Hasil Pencarian  ::  Simpan CSV :: Kembali

Abstrak :
ABSTRAK
Material La0,8Ca0,2MnO3 merupakan salah satu bahan lanthanum manganite yang memiliki rasio magnetoresistansi yang tinggi. Resistivitas dan temperatur transisi metal-insulator dipengaruhi oleh jumlah ion Mn4, jarak Mn-O dan sudut Mn-O. Subtitusi Ag pada Ca dapat meningkatkan jumlah Mn4 dan memperbesar sudut Mn-O-Mn karena Ag memiliki jari-jari ionik lebih besar serta muatannya lebih kecil. Sampel disintesis menggunakan metode sol-gel dengan variasi doping x = 0; 0,03; 0,07; 0,1; dan 0,15. Sampel yang telah dihasilkan dikarakterisasi dengan menggunakan XRD untuk mengetahui struktur kristal, parameter kisi dan volume unit cell. Berdasarkan hasil XRD, pemberian doping Ag menyebabkan transformasi struktur kristal dari orthorombic menjadi rhombohedral. Parameter kisi a dan c serta volume unit cell meningkat dengan bertambahnya doping Ag. Komposisi dari sampel dianalisis menggunakan Energy Dispersive X-ray EDX . Hasil EDX menunjukkan komposisi sampel terdiri dari seluruh unsur yang diharapkan yaitu La, Ca, Ag, Mn dan O dan tidak terdapat impuritas. Resistivitas dan nilai MR diukur dengan menggunakan cryogenic magnetometer. Resistivitas menurun dengan penambahan doping Ag serta temperatur metal-insulator mengalami peningkatan dengan bertambahnya Ag. Peningkatan doping Ag tidak berkorelasi linear dengan perubahan MR pada sampel La0,8Ca0,2-xAgxMnO3

---

ABSTRACT
Material La0,8Ca0,2MnO3 is one of lanthanum manganite compounds having high magnetoresistance (MR). The resistivity and metal insulator transition temperature are influenced by the number of Mn4+ ions, the Mn-O distance and the Mn-O-Mn angle. Substitution of Ag in Ca site can increase the amount of Mn4+ and enlarge the angle of Mn-O-Mn since Ag has a larger ionic radius and a smaller valency. All Samples were synthesized using sol gel method with doping variation x=0; 0.03; 0.07; 0.1 And 0.15. The samples that have been produced are characterized by using XRD to find out the crystal structure, lattice parameters and unit cell volume. XRD results show that the increment of doping Ag leads to transform the crystal structure from orthorombic to rhombohedral. The lattice parameters a and c and unit cell volume increase with increasing doping Ag. The composition of the sample were analysed by using SEM-EDX. The results show that the composition of the sample consists of La, Ca, Ag, Mn and O without additional impurities. Resistivity and MR values are measured using cryogenic magnetometers. Resistivity decreases with increment of Ag doping and metal insulator transition temperature increases with increasing Ag. The change of MR does not depend on increment of doping Ag in the La0,8Ca0,2-xAgxMnO3 sample.

Abstrak :
This paper reports on the magnetic properties and electromagnetic characterization of La0.8Ba0.2FexMn½(1-x)Ti½(1-x)O3 (x = 0.1–0.8). The La0.8Ba0.2FexMn½(1-x)Ti½(1-x)O3 (x = 0.1–0.8) materials were prepared using a mechanical alloying method. All the materials were made of analytical grade precursors of BaCO3, Fe2O3, MnCO3, TiO2, and La2O3, which were blended and mechanically milled in a planetary ball mill for 10h. The milled powders were compacted and subsequently sintered at 1000°C for 5h. All the sintered samples showed a fully crystalline structure, as confirmed using an X-ray diffractometer. It is shown that all samples consisted of LaMnO3 based as the major phase with the highest mass fraction up to 99% found in samples with x < 0.3. The mass fraction of main phase in doped samples decreased in samples with x > 0.3. The hysteresis loop derived from magnetic properties measurement confirmed the present of hard magnetic BaFe12O19 phase in all La0.8Ba0.2FexMn½(1-x)Ti½(1-x)O3 (x = 0.1–0.8) samples. The results of the electromagnetic wave absorption indicated that there were three absorption peaks of ~9 dB, ~8 dB, and ~23.5 dB, respectively, at respective frequencies of 9.9 GHz, 12.0 GHz, and 14.1 GHz. After calculations of reflection loss formula, the electromagnetic wave absorption was found to reach 95% at the highest peak frequency of 14.1 GHz with a sample thickness of around 1.5 mm. Thus, this study successfully synthesized a single phase of La0.8Ba0.2FexMn½(1-x)Ti½(1-x)O3 (x = 0.1–0.8) for the electromagnetic waves absorber material application.

