Effect of Drip Irrigation, N, K, and Zn Coupling on <inline-formula><math display="inline"><semantics><mrow><mi>P</mi><mi>n</mi></mrow></semantics></math></inline-formula> of Dense... by Weiyi Mu, Xiaoxian Duan, Quanjiu Wang, Xuesong Wei, Kai Wei, Yuanxin Li, Xin Guo

“…This study aimed to determine the effect of irrigation amount (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>W</mi></mrow></semantics></math></inline-formula>), nitrogen (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>N</mi></mrow></semantics></math></inline-formula>), potassium (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>K</mi></mrow></semantics></math></inline-formula>), and zinc (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>Z</mi><mi>n</mi></mrow></semantics></math></inline-formula>) on the net photosynthetic rate (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>P</mi><mi>n</mi></mrow></semantics></math></inline-formula>) of closely planted apple trees on dwarf rootstocks in arid areas of Xinjiang. …”
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Investigation on Rare Nuclear Processes in Hf Nuclides by Vincenzo Caracciolo, Pierluigi Belli, Rita Bernabei, Fabio Cappella, Riccardo Cerulli, Antonella Incicchitti, Matthias Laubenstein, Alice Leoncini, Vittorio Merlo, Serge Nagorny, Stefano Nisi, Peng Wang

“…In particular, the study of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>α</mi></semantics></math></inline-formula> decay and double beta decay of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow></mrow><mn>174</mn></msup></semantics></math></inline-formula>Hf, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow></mrow><mn>176</mn></msup></semantics></math></inline-formula>Hf, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow></mrow><mn>177</mn></msup></semantics></math></inline-formula>Hf, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow></mrow><mn>178</mn></msup></semantics></math></inline-formula>Hf, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow></mrow><mn>179</mn></msup></semantics></math></inline-formula>Hf, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow></mrow><mn>180</mn></msup></semantics></math></inline-formula>Hf isotopes either to the ground state or to the lower bounded levels have been discussed. …”
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Understanding the Effect of Conserved Charges on the Coalescence Sum Rule of Directed Flow by Kishora Nayak, Shu-Su Shi, Zi-Wei Lin

“…Recently, the rapidity-odd directed flow (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>v</mi><mn>1</mn></msub></semantics></math></inline-formula>) of produced hadrons (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mi>K</mi><mo>−</mo></msup></semantics></math></inline-formula>, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>ϕ</mi></semantics></math></inline-formula>, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mover><mi>p</mi><mo>¯</mo></mover></semantics></math></inline-formula>, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mover><mo>Λ</mo><mo>¯</mo></mover></semantics></math></inline-formula>, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mover><mo>Ξ</mo><mo>¯</mo></mover><mo>+</mo></msup></semantics></math></inline-formula>, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mo>Ω</mo><mo>−</mo></msup></semantics></math></inline-formula>, and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mover><mo>Ω</mo><mo>¯</mo></mover><mo>+</mo></msup></semantics></math></inline-formula>) has been studied. …”
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On the Properties of <i>λ</i>-Prolongations and <i>λ</i>-Symmetries by Wenjin Li, Xiuling Li, Yanni Pang

“…In this paper, (1) We show that if there are not enough symmetries and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>λ</mi></semantics></math></inline-formula>-symmetries, some first integrals can still be obtained. …”
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LFDFT—A Practical Tool for Coordination Chemistry by Harry Ramanantoanina

“…Using effective Hamiltonian in conjunction with the DFT, we are able to reasonably calculate the low-lying excited states of the molecular [Eu(NO<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>3</mn></msub></semantics></math></inline-formula>)<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>3</mn></msub></semantics></math></inline-formula>(phenanthroline)<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>2</mn></msub></semantics></math></inline-formula>] complex, subjected to the Eu<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow></mrow><mrow><mn>3</mn><mo>+</mo></mrow></msup></semantics></math></inline-formula> configuration 4<i>f</i><inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow></mrow><mn>6</mn></msup></semantics></math></inline-formula>. …”
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Entropy of Quantum Measurements by Stanley Gudder

“…If <i>a</i> is a quantum effect and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>ρ</mi></semantics></math></inline-formula> is a state, we define the <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>ρ</mi></semantics></math></inline-formula>-entropy <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>S</mi><mi>a</mi></msub><mrow><mo>(</mo><mi>ρ</mi><mo>)</mo></mrow></mrow></semantics></math></inline-formula> which gives the amount of uncertainty that a measurement of <i>a</i> provides about <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>ρ</mi></semantics></math></inline-formula>. …”
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Degree of the Product of Two Algebraic Numbers One of Which Is of Prime Degree by Paulius Virbalas

