Hasil Pencarian  ::  Simpan CSV :: Kembali

"ABSTRAKTelah dilakukan pembuatan lapisan tipis Barium Zirkonium Titanat denganmenggunakan metode CSD (Chemical Solution Deposition) pada substrat Pt.Perbandingan komposisi Zr : Ti, temperatur annealing, tebalnya lapisan, danwaktu penahanan temperatur annealing menjadi variabel untuk mendapatkan filmtipis BZT yang terbaik. BZT dengan variasi perbandingan Zr : Ti sebesar 0,1 : 0,9,temperatur annealing 800°C, dan jumlah lapisan sebanyak 5 lapis didapatkansebagai variabel terbaik. Variabel BZT terbaik digunakan sebgai variabel untukpendopingan dengan Indium, kemudian hasilnya dianalisa dan diperhitungkansecara teoritik polarisasi spontan dari BZT yang didoping dengan Indium yangnilainya sebesar 22.93 μC/cm

---

AbstractExperimental study on making of Barium Zirconium Titanate thin films using theCSD (Chemical Soulution Deposition) method on Pt substrate is reported. Theratio between Zr : Ti, annealing termperature, film thickness, and annealingtemperature holding time are the variable to achieve best BZT thin films. BZTwith Zr : Ti ratio 0,1 : 0,9, annealing temperature 800°C, and layer number 5 arethe best result acquired. The best BZT result is used as variable for doping withIndium, then the result will be analyzed and calculated the spontaneouspolarization teoritically from BZT doped by Indium and the spontaneouspolarization is 22.93 μC/cm2.;"

"Dalam penelitian ini telah dilakukan pembuatan material ferroelektrik Ba0.5Sr0.5TiO3 yang didoping dengan Mg asetat (BSMT) dengan metode Chemical Solution Deposition (CSD) dengan teknik spin coating pada kecepatan putar 3000 rpm selama 30 detik . Proses annealing dilakukan pada temperatur 800oC selama 3 jam. Variabel penelitian adalah persentase doping (0%, 1%, 2% dan 4% berat) dan jenis subtrat (Si dan Pt).Material lapisan tipis BSMT yang terdeposisi pada substrat Si dan Pt diuji komposisinya dengan XRF dan sistem kristalnya dengan XRD. Data XRF membuktikan bahwa material BSMT yang dibuat terdiri atas komponen Ba, Sr Ti dan Mg. Hasil penghalusan data dengan GSAS menunjukkan adanya kesesuaian dengan Ba0.5Sr0.5TiO3 dari ICDD dengan sistem kristal kubik. Hasil SEM menunjukkan adanya crack pada permukaan yang terjadi pada saat annealing akibat adanya perbedaan thermal expansion coefficient antara BST/BSMT dan substrat.Plot hasil pengukuran polarisasi BST dan BMST membentuk kurva histeresis yang berarti bahwa material tersebut mempunyai sifat ferroelektrik. Doping Mg mengakibatkan adanya kenaikan nilai medan koersif (Ec) pada lapisan dengan substart Pt, sedangkan pada lapisan dengan substrat Si terjadi sebaliknya.

---

In this research, ferroelectric material Ba0.5Sr0.5TiO3 doped Mg have been manufactured by Chemical Solution Deposition (CSD) method with spin coating technique on 3000 rpm for 30 seconds. The process of annealing was done by temperature 800oC for 3 hours. The variation of doping are 0%, 1%, 2% and 4% weight of Mg and substrate types are Si and Pt.

Composition of thin film material BSMT deposited on Si and Pt substrate were determined by XRF and crystal system are determined by XRD. XRF data indicates that the film are composed by Ba, Sr, Ti and Mg element. Result of refining XRD data by GSAS corespond to material Ba0.5Sr0.5TiO3 from ICDD with cubic crystal system. SEM photogragh indicate that there are crack on surface of film that happend during annealing because of differential of thermal expansion coefficient between BST/BSMT dan substrate.

Plot of result of polarisation measurement draw hysteresis. It is mean that the material has ferroelectric caracterization. Doping Mg effects Coersief Field (Ec) increase for substrat Pt, but decrease for substrat Si."