Abstrak :
Material keramik Lanthanum Manganite La0.8(Ba1-xSrx)0.2MnO3 berhasil disintesis menggunakan metode sol-gel dengan variasi komposisi doping x = 0; 0.5; 0.75; dan 1.0. Penelitian terdahulu diketahui material LBMO dan LSMO memiliki sifat penyerapan gelombang mikro di pita frekuensi C-Band dan X-Band. Melalui penelitian ini, sifat penyerapan gelombang elektromagnetik dipelajari pada material lantanum manganit yang diberikan doping Ba (Barium) dan Sr (Strontium) menjadi material LBSMO. Parameter kisi kristal dan ukuran partikel semakin mengecil seiring meningkatnya substitusi Sr daripada Ba. Ukuran rata-rata partikel terkecil diraih variasi x = 1.0 senilai 107 nm. Sifat magnetik material menjadi salah satu kriteria penentu sifat penyerapan gelombang mikro. Material teridentifikasi sebagai material magnetik lunak, lalu sifat magnetiknya semakin kuat seiring meningkatnya substitusi Sr daripada Ba. Pada medan magnet 1 Tesla nilai magnetisasi (M) terbaik diraih variasi x = 1.0 senilai 58.67 emu/gr. Kemampuan penyerapan gelombang mikro material telah diuji VNA pada frekuensi 7—13 Ghz. Hasilnya variasi x = 0.75 memiliki kemampuan penyerapan yang terbaik dengan nilai Reflection Loss -7.4 dB pada frekuensi 11.94 GHz. Semakin besar komposisi x, maka peristiwa penyerapan bergeser menuju frekuensi yang semakin tinggi. ......Ceramic Lanthanum Manganite La0.8(Ba1-xSrx)0.2MnO3 was successfully synthesized using the sol-gel method with variations in composition x = 0; 0.5; 0.75; and 1.0. Previous research found that LBMO and LSMO materials have microwaves absorption properties in the C-Band and X-Band frequency. The absorption properties of electromagnetic waves were studied here in lanthanum manganite doped with Ba (Barium) and Sr (Strontium) to become LBSMO material. The crystal lattice parameters and particle size decreased with increasing Sr substitution over Ba. The smallest mean particle size achieved by the x = 1.0 with value of 107 nm. The magnetic property of the material is one of the criteria for determining the absorption properties of microwaves. The material is identified as soft magnetic material, then its magnetic properties get stronger as the Sr substitution increases over Ba. When 1 Tesla of magnetic field applied, the highest magnetization (M) achieved by the variation x = 1.0 with value of 58.67 emu/gr. The material's microwaves absorption capability has been tested by VNA in the 7—13 Ghz frequency. The result is that the variation x = 0.75 has the best absorption capability with a Reflection Loss value of -7.4 dB at a frequency of 11.94 GHz. The greater the composition of x, the absorption occur shifted towards higher frequencies.

