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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., and W. W. Zachary, eds. 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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3

F, Naftolin, and DeCherney Alan H, eds. The Control of follicle development, ovulation, and luteal function: Lessons from in vitro fertilization. New York: Raven Press, 1987.

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4

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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5

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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6

J, Mileant, and Jet Propulsion Laboratory (U.S.), eds. 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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7

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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8

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

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9

S, Kim Y., and Zachary W. W. 1935-, eds. 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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10

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

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11

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

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12

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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13

García Velasco, Daniel, and Jan Rijkhoff, eds. 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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14

Daniel, García Velasco, and Rijkhoff Jan, eds. The noun phrase in functional discourse grammar. New York: Mouton de Gruyter, 2008.

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15

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

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16

Ebata, Takayuki, and Masaaki Fujii, eds. 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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17

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

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18

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

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19

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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20

R, Powell Michael, and Environmental Physiology/Biophysics Laboratory (Lyndon B. Johnson Space Center), eds. Project ARGO: Gas phase formation in simulated microgravity. [Houston, Tex.]: National Aeronautics and Space Administration, Environmental Physiology/Biophysics Laboratory, 1993.

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21

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

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22

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

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23

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

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24

Che, Jen-Peng. Analysis of constant phase contours of evaporation duct mode functions for waveguide mode propagation. Monterey, Calif: Naval Postgraduate School, 1992.

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25

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

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26

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

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27

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

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28

United States. National Aeronautics and Space Administration., ed. Investigations into the F-106 lightning strike environment as functions of altitude and storm phase. Rapid City, S.D: Institute of Atmospheric Sciences, South Dakota School of Mines and Technology, 1987.

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29

Ole, Nedergaard Thomsen, and Herslund Michael, eds. Complex predicates and incorporation: A functional perspective. Copenhagen: C.A. Reitzel, 2002.

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30

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

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31

Jensen, Frede. Quality Function Deployment: The Evolved 4-Phase Model. Lulu Press, Inc., 2017.

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32

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

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33

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

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34

Dallenbach-Hellweg, Gisela, and Peter Stoll. Gynecological Vital Cytology: Function · Microbiology · Neoplasia Atlas of Phase-Contrast Microscopy. Springer London, Limited, 2013.

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35

Kim, Young S., and Woodford W. Zachary. Physics of Phase Space: Nonlinear Dynamics and Chaos, Geometric Quantization,and Wigner Function. Springer London, Limited, 2006.

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36

Pomey, Patrice. Defining a Ship: Architecture, Function, and Human Space. Edited by Ben Ford, Donny L. Hamilton, and 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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37

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

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38

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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39

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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40

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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41

Felger, Jennifer C., Ebrahim Haroon, and Andrew H. Miller. Inflammation and Immune Function in PTSD. Edited by Israel Liberzon and 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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42

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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43

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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44

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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45

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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46

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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47

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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48

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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49

Vimalesvaran, Kavitha, and 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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50

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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