Pub Date : 2024-03-20DOI: 10.1134/s1064226923150159
L. Y. Fetisov, D. V. Savelev, F. A. Fedulov, D. V. Chashin, Y. K. Fetisov
Abstract
A resonant voltage frequency doubler using the nonlinear magnetoelectric effect in planar heterostructure containing a piezoelectric langatate single crystal placed between two layers of amorphous ferromagnetic Metglas alloy was fabricated and studied. The frequency doubling occurred due to the nonlinear dependence of the Metglas magnetostriction on the magnetic field. A nonlinear magnetoelectric coefficient of 7.1 V/(cm Oe2) was obtained at acoustic resonance frequency of the structure due to high acoustic quality factor of ~2820. The power conversion coefficient of the doubler reached ~1% at optimal bias magnetic field of 2 Oe and matched load resistance of 0.8 kΩ.
{"title":"Frequency Doubler Based on Nonlinear Magnetoelectric Effect in a Planar Metglas/Langatate/Metglas Heterostructure","authors":"L. Y. Fetisov, D. V. Savelev, F. A. Fedulov, D. V. Chashin, Y. K. Fetisov","doi":"10.1134/s1064226923150159","DOIUrl":"https://doi.org/10.1134/s1064226923150159","url":null,"abstract":"<h3 data-test=\"abstract-sub-heading\">Abstract</h3><p>A resonant voltage frequency doubler using the nonlinear magnetoelectric effect in planar heterostructure containing a piezoelectric langatate single crystal placed between two layers of amorphous ferromagnetic Metglas alloy was fabricated and studied. The frequency doubling occurred due to the nonlinear dependence of the Metglas magnetostriction on the magnetic field. A nonlinear magnetoelectric coefficient of 7.1 V/(cm Oe<sup>2</sup>) was obtained at acoustic resonance frequency of the structure due to high acoustic quality factor of ~2820. The power conversion coefficient of the doubler reached ~1% at optimal bias magnetic field of 2 Oe and matched load resistance of 0.8 kΩ.</p>","PeriodicalId":50229,"journal":{"name":"Journal of Communications Technology and Electronics","volume":"41 1","pages":""},"PeriodicalIF":0.5,"publicationDate":"2024-03-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140166078","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"计算机科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-03-20DOI: 10.1134/s1064226923150056
M. S. Domnina, A. S. Kryukovsky, D. V. Rastyagaev
Abstract
Methods for calculating the special function of wave catastrophe B4 and its first derivatives, which describe edge focusing of the caustic-tip type with an edge, are studied. The caustic and ray structures of this singularity are constructed. The characteristic amplitude–phase sections of the special function and its derivatives are calculated. The method of rotation of the integration contour and the method of ordinary differential equations are considered and compared both in terms of accuracy and speed. It is shown that the method of ordinary differential equations works stably in the region of negative values of the first two parameters of the special function, and the method of rotation of the integration contour exhibits stability in the region of positive values. Thus, the approaches are complementary. However, the calculation time for the method of ordinary differential equations is an order of magnitude less than the time for the method of rotation of the integration contour.
{"title":"Mathematical Modeling of the Wave-Field Structure in the Vicinity of Edge Catastrophe B4","authors":"M. S. Domnina, A. S. Kryukovsky, D. V. Rastyagaev","doi":"10.1134/s1064226923150056","DOIUrl":"https://doi.org/10.1134/s1064226923150056","url":null,"abstract":"<h3 data-test=\"abstract-sub-heading\">Abstract</h3><p>Methods for calculating the special function of wave catastrophe B<sub>4</sub> and its first derivatives, which describe edge focusing of the caustic-tip type with an edge, are studied. The caustic and ray structures of this singularity are constructed. The characteristic amplitude–phase sections of the special function and its derivatives are calculated. The method of rotation of the integration contour and the method of ordinary differential equations are considered and compared both in terms of accuracy and speed. It is shown that the method of ordinary differential equations works stably in the region of negative values of the first two parameters of the special function, and the method of rotation of the integration contour exhibits stability in the region of positive values. Thus, the approaches are complementary. However, the calculation time for the method of ordinary differential equations is an order of magnitude less than the time for the method of rotation of the integration contour.</p>","PeriodicalId":50229,"journal":{"name":"Journal of Communications Technology and Electronics","volume":"32 1","pages":""},"PeriodicalIF":0.5,"publicationDate":"2024-03-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140881779","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"计算机科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}