zhang, Lin, Lin Yao, Yanfang Chu, et al. "Hydrogen Bonds in Precursor Solution: The Origin of the Anomalous J–V Curves in Perovskite Solar Cells." Crystals 12, no. 5 (2022): 610. http://dx.doi.org/10.3390/cryst12050610.

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Perovskite Solar Cells are a promising solar energy harvesting technology due to their low cost and high-power conversion efficiency. A high-quality perovskite layer is fundamental for a highly efficient perovskite Solar Cell. Utilizing a gas quenching process (GQP) can eliminate the need for toxic, flammable, and expensive anti-solvents in the preparation of perovskite layers. It is a promising candidate technology for large scale preparation of perovskite layers, as it can be easily integrated in a production line by coupling up-scalable techniques. The GQP removes the need for polar solvent
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46

Zhang, Lin, Lin Yao, Yanfang Chu, et al. "Hydrogen Bonds in Precursor Solution: The Origin of the Anomalous J–V Curves in Perovskite Solar Cells." Crystals 12, no. 5 (2022): 610. http://dx.doi.org/10.3390/cryst12050610.

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Perovskite Solar Cells are a promising solar energy harvesting technology due to their low cost and high-power conversion efficiency. A high-quality perovskite layer is fundamental for a highly efficient perovskite Solar Cell. Utilizing a gas quenching process (GQP) can eliminate the need for toxic, flammable, and expensive anti-solvents in the preparation of perovskite layers. It is a promising candidate technology for large scale preparation of perovskite layers, as it can be easily integrated in a production line by coupling up-scalable techniques. The GQP removes the need for polar solvent
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47

Cal,, Rau´l Bayoa´n, Xia Wang,, and Luciano Castillo. "Transpired Turbulent Boundary Layers Subject to Forced Convection and External Pressure Gradients." Journal of Heat Transfer 127, no. 2 (2005): 194–98. http://dx.doi.org/10.1115/1.1842790.

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The problem of forced convection transpired turbulent boundary layers with external pressure gradient has been studied by using different scalings proposed by various researchers. Three major results were obtained: First, for adverse pressure gradient boundary layers with suction, the mean deficit profiles collapse with the free stream velocity, U∞, but into different curves depending on the strength of the blowing parameter and the upstream conditions. Second, the dependencies on the blowing parameter, the Reynolds number, and the strength of pressure gradient are removed from the outer flow
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48

Liang, Jingjing, Minfang Han, and Meng Ni. "A Comparative Study of the Performance and Electrode Processes of Solid Oxide H2O Electrolysis and CO2 Electrolysis." ECS Transactions 111, no. 6 (2023): 1297–99. http://dx.doi.org/10.1149/11106.1297ecst.

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Solid oxide CO2 electrolysis was less studied compared with H2O electrolysis and the relevant reaction mechanism and electrode processes were poorly understood. This paper investigated the performance and electrode processes differences between CO2 electrolysis and H2O electrolysis. The shape of j-V curves, electrochemical impedance spectroscopy data and calculated distribution relaxation time results were analyzed. It was found that the performance of CO2 electrolysis degraded the most compared with that in SOFC mode and for H2O electrolysis after a 65 h’ operation. Meanwhile, j-V curve of CO
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49

Li, Sai, Longcheng Huang, Jifei Ye, et al. "Study on Radiation Damage of Silicon Solar Cell Electrical Parameters by Nanosecond Pulse Laser." Electronics 13, no. 9 (2024): 1795. http://dx.doi.org/10.3390/electronics13091795.

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This experimental study investigates the damage effects of nanosecond pulse laser irradiation on silicon solar cells. It encompasses the analysis of transient pulse signal waveform characteristics at the cells’ output and changes in electrical parameters, such as I–V curves before and after laser irradiation under varying laser fluence and background light intensities, and explores the underlying action mechanisms of laser irradiation. The study reveals that as the laser fluence increases up to 4.0 J/cm2, the peak value of the transient pulse signal increases by 47.5%, while the pulse width au
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50

WANG, Z. H. "TRANSPORT CURRENT CHARACTERISTICS OF THE TEXTURED Bi-2223 THICK FILM." Modern Physics Letters B 09, no. 21 (1995): 1369–76. http://dx.doi.org/10.1142/s0217984995001364.

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The transport current characteristics of the textured Bi-2223 thick film were studied by the measurement of the voltage–current curves for different temperatures and various magnetic fields. The results show that the transitions can be fitted approximately by a power law with n-values at the low electrical field region. The n-value is observed to fall with increased applied magnetic field and temperature, and exhibits the thermally activated flux flow behavior. The activation energies U(T, H, J) derived from the V-I curves were found to follow a (n − 1)k B T × ln (J0/J). The critical temperatu
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