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Auteur : Grafiati
Publié le 14 mars 2023

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1

Church, Ronald H. Dielectric properties of low-loss minerals. [Pittsburgh] : U.S. Dept. of the Interior, 1988.

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2

Church, Ronald H. Dielectric properties of low-loss minerals. Washington, DC : U.S. Bureau of Mines, 1988.

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3

Davis, Bob. Manufactured homes acquisition program : Heat loss assumptions, calculations, and heat loss coefficient tables. Seattle, WA : Ecotope, Inc., 1992.

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4

A, Naff S., U.S. Nuclear Regulatory Commission. Office of Nuclear Regulatory Research. Division of Systems Research., Idaho National Engineering Laboratory et EG & G Idaho., dir. Thermal-hydraulic processes during reduced inventory operation with loss of residual heat removal. Washington, DC : Division of Systems Research, Office of Nuclear Regulatory Research, U.S. Nuclear Regulatory Commission, 1992.

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5

A, Naff S., U.S. Nuclear Regulatory Commission. Office of Nuclear Regulatory Research. Division of Systems Research., Idaho National Engineering Laboratory et EG & G Idaho., dir. Thermal-hydraulic processes during reduced inventory operation with loss of residual heat removal. Washington, DC : Division of Systems Research, Office of Nuclear Regulatory Research, U.S. Nuclear Regulatory Commission, 1992.

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6

Onega, Ronald J. Thermal flanking loss calculations for the National Bureau of Standards calibrated hot box. [Washington, DC] : U.S. Dept. of Commerce, National Bureau of Standards, 1985.

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7

Boyd, Christopher Fred. Predictions of spent fuel heatup after a complete loss of spent fuel pool coolant. Washington, DC : Safety Margins and Systems Analysis Branch, Office of Nuclear Regulatory Research, Nuclear Regulatory Commission, 2000.

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8

Boyd, Christopher F. Predictions of spent fuel heatup after a complete loss of spent fuel pool coolant. Washington, DC : Safety Margins and Systems Analysis Branch, Office of Nuclear Regulatory Research, Nuclear Regulatory Commission, 2000.

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9

Center, Lewis Research, dir. Adjusting measured weight loss of aged graphite fabric/PMR-15 composites. [Cleveland, Ohio] : National Aeronautics and Space Administration, Lewis Research Center, 1998.

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10

Vahe, Petrosian, et United States. National Aeronautics and Space Administration., dir. The behavior of beams of relativistic non-thermal electrons under the influence of collisions and synchrotron losses. Stanford, Calif : Center for Space Science and Astrophysics, Stanford University, 1990.

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11

S, Bang Y., Kim H. J, U.S. Nuclear Regulatory Commission. Office of Nuclear Regulatory Research et Hanʾguk Wŏnjaryŏk Anjŏn Kisurwŏn, dir. Assessment of RELAP5/MOD3.2 to the loss-of-residual-heat-removal event under shutdown condition. Washington, DC : Office of Nuclear Regulatory Research, U.S. Nuclear Regulatory Commission, 2000.

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12

S, Bang Y., Kim H. J, U.S. Nuclear Regulatory Commission. Office of Nuclear Regulatory Research et Hanʾguk Wŏnjaryŏk Anjŏn Kisurwŏn, dir. Assessment of RELAP5/MOD3.2 to the loss-of-residual-heat-removal event under shutdown condition. Washington, DC : Office of Nuclear Regulatory Research, U.S. Nuclear Regulatory Commission, 2000.

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13

S, Bang Y., Kim H. J, U.S. Nuclear Regulatory Commission. Office of Nuclear Regulatory Research. et Hanʼguk Wŏnjaryŏk Anjŏn Kisurwŏn, dir. Application of RELAP5/MOD3.2 to the loss-of-residual-heat-removal event under shutdown condition. Washington, DC : Office of Nuclear Regulatory Research, U.S. Nuclear Regulatory Commission, 2000.

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14

S, Bang Y., Kim H. J, U.S. Nuclear Regulatory Commission. Office of Nuclear Regulatory Research. et Han.guk Wfonjaryfok Anjfon Kisurwfon., dir. Assessment of RELAP5/MOD3.2 to the loss-of-residual-heat-removal event under shutdown condition. Washington, DC : Office of Nuclear Regulatory Research, U.S. Nuclear Regulatory Commission, 2000.

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15

S, Bang Y., Kim H. J, U.S. Nuclear Regulatory Commission. Office of Nuclear Regulatory Research. et Hanʼguk Wŏnjaryŏk Anjŏn Kisurwŏn, dir. Assessment of RELAP5/MOD3.2 to the loss-of-residual-heat-removal event under shutdown condition. Washington, DC : Office of Nuclear Regulatory Research, U.S. Nuclear Regulatory Commission, 2000.

