Książki: „Phase function”

1

Fung, Amy D. A novel function of the S phase regulator Dfp1. Ottawa: National Library of Canada, 2002.

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2

Kim, Y. S., i W. W. Zachary, red. The Physics of Phase Space Nonlinear Dynamics and Chaos Geometric Quantization, and Wigner Function. Berlin, Heidelberg: Springer Berlin Heidelberg, 1987. http://dx.doi.org/10.1007/3-540-17894-5.

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Simon, M. Steady-state probability density function of the phase error for a DPLL with an integrate-and-dump device. Pasadena, Calif: National Aeronautics and Space Administration, Jet Propulsion Laboratory, California Institute of Technology, 1986.

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4

Flamm, David S. Progress on H optimal sensitivity for delay systems. Part I: Minimum phase plant with input delay. l pole/zero weighting function. Cambridge, Mass: Massachusetts Institute of Technology, Laboratory for Information and Decision Systems, 1985.

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5

Hurley, Graham Robert Bruce. The effect of development and function on muscle moment power during the recovery phase of running for girls 9 to 17 years. Sudbury, Ont: Laurentian University, 1987.

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Asano, David Ken. Phase smoothing functions for continuous phase modulation. Ottawa: National Library of Canada, 1990.

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S, Kim Y., i Zachary W. W. 1935-, red. The physics of phase space: Nonlinear dynamics and chaos, geometric quantization, and Wigner function : proceedings of the First International Conference on the Physics of Phase Space, held at the University of Maryland, College Park, Maryland, May 20-23, 1986. Berlin: Springer-Verlag, 1987.

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8

Wegert, Elias. Visual Complex Functions: An Introduction with Phase Portraits. Basel: Springer Basel, 2012.

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Zhang, H. Unwrapping the phase response functions for nonlinear systems. Sheffield: University ofSheffield, Dept. of Automatic Control and Systems Engineering, 1992.

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Borovikov, V. A. Uniform stationary phase method. London: Institution of Electrical Engineers, 1994.

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García Velasco, Daniel, i Jan Rijkhoff, red. The Noun Phrase in Functional Discourse Grammar. Berlin, New York: Mouton de Gruyter, 2008. http://dx.doi.org/10.1515/9783110205374.

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Ebata, Takayuki, i Masaaki Fujii, red. Physical Chemistry of Cold Gas-Phase Functional Molecules and Clusters. Singapore: Springer Singapore, 2019. http://dx.doi.org/10.1007/978-981-13-9371-6.

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Pavlov, Sergey. Methods of catastrophe theory in the phenomenology of phase transitions. ru: INFRA-M Academic Publishing LLC., 2020. http://dx.doi.org/10.12737/1004276.

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The monograph is devoted to describing the methods of catastrophe theory and building on the basis of these methods, phenomenological models of phase transitions in solids. Methods of constructing structurally stable normal forms of functions, including functions that are imposed on the symmetry conditions. The classification of phenomenological models of phase transitions for two interacting one-component order parameter, two-component and three-component order parameters the number of control parameters varied in the experiment. Theoretical dependence of the anomalies of the physical properties of the models are compared with experimental data in ferroelectrics, magnetic materials, solid solutions of rare earth metals, multiferroics and other solids that are experiencing phase transitions. For professionals in the field of solid state physics and phase transitions.

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service), SpringerLink (Online, red. Functional Renormalization and Ultracold Quantum Gases. Berlin, Heidelberg: Springer-Verlag Berlin Heidelberg, 2010.

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Kopestyńska, Zofia. A dictionary of language functions =: Słownik funkcji językowych. Warszawa: Poltext, 1991.

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Third person references: Forms and functions in two spoken genres of Spanish. Amsterdam: John Benjamins Publishing Company, 2016.

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Iwashita, Mami. Being affected: the meanings and functions of Japanese passive constructions. München: Lincom Europa, 2007.

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Lin, Ji Hai. A functional guide to English conversation 2. Hong Kong: Wan Li, 2001.

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Lin, Ji Hai. A functional guide to English conversation 1. Hong Kong: Wan Li, 2001.