Abstrak :
Beberapa dekade terakhir ini peredam gelombang elektromagnetik (microwave absorber) dari bahan magnetik telah banyak digunakan untuk aplikasi di bidang pertahanan militer, elektronik dan telekomunikasi. Secara sederhana dapat dikatakan bahwa bahan absorber gelombang elektromagnetik adalah sebuah bahan yang dapat melemahkan energi gelombang elektromagnetik. Bahan-bahan yang memiliki kriteria sebagai bahan absorber gelombang elektromagnetik adalah bahan harus memiliki karakteristik permeabilitas (magnetic loss properties) dan permitivitas (dielectric loss properties). Kandidat potensial sebagai bahan absorber gelombang elektromagnetik adalah bahan magnetik sistem ABO3 perovskite lanthanum manganite. Dengan rekayasa struktur sistem lanthanum manganite ini diharapkan dapat menjadi bahan unggul untuk aplikasi microwave absorber. Pengembangan bahan magnetik yang dilakukan dalam penelitian ini mencakup sistem La(1-y)BayFexMn½(1-x)Ti½(1-x)O3 (x = 0 - 1,0 dan y = 0 - 1,0) telah diperoleh komposisi yang paling baik yaitu komposisi senyawa La0.8Ba0.2Fe0.3Mn0.35Ti0.35O3. Sintesis nanopartikel senyawa La0.8Ba0.2Fe0.3Mn0.35Ti0.35O3 fase tunggal telah berhasil diperoleh melalui metode pemaduan mekanik dilanjutkan dengan tahapan sintering pada suhu 1000 °C selama 10 jam. Sintered materials kemudian dihaluskan kembali selama 20 jam. Hasil refinement pola difraksi sinar-x menunjukkan bahwa senyawa La0.8Ba0.2Fe0.3Mn0.35Ti0.35O3 memiliki struktur monoklinik dengan parameter kisi a = 5,5182(8) Å, b = 5,5442(8) Å, c = 7,822(1) Å, dan  = 89,63(1)o. Ukuran rata-rata kristalit partikel senyawa La0.8Ba0.2Fe0.3Mn0.35Ti0.35O3 adalah 42 nm. Sedangkan ukuran rata-rata partikelnya berdasarkan pengujian dengan Particle Size Analyser adalah 72 nm. Material bersifat ferromagnetik memiliki karakteristik nilai permeabilitas dan permitivitas yang baik. Hasil pengujian serapan gelombang elektromagnetik pada rentang frekuensi 9 - 15 GHz menunjukkan bahwa terdapat tiga frekuensi puncak serapan pada frekuensi 9,9 GHz, 12,0 GHz, dan 14,1 GHz dengan nilai reflection loss berturut-turut sebesar ~ 9 dB, ~ 13 dB, dan ~ 25 dB. Disimpulkan bahwa bahan sistem La(1-y)BayFexMn½(1-x)Ti½(1-x)O3 (dengan x = 0 - 1,0 dan y = 0 - 1,0) menjadi kandidat yang potensial untuk digunakan sebagai bahan unggul absorber gelombang elektromagnetik.

---

Recently electromagnetic wave absorber materials haves been used for military, electronic, and telecommunication devices. In a very simple definition, electromagnetic wave absorber material is a material that can weaken the electromagnetic wave energy. Basic properties which are required of electromagnetic wave absorber materials were that the materials must have high permeability (magnetic loss properties) and high permittivity (dielectric loss properties) values. One of potential candidates for absorbing materials is ABO3 perovskite lanthanum manganite-based system. Structurals modification of the basic lanthanum manganite was applied in order to find the best the microwave absorber characteristics of the modified materials system. Current research activities were covering La(1-y)BayFexMn½(1-x)Ti½(1-x)O3 (x = 0 - 1.0 and y = 0 - 1.0) compositions. It was found that the best composition with an improve microwave absorption characteristic is La0.8Ba0.2Fe0.3Mn0.35Ti0.35O3. Single phase of La0.8Ba0.2Fe0.3Mn0.35Ti0.35O3 nanoparticles were successfully synthesized by mechanical alloying method. The mixture of all precursors were first mechanically milled for 10 hrs and then sintered at a temperature of 1000 °C for 10 hrs in which a fully crystalline material is ensured. The sintered material was then re-milled for 20 hrs to obtain powder-based nanoparticles. The refinement of x-ray diffraction trace for re-milled materials confirmed a single phase material with a monoclinic structure of lattice parameters: a = 5.5182(8) Å, b = 5.5442(8) Å, c = 7.822(1) Å, and  = 89.63(1)o. The mechanically alloyed and sintered materials in the whole mechanical milling resulted in powders with mean crystallite size 42 nm. The mean particle size as refering to the particle size analyzer was 72 nm in the second mechanically milled powders. Thus, results of mean crystallite size and crystallite size evaluations for the powder materials showed that the mean crystallite zise is almost similar to the mean particle size. In addition, the hysteresis curve evaluation showed that the sample material is ferromagnetic. Results of VNA evaluation indicated that there were three of absorption peaks with reflection loss values ~ -9.0 dB, ~ -11.5 dB, and ~ -25.0 dB at frequency 9.9 GHz, 12.0 GHz, and 14.1 GHz respectively. The study concluded that the magnetic materials of La(1-y)BayFexMn½(1-x)Ti½(1-x)O3 compositions (x = 0 - 1,0 and y = 0 - 1) have a good potential to be a candidate of electromagnetc wave absorbing materials.