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Lattice Constants Analysis of Tantalum Oxide Doped Lead Zirconium Titanate Ceramic by Delphi Program Irzaman Irzaman; Y. Darvina; P. Arifin; M. Budiman; M. Barmawi
Indonesian Journal of Physics Vol 16 No 2 (2005): Vol. 16 No. 2, April 2005
Publisher : Institut Teknologi Bandung

Show Abstract | Download Original | Original Source | Check in Google Scholar | Full PDF (216.488 KB)

Abstract

Ceramics of PbZrxTi1-xO3 (PZT) and 0.5 %, 1 %, 1.5 % tantalum oxide doped PbZr0.525Ti0.475O3 (PTZT) were successfully deposited by solid state reaction. The PZT and PTZT ceramics were analyzed by an x-ray diffraction (XRD). The XRD spectra were recorded by Diano type 2100E diffractometer using a CuKα (λcu = 1.54056 Å) radiation at 30 KV and 30 mA (900 watt). The spectra showed that PZT and PTZT ceramic are polycrystalline with tetragonal structure. The lattice constants analysis of the grown ceramics were described by Delphi program. Using Cohen’s and Cramer’s algorithms in the Delphi program, the lattice constants are a = b = 4.094 Å, c = 4.142 Å, c/a ratio = 1.012 for PZT ceramic, and a = b = 4.075 Å, c = 4.088 Å, c/a ratio = 1.003 for PTZT ceramic. The lattice constants are a = b = 4.094 Å, c = 4.142 Å, c/a ratio = 1.012 for PZT ceramic, a = b = 4.122 Å, c = 4.134 Å, c/a ratio = 1.003 for PTZT 0.5 % ceramic, a = b = 4.075 Å, c = 4.088 Å, c/a ratio = 1.003 for PTZT 1 % ceramic, a = b = 4.248 Å, c = 4.179 Å, c/a ratio = 0.984 for PTZT 1.5 % ceramic. Increasing tantalum oxide doping in PZT from 0 % to 1.5 % lead to the decrease in c/a ratio. The smaller value of the c/a ratio of PTZT ceramic than those of PZT ceramic is possibly associated with the anti site defects of Ta dopants.
Electrical Conductivity and Surface Roughness Properties of Ferroelectric Gallium Doped Ba0,5Sr0,5TiO3 (BGST) Thin Films Irzaman Irzaman; A. Marwan; A. Arief; R.A. Hamdani; M. Komaro
Indonesian Journal of Physics Vol 19 No 4 (2008): Vol. 19 No. 4, October 2008
Publisher : Institut Teknologi Bandung

Show Abstract | Download Original | Original Source | Check in Google Scholar | Full PDF (416.679 KB) | DOI: 10.5614/itb.ijp.2008.19.4.5

Abstract

Ba0.5Sr0.5TiO3 (BST) and gallium doped BST (BGST) thin films were successfully deposited on p-type Si(100) substrates. The thin films were fabricated by the chemical solution deposition (CSD) and spin coating method, with 1.00 M precursor and spinning speed of 3000 rpm for 30 seconds. The post deposition annealing of the 9 films were carried out BST without gallium (BGST 0%) annealing 850OC, BGST 0% annealing 900OC, BGST 0% annealing 950oC, BGST 5% annealing 850oC, BGST 5% annealing 900oC, BGST 5% annealing 950oC, BGST 10% annealing 850oC, BGST 10% annealing 900oC, BGST 10% annealing 950oC for 15 hour in oxygen gas atmosphere, respectively. The resistance and electrical conductivity of the grown thin films are characterized by I-V converter, meanwhile surface roughness of the grown thin films are characterized by atomic force microscopy (AFM) method. The electrical conductivity of the grown thin films BGST due to semiconductor. The results show that resistance and electrical conductivity of the thin film have strong correlation to the annealing temperature, concentration dopant and surface roughness.
DAMPAK KEGIATAN PELEDAKAN PERTAMBANGAN ANDESIT TERHADAP LINGKUNGAN PEMUKIMAN DI GUNUNG SUDAMANIK KECAMATAN CIGUDEG KABUPATEN BOGOR (The Impact of Blasting Activities for Andesite Mining to Residential Environment at Mount Sudamanik Cigudeg Bogor) Aljon Albertus Manotar Simbolon; Muhamad Yani; Irzaman Irzaman
Jurnal Manusia dan Lingkungan Vol 22, No 2 (2015): Juli
Publisher : Pusat Studi Lingkungan Hidup Universitas Gadjah Mada