"Barium Titanate telah diketahui memiliki karakteristik yang dapat dimanfaatkan dalam berbagai aplikasi. Barium Titanate merupakan material dielektrik non-linier yang bebas dari kandungan Plumbum. Konstanta dielektrik dan permitivitas yang tinggi dibandingkan material ferroelektrik lain dan adanya arus bocor yang relatif tinggi menjadikan barium titanate menarik untuk diteliti lebih lanjut. Ion Zirconium merupakan substituent efektif Barium Titanate untuk mengurangi arus bocor dikarenakan ion Zirconium cenderung lebih stabil dibandingkan ion Titanium. Lapisan tipis barium titanate yang disubstitusi dengan ion Zr(0,08 dan 0,1) dihasilkan melalui metode Chemical Solution Deposition yang dilanjutkan melalui spin coating dan perlakuan panas. Larutan BaZrTiO3 dideposisikan pada substrat Si hingga 3-5 lapisan dengan kecepatan putar 3000 rpm selama 30 s dilanjutkan dengan pirolisis pada 300°C dan annealing pada 700°C-800°C. Karakterisasi pada lapisan tipis BZT menitikberatkan pada sifat kristalografi melalui XRD dan uji histerisis. Uji histerisis dilakukan dengan sumber tegangan AC dengan 20 Vpp pada frekuensi 60 Hz. Pola XRD menunjukkan adanya peningkatan ukuran kristalit terbesar pada 800°C sekitar 113 nm dengan menggunakan metode Williamson-Hall. Perbedaan Zr pada struktur BaTiO3 menggeser bidang hkl pada 2θ. Dengan jumlah lapisan BaZrTiO3 meningkat, polarisasi pada histerisis ferroelektrik cenderung tetap.

---

Barium Titanate is well known materials for many applications. It is nonlinear dielectric material and lead free based material, then this material is enviromental friendly. High dielectric constant and permitivity compared with other ferroelectric materials dan the high leakage current make barium titanate more interesting for further development. Zirconium ion is effective substituent of Barium Titanate to reduce leakage current. This is possible because Zirconium ion more stable than Titanium ion.

Barium Titanate thin films Zr-doped(0.08 and 0.1 mol) is produced by Chemical Solution Deposition and continued by spin coating and heat treatment. BaZrTiO3 solution 0.5M is deposited on Si substrate 3-5 layers with rotational speed up to 3000 rpm for 30 s then it was treated by pyrolisis on 300°C and annealing 700°C-900°C. BZT thin films is charaterized by XRD to know its crystallographic properties and hysterisis testing. Hysterisis loop is made by using AC voltage source with 20 Vpp at frequency of 60 Hz.

The XRD curves showed that crystalite size, based on Williamson-Hall calculation, is calculated around 113 nm for heat treatment 800°C. The different of Zr substitution in BaTiO3 structure shifted hkl plane on 2θ. Multilayer of BaZrTiO3 films on 0.1 Zr increase saturate polarization and decrease coersive field. In this case ferroelectric properties of BaZrTiO3 thin films increase, in contrary the low coersive field showed that easily loses its ferroelectric properties."

"Lapisan tipis Barium Zirkonium Titanat (BaZrxTi1-xO3) dengan doping lantanum telah berhasil ditumbuhkan diatas substrat Pt/Si denga metode sol gel yang dilanjutkan dengan spin coating. Proses yang dilakukan dalam pembuatan lapisan tipis terdiri dari tiga tahap yaitu, pembuatan larutan, proses spin coating, dan proses annealing. Beberapa parameter ditetapkan untuk mendapatkan optimalisasi proses pembuatan lapisan tipis yang meliput jenis substrat, jumlah lapisan, dan temperatur annealing. Optimalisasi didapatkan pada lapisan tipis yang tumbuh pada susbtrat Pt/Si dengan temperatur annealing 800°C. Tingkat kekristalan dan polarisasi listrik spontan optimal pada lapisan tipis BZT didapatkan pada komposisi BaZr0.1Ti0.9O3. Pada variasi jumlah mol dopan didapatkan polarisasi listrik spontan optimum pada 1% mol dopan dengan nilai polarisasi listrik spontan 25 μC/cm2.

---

Barium Zirconium Titanate thin films (BaZrxTi1-xO3) doped by lanthanum have been developed in Pt/Si substrates by using sol gel method followed by spin coating. Process was done by three steps which are solvent preparation, spin coating, and annealing process. Optimum parameters were done by varying substrate, quantity of layers, and annealing temperature. The optimum parameters of BZT thin film was found on 800°C for temperature of annealing process, the optimum crystalline film and electrical spontaneous polarization was found on BaZr0.1Ti0.9O3 and doped by 1% mol of lanthanum."

