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All Journal International Journal of Public Health Science (IJPHS) International Journal of Advances in Applied Sciences INOTEKS : Jurnal Inovasi Ilmu Pengetahuan, Teknologi, dan Seni BERKALA FISIKA SAINS DAN MATEMATIKA Jurnal Penelitian Fisika dan Aplikasinya (JPFA) YOUNGSTER PHYSICS JOURNAL Jurnal Pengolahan dan Bioteknologi Hasil Perikanan Jurnal Simetris Humanitas: Indonesian Psychological Journal Empathy : Jurnal Fakultas Psikologi Abdimas Jurnal Pendidikan Teknik Mesin Jurnal Teknosains Pangan Plumula : Berkala Ilmiah Agroteknologi JAM : Jurnal Aplikasi Manajemen Journal of Medical Physics and Biophysics Agrokreatif Jurnal Ilmiah Pengabdian kepada Masyarakat POSITIF BULETIN FISIKA Jurnal Ilmiah Pendidikan Pancasila dan Kewarganegaraan JADECS (Journal of Art, Design, Art Education and Culture Studies) saintis Majalah Kesehatan FKUB Jurnal Ekonika : Jurnal Ekonomi Universitas Kadiri JURNAL LENTERA : Kajian Keagamaan, Keilmuan dan Teknologi AKSIOLOGIYA : Jurnal Pengabdian Kepada Masyarakat Risâlah, Jurnal Pendidikan dan Studi Islam Kinetik: Game Technology, Information System, Computer Network, Computing, Electronics, and Control JTM-ITI (Jurnal Teknik Mesin ITI) DAR EL-ILMI : Jurnal Studi Keagamaan, Pendidikan dan Humaniora JURNAL PENGABDI Jurnal Komtika (Komputasi dan Informatika) Journal of Physics and Its Applications Prosiding Seminar Nasional Sains dan Teknologi Terapan Conference on Innovation and Application of Science and Technology (CIASTECH) Jurnal Nasional Komputasi dan Teknologi Informasi Jurnal Kreativitas PKM Journals of Ners Community Idealog: Ide dan Dialog Desain Indonesia Madinah: Jurnal Studi Islam Societas : Jurnal Ilmu Administrasi dan Sosial Jurnal Teknologi Hasil Pertanian Jurnal Ilmu Manajemen International Journal of Education, Science, Technology, and Engineering (IJESTE) EDUTEC : Journal of Education And Technology Journal of SPORT (Sport, Physical Education, Organization, Recreation, and Training) Indonesian Journal of Electrical Engineering and Computer Science International Journal of Recent Technology and Applied Science (IJORTAS) Community Development Journal: Jurnal Pengabdian Masyarakat Jurnal EMA (Ekonomi Manajemen Akuntansi) Jurnal Kreatif : Desain Produk Industri dan Arsitektur Journal of Electrical Engineering and Computer (JEECOM) Agroradix : Jurnal Ilmu Pertanian Aktual Justice AKADEMIK: Jurnal Mahasiswa Ekonomi & Bisnis BULETIN BISNIS & MANAJEMEN (BBM) Prosiding Seminar Nasional Teknik Elektro, Sistem Informasi, dan Teknik Informatika (SNESTIK) Prosidia Widya Saintek Journal Community Service Consortium Research Trend in Technology and Management MAP (Jurnal Manajemen dan Administrasi Publik) Global Education Journal Jurnal Pengabdian Masyarakat dan aplikasi Teknologi Impression : Jurnal Teknologi dan Informasi At-Tahdzib: Jurnal Studi Islam dan Muamalah JESICA Jurnal FORTECH AL TADIB : Jurnal Ilmu Pendidikan
Choirul Anam AM Diponegoro
Department Of Physics, Faculty Of Mathematics And Natural Sciences, Diponegoro University, Jl. Prof. Soedarto SH, Tembalang, Semarang 50275, Central Java, Indonesia
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IMPLEMENTASI METODE CONTRAST LIMITED ADAPTIVE HISTOGRAM EQUALIZATION DAN LAPLACIAN OF GAUSSIAN FILTER UNTUK PENINGKATAN KONTRAS CITRA CT Awwalin, Aufi Rizqiatul; Setiawati, Evi; Anam, Choirul
BERKALA FISIKA Vol 24, No 1 (2021): Berkala Fisika
Publisher : BERKALA FISIKA

