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E-grāmata: Magnetostatic Waves in Inhomogeneous Fields [Taylor & Francis e-book]

  • Formāts: 402 pages, 115 Line drawings, black and white; 115 Illustrations, black and white
  • Izdošanas datums: 06-Sep-2021
  • Izdevniecība: CRC Press
  • ISBN-13: 9781003046226
  • Taylor & Francis e-book
  • Cena: 271,26 €*
  • * this price gives unlimited concurrent access for unlimited time
  • Standarta cena: 387,50 €
  • Ietaupiet 30%
  • Formāts: 402 pages, 115 Line drawings, black and white; 115 Illustrations, black and white
  • Izdošanas datums: 06-Sep-2021
  • Izdevniecība: CRC Press
  • ISBN-13: 9781003046226
This reference examines magnetostatic waves and their distribution in non-uniformly magnetized films and structures. The work will be of interest to researchers working on high-performance analog information processing devices including filters, delay lines, phase shifters, frequency converters, non-reciprocal and non-linear devices.

Magnetostatic waves (MSWs) in magnetodielectric media are fundamental for the creation of various highly efficient devices for analog information processing in the microwave range. These devices include various filters, delay lines, phase shifters, frequency converters, nonreciprocal and nonlinear devices, and others.

Magnetostatic Waves in Inhomogeneous Fields

examines magnetostatic waves and their distribution in non-uniformly magnetized films and structures. The propagation of magnetostatic waves in magnetodielectric environments is accompanied by numerous and very diverse physical effects, sharply distinguishing them from ordinary electromagnetic waves in isotropic media. The authors address dispersion properties and noncollinearity of phase and group velocity vectors, as well as non-reciprocal propagation.

Key Features

  • Offers mathematical tools used in the calculation of properties of magnetostatic waves
  • Includes a current literature review of magnetostatic waves and domain structures in garnet–ferrite films
    • Considers the issue of converting magnetostatic waves into electromagnetic ones
  • Introduction xi
    List of frequently used abbreviations
    xiv
    1 Magnetostatic waves and domain structures in ferrite-garnet films (literature review)
    1(32)
    1.1 Oscillations and waves in magnetically ordered media in the approximation of magnetostatics
    1(4)
    1.2 Conditions of existence and dispersion of MSWs in magnetic films and structures on their basis
    5(4)
    1.3 Spreading of SMSW (surface magnetostic waves) in an arbitrary direction along the film plane
    9(4)
    1.4 Distribution of SMSW in ferrite films and structures under the conditions of inhomogeneous magnetization
    13(3)
    1.5 Distribution of SMSW in ferrite films and structures with periodic inhomogneities
    16(5)
    1.6 Conversion of a magnetostatic wave into electromagnetic on the field inhomogeneity
    21(1)
    1.7 Domain structures in ferrite films, FMR and MSW under the conditions of the existence of domain structures
    22(2)
    1.8 Features of magnetostatic waves in the long-wave limit
    24(3)
    1.9 Use of FMR, MSW and domains in ferritle films for information processing devices
    27(1)
    1.10 Basic issues for further explanation
    28(2)
    1.11 Some new directions of research of MSW
    30(3)
    2 Mathematical apparatus used in calculating the properties of magnetostatic waves
    33(106)
    2.1 Landau-Lifshitz equation
    33(6)
    2.2 Dynamic sensitivity of a magnetic medium
    39(6)
    2.3 Walker's equation
    45(5)
    2.3.1 Walker's equation with an arbitrary susceptibility tensor
    45(3)
    2.3.2 Walker equation in the Damon--Eshbach problem
    48(2)
    2.4 Dispersion ration for magnetic plate with free surface
    50(33)
    2.4.1 Basic equations
    50(4)
    2.4.2 Border conditions
    54(1)
    2.4.3 Complete problem statement
    55(1)