"Penelitian efek substitusi Ti pada paduan La0.85Ba0.15Mn(1-x)TixO3 ( x = 0, 0.1, 0.15, and 0.2) dipersiapkan dengan metode mechanical milling selama 25 jam, suhu kalsinasi sebesar 800oC selama 10 jam dan suhu sintering 1200oC selama 12 jam berdasarkan hasil uji TGA dan DSC. Kurva XRD (X-Ray Diffraction) menunjukkan fasa tunggal, sistem kristal monoklinik dengan group ruang (space group) ’I 1 2/c 1’ pada suhu ruang. Terdapat kenaikan pada parameter kisi, volum unit sel, dan ukuran kristalit rata-rata dengan meningkatnya substitusi Ti. Hasil SEM (Scanning Electron Microscopy) menunjukkan morfologi bahan, distribusi ukuran partikel dan porositas pada paduan. Ukuran partikel rata-rata paduan didapatkan dengan menggunakan Particle Size Analyzer (PSA). Rata-rata ukuran partikel meningkat setelah mendapatkan perlakuan pemanasan sintering.

---

Research on the effect of titanium substitution on the structure and the particle morphology characterization of manganites with La0.85Ba0.15Mn(1-x)TixO3 ( x = 0, 0.1, 0.15, and 0.2) was carried out. Materials were prepared by using a mechanical milling method for 25 hours. The calcination and sintering temperatures attained based on TGA and DSC results were 800o C for 10 hours and 1200o C for 12 hours. X-ray diffraction patterns of the width La0.85Ba0.15Mn(1-x)TixO3 ( x = 0, 0.1, 0.15, and 0.2) showed single phase, monoclinic system and space group ’I 1 2/c 1’at room temperature. Lattice parameters, volume unit cell, and mean crystallite size increased along with increases in Ti substitution. Scanning electron microscopy (SEM) showed the morphology, surface, distribution of particle size, and porosity of the compound. The mean particle size of the obtained compounds was determined by using a Particle Size Analyzer. Mean particle size increased after the use of the sintering process."

"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."

"ABSTRAKAntimony (Sb) doped tin oxide (ATO) merupakan salah satu material transparan yang telah mendapatkan popularitas lebih akhir-akhir ini karena sangat berperan penting terhadap teknologi. transparansi tinggi pada cahaya tampak, konsentrasi dan mobilitas elektron tinggi membuat ATO sebagai bahan penting untuk oksida transparan konduktif, display flat-panel, sel surya, jendela arsitektur perangkat optoelektronik dan sensor gas. Dalam penelitian ini, lapisan tipis antimony doped-tin oxide (ATO) dibuat dengan biaya rendah dan sederhana menggunakan metode ultrasonic spray pyrolysis. Lapisan tipis ATO telah ditumbuhkan dengan menvariasikan konsentrasi doping antimon (0%, 1%, 2%, 3% Sb) dan waktu deposisi (10, 20, 30 menit). Sifat struktural, morfologi, optik dan listrik dari lapisan ini telah dianalisis dengan difraksi sinar-X, mikroskop elektron, UV-VIS dan instrumen four point probe. Analisis XRD menunjukkan bahwa semua lapisan polikristalin dengan struktur kristal tetragonal. Analisis sifat optik dan listrik menunjukkan bahwa konsentrasi optimum doping Sb telah diperoleh untuk meningkatkan transparansi danmeningkatkan konduktivitas listrik lapisan tipis timah oksida

---

ABSTRACTAntimony (Sb) doped tin oxide (ATO) is one transparent material that has gained its popularity more recently due to their great technological importance. High transparency in the visible light, high concentration and mobility of electron makes ATO as an important material for the field of transparent conducting oxide, flat-panel display, solar cell, architectural windows optoelectronic devices and gas sensor. In this study, Sb doped-tin oxide (ATO) thin films has been fabricated by low cost and simple, ultrasonic spray pyrolysis method. ATO thin films have been deposited with various antimony doping concentrations (0%, 1%, 2%, 3% Sb) and time deposition(10, 20, 30 minutes). The structural, morphological, optical and electrical properties of these films have been analyzed by X-ray diffraction, scanning electron microscopy, UV-VIS and four point probe instruments. XRD studies show that all films are polycrystalline with tetragonal crystal structure. The optic and electric properties studies show that the concentration optimum of Sb doping has been obtained to increase transparency and improve the electrical conductivity of tin oxide thin film."

"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."

