Results for '$${{\lambda}{\rho}}$$ λ ρ -calculus'

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  1.  68
    Argos and the argolid A. pariente, G. touchais (edd.); 'A[rho][gamma][omicron][final small sigma] [kappa][alpha][iota, accent] a[rho][gamma][omicron][lambda][delta][alpha]: Τo[pi]o[gamma][rho][alpha][phi][iota, accent][alpha] [kappa][alpha][iota] [pi]o[lambda][epsilon]o[delta]o[mu][iota, accent][alpha] /argos et l'argolide: Topographie et histoire. ( [Pi][rho][alpha][kappa]τ[iota][kappa][alpha, accent] [delta][iota][epsilon][theta][nu][omicron][upsilon, accent][final small sigma] [sigma][upsilon][nu][epsilon][delta][rho][iota, accent][omicron][upsilon] /actes de la table ronde internationale, a[theta][eta, accent][nu][alpha]–'a[rho][gamma][omicron][final small sigma] 28/4–1/5/1990 athènes–argos). (E[lambda][lambda][eta][nu][omicron][gamma][alpha][lambda][lambda][iota][kappa][epsilon, accent][final small sigma] [epsilon, accent][rho][epsilon][upsilon][nu][epsilon][final small sigma] /recherches Franco-helléniques, 3.) pp. XIV + 507, text figs, 14 pls, 9 overlays, 2 foldout plans. Nafpli. [REVIEW]Graham Shipley - 2000 - The Classical Review 50 (02):550-.
  2.  65
    Z. Bonias: '[Epsilon, accent][nu][alpha] [alpha][gamma][rho][omicron][tau][iota][kappa][omicron, accent] [iota][epsilon][rho][omicron, accent] [sigma][tau][iota][final small sigma] A[iota][gamma][iota][epsilon, accent][final small sigma] [Lambda][alpha][kappa][omega][nu][iota, accent][alpha][final small sigma] ( [Delta]η[mu][omicron][sigma][iota][epsilon][upsilon, accent][mu][alpha][tau][alpha] [tau][omicron][upsilon] [alpha][rho][chi][alpha][iota][omicron][lambda][omicron][gamma][iota][kappa][omicron][upsilon, accent] [delta][epsilon][lambda][tau][iota, accent][omicron][upsilon] , 62). Pp. 230, 67 pls. Athens: Ypourgeio Politismou, 1998. Price: drs 10,000. ISBN: 960-214-190-5 (ISSN: 1108-1244). [REVIEW]Graham Shipley - 2000 - The Classical Review 50 (02):663-.
  3.  25
    Wormholes Within the Framework of f(R,T)=R+αR2+λT\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$f(R, T)=R+\alpha R^2+\lambda T$$\end{document} Gravity. [REVIEW]Ambuj Kumar Mishra & Umesh Kumar Sharma - 2021 - Foundations of Physics 51 (2):1-16.
    In this work, we explore modeling of wormholes in framework of f(R, T) gravity with the functional form f(R,T)=R+αR2+λT\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$f(R, T)= R+\alpha R^2 +\lambda T$$\end{document}, where R and T are the Ricci scalar and trace of energy-momentum tensor respectively, α\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\alpha$$\end{document} and λ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\lambda$$\end{document} are arbitrary constants. Using the equation of state (EoS) pr=ωρ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} (...))
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  4. Truth's Harmony in Plato's Musical Cosmos.Douglas V. Henry - 1996 - Dissertation, Vanderbilt University
    Plato provocatively characterizes truth $$ in terms of harmony $$ at various points throughout his dialogues. While limited attention has been directed toward the role of musical concepts in Plato's general cosmology, not any attention has been directed toward how musical concepts function in relation to Plato's characterization of truth. In fact, this issue has had little occasion for consideration. Almost every contemporary translator empties terms such as $\grave\alpha\rho\mu o\nu\acute\iota\alpha,$ when co-incidental with $\acute\alpha\lambda\acute\eta\theta\varepsilon\iota\alpha,$ of their musical content. As a consequence, (...)
     
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  5.  29
    Negative Größen bei Diophant? Teil II.Klaus Barner - 2007 - NTM Zeitschrift für Geschichte der Wissenschaften, Technik und Medizin 15 (2):98-117.
    In this second part of “Negative Größen bei Diophant?” we start, as announced, by giving 33 places where Diophantus uses negative quantities as intermediate results; they appear as differences a − b of positive rational numbers, the subtrahend b being bigger than the minuend a; they each represent the (negative) basis $(\pi\lambda\varepsilon\upsilon\rho\acute{\alpha})$ of a square number $(\tau\varepsilon\tau\rho\acute{\alpha}\gamma\omega\nu o \zeta)$ , which is afterwards computed by the formula (a - b)2 = a 2 + b 2 - 2ab. Finally, we report (...)
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  6. Epicurus' Libertarian Atomism.Jeffrey Stephen Purinton - 1992 - Dissertation, Princeton University
    My dissertation is concerned with Epicurus' attempt to reconcile libertarianism and atomism. I begin by offering my solution to 'the problem of the swerve,' arguing that Lucretius is claiming that swerves cause volitions 'from the bottom up' and that the attempts of scholars to construct a better position for Epicurus to have held were doomed to fail, since this is the only position open to the libertarian atomist. ;I also examine the swerve's role in cosmogony, arguing that 'the cosmogonic argument' (...)
     
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  7.  91
    The Extended Relativity Theory in Born-Clifford Phase Spaces with a Lower and Upper Length Scales and Clifford Group Geometric Unification.Carlos Castro - 2005 - Foundations of Physics 35 (6):971-1041.
    We construct the Extended Relativity Theory in Born-Clifford-Phase spaces with an upper R and lower length λ scales (infrared/ultraviolet cutoff). The invariance symmetry leads naturally to the real Clifford algebra Cl (2, 6, R) and complexified Clifford Cl C (4) algebra related to Twistors. A unified theory of all Noncommutative branes in Clifford-spaces is developed based on the Moyal-Yang star product deformation quantization whose deformation parameter involves the lower/upper scale $$(\hbar \lambda / R)$$. Previous work led us to show from (...)
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  8.  26
    Canonical quantization of a nonrelativistic singular quasilinear system.T. Kawai - 1977 - Foundations of Physics 7 (3-4):185-204.
    Following Dirac's generalized canonical formalism, we develop a quantization scheme for theN-dimensional system described by the Lagrangian $L_0 (\dot y,y) = \frac{1}{2}h_{ij} (y)\dot y^i \dot y^j + b_i (y)\dot y^i - w(y)$ which is supposed to be invariant under the gauge transformation $y^i \to y\prime ^i = y^i + (\rho ^i _\alpha + \sigma ^i _{\alpha j} \dot y^j )\delta \Lambda ^\alpha + \tau ^i _\alpha \delta \dot \Lambda ^\alpha$ . The gauge invariance necessarily implies that the Lagrangian is singular. (...)
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