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Ströbel, Liane. Auf den Spuren der Entstehung einer neuen Kategorie: Leerverben als paralleler Kopulastrang. Frankfurt am Main: Peter Lang, 2010.

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21

Ferrer-Hanreddy, Jami. Mosaic one: With learning strategies and language functions. Wyd. 3. New York: McGraw-Hill, 1996.

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22

Narendra. Saṃskr̥tasya vyāvahārikasvarūpam =: Functional Sanskrit, its communicative aspects. Puduccerī: Saṃskr̥takāryālayaḥ, Śrīaravindāśramaḥ, 1996.

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23

Bartnik, Artur. Noun phrase structure in Old English: Quanitfiers and other functional categories. Lublin: Wydawn. KUL, 2011.

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The syntax of Hungarian noun phrases: A lexical-functional approach. Frankfurt am Main: P. Lang, 1995.

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25

Basic Spanish conversation: A functional approach. Lincolnwood, Ill., USA: National Textbook Co., 1985.

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26

United Christian Council (Sierra Leone). Provincial Literature Bureau. Community advancement programme (Project CAP phase II): A functional literacy programme : an interim progress report, January-June, 1987. Bo, Sierra Leone: U.C.C. Literature Bureau, 1987.

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27

EOSAEL92 Aerosol Phase Function Data Base PFNDAT. Storming Media, 1997.

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28

Bilateral lower extremity function during the support phase of running. 1990.

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Bilateral lower extremity function during the support phase of running. 1989.

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30

Pomey, Patrice. Defining a Ship: Architecture, Function, and Human Space. Redaktorzy Ben Ford, Donny L. Hamilton i Alexis Catsambis. Oxford University Press, 2012. http://dx.doi.org/10.1093/oxfordhb/9780199336005.013.0001.

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This article is an introduction to the concept of maritime archaeology. In the field of archaeology, the study of a shipwreck endeavors to reconstitute the original ship. Thus, nautical archaeology belongs to the larger domain of maritime archaeology. The study of shipboard artifacts and cargo comes before a structural analysis is possible. Therefore, one must know how to anticipate the expected results in order to take into consideration the ensemble of data. A ship is an assembly of elements closely linked together, which express their true role in their relation to the whole. This article explains the conception phase. Several operations are necessary to achieve construction of a ship. The conception phase must then lead to a realization phase. The realization phase must materialize, with the help of diverse processes or methods, the construction principles chosen for the structural and shape concept of the ship.

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31

Kim, Young S., i Woodford W. Zachary. The Physics of Phase Space: Nonlinear Dynamics and Chaos, Geometric Quantization, and Wigner Function. Springer, 2014.

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32

Sargent, Eva Lee. The effects of intraluteal infusion of prostaglandin-synthesis inhibitors on the function of the primate corpus luteum. 1988.

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33

Mann, Peter. Hamilton’s Principle in Phase Space. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198822370.003.0015.

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This chapter derives Hamilton’s equations using the Legendre transform and the definition of the Hamiltonian function. While, in the Newtonian formalism, conservation laws were rather difficult to tease out, the Lagrangian formalism revolutionised the way of looking at them; however, the Hamiltonian formalism is perhaps even simpler than the Lagrangian formalism, making it straightforward to identify conservation laws and the symmetries of the system associated with each conserved property. In this chapter, the Hamiltonian is treated as being explicitly dependent on time, as this form is more general and will lead to an important relation that, although not an equation of motion, is still useful to discuss. The chapter also introduces Routhian mechanics as a symplectic reduction technique, using integrals of the motion.

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34

Mann, Peter. The Hamiltonian & Phase Space. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198822370.003.0014.

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This chapter discusses the Hamiltonian and phase space. Hamilton’s equations can be derived in several ways; this chapter follows two pathways to arrive at the same result, thus giving insight into the motivation for forming these equations. The importance of deriving the same result in several ways is that it shows that, in physics, there are often several mathematical avenues to go down and that approaching a problem with, say, the calculus of variations can be entirely as valid as using a differential equation approach. The chapter extends the arenas of classical mechanics to include the cotangent bundle momentum phase space in addition to the tangent bundle and configuration manifold, and discusses conjugate momentum. It also introduces the Hamiltonian as the Legendre transform of the Lagrangian and compares it to the Jacobi energy function.