Show Abstract | Download Original | Original Source | Check in Google Scholar | DOI: 10.22146/jml.18735

Abstract

ABSTRAKAspek lingkungan hidup kemungkinan terganggu akibat kegiatan eksploitasi sumber daya alam. Mineral dan batuan sebagai salah satu sumber daya alam pada umumnya tersebar di daerah terpencil yang masih memerlukan pengembangan. Pada sisi ini, kehadiran perusahaan pertambangan sangat penting peranannya bagi kemajuan dan pembangunan serta meretas keterisolasian suatu daerah. Wilayah sekitar Gunung Sudamanik, Kecamatan Cigudeg, Kabupaten Bogor tumbuh dan berkembang karena pertambangan andesit. Gunung Sudamanik telah dan masih dieksploitasi lima perusahaan tambang andesit yang memiliki Izin Usaha Pertambangan (IUP) dengan luas total Wilayah Izin Usaha Pertambangan (WIUP) seluas 113 hektar. Pada tahun 2012, total produksi batuan kelima perusahaan adalah 3.984.785 ton atau rata-rata 332.065,4 ton per bulan. Produksi batuan tersebut dihasilkan dari peledakan yang dapat mencapai lima kali peledakan atau lebih setiap hari. Getaran dan bunyi ledakan yang disebabkan peledakan ini kemungkinan berdampak terhadap lingkungan hidup, terutama pada konstruksi rumah dan kenyamanan masyarakat yang bermukim di sekitar kaki Gunung Sudamanik. Pemukiman penduduk yang paling dekat lokasi peledakan andesit berada pada tiga kampung/dusun yaitu Kampung Kadaung, Lebakwangi Lapangan dan Lebakwangi Girang. Ketiga kampung tersebut secara administratif berada dalam Desa Rengasjajar. Rumah warga pada pemukiman yang paling dekat ke lokasi peledakan batuan andesit berjarak sekitar 337 – 616 meter. Hasil penelitian menunjukkan bahwa pemakaian 90,5 kg bahan peledak delay yang sama pada jarak 148 m mengakibatkan tingkat getaran tanah maksimum 7,71 mm/s yang telah melewati baku mutu kelas 3 SNI 7571 : 2010. Dan pemakaian bahan peledak mulai dari 77,4 kg sampai 1310,4 kg setiap peledakan tidak menimbulkan dampak kebisingan pada pemukiman warga.ABSTRACTLiving environment aspects are possibility disrupted by the exploitation of natural resources. Minerals and rocks as one of the natural resources in general are scattered in remote areas that still need development. On this side, the presence of mining companies is important for the progress and development as well as rip off the isolation area. The region around Mount Sudamanik, Cigudeg District, Bogor Regency grows due to the mining of andesite rock. Mount Sudamanik has been and is being mined out by five companies that have mining business license (IUP) covering an area of 113 hectares of region mining business permit (WIUP). In 2012, total andesite production of the all company reached 3,984,785 tons, or an average of 332,065.4 tons per month. Production of these andesite generated from blasting that can reach five times the blasting or more every day. Ground vibrations and air blast caused by blasting probably effect to the living environment, mainly to the house construction and comfort communities who resides around the foot of Mount Sudamanik. Three villages are situated at the nearest the andesite mining inculuding Kampung Kadaung, Lebakwangi Lapangan and Lebakwangi Girang. Residential homes on the nearest location to the andesite blasting is about 337- 616 meters. The results showed that the use of 90.5 kg of explosives same delay at distance 148 resulted in maximum ground vibration levels of 7.71 m/s that have full filled the quality standard of the third grade SNI 7571: 2010. And the use of explosives ranging from 77.4 kg to 1310.4 kg blasting did not cause any noise impact on residential areas. 
Effect of Different Hydrothermal Temperatures on the Properties on Nano-Silica (SiO2) of Rice Husk Irzaman Irzaman; Irmansyah Irmansyah; Siti Aisyah; Nazopatul Patonah Har; Aminullah Aminullah
International Journal of Renewable Energy Development Vol 11, No 3 (2022): August 2022
Publisher : Center of Biomass & Renewable Energy, Diponegoro University