    2.4.4 Solving equations without boundary conditions
    56(7)
    2.4.5 Frequency regions of body and surface waves
    63(2)
    2.4.6 Derivation of the dispersion relation from the solution and boundary conditions
    65(4)
    2.4.7 Transition to the polar coordinate system
    69(3)
    2.4.8 Potentials
    72(3)
    2.4.9 Fields
    75(1)
    2.4.10 Magnetization
    76(2)
    2.4.11 Cutoff angle for the Damon--Eshbach ratio
    78(2)
    2.4.12 Damon--Eshbach dispersion relation in the Cartesian coordinate system
    80(3)
    2.5 Dispersion ratio for metal--dielectric--ferrite--metal (MDFDM) structure and its particular cases
    83(15)
    2.5.1 General derivation of the dispersion relation
    84(7)
    2.5.2 Dispersion relation for an arbitrary direction of propagation of the phase front
    91(1)
    2.5.3 Transition to the polar coordinate system
    92(3)
    2.5.4 Passage to the limit for dispersion relations for other structures
    95(3)
    2.6 Dispersion ration for metal--dielectric--ferrite--ferrite--dielectric--metal structure (MDFFDM)
    98(7)
    2.6.1 General conclusion and character of the dispersion relation
    98(5)
    2.6.2 Passage to the limit for dispersion relations for other structures
    103(2)
    2.7 Phase and group velocities, phase rise and delay time of wave beams SMSW
    105(8)
    2.7.1 Phase and group velocities
    106(6)
    2.7.2 Phase run and delay time
    112(1)
    2.8 System of equations for the Hamilton-Auld method
    113(10)
    2.8.1 General derivation of the Hamilton-Auld equations
    114(1)
    2.8.2 Transition to the polar coordinate system
    115(8)
    2.9 Derivatives from the dispersion relationship for the ferritic--dielectric--metal structure
    123(4)
    2.10 Equivalence of different kinds of equations of dynamics in classical mechanics
    127(2)
    2.11 Cauchy's proble in the distribution of SMSW
    129(5)
    2.12 Technique for calculating the trajectories of wave beams of MSW in an inhomogeneous field
    134(5)
    3 Magnetostatic waves in homogenized magnetized ferrite films and structures on their basis
    139(46)
    3.1 Conditions of existence and dispersion of SMSW (surface magnetostatic waves) in ferrite films and structures on their basis
    139(19)
    3.1.1 Dispersion properties of forward and backward SMSWs in the FDM structure
    140(7)
    3.1.2 Experimental study of the dispersion of the SMSW in the structure of the FDM
    147(1)
    3.1.2.1 Basic experimental technique
    147(7)
    3.1.2.2 Results of an experimental study of the dispersion properties of SMSW
    154(3)
    3.1.3 On the possibility of experimental observation of backward waves
    157(1)
    3.2 Distribution of SMSW in a two-component environment consists of a free ferrite film and FDM (ferrite--dielectric--metal) structure
    158(19)
    3.2.1 Analysis of the refraction of the SMSW using the method of isofrequency curves
    159(1)
    3.2.1.1 Formulation of the problem
    159(3)
    3.2.1.2 Analysis of orientation dependences by the method of isofrequency curves
    162(1)
    3.2.1.3 Strip orientation along the field
    162(3)
    3.2.1.4 The orientation of the strip is arbitrary
    165(1)
    3.2.1.5 Evaluation of the possibility of manifestation of the effects of dispersive splitting of a wave beam under the conditions of a real experiment
    166(1)
    3.2.2 Experimental study of the refraction of the SMSW
    167(2)
    3.2.2.1 Strip orientation along the field
    169(5)
    3.2.2.2 The orientation of the strip is arbitrary
    174(2)
    3.2.3 Reflection coefficient of the SMSW from the interface
    176(1)
    3.3 Dispersional properties of SMSW in structures containing two ferrite layers
    177(8)
    3.3.1 Ferrite--ferrite (FF) structure
    178(1)
    3.3.2 Metal--dielectric--ferrite--ferrite--dielectric--metal structure (MDFFDM)
    179(2)
    3.3.3 Experimental study of the variance of SMSW