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35

Felger, Jennifer C., Ebrahim Haroon i Andrew H. Miller. Inflammation and Immune Function in PTSD. Redaktorzy Israel Liberzon i Kerry J. Ressler. Oxford University Press, 2016. http://dx.doi.org/10.1093/med/9780190215422.003.0013.

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Numerous reports have described an association between PTSD and alterations in the immune response primarily characterized by increased biomarkers of inflammation, including inflammatory cytokines and acute phase reactants as well as increased inflammatory responses to immune stimuli. When considering systems that evolved to protect and prepare organisms during challenge, it is not surprising that the immune system is affected by exposure to trauma, or to the chronic stress associated with PTSD symptoms. Conversely, inflammatory cytokines have been shown to affect the brain, and may influence neural circuits of fear and anxiety to contribute to PTSD symptoms. This chapter discusses the evolutionary legacy of a primed inflammatory response in the context of trauma and stress, examines the evidence of altered immune function and inflammation in PTSD, explores the potential mechanisms involved, characterizes the consequences on neurocircuitry and health, and discusses potential translational implications.

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36

Horing, Norman J. Morgenstern. Random Phase Approximation Plasma Phenomenology, Semiclassical and Hydrodynamic Models; Electrodynamics. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198791942.003.0010.

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Chapter 10 reviews both homogeneous and inhomogeneous quantum plasma dielectric response phenomenology starting with the RPA polarizability ring diagram in terms of thermal Green’s functions, also energy eigenfunctions. The homogeneous dynamic, non-local inverse dielectric screening functions (K) are exhibited for 3D, 2D, and 1D, encompassing the non-local plasmon spectra and static shielding (e.g. Friedel oscillations and Debye-Thomas-Fermi shielding). The role of a quantizing magnetic field in K is reviewed. Analytically simpler models are described: the semiclassical and classical limits and the hydrodynamic model, including surface plasmons. Exchange and correlation energies are discussed. The van der Waals interaction of two neutral polarizable systems (e.g. physisorption) is described by their individual two-particle Green’s functions: It devolves upon the role of the dynamic, non-local plasma image potential due to screening. The inverse dielectric screening function K also plays a central role in energy loss spectroscopy. Chapter 10 introduces electromagnetic dyadic Green’s functions and the inverse dielectric tensor; also the RPA dynamic, non-local conductivity tensor with application to a planar quantum well. Kramers–Krönig relations are discussed. Determination of electromagnetic response of a compound nanostructure system having several nanostructured parts is discussed, with applications to a quantum well in bulk plasma and also to a superlattice, resulting in coupled plasmon spectra and polaritons.

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37

Steady-state probability density function of the phase error for a DPLL with an integrate-and-dump device. Pasadena, Calif: National Aeronautics and Space Administration, Jet Propulsion Laboratory, California Institute of Technology, 1986.

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38

Steady-state probability density function of the phase error for a DPLL with an integrate-and-dump device. Pasadena, Calif: National Aeronautics and Space Administration, Jet Propulsion Laboratory, California Institute of Technology, 1986.

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39

J, Mileant, i Jet Propulsion Laboratory (U.S.), red. Steady-state probability density function of the phase error for a DPLL with an integrate-and-dump device. Pasadena, Calif: National Aeronautics and Space Administration, Jet Propulsion Laboratory, California Institute of Technology, 1986.

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40

Stage loading versus progressive loading in cardiac rehabilitation functional evaluation: Comparison of the Bruce and Roy ramp treadmill protocols on post-Phase II CAD patients. 1995.

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Stage loading versus progressive loading in cardiac rehabilitation functional evaluation: Comparison of the Bruce and Roy ramp treadmill protocols on post-Phase II CAD patients. 1995.

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42

Stage loading versus progressive loading in cardiac rehabilitation functional evaluation: Comparison of the Bruce and Roy ramp treadmill protocols on post-Phase II CAD patients. 1995.

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43

Vimalesvaran, Kavitha, i Michael Marber. Myocardial Remodelling after Myocardial Infarction. Oxford University Press, 2014. http://dx.doi.org/10.1093/med/9780199653461.003.0031.