Show Abstract | Download Original | Original Source | Check in Google Scholar | DOI: 10.14710/ijred.2022.43904

Abstract

Rice husk has high silica (SiO2) content and can be used as the primary material for making nano-silica. One of the methods for synthesizing nano-silica was the hydrothermal method. The objective of this study was to synthesize nano-silica from rice husks by observing the effect of temperature in the hydrothermal process on the structure, electrical and particle properties of nano-silica. The hydrothermal process temperature was 150, 200, and 250 °C for 4 hours. The results showed that all nano-silicas were in the amorphous phase. The particle size was in the range of 0.16-13.49 nm with more uniform size distribution on nano-silicas of 200 °C and 250 °C than nano-silica at 150 °C. These three nano-silicas were included in the semiconductor category by increasing temperature and frequency. In addition, these treatment variations resulted 200 °C for 4 hours and pressure of 2 atm as the optimum treatment for manufacturing nano-silica of rice husk ash. This nano-silica could be used as semiconductor material for electronic industry.
Engineering of Information Monitoring System Sensor Reading Data Based on Smart Wireless using NVDIA Jetson Nano and Arduino Mega on Agricultural Spraying Machines Ridwan Siskandar; Tineke Mandang; Wawan Hermawan; Irzaman Irzaman
Jurnal Teknik Pertanian Lampung (Journal of Agricultural Engineering) Vol 12, No 4 (2023): December 2023
Publisher : The University of Lampung

Show Abstract | Download Original | Original Source | Check in Google Scholar | DOI: 10.23960/jtep-l.v12i4.921-936

Abstract

The focus of the research is monitoring data from sensors on the agricultural sprayer. The monitoring system support by some sensors in camera, tank capacity, boom sprayer balance and battery capacity. The research method was carried out using the waterfall model, because according to the needs that require a sequential flow in the process. This model is divided into four parts, namely analysis (to identify problems and needs), design (plans to solve problems to be solved), implementation (implementation of plans that have been made), and testing. Engineering of Information Monitoring System Sensor Reading Data Based on Smart Wireless using NVDIA Jetson Nano and Arduino Uno on Agricultural Spraying Machines. The test results for the CNN model for the detection of the “Jajar Legowo” object were carried out to obtain 90% accuracy, 82.35% precision and 100% recall. Tests an accuracy value cappacity tank of 100%. Testing the balance sensor, if rotates clockwise on the Y axis the output voltage decreases, and vice versa. However, if the sensor at rest, the output voltage will same as the offset value. Besides that, testing the optimum PWM value fuzzy approach is carried out with aim that the droplets hit the target zone when sprayer is working. The result are Arduino IDE and Matlab produce same value, which is 42 for the optimum PWM value. Testing the battery capacity sensor get accuracy value of 100% by difference in the voltage increase of 0.5 volts is equivalent to increase of 10%. All information read by the sensors is displayed on the LCD using WMS-2000 (smart wireless). Keyword: Fuzzy, Microcontroller, Monitoring, Sensor data, Smart wireless
PERHITUNGAN POLARISASI SPONTAN DAN MOMEN QUADRUPOL POTENSIAL LISTRIK BAHAN PIZT (PbInxZryTi1-x-yO3-x/2) Hikam, Muhammad; Sarwono, Edy; Irzaman, Irzaman
Makara Journal of Science Vol. 8, No. 3
Publisher : UI Scholars Hub