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Abstract

The  image  obtained  from  the  CT  scanner  has  a  relatively  low  contrast.  Image  contrast  can  be enhanced  by  using  an  algorithm  of  contrast  limited  adaptive  histogram  equalization  (CLAHE). However, the implementation of CLAHE causes an increase  of noise. Furthermore, noise can be reduced  using  a  noise  reduction  filter,  but  it  reduces  the  spatial  resolution  of  the  image.  This study proposed a combination of the CLAHE method and the Laplacian of Gaussian (LoG) filter noise reduction algorithm to obtain images with high contrast,  while maintaining the  noise and spatial  resolution.  In  this  study,  27  abdominal  CT  images  and  MTF  phantom  CT  images  were investigated using our proposed method. As a comparison, this study also evaluated the results of combination  of  CLAHE  and  Gaussian  filters.  Evaluation  of  the  results  of  image  quality improvement  was carried out qualitatively (visually) and quantitatively by calculating the mean squared  error  (MSE),  peak-signal  to  noise  ratio  (PSNR)  and  spatial  resolution  using  a modulation transfer function (MTF) of 10%. The results of this study qualitatively (visually) and quantitatively showed that the combination of CLAHE and LoG filters produces images with high contrast,  while  maintaining the  noise  and  the  spatial  resolution  of  the  image.  Compared  to  the combination of  CLAHE and Gaussian filters or CLAHE alone,  the  combination of CLAHE and Log  filters  provides less  noise  and  higher  spatial  resolution.  Thus,  combination  of  CLAHE  and LoG filters can be used as an alternative algorithm to increase the contrast in CT images.
PELAKSANAAN PENILAIAN HASIL BELAJAR TAHFIDZUL QUR’AN USIA DEWASA DI YAYASAN GRIYA AL QUR’AN SURABAYA Rokhim, Ahmad Abdur; Anam, Choirul; Alindra, Bagoes Malik
Risâlah, Jurnal Pendidikan dan Studi Islam Vol 8 No 1 (2022): Pendidikan dan Studi Islam
Publisher : Fakultas Agama Islam Universitas Wiralodra Indramayu

Show Abstract | Download Original | Original Source | Check in Google Scholar | DOI: 10.31943/jurnal_risalah.v8i1.184

Abstract

The purpose of this study was to determine the implementation of the assessment of Tahfidzul Qur'an learning outcomes for adults at the Griya Al Qur'an Foundation Surabaya. The approach used in this research is a descriptive qualitative approach using field research methods. The results of this study reveal that the implementation of the assessment of Tahfidzul Qur'an learning outcomes for adults at the Griya Al Qur'an Foundation Surabaya is carried out 4 times a year, which includes odd mid-semester assessments (PTS), end-semester assessments (PAS), mid-semester assessments (PTS) even and year-end assessment (PAT). The form of assessment used is an oral test, while the assessment instrument uses questions and answers with the aim of confirming or checking the quality of each student's memorization. There are 2 forms of tests used in the assessment of tahfidz learning, namely: 1) Reading and listening tests. Students read in their entirety the last 2 juz of the entire memorization they have by listening to their study friends. 2) Test connecting verses. The examiner reads the verse, then the student being tested continues reading the verse that has been read by the examiner. The verse connecting question consists of 4 questions that are determined randomly. The mid-semester assessment questions (PTS) are taken from the last 2 juz that have been read before, while the end-of-semester assessment questions (PAS) and year-end assessments (PAT) are taken from all the memorization that students have. Students are declared passed when they get a minimum value of C with a score of 80 and vice versa if they get a D score with a score of 75.
Dose Volume Product (DVP) As Descriptor for Estimating Total Energy Imparted to Patient Undergoing CT Examination Choirul Anam; Freddy Haryanto; Rena Widita; Idam Arif; Geoff Dougherty
Journal of Medical Physics and Biophysics Vol 3, No 1 (2016)
Publisher : Indonesian Association of Physicists in Medicine (AIPM/AFISMI)