"Nanorods ZnO telah menarik minat banyak peneliti karena memiliki karakteristik unik yang berpotensi untuk diaplikasikan pada berbagai divais seperti light-emitting diode (LED), dye-sensitized solar cells (DSSC), dan field-effect transistor. Pengaturan parameter-parameter sintesis untuk mendapatkan karakteristik nanorods ZnO yang sesuai dengan aplikasi-aplikasi strategis tersebut telah dilakukan oleh banyak peneliti. Namun, belum banyak penelitian yang berkaitan dengan karakteristik nanorods ZnO yang sesuai untuk aplikasi pemanasan transparan yang menggabungkan performa panas dan transparansi optik yang tinggi. Oleh karena itu, penelitian ini bertujuan untuk menyelidiki pengaruh variasi waktu pertumbuhan dan temperatur larutan bibit pada sifat optik dan elektrotermal lapisan tipis nanorods ZnO untuk aplikasi pemanas transparan. Untuk keperluan investigasi, larutan bibit disiapkan pada suhu 0, 30, dan 60 ℃ selama 1 jam dengan menggunakan seng nitrat tetrahidrat dan hexamethylenetetramine sebagai prekursor. Lapisan bibit tersebut kemudian diteteskan ke atas substrat kaca ITO dan didiamkan selama 10 menit. Selanjutnya, kaca ITO yang telah ditetesi larutan bibit tersebut diputar menggunakan spin coater dengan kecepatan 2000 rpm selama 20 detik lalu dianil pada temperatur 200℃ selama 5 menit. Setelah proses spin coating, lapisan nanorods ZnO ditumbuhkan menggunakan metode chemical bath deposition (CBD) pada suhu 90 ℃ dengan variasi waktu pertumbuhan yang berbeda (3, 4, dan 5 jam). Sampel yang telah disintesis dikarakterisasi menggunakan X-Ray Diffractometer (XRD), scanning electron microscope (SEM), ultraviolet-visible (UV-Vis) spectrophotometry. Untuk melihat hubungan antara struktur dan morfologi sampel dengan karakterisik optik dan elektrotermalnya, resistivitas listrik diukur menggunakan four-point probe dan performa panas menggunakan termokopel. Hasil penelitian menunjukkan bahwa kinerja pemanas transparan optimal yang menggabungkan transmitansi tinggi dan resistivitas rendah ditemukan dalam sampel yang disiapkan dengan temperatur larutan bibit 30°C dan waktu pertumbuhan 3 jam dengan resistivitas sekitar 0,882×10−4 ohm.cm dan transmitansi sebesar 60,01%. Selain itu, nanorods ZnO dengan waktu pertumbuhan yang lebih lama, kristalinitas yang lebih baik, cakupan substrat yang baik dengan ukuran diameter yang seragam menunjukkan suhu keadaan tunak (steady-state temperature) dan laju pemanasan/pendinginan yang tinggi. Namun, transparansi optiknya menurun secara bertahap dengan pertambahan waktu tumbuh yang diduga sebagai konsekuensi dari peningkatan cakupan nanorods ZnO pada substrat

---

ZnO nanorods have been attracting much interest of researchers owing to their unique properties and extensive potential for various applications including light-emitting diode, dye-sensitized solar cells, and field-effect transistor. Controlling synthesis parameters to obtain the desired characteristics of ZnO nanorods for those strategic applications has been done by many investigators. However, there has not been much research related to the suitable characteristics of ZnO nanorods required for a transparent heating application combining high thermal performance and optical transparency. Therefore, this study was aimed at investigating the effect of different growth time and seeds solution temperature on the optical and electrothermal properties of ZnO nanorods thin films. For investigation purposes, the seed solutions were initially prepared at the temperature of 0, 30, and 60℃ for 1 hour by using zinc nitrate tetrahydrate and hexamethylenetetramine as precursors. The ZnO seed layers were subsequently deposited onto ITO glass substrates by spin coating technique before the chemical bath deposition (CBD) growth at temperature of 90℃ for three different growth times (3, 4, and 5 hours). The synthesized ZnO nanorods were characterized by field-emission scanning electron microscopy, x-ray diffraction, and ultraviolet-visible spectrophotometry. To investigate the relationship between the structural and morphological characteristics of the synthesized ZnO nanorods with its electrothermal properties, we measured electrical resistivity using the Four Point Probe and heat performance using thermocouples. The results showed that optimum transparent heater performance combining high transmittance and low resistivity was found in samples prepared with seeds solution temperature of 30°C and growth time of 3 hours with resistivity of 0.882×10−4 ohm.cm and transmittance of 60.01%. In addition, the films for longer growth time with better crystallinity, good substrate coverage, and uniformity in their size exhibited a higher steady-state temperature with higher heating/cooling rate. However, its optical transparency decreased gradually with the prolongation of the growth time, which was expected as a consequence of the increase in ZnO nanorods coverage on the substrates."