Show Abstract | Download Original | Original Source | Check in Google Scholar

Abstract

PZT (PbZr1-xTixO3 ) merupakan bahan berbentuk kristal perovskite yang dapat dimanfaatkan sebagai sensor inframerah. Penambahan sedikit dopan (bahan pendoping) dapat mengubah secara drastis karakteristik spesifik dari bahan keramik-ferroelektrik seperti polarisasi spontan, sifat dielektrik, sifat elektromekanik, elektrooptik dan sifat lainnya. Hard doping dengan menggunakan ion In3+ diaplikasikan pada penelitian ini dan dilakukan penumbuhan lapisan tipis dari bubuk PIZT (PbInxZryTi1-x-yO3-x/2) pada substrat Si(100) dengan metode Chemical Solution Deposition (CSD) dengan konsentrasi 0,5 M dan kecepatan putar spin coating 3000 rpm. Karakteristik bahan PIZT baik bubuk maupun lapisan tipisnya diuji dengan difraksi sinar x. Analisis Rietveld dilakukan dengan menggunakan program GSAS-EXPGUI dan diperoleh parameter kisi dan komposisi fasa dari kristal. Polarisasi spontan (Ps ) PIZT bubuk dan lapisan tipisnya mengalami penurunan dibandingkan dengan bahan asalnya (PZT). Polarisasi spontan yang optimum dari lapisan tipis PIZT dicapai pada rentang doping 0,5% - 1% In2O3. Momen quadrupol potensial listrik (FQ(r) ) bahan PIZT pada suatu titik P (0,0,2a) mencapai kondisi optimum pada % doping 6% In2O3 dan dari hasil penelitian ini juga menunjukkan bentuk lapisan tipis PIZT memiliki nilai (FQ(r)) yang lebih baik daripada bentuk bubuknya untuk rentang doping > 1% In2O3.
Structure and Morphology of ZnO Nanoparticles Prepared by Sonochemical Method Maddu, Akhiruddin; Zetria Zikri; Irzaman, Irzaman
TIME in Physics Vol. 1 No. 2 (2023): August
Publisher : Universitas Mandiri

Show Abstract | Download Original | Original Source | Check in Google Scholar | DOI: 10.11594/timeinphys.2023.v1i2p51-58

Abstract

Ultrasonic wave has been utilized to synthesize the ZnO nanoparticle. ZnO is formed from a mixture of zinc acetate (ZnAc) and Natrium Hydroxide (NaOH) with various concentrations of ZnAc 0.5 M (ZnO 1:1) and 1.5 M (ZnO 3:1) and the concentration of NaOH remained at a concentration of 0.5 M. The Structure and crystal size were characterized using X-ray Diffraction (XRD), while its morphology was examined by Scanning Electron Microscopy (SEM). The results show that ZnO 1:1 has a higher (stronger) diffraction intensity than the ZnO 3:1. The crystallite size of ZnO 1:1 averaged 30.57 ± 4.31 nm while the ZnO 3:1 had an average crystallite size of 20.25 ± 7.12 nm. From the size of the crystallites ZnO particles that are formed include nanoparticles. ZnO 1:1 SEM image shows the shape of microrods in the 1:1 ZnO sample while in the 3:1 ZnO sample no microrods are formed. Based on the morphology, the 1:1 ZnO sample has an average size of 230 nm and is larger than the 3:1 ZnO sample which has an average size of 50 nm.
Analysis Lattice Constant of Ceramic SrTiO3 Doped Cuprum(II) Acetate Cube Structure by Cramer-Cohen Method Handayani, Pipit; Mufarrohah, Fatihatul; Asih, Asih; Rahmawaty, Vania; Santi, Maya Ary; Rukyati, Anis Munir; Siskandar, Ridwan; Syafutra, Heriyanto; Pratama, Erdiansyah; Setiawan, Ardian Arif; Irzaman, Irzaman
JIPF (Jurnal Ilmu Pendidikan Fisika) Vol 9, No 2 (2024): May 2024
Publisher : STKIP Singkawang

Show Abstract | Download Original | Original Source | Check in Google Scholar | DOI: 10.26737/jipf.v9i2.5004

Abstract

Analysis of SrTiO3 ceramics with the doping Cuprum(II) acetate (Cu(CH3COO)2), the variation in the concentration of doping used 0%; 0,5%; and 1% using the solid state reaction method was successful. The annealing process is carried out starting from room temperature then raised to an annealing temperature of 850 oC with a temperature increase of 1,67 oC / minute and held constant for 8 hours. Next proceed with the cooling process until it returns to room temperature for 13 hours. Analysis of XRD data using the Cramer-Cohen method yielded a lattice parameter of 3,909 Å; 3,906 Å; and 3,905 Å, a cubic crystal structure.
A-OPTIMAL DESIGN IN NON-LINEAR MODELS TO INCREASE SILICON DIOXIDE PURITY LEVELS Weisha, Ghea; Erfiani, Erfiani; Irzaman, Irzaman; Syafitri, Utami Dyah
MEDIA STATISTIKA Vol 17, No 1 (2024): Media Statistika
Publisher : Department of Statistics, Faculty of Science and Mathematics, Universitas Diponegoro