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Abstract

The purpose of this study is to expand a descriptor for estimating the total energy imparted to a patient undergoing a CT examination and to investigate its relationship to the currently used descriptor. Estimating the total energy imparted to a patient has previously been characterized by dose length product (DLP). We propose a descriptor which we call the dose volume product (DVP), defined as the product of the size specific-dose estimate (SSDE) and the volume irradiated in the patient (V). We also present algorithm to automate the calculation of DVP. There are several steps in calculating the DVP: the first is to contour the patient automatically, the second is to calculate the area of patient in every single slice, the third is to calculate the volume of the radiated part of the patient, the fourth is to calculate the water equivalent diameter (DW) automatically, the fifth is to calculate the SSDE, and the last is to calculate the DVP. To investigate the effectiveness of the algorithm, we used it on images of phantoms and patients. The results of this study show that the automated calculations of DVP for both body and head phantoms were in good agreement with theoretical calculations. The differences between them were within 2%. DVP and DLP had a linear relationship with R2 = 0.971 (slope 1099 cm2, 95% confidence interval (CI), 1047 to 1157 cm2) and R2 = 0.831 (slope 248.6 cm2: CI, 237.6 to 259.7 cm2), for thorax and head patients respectively.
Scatter index measurement using a CT dose profiler Choirul Anam; Freddy Haryanto; Rena Widita; Idam Arif; Toshioh Fujibuchi; Takatoshi Toyoda; Geoff Dougherty
Journal of Medical Physics and Biophysics Vol 4, No 1 (2017)
Publisher : Indonesian Association of Physicists in Medicine (AIPM/AFISMI)

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Abstract

The CT dose index (CTDI) is usually measured using a pencil chamber with a length of 100 mm on a CTDI phantom with a length of 150 mm. The scattering radiation dose beyond 100 mm is usually still significant despite using a small beam width (below 10 mm). This study aims to measure the scattering index of CT dose for several variations of input parameters. The scatter index measurements were performed on a multi-slice CT (MSCT) Alexion™ using a CT dose profiler detector connected to a Black Piranha electrometer (RTI Electronic, Sweden). The measurements used the helical mode and a beam width of 2 x 4 mm, and resulted in 150 mm dose profiles. Values of CTDI150, CTDI130 and CTDI100 were calculated and used to obtain values of the scatter indices (SI130 and SI150). We varied input parameters, such as tube voltage, tube current, and pitch, and used two types of CTDI phantoms, i.e. body and head. In the tube voltage variation (from 80 to 135 kV), we found SI130 and SI150 values of 1.13 ± 0.01 and 1.19 ± 0.01 for the body CTDI phantom; and  SI130 and SI150 values of 1.08 ± 0.01 and 1.11 ± 0.01 for the head CTDI phantom. For tube current variations from 25 to 120 mA, and pitch variations from 0.75 to 1.5, SI130 and SI150 values were 1.14 ± 0.00 and 1.20 ± 0.00 for the body CTDI phantom; and 1.08 ± 0.00 and 1.11 ± 0.00 respectively for the head CTDI phantom. We showed that the more frequently used CTDI100 value is too small because it ignores scattering beyond the 100 mm boundary, even for beam widths less than 10 mm. The scatter index values were strongly influenced by the size of the CTDI phantom, and were slightly affected by the tube voltage. Variations in tube currents and pitch did not affect the value of the scatter index. The scatter index values of SI130 and SI150 were significantly different, and suggests that the use of SI150 is even more appropriate for describing the scattering dose.
Automated Universal Image Quality Index Measurement vs. Automated Noise Measurement: Which Method is Better to Define CT Image Quality? Fauzia Puspa Lestari; Choirul Anam; Yati Hardiyanti; Freddy Haryanto
Jurnal Penelitian Fisika dan Aplikasinya (JPFA) Vol. 9 No. 2 (2019)
Publisher : Universitas Negeri Surabaya