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16

G, Stanley Richard, et Geological Survey (U.S.), dir. Preliminary report on petroleum source potential and thermal maturity of the Lospe Formation (lower Miocene) near Point Sal, onshore Santa Maria basin, California. [Menlo Park, CA] : U.S. Geological Survey, 1995.

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17

G, Stanley Richard, et Geological Survey (U.S.), dir. Preliminary report on petroleum source potential and thermal maturity of the Lospe Formation (lower Miocene) near Point Sal, onshore Santa Maria basin, California. [Reston, Va] : U.S. Dept. of the Interior, U.S. Geological Survey, 1995.

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18

G, Stanley Richard, et Geological Survey (U.S.), dir. Preliminary report on petroleum source potential and thermal maturity of the Lospe Formation (lower Miocene) near Point Sal, onshore Santa Maria basin, California. [Reston, Va] : U.S. Dept. of the Interior, U.S. Geological Survey, 1995.

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19

United States. National Aeronautics and Space Administration., dir. A model for the scattering of high-frequency electromagnetic fields from dielectrics exhibiting thermally-activated electrical losses. [Washington, DC] : National Aeronautics and Space Administration, 1991.

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20

United States. National Aeronautics and Space Administration., dir. A model for the scattering of high-frequency electromagnetic fields from dielectrics exhibiting thermally-activated electrical losses. [Washington, DC] : National Aeronautics and Space Administration, 1991.

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21

G, Miao, Cheng Z, U.S. Nuclear Regulatory Commission. Division of Systems Analysis and Regulatory Effectiveness. et Energy and Environmental Science, Inc., dir. Analysis of spent fuel heatup following loss of water in a spent fuel pool : A users' manual for the computer code SHARP : final report. Washington, DC : Division of Systems Analysis and Regulatory Effectiveness, Office of Nuclear Regulatory Research, U.S. Nuclear Regulatory Commission, 2002.

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22

G, Miao, Cheng Z, U.S. Nuclear Regulatory Commission. Office of Nuclear Regulatory Research. Division of Regulatory Applications. et Brookhaven National Laboratory, dir. Analysis of spent fuel heatup following loss of water in a spent fuel pool : A users' manual for the computer code SHARP : draft report for comment. Washington, DC : Division of Regulatory Applications, Office of Nuclear Regulatory Research, U.S. Nuclear Regulatory Commission, 1998.

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23

Kravchenko, Igor', Maksim Glinskiy, Sergey Karcev, Viktor Korneev et Diana Abdumuminova. Resource-saving plasma technology in the repair of processing equipment. ru : INFRA-M Academic Publishing LLC., 2020. http://dx.doi.org/10.12737/1083289.

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In the monograph methodological bases of selection of method of coating, design of technological processes of hardening and recovery of the wearing surfaces of parts using a systems engineering analysis and information support technologist. The mathematical model of plasma spraying of materials with different thermal conductivity and methods criteria for evaluation of technical and technological opportunities of a plasma coating method. Describes the methods and results of experimental studies, the analysis of the conditions and causes of loss of efficiency of processing equipment APK. The proposed scientific and methodical approach to the justification of expediency of the recovery and strengthening of the working bodies and parts expensive imported technological equipment. The proposed mathematical model describing the physical processes in plasma coating for various applications. The structure of the algorithm for solving the task of hardening and recovery of worn parts plasma methods on the basis of the integrated CAE system. This monograph is intended for employees of scientific research institutions, specialists of machine-building production and enterprises of technical service, as well as teachers, postgraduates and students of agricultural engineering areas of training.
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24

Loose Leaf for Fundamentals of Thermal-Fluid Sciences. McGraw-Hill Education, 2021.

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25

Loose Leaf for Fundamentals of Thermal-Fluid Sciences. McGraw-Hill Education, 2016.

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26

Guyer, J. Paul. Model Specifications : Mineral Fiber Blanket and Loose Fill Thermal Insulation. CreateSpace Independent Publishing Platform, 2014.

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27

Yarbrough, David W. Thickness and Density Measurements for Attic Loose-Fill Thermal Insulations in Eight Cities. Oak Ridge National Laboratory, 1987.

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28

Thermal-hydraulic processes during reduced inventory operation with loss of residual heat removal. Washington, DC : Division of Systems Research, Office of Nuclear Regulatory Research, U.S. Nuclear Regulatory Commission, 1992.

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29

Predictions of spent fuel heatup after a complete loss of spent fuel pool coolant. Supt. of Docs., U.S. G.P.O. [distributor], 2000.