Show Abstract | Download Original | Original Source | Check in Google Scholar | DOI: 10.14710/medstat.17.1.36-44

Abstract

Silica is the most mineral found on earth and is widely used in industry. Silica used in industry is usually silicon dioxide with a purity ≥ 95% and its often sold at a higher cost. To obtain the silica at a lower cost, silica extraction from biomass such as rice husk can be conducted. The purity of silica extracted from biomass tends to be lower than that of mineral silica. Silica with low purity can be increased by adjusting the temperature and the rate of temperature rise. This research aims to obtain the best design to determine the purity of silicon dioxide. The design of this study was generated based on the A-optimality criterion using the DETMAX algorithm. The A-optimality criterion is minimizing the trace of the variance-covariance of the parameter estimation. The best design points obtained using A-optimal design consist of three temperature groups: the minimum temperature of 800°C, the middle temperature of 850°C, and the maximum temperature of 900°C, with varying rates of temperature rise. Points were repeated at the temperature of 850°C, with rates of temperature rise of 1.67°C/min and 3.34°C/min. 
The Comparison A-Optimal and I-Optimal Design in Non-Linear Models to Increase Purity Levels Silicon Dioxide Aliu, Muftih Alwi; Syafitri, Utami Dyah; Fitrianto, Anwar; Irzaman, Irzaman
Jambura Journal of Mathematics Vol 6, No 2: August 2024
Publisher : Department of Mathematics, Universitas Negeri Gorontalo

Show Abstract | Download Original | Original Source | Check in Google Scholar | DOI: 10.37905/jjom.v6i2.26253