Show Abstract | Download Original | Original Source | Check in Google Scholar | DOI: 10.26740/jpfa.v9n2.p132-139

Abstract

Automatitation method in defining the quality of CT image is needed to optimize CT Scan treatment planning. So, the optimization of treatment planning can also be done automatically. There are various methods proposed to define the quality of an image. The purpose of this study was to find the simple and precision method to define CT image. We compared the performance of Automated Noise Measurement (ANM) and Automated Universal Image Quality Index (UIQI). We also compared them with the Manual noise measurement method based on the level of convergence in homogeneous images. The first step of Automated Noise Measurement was to create binary density slice using threshold values. Then, a masked image was performed by masking the original image and binary image. The standard deviation of every pixel for a certain kernel size was calculated by using a sliding window operation. The fourth step was to make a noise histogram from the noise map and determine the final noise in the image as the histogram peak. Then this calculation was normalized by the peak of the Hounsfield Unit (HU) histogram. All these steps were done with various kernel sizes for different slices in-homogenous phantom. In the Automatic UIQI method, the steps in the ANM method are carried out until the masked image stage, then UIQI is calculated for the masked image. The results show that automatic UIQI was more convergence in defining image quality than manual noise measurement and automated noise measurement by the lowest standard deviation which was only 0.00032867.
SIMULASI MONTE CARLO UNTUK EVALUASI ANODE HEEL EFFECT PADA PESAWAT SINAR-X MENGGUNAKAN PAKET PROGRAM EGSnrc Sanggam Ramantisan; Choirul Anam; Priyono Priyono
BULETIN FISIKA Vol 13 No 1 (2012): BULETIN FISIKA
Publisher : Departement of Physics Faculty of Mathematics and Natural Sciences, and Institute of Research and Community Services Udayana University, Kampus Bukit Jimbaran Badung Bali

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Abstract

This study aimed to evaluate the anode heel effect on the x-ray machine for the variation of angle of anode target and tube potential. The research was conducted using Monte Carlo simulations with the EGSnrc package. The x ray was designed by BEAMnrc, whereas the phase space file was analyzed by BEAMDP. The x ray unit was designed by using Tungsten material in anoda structure. Total filtration that used was equivalent with 2,5 mm Aluminium. From the simulation found that the anode heel effect occurs only on an axis parallel to the axis x-ray tube, i.e. fluence of radiation on the cathode side is greater than the anode side. Provided that a larger angle of target will decrease the anode heel effect. Anode heel effect for angle variation on the voltage 80 kV were 17,25% (50), 15,65% (7,50), 14,65% (100), 6,96% (12,50), and 3,14% (150) respectively. As for variations in tube voltage was obtained that the anode heel effect is relatively small. Anode heel effect for the tube voltage variation on the tube anode angle 150 were 1.99% (40 kV), 2.20% (60 kV), 3.14 (80 kV), and 3.81% (100 kV) respectively.
PENGARUH VARIASI JARAK DETEKTOR, LUAS LAPANGAN RADIASI DAN POSISI DETEKTOR DARI PUSAT BERKAS RADIASI MENGGUNAKAN MULTI PURPOSE DETECTOR (MPD) PADA PENGUKURAN TEGANGAN SINAR-X Evi Handriani Bertua Simamora; Choirul Anam; Evi Setiawati
Youngster Physics Journal Vol 2, No 2 (2013): Youngster Physics Journal April 2013
Publisher : Jurusan Fisika, Fakultas Sains dan Matematika, Universitas Diponegoro

