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Books on the topic 'Magnetic parameter'

Author: Grafiati

Published: 28 May 2022

Last updated: 30 July 2025

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1

Pijnappel, Wilhelmus Wilhelmina Francisca. Quantification of 1-D and 2-D magnetic resonance spectroscopic data. Technische Universiteit Delft, 1991.

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2

Marqués, Ricardo. Metamaterials with negative parameter: Theory, design and microwave applications. John Wiley, 2007.

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3

Frederichs, Thomas. Regionale und altersabhängige Variation gesteinsmagnetischer Parameter in marinen Sedimenten der Arktis =: Regional and temporal variations of rock magnetic parameters in Arctic marine sediments. Alfred-Wegener-Institut für Polar- und Meeresforschung, 1995.

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4

Pavlov, Sergey. Methods of catastrophe theory in the phenomenology of phase transitions. 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 propert

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5

T, Tsurutani Bruce, and United States. National Aeronautics and Space Administration., eds. Criteria of interplanetary parameters causing intense magnetic storms (Dst < -100 nT). National Aeronautics and Space Administration, 1987.

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6

Dekkers, Marinus Jacobus. Some rockmagnetic parameters for natural goethite, pyrrhotite, and fine-grained hematite =: Gesteente-magnetische parameters voor natuurlijke goethiet, pyrrhotien, en fijnkorrelige hematiet. Instituut voor Aardwetenschappen der Rijksuniversiteit te Utrecht, 1988.

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7

Dekkers, Marinus Jacobus. Some rockmagnetic parameters for natural goethite, pyrrhotite, and fine-grained hematite. Instituut voor Aardwetenschappen der Rijksuniversiteit te Utrecht, 1988.

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8

Martin, Kaupp, Bühl Michael, and Malkin Vladimir G, eds. Calculation of NMR and EPR parameters: Theory and applications. Wiley-VCH, 2004.

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9

Martin, Loren John. Systematic manipulation of complex magnetic field parameters and pharmacological interactions to produce analgesia in wistar rats. Laurentian University, School of Graduate Studies, 2004.

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10

Rehn, Suzanne. Prognosis and diagnosis of non-hodgkin lymphomas the role of proliferation associated parameters and magnetic resonance imaging. Uppsala Universitet, 1991.

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11

Gibbons, Laura. Back function testing and paraspinal muscle magnetic resonance image parameters, their associations and derterminants: A study of male, monozygotic twins. University of Jyväskylä, 1998.

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12

Paula, Benaglia, Bosch Guillermo 1968-, Cappa Cristina, Niemela Virpi, and Universidad Nacional Autónoma de México. Instituto de Astronomía., eds. Massive stars: Fundamental parameters and circumstellar interactions : Cariló, Buenos Aires, Argentina, diciembre 11-14, 2006. Instituto de Astronomía, Universidad Nacional Autónoma de México, 2008.

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13

Deniszczyk, Józef. Struktura elektronowa, właściwości magnetyczne i parametry struktury nadsubtelnej wybranych międzymetalicznych związków żelaza o strukturze typu B2, DO3 i L21. Wydawnictwo Uniwersytetu Śląskiego, 2005.

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14

Page, J. H. R. Relationship between crystallographic textures in fully annealed silicon bearing non-oriented electrotechnical steels and magnetic parameters, in particular, energy loss in rotating machines. Commission of the European Communities, 1986.

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15

Vaez-Zadeh, Sadegh. Parameter Estimation. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198742968.003.0007.

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In this chapter, the estimation of permanent magnetic synchronous (PMS) motor parameters, including stator winding resistance, motor inductances, and magnitude of permanent magnet flux linage, is presented in two main categories, i.e., offline and online. Several offline schemes, including DC and AC standstill tests, no-load test, load test, and vector control schemes, are presented for estimation of all the motor parameters. Major online schemes used in the estimation of PMS motor parameters are also presented in this chapter. They include closed-loop observer-based estimation, model referenc

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16

Eriksson, Olle, Anders Bergman, Lars Bergqvist, and Johan Hellsvik. Density Functional Theory. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198788669.003.0001.