“…Let <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>α</mi></semantics></math></inline-formula> and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>β</mi></semantics></math></inline-formula> be two algebraic numbers such that <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mo form="prefix">deg</mo><mo>(</mo><mi>α</mi><mo>)</mo><mo>=</mo><mi>m</mi></mrow></semantics></math></inline-formula> and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mo form="prefix">deg</mo><mo>(</mo><mi>β</mi><mo>)</mo><mo>=</mo><mi>p</mi></mrow></semantics></math></inline-formula>, where <i>p</i> is a prime number not dividing <i>m</i>. …”
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The Effects of Cracking Ratio on Ammonia/Air Non-Premixed Flames under High-Pressure Conditions Using Large Eddy Simulations by Chengming Wang, Haiou Wang, Kun Luo, Jianren Fan

“…However, one of the main challenges for ammonia combustion is the high level of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>NO</mi></semantics></math></inline-formula> emissions. …”
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The <i>α_σ</i>-Approximation Property and Its Related Operator Ideals by Ju Myung Kim

“…In this paper, we study the <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>σ</mi></semantics></math></inline-formula>-tensor norm (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>α</mi><mi>σ</mi></msub></semantics></math></inline-formula>), the absolutely <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>τ</mi></semantics></math></inline-formula>-summing operator and the <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>σ</mi></semantics></math></inline-formula>-nuclear operator. …”
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Technique-Dependent Relationship between Local Ski Bending Curvature, Roll Angle and Radial Force in Alpine Skiing by Christoph Thorwartl, Andreas Tschepp, Michael Lasshofer, Helmut Holzer, Martin Zirkl, Matthias Hammer, Barbara Stadlober, Thomas Stöggl

“…The value of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msup><mi>w</mi><mo>″</mo></msup></mrow></semantics></math></inline-formula> increases as a result of enlargement of the roll angle (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>R</mi><mi>A</mi></mrow></semantics></math></inline-formula>) and the radial force (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>R</mi><mi>F</mi></mrow></semantics></math></inline-formula>) and consequently minimizes the radius of the turn, preventing skidding. …”
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A Single Sacral-Mounted Inertial Measurement Unit to Estimate Peak Vertical Ground Reaction Force, Contact Time, and Flight Time in Running by Aurélien Patoz, Thibault Lussiana, Bastiaan Breine, Cyrille Gindre, Davide Malatesta

“…Peak vertical ground reaction force (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>F</mi><mrow><mi>z</mi><mo>,</mo><mi>max</mi></mrow></msub></mrow></semantics></math></inline-formula>), contact time (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>t</mi><mi>c</mi></msub></mrow></semantics></math></inline-formula>), and flight time (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>t</mi><mi>f</mi></msub></mrow></semantics></math></inline-formula>) are key variables of running biomechanics. …”
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Numerical Simulation of the Hydrodynamic Performance and Self-Propulsion of a UUV near the Seabed by Xiaodong Liu, Yuli Hu, Zhaoyong Mao, Wenlong Tian

“…The <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>t</mi></semantics></math></inline-formula> and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>η</mi><mi>i</mi></msub></mrow></semantics></math></inline-formula> increase with the increasing of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>R</mi><msub><mi>e</mi><mi>L</mi></msub></mrow></semantics></math></inline-formula>, while <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>η</mi><mi>H</mi></msub></mrow></semantics></math></inline-formula> and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>w</mi></semantics></math></inline-formula> decrease with the increasing of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>R</mi><msub><mi>e</mi><mi>L</mi></msub></mrow></semantics></math></inline-formula>.…”
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Tuning Charge Order in (TMTTF)₂<i>X</i> by Partial Anion Substitution by Andrej Pustogow, Daniel Dizdarevic, Sebastian Erfort, Olga Iakutkina, Valentino Merkl, Gabriele Untereiner, Martin Dressel