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Abstract

An evaluation of the distance effect of Multi-Purpose Detector (MPD)-X ray source, variations of field size of radiation and position of the MPD on the X-ray voltage measured, have been done. There are necessary because they have not been recommended from the MPD procedure manual yet. The detector operated at voltage of 70 kV and current-time of 12.5 mAs. The measurement of voltage using MPD from RTI Electronics product. It is multifunction detector that can measure dose and voltage invasively. The previous step is measurement of dose for ensure correct equipment setting. These measurements is done for several variations such as MPD-X ray distance of  60 - 160 cm, field sizes 0f 4x4 cm - 40x40 cm2, detector's position of 0 (at center of beam) and 1-11 cm from centre of beam.   The results are obtained that the voltage that measured is not affected by all of variation values such as distance difference of MPD-X ray source,  field sizes and detector's position. Furthermore, for measurement of outside of radiation beam, MPD   can still measur voltage with good validation. Therefore, the measurement of voltage using MPD has high flexibility because it is not influenced by set up measurement.Keywords: The X ray voltage measurement, Multi-Purpose Detector (MPD), Barracuda.
PENGARUH VARIASI FAKTOR EKSPOSI (TEGANGAN TABUNG DAN ARUS WAKTU) SERTA PITCH TERHADAP COMPUTED TOMOGRAPHY DOSE INDEX (CTDI) DI UDARA MENGGUNAKAN CT DOSE PROFILER Puput Khusnaiatul; Eko Hidayanto; Zaenal Arifin; Choirul Anam
Youngster Physics Journal Vol 3, No 4 (2014): Youngster Physics Journal Oktober 2014
Publisher : Jurusan Fisika, Fakultas Sains dan Matematika, Universitas Diponegoro

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Abstract

The measurements of CTDI have been done as the method used to measure of dose in CT scans. The Measurement method is CTDI air method. Measuremeans of CTDI air using the CT dose profiler was placed in the center of the gantry rotation using tube voltage variations (80 kVp, 100 kVp, 120 kVp and 140 kVp), current time variations (100 mAs, 200 mAs, 300 mAs and 370 mAs) and pitch variations (0,75, 1, 1,25 and 1,5). The results of measurements  tube voltage variations in 370 mAs, pitch 1 and collimation 5 mm were 28,8-105 mGy, current time variations in tube voltage120 kVp, pitch 1 and collimation 5 mm were 19,7-73 mGy and Pitch variation in tube voltage 120 kVp, effective current time 370 mAseff, and collimation 5 mm were 55,9-116 mGy. The measurement results showed that greater the tube voltage, current time and pitch are used then the resulting CTDI air gets greater. The smaller tube voltage, current time and pitch are used then the resulting CTDI air gets smaller. FWHM and  geometric effisiency value of tube voltage variation were 6,2-6,37 mm and 68,40%-71,30%, current time variation were 6,17-6,27 mm and 69,5%-72,5% and pitch variation were 6,19-6,51 mm and 69,2%-71,4%. FWHM values of the three variations were larger than the width of collimation because the penumbra effect and geometric effisiency values were still within tolerance limits of 55%-75%. Keywords: CT dose profiler, CTDI air, FWHM, geometric effisiency 
PENGHITUNGAN OTOMATIS JUMLAH SEL DARAH MERAH DAN IDENTIFIKASI FASE PLASMODIUM FALCIPARUM MENGGUNAKAN OPERASI MORFOLOGI Adi Pamungkas; Kusworo Adi; Choirul Anam
Youngster Physics Journal Vol 1, No 1 (2012): Youngster Physics Journal Oktober 2012
Publisher : Jurusan Fisika, Fakultas Sains dan Matematika, Universitas Diponegoro

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Abstract

Malaria disease still a public health issue in Indonesia. The incidence of malaria in Indonesia is increasing every year. The cause of malaria is a parasite of the genus plasmodium that infected red blood cells through the bite of Anopheles mosquitoes. One of plasmodium type that often the cause of malaria in Indonesia is the plasmodium falciparum. This type of plasmodium causes malignant tertian malaria which threatening for the sufferer’s life. This study’s function is to design a program that capable automatically to calculate the total number of red blood cells, the number of parasites, and identified the plasmodium falciparum phase. The image processing of red blood cells in digital using morphological operations. The results of the testing program has been designed showed the correlation coefficient for counting the total number of red blood cells is 0.997, the validation value for parasit counting is 87.5%, and validation value for phase identification of plasmodium falciparum is 87.5%. Key words : red blood cell, falciparum, calculation, identification, automatic http://ejournal-s1.undip.ac.id/index.php/bfd/article/view/63
DISTRIBUSI FLUKS NEUTRON SEBAGAI FUNGSI BURN-UP BAHAN BAKAR PADA REAKTOR KARTINI Fatkhiyatul Athiqoh; Wahyu Setia Budi; Choirul Anam; Tri Wulan Tjiptono
Youngster Physics Journal Vol 3, No 2 (2014): Youngster Physics Journal April 2014
Publisher : Jurusan Fisika, Fakultas Sains dan Matematika, Universitas Diponegoro