Abstract

One of the obstacles that arise in optimal design is the non-linear model. The relationship between temperature factors and the temperature increase rates with the purity of silicon dioxide (SiO2) forms a non-linear pattern. Determining the optimal design for a non-linear model is relatively more complex than a linear model because it requires additional information in its information matrix. Therefore, this issue necessitates further research on optimal design in non-linear models. This study uses the polynomial Taylor approach to approximate the non-linear equation through a linear equation using the appropriate optimal design methods, namely A-Optimal and I-Optimal criterion. The point search algorithm used was variable neighborhood search, this algorithm searches for design points by exploring several different neighborhood structures. These two methods were chosen to compare the characteristics and performance of the designs produced, aiming to obtain an optimal design to improve SiO2 purity (non-linear case) using the same algorithm, VNS. The research results showed that the design pattern produced by the A-Optimal design formed three temperature groups, namely the minimum temperature of 800°C - 820°C, the middle temperature of 850°C, 860°C, and the maximum temperature of 900°C, with varying temperature increase rates in the design area. The design pattern produced by the I-Optimal design formed a full quadratic pattern, namely the minimum temperature of 800°C and the maximum temperature of 900°C, with varying temperature increase rates in the design area. The I-Optimal design demonstrated the best performance (most optimal) in the aspect of prediction variance compared to the A-Optimal design across all alternative points in this study to improve SiO2 purity.
Co-Authors -, A.Maddu -, R.Putri . Irmansyah . Masitoh . Mursyidah . Sucipto A M Fauzi A Maddu A. Ardian A. Arief A. Maddu A. Marwan A. Subagio A. Subagio A.D. Husin A.Maddu - Abdul Djamil Husin Abdurahman Abdurrahman Abu Sonip Abu Sonip Ade Irma Ade Kurniawan Ade Kurniawan Ade Kurniawan Ade Kurniawan Ade Kurniawan Ade Kurniawan Adi, Langit Cahya Aditya Kurniawan Aditya Kurniawan Adnan Prasetyo Alamsyah Adrian Fadhillah Agnes Tiara Vinanda Agus Ismangil Agus Wahyana Anggara Agus Wahyana Anggara Agus Wahyana Anggara, Agus Wahyana Ahmad Fakhrudin Ahmad Khairul Reza Ahmad Yani Ajat Sudrajat Akhiruddin Akhiruddin Akhiruddin Maddu Aldi Destia Lesmana Alfi Afriliani Alif Musthafa Thariq ALIU, MUFTIH ALWI Aljon Albertus Manotar Simbolon Aljon Albertus Manotar Simbolon, Aljon Albertus Manotar Aminullah Aminullah Ana Fitriana Ana Fitriana Angga Khalifah Tsauqi Angga Khalifah Tsauqi Anis Munir Rukyati Anissa Tsalsabila Annisa Tsalsabila Antomi Saregar Ardian Arif Ardian Arif Ari Firia ARI SETIAWAN Ari Setiawan Asih Asih, Asih Astri Wahyuningtyas Ayu Bonita Pertiwi Harianja Azka Zakiyyatuddin B. Sastri Baba Barus Bambang Hendro Trisasongko Bambang Herawan Bambang Herawan, Bambang Billi Rifa Kusumah Boedi Tjahjono Budi Harsono Budi Mulyanti Casnan Casnan Casnan, Casnan D Puspita Dea Amelia Saputri Dea Widiawati Demijati Demijati Dendy Handy Saputra Dendy Handy Saputra Dendy Handy Saputra Dendy Handy Saputra Desna Desna Deti Anggraeni Ekawati Dion Sanaha Dwi Lestariningsih Dwiky Agung Adi Nugroho Dyah R Panuju Dyah R. Panuju Dyah R. Panuju E. Ridwan E. Supriyanto Edy Sarwono Ella Rahmadani Endah Kinarya Palupi Erawan Kurniadi Erfiani Erfiani Erliza Hambali Erliza Noor Erna Rusliana Muhamad Saleh Erni Apriliana Erni Aprilina Erni Aprilina Eti Rohaeti Eti Roharti Eva Musyafaah Evvy Kartini F Nawafi F. Huriawati F. S. Arsyad Fadhilah Chandra Fajrul Kamil Ramadhan Fanny Amalia Fara, Aulia Azzahra Farida Huriawati, Farida Firmansyah Firmansyah Fitrah Hadi Firdaus Fitrah Hadi Firdaus Fitrah Hadi Firdaus Fitrah Hadi Firdaus, Fitrah Hadi Fitri Melinda Fitrianto, Anwar Gagat Mughni Pradipta Gagat Mughni Pradipta Gagat Mughni Pradipta Gagat Mughni Pradipta H Syafutra H. Darmasetiawan H. Darmasetiawan H. Darmasetiawan H. Darmasetiawan H. DarmasetiawanArifin H. Hardhienata H. Sutanto