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30

Wachs, Daniel M. A study of thermal stratification in the cold legs during the subcooled blowdown phase of a loss of coolant accident in the OSU APEX Thermal Hydraulic Testing Facility. 1998.

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31

Wachs, Daniel M. A study of thermal stratification in the cold legs during the subcooled blowdown phase of a loss of coolant accident in the OSU APEX Thermal Hydraulic Testing Facility. 1998.

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32

Cengel, Yunus A. Package : Loose Leaf for Fundamentals of Thermal-Fluid Sciences with 1 Semester Connect Access Card. McGraw-Hill Education, 2016.

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33

Lecouffe, Aude, João Marafona et Pedro Romio, dir. Porto-Lyon Seminar 2021 : Book of Abstracts. FEUP, 2022. http://dx.doi.org/10.24840/978-972-752-293-4.

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This book contains the abstracts supporting the oral communications that constituted the program of the Porto-Lyon Seminar 2021, held in Lyon (France), between the 23rd and 25th of February 2022. Porto-Lyon Seminar was an opportunity for PhD students, in the area of tribology, to discuss their ongoing research with peers. The addressed topics included: bearing modelling, gear modelling, lubricant oil analysis, maintenance, power loss, rolling contact fatigue, thermal contact modelling.
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34

Parker, Philip M. The 2007-2012 World Outlook for Loose Fiber and Granulated Fiber Mineral Wool for Thermal and Acoustical Envelope Insulation. ICON Group International, Inc., 2006.

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35

The 2006-2011 World Outlook for Loose Fiber and Granulated Fiber Mineral Wool for Thermal and Acoustical Envelope Insulation. Icon Group International, Inc., 2005.

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36

Application of RELAP5/MOD3.2 to the loss-of-residual-heat-removal event under shutdown condition. Washington, DC : Office of Nuclear Regulatory Research, U.S. Nuclear Regulatory Commission, 2000.

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37

Assessment of RELAP5/MOD3.2 to the loss-of-residual-heat-removal event under shutdown condition. Washington, DC : Office of Nuclear Regulatory Research, U.S. Nuclear Regulatory Commission, 2000.

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38

Application of RELAP5/MOD3.2 to the loss-of-residual-heat-removal event under shutdown condition. Washington, DC : Office of Nuclear Regulatory Research, U.S. Nuclear Regulatory Commission, 2000.

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39

Graves, R. S. Thicknesses, Densities, and Calculated Thermal Resistances for Loose-Fill Rock Wool Installed in Two Attic Sections of a Manufactured House. Oak Ridge National Laboratory, 1986.

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40

Schetz, Miet, et Andrew Davenport. Continuous renal replacement therapy. Sous la direction de Norbert Lameire. Oxford University Press, 2015. http://dx.doi.org/10.1093/med/9780199592548.003.0234.

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After its introduction, continuous renal replacement therapy (CRRT) has found widespread acceptance amongst physicians taking care of critically ill patients. Various modalities (haemofiltration, haemodialysis, haemodiafiltration) are used. As for all types of renal replacement therapy, a good functioning vascular access is an absolute requirement. Whether CRRT is to be preferred over intermittent haemodialysis remains a matter of debate, but haemodynamic instability and risk of cerebral oedema are generally considered indications for CRRT. Whereas under-dosing should certainly be avoided, increasing the dose over an actually delivered effluent flow of 20–25 mL/kg/hour does not appear to improve outcome.One of the major drawbacks of CRRT is the requirement for continuous anticoagulation. Citrate anticoagulation is gaining popularity and represents a valuable alternative, especially in patients with bleeding risk. Other potential complications of CRRT include thermal, nutrient, and drug losses, and acid–base and electrolyte disturbances.
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41

Clarke, Andrew. Temperature and its measurement. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780199551668.003.0003.

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Temperature is that property of a body which determines whether it gains or loses energy in a particular environment. In classical thermodynamics temperature is defined by the relationship between energy and entropy. Temperature can be defined only for a body that is in thermodynamic and thermal equilibrium; whilst organisms do not conform to these criteria, the errors in assuming that they do are generally small. The Celsius and Fahrenheit temperature scales are arbitrary because they require two fixed points, one to define the zero and the other to set the scale. The thermodynamic (absolute) scale of temperature has a natural zero (absolute zero) and is defined by the triple point of water. Its unit of temperature is the Kelvin. The Celsius scale is convenient for much ecological and physiological work, but where temperature is included in statistical or deterministic models, only thermodynamic temperature should be used. Past temperatures can only be reconstructed with the use of proxies, the most important of which are based on isotope fractionation.
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42

Schaible, Hans-Georg, et Rainer H. Straub. Pain neurophysiology. Oxford University Press, 2013. http://dx.doi.org/10.1093/med/9780199642489.003.0059.

