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"Telah dilakukan perhitungan energi ikat, fungsi gelombang, rapat keadaan, rapat magnetisasi serta momen magnetik pada atom Co dan Ni padat dengan data potensial LMTO (Linear Muffin Tin Orbital) yang mempunyai karakteristik simetri sferis pada daerah sekitar inti serta datar I flat pada daerah antar inti. Fungsi gelombang dihitung secara numerik dari pendekatan Fox-Goodwin dengan hasil untuk potensial standar telah dicek kesesuaiannya dengan metode analitik. Pada perhitungan secara numerik juga ditandai dengan tercapainya keadaan konsistensi potensial. Dari perhitungan momen magnetik, diperoleh 1.69 magneton bohr untuk Co dan 0.51 magneton bohr untuk Ni.

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The calculation of binding energy, wave function, density of states, magnetization density and magnetic moment of Co and Ni used LMTO (linear Muffin Tin Orbital) has been investigated. The LMTO Potential model has characteristic symmetric within a sphere and to be zero/constant elsewhere. By Fox-Goodwin approximation, the numeric calculation of the basic wave function has been checked and the solution has been succeed/matched in compared by analytical solution. From the moment magnetic calculation, we have 1.69 magneton bohr for Co and 0.51 magneton bohr for Ni."

"ABSTRAKTelah dilakukan suatu studi pangembangan rangkaian Osilator Colpitts sebagai pengkondisi sinyal system pengukuran parameter Kerentanan magnetik bahan. Penelitian ini merupakan pengembangan lanjutan dari pemanfaatan rangkaian Osilator sebagai pengkondisi sinyal sensor resistif, kapasitif, dan Induktif.Dari pengukuran didapat bahwa frekuensi Osilator berbanding lurus dengan invers akar Induktansi, yang berarti pula berbanding lurus dengan invers akar parameter kerentanan magnetik bahan.

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ABSTRACT

A development study of Colpitts Oscillator circuit as The Magnetic Susceptibility parameter measurement system has described. This research is an advanced development of the usage of Oscillator as The Signal Conditioner part of resistive, capacitive, and inductive type of sensor.

Measurement yields a relation where Oscillator frequency equals to inverse of inductance root, these means that it also equal to inverse of root of sample's magnetic susceptibility parameter."

"Information about magnetic structure can not be obtained through X ray diffraction method. Therefore data from neutron diffraction are needed to find out substance magnetic structure. From that structure, we can get information about magnetic crystal structure and magnetic momentum or the structure of the spin. The research is aimed to find out magnetic structure at CaMnO3 dan LaMnO3 in powder. The preparation of CaMnO3 and LaMnO3 substance is made through powder method and stoikiometric calculation. Basic substance of CaMnO3 is CaCO3 and MnO2, while basic substance of LaMnO3 is La2O3 and MnO2. After the substances are mixed, time varied milling, temperature varied sintering and annealing are conducted. It is hoped that the substances will be united or form a new phase.The magnetic structure study of CaMnO3 and LaMnO3 at this research are explained by neutron powder diffraction. CaMnO3 is good analisis at crystal system on orthorhombic space group Pnma with lattice parameter at 12 k is a = 5.2692 Å, b = 7.4403 Å, c = 5.2596 Å. LaMnO3 is good analisis at crystal system on monoklinik space group P1121/a with lattice parameter at 12 K is a = 5.4726 Å, b = 7.7613 Å, c = 5.5324 Å. Magnetic parameter Mn atomic has charge ordered of CaMnO3 and LaMnO3 is Mn4+ ion and Mn3+ ion.Result at research with High Resolution Powder Diffractometer, HRPD to find, CaMnO3 has properties magnetic at Mn atomic with indeks miller hkl (011) angle θ 2 = 24.486 on 12 K. LaMnO3 has properties magnetic at Mn atomic with indeks miller hkl (200) and angle θ 2 = 38.966°. Magnetic structure Mn atomic at 4b(0,0, 2 1 ) simetri of CaMnO3 is four possible nonkolinear ferromagnetic, with value magnetic momen is m(Mn) = 1.73 B µ . Magnetic structure Mn atomic of LaMnO3 at 2c(0,0, 2 1 ) is two possible (antiferomagnetik and ferromagnetic) and 2d( 2 1 , 2 1 ,0) simetri is two possible antiferromagnetic, with value magnetic momen is m(Mn) = 2.23 B µ ."

"Pengujian tingkat ketelitian metode reduksi anomali medan magnetik total bumi ke kutub utara menggunakan sumber ekivalen dipol berbasis model komputasi telaah prisma tegak. Ketidakrataan permukaan topografi, variasi dimensi sumber anomali (distrubusi magnetisasi) dan ketidakteraturan distribusi titik pengukuran tidak berpengaruh secara signifikan terhadap ketelitian metode. Tingkat ketelitian metode sangat tergantung pada kedalaman lapisan sumber ekivalen dipol. Batas atas dan bawah kedalaman lapisan sumber ekivalen dipol tergantung pada spasi pengukuran. Batas atas kedalaman lapisan sumber ekivalen dipol dengan penyimpanan rata-rata di bawah 10 % berkisar 3 kai spasi pengukuran sedang batas bawah kedalaman lapisan sumber ekivalen dipol tergantung pada dimensi sumber anomali "