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Density functional theory (DFT) has established itself as a very capable platform for modelling from first principles electronic, optical, mechanical and structural properties of materials. Starting out from the Dirac equation for the many-body system of electrons and nuclei, an effective theory has been developed allowing for materials specific and parameter free simulations of non-magnetic and magnetic solid matter. In this Chapter an introduction will be given to DFT, the Hohenberg-Kohn theorems, the Kohn-Sham equation, and the formalism for how to deal with non-collinear magnetism.

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17

Eriksson, Olle, Anders Bergman, Lars Bergqvist, and Johan Hellsvik. The Damping Term, from First Principles. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198788669.003.0006.

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In the previous chapters we described the basic principles of density functional theory, gave examples of how accurate it is to describe static magnetic properties in general, and derived from this basis the master equation for atomistic spin-dynamics; the SLL (or SLLG) equation. However, one term was not described in these chapters, namely the damping parameter. This parameter is a crucial one in the SLL (or SLLG) equation, since it allows for energy and angular momentum to dissipate from the simulation cell. The damping parameter can be evaluated from density functional theory, and the Kohn-

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18

Eriksson, Olle, Anders Bergman, Lars Bergqvist, and Johan Hellsvik. Atomistic Spin Dynamics. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198788669.001.0001.

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The purpose of this book is to provide a theoretical foundation and an understanding of atomistic spin-dynamics, and to give examples of where the atomistic Landau-Lifshitz-Gilbert equation can and should be used. The contents involve a description of density functional theory both from a fundamental viewpoint as well as a practical one, with several examples of how this theory can be used for the evaluation of ground state properties like spin and orbital moments, magnetic form-factors, magnetic anisotropy, Heisenberg exchange parameters, and the Gilbert damping parameter. This book also outl

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19

Moeller, Torsten B. Mri Parameters And Positioning. George Thieme Verlag, 2003.

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20

Torsten Bert, M.d. Moeller and Emil R. Reif. Mri Parameters and Positioning. Thieme Medical Publishers, 2003.

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21

Eriksson, Olle, Anders Bergman, Lars Bergqvist, and Johan Hellsvik. Outlook on Magnetization Dynamics. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198788669.003.0012.

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Since its original formulation in the mid-1990's, atomistic spin-dynamics has become an important tool for modelling of dynamic processes in magnetic materials. So far this book has described current methodological methods and functionalities of atomistic spin-dynamics simulations. Applications of DFT and ASD techniques to selected topics have been presented in this book, for instance methods for calculation of the microscopic Heisenberg and Gilbert parameter from first principles (Chapters 2 and 6), multiscale modelling of magnon spectra in bulk and thin film magnets (Chapter 9), and theoreti

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22

Faraj, Yahia Abdullah. Transducer parameter selection for two phase flowmetering: A study of the sensitivity and performance of magnetic, ultrasonic, conductivity and electrostatic flowmeters for the measurement of two phase flow. 1985.

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23

Eriksson, Olle, Anders Bergman, Lars Bergqvist, and Johan Hellsvik. Ferromagnetic Resonance. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198788669.003.0008.

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In the previous chapters we covered theoretical aspects of magnetism and magnetization dynamics, as well as practical aspects of implementation of the SLL equation in efficient softwares. In this chapter we focus on the most natural and frequently used experimental method to study magnetization dynamics, namely ferromagnetic resonance (FMR). This experimental technique has evolved into a powerful experimental technique for studies of magnetization dynamics of materials. It is, by far, the most common method for extracting damping parameters in materials, and is also a reliable technique for es

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24

Sorolla, Mario, Ricardo Marqu�s, and Ferran Mart�n. Metamaterials with Negative Parameters: Theory, Design, and Microwave Applications. Wiley & Sons, Incorporated, John, 2011.

