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  1. 81
  2. 82

    EFECTO DEL MÉTODO DE ESTIRAMIENTO PNF Y ESTÁTICO EN LA MEJORA DE LA FLEXIBILIDAD DE LA ARTICULACIÓN DE LA CADERA EN PRACTICANTES DE KUNG FU by Juan Diego Zamora Salas, Wálter Salazar Rojas

    Published 2001-12-01
    “…El presente estudio analizó el efecto de dos métodos de estiramiento (estático y P.N.F.) para mejorar el rango de movimiento en la articulación de la cadera en practicantes de Kung Fu Wing Chun, utilizando una prueba de flexibilidad de cadera. …”
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  3. 83
  4. 84

    A Deconstruction Lattice Description of the D1/D5 Brane World-Volume Gauge Theory by Joel Giedt

    Published 2011-01-01
    “…I specialize to a particularly interesting (4,4) gauge theory, with gauge group U ( N c ) × U ( N f ) , and U ( N f ) being weakly gauged. …”
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  5. 85

    Studying the Attribution of LiF in OLED by the 𝐶-𝑉 Characteristics by Chun-lin Zhang, Fang-cong Wang, Yong Zhang, Hai-xia Li, Su Liu

    Published 2010-01-01
    “…We used the 𝐶-𝑉 characteristics to investigate the contribution of LiF in OLED and found that the capacitance of the above-mentioned structures was 12.5 nF and 77.5 nF, respectively. It is shown that the LiF layer affects the property of OLED resulting in the change of the capacitance of the device.…”
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  6. 86

    Оцінки похибок наближення класів неперервних диференційованих функцій ламаними by Олександр Щитов, Микола Мормуль

    Published 2024-06-01
    “… У метриках неперервних та неспадних функцій φ(x) отримано наступне: а) оцінки апроксимації класів 1-періодичних функцій W^(2ν+1) Hω* (ν ∈ N), де ω(t) є вверхньою опуклою модулем неперервності, та інтерполяція функцій f(t) ∈ W^(2ν+1) Hω*; б) за допомогою кусково-сталих функцій σ_n (f,t) в інтегральній метриці L_p (0 < p < ∞); в) за допомогою кусково-сталих функцій σ_n (f,t) в однообразній метриці. …”
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  7. 87
  8. 88

    A note on global existence for boundary value problems by Chuan J. Chyan, Johnny Henderson

    Published 1989-01-01
    “…Upper and lower solutions are used in establlsning global existence results for certain two–point boundary value problems for y‴=f(x,y,y′,y″) and y(n)=f(x,y,y′,...,y(n−1)).…”
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  9. 89

    NNLO PDFs driven by top-quark data by S. Alekhin, M. V. Garzelli, S.-O. Moch, O. Zenaiev

    Published 2025-02-01
    “…At NNLO in QCD we obtain for the strong coupling the value $$\alpha _s^{(n_f=5)}(M_Z)= 0.1150 \pm 0.0009$$ α s ( n f = 5 ) ( M Z ) = 0.1150 ± 0.0009 and for the top-quark mass in the $${\overline{\text{ MS }}}$$ MS ¯ -scheme $$m_t(m_t) = 160.6 \pm 0.6$$ m t ( m t ) = 160.6 ± 0.6  GeV, corresponding to $$m_t^\textrm{pole} = 170.2 \pm 0.7$$ m t pole = 170.2 ± 0.7  GeV in the on-shell scheme. …”
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  10. 90

    Some characterizations of specially multiplicative functions by Pentti Haukkanen

    Published 2003-01-01
    “…A multiplicative function f is said to be specially multiplicative if there is a completely multiplicative function fA such that f(m)f(n)=∑d|(m,n)f(mn/d2)fA(d) for all m and n. For example, the divisor functions and Ramanujan's τ-function are specially multiplicative functions. …”
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  11. 91