“…Here, we investigate the charge-ordered state through partial substitution of the anions in (TMTTF)<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>2</mn></msub></semantics></math></inline-formula>[AsF<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>6</mn></msub></semantics></math></inline-formula>]<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mrow><mn>1</mn><mo>−</mo><mi>x</mi></mrow></msub></semantics></math></inline-formula>[SbF<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>6</mn></msub></semantics></math></inline-formula>]<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mi>x</mi></msub></semantics></math></inline-formula> with <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>x</mi><mo>≈</mo><mn>0.3</mn></mrow></semantics></math></inline-formula>, determined from the intensity of infrared vibrations, which is sufficient to suppress the spin-Peierls state. …”
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Moiré-like Superlattice Generated van Hove Singularities in a Strained CuO₂ Double Layer by Artem O. Sboychakov, Kliment I. Kugel, Antonio Bianconi

“…While it is known that the double-layer Bi<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>2</mn></msub></semantics></math></inline-formula>Sr<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>2</mn></msub></semantics></math></inline-formula>CaCu<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>2</mn></msub></semantics></math></inline-formula>O<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mrow><mn>8</mn><mo>+</mo><mi>y</mi></mrow></msub></semantics></math></inline-formula> (BSCCO) cuprate superconductor exhibits a one-dimensional (1D) incommensurate superlattice (IS), the effect of IS on the electronic structure remains elusive. …”
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X17: Status and Perspectives by Carlo Gustavino

“…Krasznahorkay observed an anomaly in the emission of electron–positron pairs in three different nuclear reactions, namely, the <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow><mspace width="-2.pt"></mspace><mo> </mo></mrow><mn>3</mn></msup></semantics></math></inline-formula>H(p,e<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow><mspace width="-2.pt"></mspace><mo> </mo></mrow><mo>−</mo></msup></semantics></math></inline-formula>e<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow><mspace width="-2.pt"></mspace><mo> </mo></mrow><mo>+</mo></msup></semantics></math></inline-formula>)<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow><mspace width="-2.pt"></mspace><mo> </mo></mrow><mn>4</mn></msup></semantics></math></inline-formula>He, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow><mspace width="-2.pt"></mspace><mo> </mo></mrow><mn>7</mn></msup></semantics></math></inline-formula>Li(p,e<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow><mspace width="-2.pt"></mspace><mo> </mo></mrow><mo>−</mo></msup></semantics></math></inline-formula>e<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow><mspace width="-2.pt"></mspace><mo> </mo></mrow><mo>+</mo></msup></semantics></math></inline-formula>)<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow><mspace width="-2.pt"></mspace><mo> </mo></mrow><mn>8</mn></msup></semantics></math></inline-formula>Be, and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow><mspace width="-2.pt"></mspace><mo> </mo></mrow><mn>11</mn></msup></semantics></math></inline-formula>B(p,e<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow><mspace width="-2.pt"></mspace><mo> </mo></mrow><mo>−</mo></msup></semantics></math></inline-formula>e<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow><mspace width="-2.pt"></mspace><mo> </mo></mrow><mo>+</mo></msup></semantics></math></inline-formula>)<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow><mspace width="-2.pt"></mspace><mo> </mo></mrow><mn>12</mn></msup></semantics></math></inline-formula>C processes. …”
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Centrally Extended Jordan (∗)-Derivations Centralizing Symmetric or Skew Elements by Amal S. Alali, Hafedh M. Alnoghashi, Nadeem ur Rehman

“…Let <i>A</i> be a non-commutative prime ring with involution <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mo>∗</mo><mo>,</mo></mrow></semantics></math></inline-formula> of characteristic <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mo>≠</mo><mn>2</mn><mspace width="3.33333pt"></mspace><mo>(</mo><mi>and</mi><mspace width="4.pt"></mspace><mn>3</mn><mo>)</mo><mo>,</mo></mrow></semantics></math></inline-formula> with <i>Z</i> as the center of <i>A</i> and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mo>Π</mo></semantics></math></inline-formula> a mapping <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mo>Π</mo><mo>:</mo><mi>A</mi><mo>→</mo><mi>A</mi></mrow></semantics></math></inline-formula> such that <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mo>[</mo><mo>Π</mo><mo>(</mo><mi>x</mi><mo>)</mo><mo>,</mo><mi>x</mi><mo>]</mo><mo>∈</mo><mi>Z</mi></mrow></semantics></math></inline-formula> for all (skew) symmetric elements <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>x</mi><mo>∈</mo><mi>A</mi><mo>.…”
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Performance of Quad Mass Gyroscope in the Angular Rate Mode by Sina Askari, Mohammad H. Asadian, Andrei M. Shkel