    181(4)
    4 Methods of research and analysis of the propagation of SMSW under conditions of magnetization by a longitudinal in homogeneous field
    185(63)
    4.1 Basic types of inhomogeneities of a magnetizing field
    186(1)
    4.2 Spatial configuration of the areas if distribution of the SMSW
    187(2)
    4.3 Methods for analysis of SMSW propation under the conditions of inhomogeneous binding (frequency curves and Hamilton--Auld)
    189(4)
    4.3.1 Isofrequency curve method
    189(2)
    4.3.2 The Hamilton--Auld method
    191(2)
    4.3.3 Comparison of methods for analyzing SMSW trajectories
    193(1)
    4.4 Distribution of SMS Ws in ferrite films with free surfaces
    193(15)
    4.4.1 Analysis of SMSW trajectories by the method of isofrequency curves
    194(1)
    4.4.1.1 Linearly inhomogeneous field
    194(2)
    4.4.1.2 Valley-type field
    196(1)
    4.4.1.3 Shaft-type field
    197(1)
    4.4.2 Analysis of SMSW trajectories by the Hamilton--Auld method
    198(1)
    4.4.2.1 Linearly inhomogeneous field
    198(5)
    4.4.2.2 Valley-type field
    203(1)
    4.4.2.3 Shaft-type field
    203(5)
    4.5 Distribution of SMSW in the ferrite-metal structure
    208(4)
    4.5.1 Linearly inhomogeneous field
    208(2)
    4.5.2 Valley-type field
    210(1)
    4.5.3 Shaft-type field
    211(1)
    4.5.4 Channels of the first and second type
    211(1)
    4.6 Distribution of SMSWs in the structure of ferrite-dielectric metal
    212(15)
    4.6.1 Analysis of SMSW trajectories by the method of isofrequency curves
    213(1)
    4.6.1.1 Linearly inhoimogeneous field
    213(3)
    4.6.1.2 Valley-type field
    216(2)
    4.6.1.3 Shaft-type field
    218(2)
    4.6.1.4 General comment
    220(1)
    4.6.2 Analysis of SMSW trajectories by the Hamilton-Auld method
    220(1)
    4.6.2.1 Linearly inhomogeneous field
    221(2)
    4.6.2.2 Valley-type field
    223(1)
    4.6.2.3 Shaft-type field
    224(3)
    4.7 Phase rise and delay time
    227(8)
    4.7.1 Linearly inhomogeneous field
    227(2)
    4.7.2 Valley-type field
    229(2)
    4.7.3 Shaft-type field
    231(4)
    4.8 Experimental study of SMSW trajectories
    235(13)
    4.8.1 The main parameters of the experiment
    235(1)
    4.8.2 Linearly inhomogeneous field
    236(1)
    4.8.3 Valley-type field
    237(1)
    4.8.4 Shaft-type field
    238(2)
    4.8.5 Change of various parameters of the experiment
    240(8)
    5 Propagation of wave beams of finite width in inhomogeneous magnetized ferrite films
    248(93)
    5.1 Spatial transformation of wide beams of SMSW propagating in inhohogensouly magnetized films
    248(5)
    5.1.1 Linearly inhomogeneous field
    249(2)
    5.1.2 Valley-type field
    251(1)
    5.1.3 Shaft-type field
    252(1)
    5.2 Method for analysis of amplitude-frequency and phase-frequency characteristics of transmission lines of SMSW
    253(7)
    5.2.1 General scheme of the method for calculating the frequency phase responses
    253(3)
    5.2.2 Frequency response diagram
    256(1)
    5.2.3 PFC construction scheme
    257(3)
    5.3 Amplitude-frequency characteristics of transmision lines on ferrite films magnetized by fields of different configurations
    260(17)
    5.3.1 Homogeneous field
    260(5)
    5.3.2 Linearly inhomogeneous field
    265(2)
    5.3.3 Valley-type field
    267(3)
    5.3.4 Shaft-type field
    270(7)
    5.4 Ampliture--frequency characteristics of waveguard channel for SMSW formed by inhomogeneous `shaft'-type field
    277(7)
    5.4.1 Changing the length of the channel
    278(1)
    5.4.2 Changing the channel excitation conditions
    279(1)
    5.4.2.1 Symmetrical arousal
    280(1)
    5.4.2.2 Asymmetrical excitement
    281(1)
    5.4.2.3 Transverse shift of the emitting transducer
    282(2)
    5.5 Amplitude--frequency characteristics of the transmission line to the SMSW at an arbitrary orientation of the magnetizing field