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This chapter focuses on myocardial remodelling, a process that affects the heart’s shape, structure, and function, following myocardial injury (MI). Post-MI remodelling can be divided into three phases, with the first phase 0–72 hours beginning at the time of ischaemic injury, the second phase 72 hours to 6 weeks, and the third and last phase 6 weeks and beyond. During post-infarction remodelling, hypertrophy is an adaptive response that compensates for the increased load, reduces the effect of progressive dilatation, and balances contractile function. The chapter discusses the factors involved in ventricular remodelling and its association with heart failure progression. The effects of therapies designed to prevent or attenuate post-infarction left ventricular remodelling, with reference to the pathophysiological mechanisms involved, are then considered. Therapies specifically discussed include angiotensin-converting enzyme (ACE) inhibitors, angiotensin receptor blockers (ARBs), β‎-adrenoreceptor blockers, and aldosterone receptor antagonists.

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44

Ackland, Gareth L. Neural and endocrine function in the immune response to critical illness. Oxford University Press, 2016. http://dx.doi.org/10.1093/med/9780199600830.003.0310.

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The neurohormonal physiological response to various stressors is pivotal for maintaining homeostasis. However, the advent of modern critical care has distorted evolutionary biology by generating the entirely new (patho)physiological entity of critical illness. By extending the biological features of the ‘fight or flight’ response beyond the acute phase, distinct neurohormonal, and immune profiles have become increasingly apparent. Both direct and off-target effects of neurohormonal control on immune function are implicated in the disruption of bidirectional links between neurohormones and immune effectors that limit organ dysfunction. Iatrogenic factors introduced by critical care therapy may exacerbate neurohormonal dysregulation, further distorting the biology of the ‘fight or flight’ response. Neural mechanisms underlying this newly-characterized clinical syndrome remain poorly understood. Furthermore, the same neurohormonal responses are chronically dysregulated in pre-existing comorbidities diseases associated with an increased risk of sepsis, multi-organ failure and critical illness. Off-target local immune effects may explain the failure of clinical trials aimed at altering systemic neurohormonal physiology. Recent laboratory and translational human clinical studies, particularly in diseases characterized by chronic neurohormonal dysregulation, have provided new insights into the possibility of therapeutic interventions that could minimize the pathophysiological features of critical illness.

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45

Horing, Norman J. Morgenstern. Non-Equilibrium Green’s Functions: Variational Relations and Approximations for Particle Interactions. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198791942.003.0009.

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Chapter 09 Nonequilibrium Green’s functions (NEGF), including coupled-correlated (C) single- and multi-particle Green’s functions, are defined as averages weighted with the time-development operator U(t0+τ,t0). Linear conductivity is exhibited as a two-particle equilibrium Green’s function (Kubo-type formulation). Admitting particle sources (S:η,η+) and non-conservation of number, the non-equilibrium multi-particle Green’s functions are constructed with numbers of creation and annihilation operators that may differ, and they may be derived as variational derivatives with respect to sources η,η+ of a generating functional eW=TrU(t0+τ,t0)CS/TrU(t0+τ,t0)C. (In the non-interacting case this yields the n-particle Green’s function as a permanent/determinant of single-particle Green’s functions.) These variational relations yield a symmetric set of multi-particle Green’s function equations. Cumulants and the Linked Cluster Theorem are discussed and the Random Phase Approximation (RPA) is derived variationally. Schwinger’s variational differential formulation of perturbation theories for the Green’s function, self-energy, vertex operator, and also shielded potential perturbation theory, are reviewed. The Langreth Algebra arises from analytic continuation of integration of products of Green’s functions in imaginary time to the real-time axis with time-ordering along the integration contour in the complex time plane. An account of the Generalized Kadanoff-Baym Ansatz is presented.

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46

Mann, Peter. Hamilton-Jacobi Theory. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198822370.003.0019.

