SU1698856A1 - Method of determining width of ferromagnetic resonance line in ferrite films at microwave frequencies - Google Patents
Method of determining width of ferromagnetic resonance line in ferrite films at microwave frequencies Download PDFInfo
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- SU1698856A1 SU1698856A1 SU894718181A SU4718181A SU1698856A1 SU 1698856 A1 SU1698856 A1 SU 1698856A1 SU 894718181 A SU894718181 A SU 894718181A SU 4718181 A SU4718181 A SU 4718181A SU 1698856 A1 SU1698856 A1 SU 1698856A1
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- width
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- magnetic field
- ferromagnetic resonance
- resonance line
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Abstract
Изобретение предназначено дл измерени ширины линии ферромагнитного резонанса в пленках феррита на ( СВЧ. Цель изобретени - расширение функциональных возможностей за счет измерени толстых пленок большого диаметра. Определение ширины линии ферромагнитного резонанса осуществл етс путем расчета по формуле, при регистрации момента генерации СВЧ- сигнала на частоте, равной половине частоты входного СВЧ-магнитного пол , 2 и л оThe invention is intended to measure the width of a ferromagnetic resonance line in ferrite films (microwave. The purpose of the invention is to expand the functionality by measuring thick films of large diameter. Determining the width of the ferromagnetic resonance line is carried out by calculating the formula when registering the generation time of a microwave signal at a frequency equal to half the frequency of the input microwave magnetic field, 2 and l o
Description
Изобретение относитс к радиоизмерени м на СВЧ и может быть использовано дл измерени ширины линии ферромагнитного резонанса в пленках феррита на СВЧ.The invention relates to radio measurements on microwave and can be used to measure the width of the ferromagnetic resonance line in ferrite films on microwave.
Целью изобретени вл етс расширение диапазона измер емых пленок.The aim of the invention is to expand the range of measured films.
На фиг. 1 приведена функциональна схема, реализующа способ измерени ; на фиг. 2 - зависимость мощности выходного сигнала о возбудител х на половинной частоте от мощности входного сигнала.FIG. 1 shows a functional diagram implementing the measurement method; in fig. 2 shows the dependence of the output power of the exciters at half the frequency on the power of the input signal.
Способ осуществл етс следующим образом.The method is carried out as follows.
Входной сигнал переменного уровн мощности на частоте 6) поступает с генератора 1 на возбудитель 2 ферри- товой пленки 3. В качестве возбудител может использоватьс отрезок микрополосковой линии (11Ш1) . С выхода возбудител сигнал Рвь1){ подаетс на приемник 4, который выдел етThe input signal of a variable power level at a frequency of 6) is fed from the generator 1 to the exciter 2 of the ferrite film 3. A segment of the microstrip line (11Š1) can be used as the exciter. From the output of the exciter, the signal Pvb1) {is fed to the receiver 4, which selects
из него спектральную компоненту на частоте(J/2. Возбудитель с феррито- вой пленкой помещены во внешнее магнитное поле HO. При подаче сигнала на магнитнополосковую линию в пленке феррита возбуждаетс магнитостати- ческа волна (МСБ), например, поверхностна . Если уровень входно. мощности Pnv, превышает пороговый уровеньfrom it, the spectral component at the frequency (J / 2. The causative agent with a ferrite film is placed in an external magnetic field HO. When a signal is fed to a magnetic strip line in a ferrite film, a magnetostatic wave (MSB) is excited, for example, surface. If the level is input. power Pnv, exceeds threshold level
DADA
Рпор , то происходит параметрическое возбуждение спиновых волн на частоте 0)/2. Спиновые волны в свою очередь возбуждают I D и на ее выходе по вл етс спектральна компонента на частоте (0/2. По вление этой компоненты на выходе МПЛ соответствует достижению мощности оходного сигнала порогового уровн (фиг с 2). Величина порогового уровн мощности пропорциональна квадрату ширины линчи ФМР.Ppor, then a parametric excitation of spin waves occurs at a frequency of 0) / 2. Spin waves, in turn, excite ID and at its output a spectral component appears at the frequency (0/2. The appearance of this component at the output of the MLR corresponds to the achievement of the power of the bypass signal of the threshold level (FIG. 2). The threshold power level is proportional to the square of the width lynch frm.
шsh
сwith
фf
со ооwith oo
0000
сдsd
аbut
AHR К |pnop Z6 /2w,AHR K | pnop Z6 / 2w,
де Рde P
ПорPore
ww
КTO
J1698856J1698856
пороговый уровень мощности; волновое сопротивление микрополосковой линии; ширина микрополосковой линии;threshold power level; the impedance of the microstrip line; microstrip width;
инструментальна константа .instrumental constant.
с ди ни СВ ча пул ри са from di ni sv cha pul ri sa
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Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
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SU894718181A SU1698856A1 (en) | 1989-07-10 | 1989-07-10 | Method of determining width of ferromagnetic resonance line in ferrite films at microwave frequencies |
Applications Claiming Priority (1)
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SU894718181A SU1698856A1 (en) | 1989-07-10 | 1989-07-10 | Method of determining width of ferromagnetic resonance line in ferrite films at microwave frequencies |
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SU1698856A1 true SU1698856A1 (en) | 1991-12-15 |
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SU894718181A SU1698856A1 (en) | 1989-07-10 | 1989-07-10 | Method of determining width of ferromagnetic resonance line in ferrite films at microwave frequencies |
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SU (1) | SU1698856A1 (en) |
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1989
- 1989-07-10 SU SU894718181A patent/SU1698856A1/en active
Non-Patent Citations (1)
Title |
---|
Шлеман Е. и др. Нелинейные свойства ферритов в пол х СВЧ. И., 1963, с. 34. 54) СПОСОБ ОПРЕДЕЛЕНИЯ ШИРИНЫ ЛИШИ ФЕРРОМАГНИТНОГО РЕЗОНАНСА В ПЛЕНКАХ ФЕРРИТА НА СВЧ . * |
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