    284(7)
    5.5.1 The general geometry of two variants of the location of the transducers: mutually opposite and mutually shifted
    284(2)
    5.5.2 Filtration of the first type, mutually opposite geometry
    286(3)
    5.5.3 Filtering of the second type, mutually shifted geometry
    289(2)
    5.6 Experimental study of SMSW beams of finite width and amplitude - frequency characteristics
    291(8)
    5.6.1 Linearly inhomogeneous field
    292(1)
    5.6.2 Valley type field
    293(1)
    5.6.3 Shaft-type field
    294(5)
    6.1 Amplitude-frequency properties of trasmission lines on magnetostatic waves taking into account the phase run
    299(1)
    6.1 General characteristics of typical transmission lines to SMSW
    299(1)
    6.2 General case of waves in a magnetic medium
    300(6)
    6.3 The case of surface magnetostatic waves (SMSW)
    306(1)
    6.4 Amplitude transmission line characteristics and its different geometric parameters
    307(10)
    6.4.1 Dependence of the amplitude of the transmitted signal on frequency when changing the relative orientation of the transducers
    308(2)
    6.4.2 Dependence of the amplitude of the transmitted signal on the frequency with a change in the width of the wave beam
    310(1)
    6.4.3 Dependence of the amplitude of the transmitted signal on the relative orientation of the transducers at a fixed signal frequency
    311(4)
    6.4.4 Dependence of the phase of the transmitted signal on frequency when changing the relative orientation of the transducers
    315(2)
    6.5 Effect of the phase run on AFC
    317(8)
    6.5.1 Geometry of the problem with relative mutual displacement of transducers
    318(1)
    6.5.2 Formation of the amplitude-frequency characteristic
    319(2)
    6.5.3 Formation of the phase-frequency response
    321(1)
    6.5.4 The influence of the length of the transducers on the structure of the frequency response
    322(3)
    6.6 Deformation of the wave front of surface magnetostatic waves in ferrite films magnetized by linearly inhomogeneous field
    325(9)
    6.6.1 General geometry of the problem
    325(3)
    6.6.2 Various cases of orientation of the emitting transducer
    328(1)
    6.6.2.1 Orientation corresponding to Φ= 30°
    328(3)
    6.6.2.2 Other orientations
    331(3)
    6.6 General character of transformation of the area of distribution of SMSW when various parameters of the structure change
    334(3)
    6.6.1 Changing the orientation of the emitting transducer
    334(1)
    6.6.2 Frequency change
    335(1)
    6.6.3 Changing the gradient of the field
    336(1)
    6.7 Recommendations for optimizing the parameters of the transmission line of the SMSW
    337(4)
    7 Use of magnetostatic waves in inhomogeneously magnetic ferrite films for information processing devices and other technical applications
    341(24)
    7.1 Brief overview of possible technical applications
    341(2)
    7.2 Wave guiding structures for SMSW on ferrite films magnetized by a shaft-type field
    343(3)
    7.3 Optimization of the shape of SMSW converters for devices on inhomogeneous magnetized ferrite films
    346(3)
    7.4 Multi-channel filter on ferrite film magnetized by a valley-type field
    349(2)
    7.5 Multi-channel filter on packed ferrite structures
    351(4)
    7.6 Microwave signal delay line on a ferrite film magnetized by a shaft-type field
    355(2)
    7.7 Measurements of parameters of yttrium iron garnet films with a complex anisotropy character
    357(2)
    7.8 Study of the spatial distribution of the magnetic field with the help of the sensor on the SMSW
    359(1)
    7.9 Use of the transmission line to SMSW to determine the orientation of the magnetic field
    360(5)
    Bibliography 365(35)
    Index 400
    V.G. Shavrov, Professor, Russian Academy of Science, Moscow, RU V.S. Shcheglov, Professor, Russian Academy of Science, Moscow, RU