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Abstract

The effective multiplication factor (keff) and the flux distribution in the Kartini reactor which used Uranium Zirconium Hydride (UZrH) as fuel, pure water (H2O) as moderators and cooland has been analyzed using Monte Carlo simulation. The flux distribution analyzed by splitting core reactor become 5 rings (B, C, D, E and F). The effective multiplication factor (keff) and flux distribution calculated by MCNP 4C with burn-up variation 0%, 2,5%, 5%, 7,5%, 10%, 12,5%, 15%. The result shows that the critical condition obtained from burn-up rate 0% up to 5%. The highest value of flux distribution in the middle, at ring B and the value gets smaller towards to edge of reactor core.Keywords : flux distribution, keff, MCNP, Kartini reactor
Co-Authors - Basyirun A.A. Ketut Agung Cahyawan W Achmad Helmy Djawahir Adi Pamungkas Aditya, Wahyu Yoga Agung, Fikri Mudzakki Syam Ahadiyah, Naeli Ni'matin Ahmad Zainudin Ahmad, Karyoto Al Farobi, Mohammad Alan Tanjung Aji Prastowo Alfian Rizani Alfiana Alfiana Alhamid, Mohammad Zamakhsari Ali, Mohd Hanafi Alindra, Bagoes Malik Amalia, Laili Amilia, Riska Amirul Mukminin Ana Amiroh Anak Agung Gede Sugianthara Andika, Febri Dwi Andri Febrianto, Andri Andy Rachman Andy Suryowinoto Annisa Tenri Maya Anugrah Ariyani S. Ariefin, Mesra Surya Ariij Naufal Armanu Thoyib Aulia, Febriana Nur Awalizan, Mochamad Sigit Awwalin, Aufi Rizqiatul Azhar Azhar Aziz Nugroho Azraini, Dinda Basito Basito, Basito Betri Arisa Bramada Winiar Putra Cahyo Indarto Catur Edi Widodo Conoras, Moch El Bahar Daffafauzan, Daffafauzan Damayanti, Elok Darmawan, Bayu Sigit Dayanti, Putri Rahma Dewi A. Insiano Dewi Dewandari, Dewi Dewi Tri Nugraheni, Dewi Tri Diaguna, Ridwan Dian Eka Kusumawati Dougherty, Geoff Dwi Siwi Retnoningsih Efendi, Muhammad Yusuf Efendi, Nur Mahfud Eka Putra, Ricky Eko Hidayanto Eko Sulistijono Elvira Rizqi Widyanti Emi Widiyanti Emmy Hamidah Erita Yuliasesti Diah Sari Erlyna Wida R, Erlyna Wida Erlyna Wida Riptanti Esti Widowati, Esti Evi Handriani Bertua Simamora Evi Setiawati Fadilah, Mega Fianita Faiza, Nadia Mayla Fakhrur Rozi, Nanang Farhatin Nurul Ihya Fatichin, Khusnul Fatkhiyatul Athiqoh Fauzia Puspa Lestari Firmansyah, Riza Agung Firnanda, Rony Freddy Haryanto Freddy Haryanto Fuad, Ali Geoff Dougherty Geoff Dougherty Geoff Dougherty Gusti Ngurah Sutapa Hananur Rohiem, Nasyith Handayani, Heni Yuli Handini Devi Yunitasari Hanif Rani Iswari Hardiyanti, Yati Harini Harini Harsono Harsono Herfan, Mohammad Heri Pratikto Heri Susanto Heri Sutanto Heri Sutanto Hermawan, Akbar Hidayatullah, Fajar Hima, Mulk HMS Chandra Kusuma Huda, M Masrur I Wayan Ari Makmur Idam