H. Syafutra H. Syafutra Habibah Assa’addah Habibah, Assa'addah Hadjomidjojo, Hartrisari Halimah Sa'diyah Handayani, Pipit Hanedi Darmasetiawan Hanifan, Rahmah Asri Nurani Hannif Izzatul Islam Hannif Izzatul Islam Hannif Izzatul Islam Hannif Izzatul Islam Har, Nazopatul Patonah Hari Wijayanto Hartrisari Hadjomidjojo Hartrisari Hardjomidjojo Heriyanto Safutra Heriyanto Syafutra Heriyanto, Syafutra Herlan Darmawan Herlan Darmawan Hilal Fauzi Ramadhan Husin Alatas Imam Suyanto Indriyati Rahmi Setyani Iqbal, Mochamad Ira Saira Ira Ukhtianingsih Ira Ukhtiningsih Ira Ukhtiningsih, Ira Irlian Nurmaniah Irlian Nurmaniah Irlian Nurmaniah Irlian Nurmaniah, Irlian Irmansyah . Irmansyah Irmansyah Irmansyah Irmansyah Irmansyah Irmansyah Irmansyah Irmansyah Irwan Meilano irwan meilano Ismangil, Agus Ivander Manuel Jajang Juansah Jenie, Renan Prasta Johan Iskandar Johan Iskandar Johansah Liman Kamelia Fikriah Karin, Fay Ivana Khafit Pratama Hendratno Khusnul Yakin Kinanthi Freda Bhanuwati Koharudin Koharudin L. Nady La Isa Leni Ariyanti Lulu Lutfiah Lusia Anita Boru Sagala Lusia Anita Br. Sagala Lusia Anita Br. Sagala M Hikam M. Barmawi M. Barmawi M. Barmawi M. Barmawi M. Barmawi M. Budiman M. Budiman M. Budiman M. Hikam M. Hikam M. Hikam M. Hikam M. Komaro M. N. Indro M.A. Idris Mahfuddin Zuhri Mahmud A. Raimadoya Mahmud A. Raimadoya Maman Budiman Maria Evita Maria Evita Marina, Indriasari Maya Risanti Maya Risanti Maya Risanti Maya Risanti, Maya Mersi Kurniati Meutia Awani Mitra Djamal Mitra Djamal Mochamad Iqbal Moh Yasin Mohammad Yasin Mufarrohah, Fatihatul Muhamad Syazali Muhamad Yani Muhamad Yani, Muhamad Muhammad A Fadhil Muhammad Ahyad Muhammad Fikri Fakhrurozi Muhammad Hikam Muhammad Hikam Muhammad Hikam, Muhammad Muhammad Izatul Al Fajar Muhammad Khalid Murtezha Hadijaya N. G. Pamungkas N. P. Bo Nada Huwaidah Nadia Septiani Naila Nur Alifa Naila, Nur Alifa Naufal Muharram Nurdin Nazopatul Patonah Har Nazopatul Patonah Har Ngurah Ayu Ketut Umiati Nida Nabilah Nida Nabilah Nida Nabilah Nida Nabilah Nina Siti Aminah Nina Siti Aminah Noer A Indrawan Nora Idiawati Novia Fransiska Simbolo Novia Fransiska Simbolon Novitri Novitri P. Arifin P. Arifin P. Arifin P. Arifin P. Arifin P. Arifin P. Perdinan P. W. K. Anggraini Palupi, Endah Kinarya Pratama, Erdiansyah Purnawan Purnawan Purnawan Purnawan Putra, Heriansyah Putri Tarigan R Erviansyah R. D. Puspita R. Erviansyah R. Erviansyah R. Putri R.A. Hamdani R.Putri - Raden Silfia Epriyanti Rahmad Junaidi, Rahmad Rahmah Asri, Nurani Hanifan Rahmawaty, Vania Ratih Dwi Septiani Renan, Prasta Jenie Renny Apriani Dwika Saputri Renny, Apriani Dwika Saputri Retna Apsari Retno Dwi Jayanti Retno Dwi Kartika Sari Riani Eka Fitri Ridwan Siskandar Ridwan, Siskandar Rizki Nurhikmah Rofiqul Umam Rohul Rizki Mubaroq Hartman Rony Febryarto Royyan Faizin Rukyati, Anis Munir Rustami, Erus S. G. Sukaryo S. Taking S.N. Jusoh Salahuddin Perdana Salamet Nur Himawan Santi, Maya Ary Sarah Aribah Miftahulfallah Sarah Nabilah Sarmilah Sarwono, Edy Sejahtera Sejahtera Sensius Seno Sesar Husen Santosa Setiawan, Aep Shelvie Nidya Neiman Sidikrubadi Sidikrubadi Sigit Ahmad Fatoni Sinta Puspita Apriliani Siregar, Rahmat Nawi Siswadi Siswadi Siti Aisyah Siti Hajar Siti Hajar Siti Nikmatin Sofyan Sa'id Atsaurry Sofyan Sa'id Atsaurry Sofyan Said Sofyan Said Atsaurri Sri Mulatsih Stefiana Sondary Az Zahrah Suharno Suharno Sukirno Sukirno Sumarjono Effendy Supandi Supandi Suryanto, Wiwit Susi Susilawati T. Sumardi Talitha Alya Syaharani Tantan Taopik Ramlan Tantan Taopik Ramlan, Tantan Taopik Tantan Taopik Rohman TARUNI SRI PRAWAST MIEN KAOMINI ANY ARYANI DEDY DURYADI SOLIHIN Taufik Djatna Teguh Yogaraksa Tetinia Gulo Tineke Mandang Titin Yuliana Touwil Umrih Tun Tedja I U. Hashim Umi Trimukti Utami Dyah Syafitri Venas Miftah Hasan Wahyu Srigutomo Wahyu Srigutomo Wahyudi Wahyudi Wahyudi Wahyudi Wahyudianto, Benny Wasmen Manalu Wawan Hermawan Wawan Hermawan Weisha, Ghea Widya Rahma Witri Desmulyani Y. Darvina Yakin, Khusnul Yulia Christina Yulia Sani Yulia Sani Yulia Sani, Yulia Z. Jamal Z. Jamal Zahra Syahira Zetria Zikri Zulaeha Ma’bud