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25

Sorolla, Mario, Ricardo Marqu�s, and Ferran Mart�n. Metamaterials with Negative Parameters: Theory, Design, and Microwave Applications. Wiley & Sons, Incorporated, John, 2008.

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26

Marqués, Ricardo, Ferran Martín, and Mario Sorolla. Metamaterials with Negative Parameters: Theory, Design and Microwave Applications. Wiley & Sons, Limited, John, 2007.

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27

Sorolla, Mario, Ricardo Marqu�s, and Ferran Mart�n. Metamaterials with Negative Parameters: Theory, Design, and Microwave Applications. Wiley & Sons, Incorporated, John, 2011.

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28

Eriksson, Olle, Anders Bergman, Lars Bergqvist, and Johan Hellsvik. Applications of Density Functional Theory. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198788669.003.0003.

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In this chapter we give examples of how density functional theory describes some of the most basic magnetic properties of a material. This involves spin and orbital moments, Heisenberg exchange parameters and magnetic form factors. Relativistic effects couple spin and orbital space and make magnetic materials anisotropic, which means that the ground state magnetization is oriented parallel or perpendicular to high symmetry directions of the crystalline structure. We also illustrate how well density functional theory describes cohesive properties and how magnetism influence these properties. Th

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29

Graham, Simon James. Quantitative measurement of tissue parameters in vivo using magnetic resonance. 1995.

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30

Canet, Daniel, Fabien Ferrage, Kavita Dorai, and Bernard Ancian. Cross-Relaxation and Cross-correlation Parameters in NMR: Molecular Approaches. Royal Society of Chemistry, The, 2017.

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31

Kaupp, Martin, Vladimir G. Malkin, and Michael B�hl. Calculation of NMR and EPR Parameters: Theory and Applications. Wiley & Sons, Limited, John, 2004.

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32

(Editor), Martin Kaupp, Michael Bühl (Editor), and Vladimir G. Malkin (Editor), eds. Calculation of NMR and EPR Parameters: Theory and Applications. Wiley-VCH, 2004.

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33

Clark, Caroline, Jeffrey Cole, Christine Winter, and Geoffrey Grammer. Transcranial Magnetic Stimulation Treatment of Posttraumatic Stress Disorder. Oxford University Press, 2016. http://dx.doi.org/10.1093/med/9780190205959.003.0005.

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Symptoms of post-traumatic stress disorder (PTSD) often fail to resolve with psychotherapy, pharmacotherapy, or integrative medicine treatments. Given these limitations, there is a continued push to discover treatment methods utilizing novel mechanisms of action. Transcranial magnetic stimulation (TMS) offers a non-invasive and safe method of brain stimulation that modulates neuronal activity in a focal area to achieve excitation or inhibition, and may have utility for patients suffering from PTSD, although, to date, evidence of efficacy is limited. The TMS treatment can be varied to suit the

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34

Luo, Yutian, ed. Study on key physical parameters of tight reservoir based on nuclear magnetic resonance technology. Ausasia Science and Technology Press, 2022. http://dx.doi.org/10.26804/0104142022.

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35

Mughabghab, Said F. Atlas of Neutron Resonances: Resonance Parameters and Thermal Cross Sections. Z=1-100. Elsevier Science & Technology Books, 2006.

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36

Kaupp, Martin, Vladimir G. Malkin, and Michael Bühl. Calculation of NMR and EPR Parameters: Theory and Applications. Wiley & Sons, Incorporated, John, 2006.

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37

Quantification of observed flare parameters in relation to a shear-index and verification of MHD models for flare prediction: Semi-annual report for period March 26, 1987 through September 26, 1987. The Center, 1987.

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38

Horing, Norman J. Morgenstern. Superfluidity and Superconductivity. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198791942.003.0013.