    大鼠外伤性脑干损伤脑干的双重免疫组化及超微病理研究 by 周 伟 徐小虎 祝家镇

    Published 1997-01-01
    “…摘 要 报告建立大鼠外伤性脑干损伤模型,并以死后脑干伤作对照,用神经微丝( neu rof ilament , N F)及 胶质纤维酸性蛋白( gli al f ib ril lary acidic protein, GFAP)双重免疫组化染色观察了脑干神经轴索及星形胶质细 胞的变化,且对轴索的直径和星形胶质细胞数进行了图像分析及统计处理。…”
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  12. 92

    Separation of infrared and bulk in thermal QCD by The χQCD collaboration and the CLQCD collaboration, Xiao-Lan Meng, Peng Sun, Andrei Alexandru, Ivan Horváth, Keh-Fei Liu, Gen Wang, Yi-Bo Yang

    Published 2024-12-01
    “…Abstract A new thermal regime of QCD, featuring decoupled scale-invariant infrared glue, has been proposed to exist both in pure-glue (N f =0) and “real-world” (N f =2+1 at physical quark masses) QCD. …”
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  13. 93
  14. 94

    Variation of constants formulae for difference equations with advanced arguments by Lolimar Díaz, Raúl Naulin

    Published 2000-01-01
    “…The construction of a variation of constants formula for the difference equation with advanced arguments y(n+1)=A(n)y(n)+B(n)y(g(n))+f(n), g(n)≥n+1, is given for specific sequential spaces.…”
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  15. 95

    Integral-Type Operators from Bloch-Type Spaces to QK Spaces by Stevo Stević, Ajay K. Sharma

    Published 2011-01-01
    “…The boundedness and compactness of the integral-type operator Iφ,g(n)f(z)=∫0zf(n)(φ(ζ))g(ζ)dζ, where n∈N0, φ is a holomorphic self-map of the unit disk D, and g is a holomorphic function on D, from α-Bloch spaces to QK spaces are characterized.…”
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  16. 96

    Schur m-Power Convexity of a Class of Multiplicatively Convex Functions and Applications by Wen Wang, Shiguo Yang

    Published 2014-01-01
    “…We investigate the conditions under which the symmetric functions Fn,k(x,r)=∏1≤i1<i2<⋯<ik≤n ‍f(∑j=1k‍xijr)1/r,  k=1,2,…,n, are Schur m-power convex for x∈R++n and r>0. …”
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  17. 97

    Oscillation of certain partial difference equations by Sung Kyu Choi, Bing Gen Zhang

    Published 1998-01-01
    “…Next, we establish a linearized oscillation result for the nonlinear partial difference equation Am+1,n+1+Am+1,n+Am,n+1−Am,n+Pm,n f(Am−k,n−l)=0.…”
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  18. 98

    A Regularized Gradient Projection Method for the Minimization Problem by Yonghong Yao, Shin Min Kang, Wu Jigang, Pei-Xia Yang

    Published 2012-01-01
    “…We investigate the following regularized gradient projection algorithm xn+1=Pc(I−γn(∇f+αnI))xn, n≥0. Under some different control conditions, we prove that this gradient projection algorithm strongly converges to the minimum norm solution of the minimization problem minx∈Cf(x).…”
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  19. 99

    Anatomical Covariance Analysis: Detection of Disrupted Correlation Network Related to Clinical Trait Fatigue in Multiple Sclerosis: A Pilot Study by Rosalia Dacosta-Aguayo, Glenn Wylie, John DeLuca, Helen Genova

    Published 2020-01-01
    “…PwMS were stratified into nonclinical fatigue (nF-MS, FSS≤4.0) (n=10) and clinical fatigue (F-MS, FSS≥5.0) (n=10). …”
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  20. 100

    k-component disconjugacy for systems of ordinary differential equations by Johnny Henderson

    Published 1986-01-01
    “…Disconjugacy of the kth component of the mth order system of nth order differenttal equations Y(n)=f(x,Y,Y′,…,Y(n−1)), (1.1), is defined, where f(x,Y1,…,Yn), ∂f∂yij(x,Y1,…,Yn):(a,b)×Rmn→Rm are continuous. …”
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