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Physiological pain is evoked by intense (noxious) stimuli acting on healthy tissue functioning as a warning signal to avoid damage of the tissue. In contrast, pathophysiological pain is present in the course of disease, and it is often elicited by low-intensity stimulation or occurs even as resting pain. Causes of pathophysiological pain are either inflammation or injury causing pathophysiological nociceptive pain or damage to nerve cells evoking neuropathic pain. The major peripheral neuronal mechanism of pathophysiological nociceptive pain is the sensitization of peripheral nociceptors for mechanical, thermal and chemical stimuli; the major peripheral mechanism of neuropathic pain is the generation of ectopic discharges in injured nerve fibres. These phenomena are created by changes of ion channels in the neurons, e.g. by the influence of inflammatory mediators or growth factors. Both peripheral sensitization and ectopic discharges can evoke the development of hyperexcitability of central nociceptive pathways, called central sensitization, which amplifies the nociceptive processing. Central sensitization is caused by changes of the synaptic processing, in which glial cell activation also plays an important role. Endogenous inhibitory neuronal systems may reduce pain but some types of pain are characterized by the loss of inhibitory neural function. In addition to their role in pain generation, nociceptive afferents and the spinal cord can further enhance the inflammatory process by the release of neuropeptides into the innervated tissue and by activation of sympathetic efferent fibres. However, in inflamed tissue the innervation is remodelled by repellent factors, in particular with a loss of sympathetic nerve fibres.
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43

U.S. Nuclear Regulatory Commission. Characterization of Thermal-Hydraulic and Ignition Phenomena in Prototypic, Full-Length Boiling Water Reactor Spent Fuel Pool Assemblies After a Postulated Complete Loss-of-Coolant Accident. CreateSpace Independent Publishing Platform, 2014.

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44

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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45

Falk, Bareket, et Raffy Dotan. Temperature regulation. Sous la direction de Neil Armstrong et Willem van Mechelen. Oxford University Press, 2017. http://dx.doi.org/10.1093/med/9780198757672.003.0014.

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Under all but the most extreme environmental heat conditions, children control their body temperature (at rest and during exercise) as well as adults. Children, however, use a different thermoregulatory strategy. Compared with adults, children rely more on dry heat dissipation and less on evaporative cooling (sweating). Their larger skin surface-area relative to mass does put children at increasing disadvantage, relative to adults, as ambient temperatures rise above skin temperature. Similarly, they become increasingly disadvantaged upon exposure to decreasing temperatures below the thermo-neutral zone. Like adults, children inadvertently dehydrate while exercising in hot conditions and are often hypohydrated, even before exercise, and their core temperature rises considerably more than adults in response to a given fluid (sweat) loss, which may put them at higher risk for heat-related injury. However, epidemiological data show rates of both heat- and cold-related injuries among children and adolescents as similar or lower than at any other age.
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46

Woodburne, Michael O., Gregg F. Gunnell et Richard K. Stucky. Land Mammal Faunas of North America Rise and Fall During the Early Eocene Climatic Optimum. Denver Museum of Nature & Science, 2009. http://dx.doi.org/10.55485/rkck3803.

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Climatic warming at the beginning of the Early Eocene Climatic Optimum (EECO) resulted in major increases in plant diversity and habitat complexity reflective of temporally unique, moist, paratropical conditions from about 53–50 Ma in the Western Interior of North America. In the early part of the EECO, mammalian faunal diversity increased at both local and continental scales in conjunction with a major increase in tropicality resulting from mean annual temperatures reaching 23 ̊C and mean annual precipitation approaching 150 cm/yr. A strong episode of taxonomic origination (high number of first appearances) in the latest Wasatchian and earliest Bridgerian Land Mammal Ages apparently was in response to these greatly diversified floral and habitat associations along with increasing temperature and precipitation. This is in contrast to a similar increase in first appearances at the beginning of the Wasatchian (Paleocene-Eocene Thermal Maximum, or PETM) that can be traced instead to climate-induced transcontinental immigration. In the later part of the EECO, from Br-1b–Br-3, climatic deterioration resulted in a major loss of faunal diversity at both continental and local levels, apparently mirroring climatic deterioration. Relative abundance shifted from diverse, evenly distributed communities to much less diverse, skewed distributions dominated by the condylarth Hyopsodus. Evolutionary innovation through the 53–50 Ma interval included a modest overall increase in body size and increased efficiency in carnivory and folivory as reflected by within-lineage patterns of evolution. Rather than being “optimum,” the EECO engendered the greatest episode of mammalian faunal turnover of the first 15 million years of the Cenozoic era, with both first and last appearances at their highest levels. Both the PETM and EECO faunas were climatically shaped.
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