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Chapter 13 addresses Bose condensation in superfluids (and superconductors), which involves the field operator ψ‎ having a c-number component (<ψ(x,t)>≠0), challenging number conservation. The nonlinear Gross-Pitaevskii equation is derived for this condensate wave function<ψ>=ψ−ψ˜, facilitating identification of the coherence length and the core region of vortex motion. The noncondensate Green’s function G˜1(1,1′)=−i<(ψ˜(1)ψ˜+(1′))+> and the nonvanishing anomalous correlation function F˜∗(2,1′)=−i<(ψ˜+(2)ψ˜+(1′))+> describe the dynamics and elementary excitations of the

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39

Marqués, Ricardo, Ferran Martín, and Mario Sorolla. Metamaterials with Negative Parameters: Theory, Design and Microwave Applications (Wiley Series in Microwave and Optical Engineering). Wiley-Interscience, 2008.

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40

Eriksson, Olle, Anders Bergman, Lars Bergqvist, and Johan Hellsvik. The Atomistic Spin Dynamics Equation of Motion. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198788669.003.0004.

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From the information obtained in DFT, in particular the magnetic moments and the Heisenberg exchange parameters, one has the possibility to make a connection to atomistic spin-dynamics. In this chapter the essential features of this connection is described. It is also discussed under what length and time-scales that this approach is a relevant approximation. The master equation of atomistic spin-dynamics is derived, and discussed in detail. In addition we give examples of how this equation describes the magnetization dynamics of a few model systems.

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41

Sandbrink, Friedhelm. The MEP in clinical neurodiagnosis. Edited by Charles M. Epstein, Eric M. Wassermann, and Ulf Ziemann. Oxford University Press, 2012. http://dx.doi.org/10.1093/oxfordhb/9780198568926.013.0019.

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This article gives information on the clinical application of motor-evoked potential (MEP). Transcranial stimulation of the cerebral cortex to elicit MEPs is a noninvasive method for assessing the integrity of the central motor pathway function. Transcranial magnetic stimulation (TMS) is used in diagnosing and monitoring neurological disorders. This article highlights the neurophysiological differences between TMS and transcranial electric stimulation. All the different MEP parameters that can be measured by TMS, the latency of the MEP is generally regarded as the most reliable and useful. TMS

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42

Mavi, Jagroop, Anne C. Boat, Senthilkumar Sadhasivam, and Catherine P. Seipel. Congenital Diaphragmatic Hernia Repair. Edited by Erin S. Williams, Olutoyin A. Olutoye, Catherine P. Seipel, and Titilopemi A. O. Aina. Oxford University Press, 2018. http://dx.doi.org/10.1093/med/9780190678333.003.0050.

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Congenital diaphragmatic hernia is an embryologic defect in diaphragm formation that allows abdominal contents to enter into the fetal pleural cavity, resulting in ipsilateral lung compression, pulmonary hypoplasia, and abnormal pulmonary vasculature. Though diagnosis is frequently made on prenatal imaging, the diagnosis should be considered in any newborn with respiratory distress. Prenatal predictors of defect severity include evaluation of observed-to-expected lung volumes on fetal magnetic resonance imaging and lung-to-head ratio on fetal ultrasound. Treatment focuses on medical stabilizat

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43

K, Rajendran, and Veeramanikandasamy T. Structural, Optical, Electrical and Magnetic Properties of Synthesized Manganese Sulfide Nanocrystals: A Study on the Influence of Process Parameters on Synthesis of MnS Nanocrystals. Independently Published, 2019.

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44

Vaez-Zadeh, Sadegh. Introduction. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198742968.003.0001.

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An overview of permanent magnet synchronous (PMS) motors and the related control system are presented in this chapter as introductory materials for the rest of the book. The interconnections of the control system to the power electronic inverter and the motor are emphasized. In addition, the major parts of the system are overviewed. Pulse width-modulated voltage source inverter, as the most commonly used power converter in PMS motor drives, is briefly discussed. PMS motors configurations and operating principles are also presented after considering characteristics of permanent magnet materials

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45

Launay, Jean-Pierre, and Michel Verdaguer. The moving electron: electrical properties. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198814597.003.0003.