Arif Idam Arif Ilafi, Rasi Insani, Auralia Fikri Intan Andriani istiqomah istiqomah Iva Khoiril Mala Jamal Jamal Jamhari Jamhari Japeri Japeri Jujun Septiadi K Sofjan Firdausi K. Sofjan Firdausi Khadafi, Shah khusnul khotimah Kliwon Hidayat Kristiyono, Antonius Edy Kusworo Adi Laksono, Bagus Yudit Leksono, Sonny Lestari, Fauzia Puspa Luh Putu Ratna Sundari M IRFAN, M Mahendra, Alief Thufail Mahfudz Fauzan Maman Herman Mariyatul Qibtiyah Masdi Masdi Masfufiah, Ilmiatul Maulania, Raudya Zahra Moch. Junaidi Hidayat Mohammad Haekal Mohd Hanafi Ali Mubarok, M. Rifqi Much Azam Muchammad Kurniawan Muhammad Farhan Muhammad Khumaedi Muhammad Nur Muharom, Syahri Mukhtar Hanafi Munawir Munawir Nafisah, Thohirotun Natih, Made Naradhara Ayuko Naufal, Ariij Nazil Ainurrofik Nira Radita Nopendri Nopendri Nugraha, Larasadi Harya Nugroho Agung, Nugroho Nur Dwi Prasetyo Nur Paramita Nira Mulyono Nurul Firdausi Nuzula, Nurul Firdausi Oktafiana, Brina Oktavia, Armida Patria Uman Putra, Novian Permana, Rizal Bagus Prabowo, Rizkianto Prasetyo, Indra Prawoto, Agus Priharto, Muria Ilham Priyono Priyono Priyono, Setyo Puput Khusnaiatul Purwoto, Septyaningrum Putri Putri, Maulidia Qonita, Qonita Rahmawati, Widiya Raji, Moh. Ramadan, Arief Dian Rena Widita Rena Widita Rika Fitriani Rinaldi, Ade Rizky Riris Trima Derita Sari Riska Amilia Rizalnur Firdaus Rokhim, Ahmad Abdur Romadhon Romadhon Ryan Kurniawan Sabiliat, Nur Edy Sabiliat, Nur Edy Salim, Ach. Khafid Salsabila, Sagita Samponu, Yohakim Benedictus Samponu, Yohakim Benedictus Sanggam Ramantisan Saptaria, Lina Saragih, Jhon Hadearon Sari, Devi Nur Mayang Sari, Virda Nawang Septyan, Mamat Setiawan, Agus Saleh Setyawati, Rohmah Cahya Eka Setyowati Setyowati Sirojudin Sirojudin Siti A'isyah Siti Maesaroh Siti Nur Endahyani Slamet Riyanto Sofyan, Misba Maulana Sri Adikadarsih, Sri SRI RAHAYU Subari Subari Sugiyanto - Sulistyowati Sulistyowati, Riny Sumariyah Sumariyah Suminah, - SURVIVAL - - Suryono Suryono Sutikno, Bambang Sutrisno, Sutrisno Syafitri, Diva Kaila Syah, Iwan Nur Dian Syahrorini, Syamsudduha Syaifudin, Ahmad Bahron Syaikhuddin, Muhammad Miftakhul Takatoshi Toyoda Tampubolon, Bahroin Idris Tamrin Fathoni Titiek Suheta Toshioh Fujibuchi Tri Winarni Agustini Tri Wulan Tjiptono Trisna Budiwati Tuffahati, Andira Shafa Tunggul Drajat Mulatomo Vincensius Gunawan S.K. Virgia Ningrum Fatnar, Virgia Ningrum VITA FIBRIYANI, VITA Wahyu Edy Wibowo, Wahyu Edy Wahyu S. Budi Wahyu Setia Budi Wati, Sulistyowati Sulis Widi, Sayekti Nugrahaning Yanto, Dwi Yanurita Dwihapsari, Yanurita Yati Hardiyanti Yoel Midel Leitabun Yunianti, Nina Yunus Abu Bakar, M. Yusuf HR, Mohammad Zaenal Arifin Zaenul Muhlisin Zakaria, Moch. Bagus