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This chapter focuses on Liouville’s theorem and classical statistical mechanics, deriving the classical propagator. The terms ‘phase space volume element’ and ‘Liouville operator’ are defined and an n-particle phase space probability density function is constructed to derive the Liouville equation. This is deconstructed into the BBGKY hierarchy, and radial distribution functions are used to develop n-body correlation functions. Koopman–von Neumann theory is investigated as a classical wavefunction approach. The chapter develops an operatorial mechanics based on classical Hilbert space, and discusses the de Broglie–Bohm formulation of quantum mechanics. Partition functions, ensemble averages and the virial theorem of Clausius are defined and Poincaré’s recurrence theorem, the Gibbs H-theorem and the Gibbs paradox are discussed. The chapter also discusses commuting observables, phase–amplitude decoupling, microcanonical ensembles, canonical ensembles, grand canonical ensembles, the Boltzmann factor, Mayer–Montroll cluster expansion and the equipartition theorem and investigates symplectic integrators, focusing on molecular dynamics.

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47

Chance, Kelly, i Randall V. Martin. Atmospheric Scattering. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780199662104.003.0007.

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This chapter describes elastic scattering events, where the wavelength of the scattered light is unchanged from that of the incident light and conservative scattering, scattering without absorption, sometimes closely approximated in clouds. The scattering regime, scattering versus wavelengths and scatterer size are introduced. Polarization in scattering is described by the Stokes vector and the polarization ellipse. Molecular (Rayleigh) scattering is presented and its atmospherically-important inelastic component, Raman scattering (the Ring effect) quantified. Mie scattering for spherical particles is described as is the commonly-used Henyey-Greenstein Mie phase function approximation. Non-spherical scatterers are introduced. The Ångstrom exponent and the expansion of phase functions in Legendre polynomials are described.

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48

Mann, Peter. Noether’s Theorem for Fields. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198822370.003.0028.

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This is a unique chapter that discusses classical path integrals in both configuration space and phase space. It examines both Lagrangian and Hamiltonian formulations before qualitatively discussing some interesting features of gauge fixing. This formulation is then linked to superspace and Grassmann variables for a fermionic field theory. The chapter then shows that the corresponding operatorial formulation is none other than the Koopman–von Neumann theory. In parallel to quantum theory, the classical propagator or the transition amplitude between two classical states is given exactly by the phase space partition function. The functional Dirac delta is discussed, and the chapter closes by briefly mentioning Faddeev–Popov ghosts, which were introduced earlier in the chapter.

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Veas, Francisco, red. Acute Phase Proteins - Regulation and Functions of Acute Phase Proteins. InTech, 2011. http://dx.doi.org/10.5772/756.

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Golper, Thomas A., Andrew A. Udy i Jeffrey Lipman. Drug dosing in acute kidney injury. Redaktor William G. Bennett. Oxford University Press, 2015. http://dx.doi.org/10.1093/med/9780199592548.003.0364.

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Drug dosing in acute kidney injury (AKI) is one of the broadest topics in human medicine. It requires an understanding of markedly altered and constantly changing physiology under many disease situations, the use of the drugs to treat those variety of diseases, and the concept of drug removal during blood cleansing therapies. Early in AKI kidney function may be supraphysiologic, while later in the course there may be no kidney function. As function deteriorates other metabolic pathways are altered in unpredictable ways. Furthermore, the underlying disorders that lead to AKI alter metabolic pathways. Heart failure is accompanied by vasoconstriction in the muscle, skin and splanchnic beds, while brain and cardiac blood flow proportionally increase. Third spacing occurs and lungs can become congested. As either kidney or liver function deteriorates, there may be increased or decreased drug sensitivity at the receptor level. Acidosis accompanies several failing organs. Protein synthesis is qualitatively and quantitatively altered. Sepsis affects tissue permeability. All these abnormalities influence drug pharmacokinetics and dynamics. AKI is accompanied by therapeutic interventions that alter intrinsic metabolism which is in turn complicated by kidney replacement therapy (KRT). So metabolism and removal are both altered and constantly changing. Drug management in AKI is exceedingly complex and is only beginning to be understood. Thus, we approach this discussion in a physiological manner. Critically ill patients pass through phases of illness, sometimes rapidly, other times slowly. The recognition of the phases and the need to adjust medication administration strategies is crucial to improving outcomes. An early phase involving supraphysiologic kidney function may be contributory to therapeutic failures that result in the complication of later AKI and kidney function failure.

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