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The three basic parameters controlling electron transfer are presented: electronic interaction, structural change and interelectronic repulsion. Then electron transfer in discrete molecular systems is considered, with cases of inter- and intramolecular transfers. The semi-classical (Marcus—Hush) and quantum models are developed, and the properties of mixed valence systems are described. Double exchange in magnetic mixed valence entities is introduced. Biological electron transfer in proteins is briefly presented. The conductivity in extended molecular solids (in particular organic conductors)

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46

Glazov, M. M. Hyperfine Interaction of Electron and Nuclear Spins. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198807308.003.0004.

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This chapter discusses the key interaction–hyperfine coupling–which underlies most of phenomena in the field of electron and nuclear spin dynamics. This interaction originates from magnetic interaction between the nuclear and electron spins. For conduction band electrons in III–V or II–VI semiconductors, it is reduced to a Fermi contact interaction whose strength is proportional to the probability of finding an electron at the nucleus. A more complex situation is realized for valence band holes where hole Bloch functions vanish at the nuclei. Here the hyperfine interaction is of the dipole–dip

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47

Nixdorff, Uwe, Stephan Achenbach, Frank Bengel, et al. Imaging in cardiovascular prevention. Oxford University Press, 2015. http://dx.doi.org/10.1093/med/9780199656653.003.0006.

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Imaging tools in preventive cardiology can be divided into imaging modalities to assess pre-clinical and clinical atherosclerosis and functional assessments of vascular function or vascular inflammation. To calculate the likelihood of pre-clinical atherosclerosis intima-media thickness as well as coronary calcium scoring are most frequently used. However, beyond these two there are other parameters derived by ultrasound and multi-detector computed tomography as well as magnetic resonance imaging and nuclear/molecular imaging which are discussed in the chapter. Functional tests include flow-med

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48

Lo, Meng-chen, Marie-France Marin, Alik S. Widge, and Mohammed R. Milad. Device-Based Treatment for PTSD. Edited by Frederick J. Stoddard, David M. Benedek, Mohammed R. Milad, and Robert J. Ursano. Oxford University Press, 2018. http://dx.doi.org/10.1093/med/9780190457136.003.0025.

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Device-based neuromodulation is an emerging tool with great potential for significant scientific and clinical implications for a number of mental disorders. Neuromodulation techniques deliver electro-magnetic pulses into the brain via invasive or noninvasive electrodes, with various timing and stimulation parameters. The stimulation is thought to work as a “brain pacemaker” that either activates or inactivates targeted brain regions to restore normal homeostasis. There have been significant recent efforts to explore the clinical utility of device-based approaches for the treatment of mood, anx

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49

Wright, A. G. Secondary emission and gain. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780199565092.003.0005.

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Secondary-electron emission generates gain in conventional vacuum photomultipliers with discrete dynodes. This is a cascade process involving between 6 and 20 elements. Generally, the higher the number of stages, the higher is the gain and similarly for applied voltage. Gain is dependent on the composition of the dynodes, with SbCs and activated BeO being the most common materials. There are ten different dynode types, each of which serves a particular purpose: for example, operation in high magnetic fields and high temperature. The continuous channel dynode is available as a single unit and a

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50

Bass, Cristina, Barbara Bauce, and Gaetano Thiene. Arrhythmogenic right ventricular cardiomyopathy: diagnosis. Oxford University Press, 2018. http://dx.doi.org/10.1093/med/9780198784906.003.0360.

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Arrhythmogenic cardiomyopathy is a heart muscle disease clinically characterized by life-threatening ventricular arrhythmias and pathologically by an acquired and progressive dystrophy of the ventricular myocardium with fibrofatty replacement. The clinical manifestations of arrhythmogenic cardiomyopathy vary according to the ‘phenotypic’ stage of the underlying disease process. Since there is no ‘gold standard’ to reach the diagnosis of arrhythmogenic cardiomyopathy, multiple categories of diagnostic information have been combined. Different diagnostic categories include right ventricular morp

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