“…For the high Q-factor device of over 2 million, and uncompensated frequency asymmetry of 60 <inline-formula><math display="inline" xmlns="http://www.w3.org/1998/Math/MathML"><semantics><mi mathvariant="normal">m</mi></semantics></math></inline-formula><inline-formula><math display="inline" xmlns="http://www.w3.org/1998/Math/MathML"><semantics><mi>Hz</mi></semantics></math></inline-formula>, we demonstrated bias instability of <inline-formula><math display="inline" xmlns="http://www.w3.org/1998/Math/MathML"><semantics><mrow><mn>0.095</mn></mrow></semantics></math></inline-formula><inline-formula><math display="inline" xmlns="http://www.w3.org/1998/Math/MathML"><semantics><msup><mrow></mrow><mo>∘</mo></msup></semantics></math></inline-formula>/<inline-formula><math display="inline" xmlns="http://www.w3.org/1998/Math/MathML"><semantics><mi mathvariant="normal">h</mi></semantics></math></inline-formula>r and Angle Random Walk (ARW) of <inline-formula><math display="inline" xmlns="http://www.w3.org/1998/Math/MathML"><semantics><mrow><mn>0.0107</mn></mrow></semantics></math></inline-formula><inline-formula><math display="inline" xmlns="http://www.w3.org/1998/Math/MathML"><semantics><msup><mrow></mrow><mo>∘</mo></msup></semantics></math></inline-formula>/<inline-formula><math display="inline" xmlns="http://www.w3.org/1998/Math/MathML"><semantics><msqrt><mi mathvariant="normal">hr</mi></msqrt></semantics></math></inline-formula> in the OL mode of operation and bias instability of <inline-formula><math display="inline" xmlns="http://www.w3.org/1998/Math/MathML"><semantics><mrow><mn>0.065</mn></mrow></semantics></math></inline-formula><inline-formula><math display="inline" xmlns="http://www.w3.org/1998/Math/MathML"><semantics><msup><mrow></mrow><mo>∘</mo></msup></semantics></math></inline-formula>/<inline-formula><math display="inline" xmlns="http://www.w3.org/1998/Math/MathML"><semantics><mi mathvariant="normal">h</mi></semantics></math></inline-formula>r and ARW of <inline-formula><math display="inline" xmlns="http://www.w3.org/1998/Math/MathML"><semantics><mrow><mn>0.0058</mn></mrow></semantics></math></inline-formula><inline-formula><math display="inline" xmlns="http://www.w3.org/1998/Math/MathML"><semantics><msup><mrow></mrow><mo>∘</mo></msup></semantics></math></inline-formula>/<inline-formula><math display="inline" xmlns="http://www.w3.org/1998/Math/MathML"><semantics><msqrt><mi mathvariant="normal">hr</mi></msqrt></semantics></math></inline-formula> in the FRB mode of operation. …”
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Electronic Structures of Kitaev Magnet Candidates RuCl₃ and RuI₃ by Subhasis Samanta, Dukgeun Hong, Heung-Sik Kim

“…<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>α</mi></semantics></math></inline-formula>-RuCl<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>3</mn></msub></semantics></math></inline-formula> has been the most promising candidate, and there have been several reports on the realization of sibling compounds <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>α</mi></semantics></math></inline-formula>-RuBr<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>3</mn></msub></semantics></math></inline-formula> and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>α</mi></semantics></math></inline-formula>-RuI<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>3</mn></msub></semantics></math></inline-formula> with the same crystal structure. …”
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Numerical and Experimental Analysis of Vortex Profiles in Gravitational Water Vortex Hydraulic Turbines by Laura Velásquez, Ainhoa Rubio-Clemente, Edwin Chica

“…This work compared the suitability of the k-<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>ϵ</mi></semantics></math></inline-formula> standard, k-<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>ϵ</mi></semantics></math></inline-formula> RNG, k-<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>ω</mi></semantics></math></inline-formula> SST, and k-<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>ω</mi></semantics></math></inline-formula> standard turbulence models for simulating a gravitational water vortex hydraulic turbine using ANSYS Fluent. …”
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On Two-Stage Guessing by Robert Graczyk, Igal Sason

“…Stationary memoryless sources produce two correlated random sequences <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mi>X</mi><mi>n</mi></msup></semantics></math></inline-formula> and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mi>Y</mi><mi>n</mi></msup></semantics></math></inline-formula>. …”
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