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ANALISIS NOISE LEVEL HASIL CITRA CT SCAN PADA TEGANGAN TABUNG 120 kV DAN 135 kV DENGAN VARIASI KETEBALAN IRISAN (SLICE THICKNESS) Ayu Adriyuni Lestari; Heri Sutanto; Zaenal Arifin
Youngster Physics Journal Vol 3, No 3 (2014): Youngster Physics Journal Juli 2014
Publisher : Jurusan Fisika, Fakultas Sains dan Matematika, Universitas Diponegoro

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Abstract

Some of the parameters that influence noise level are tube voltage and slice thickness, that can affect image quality and accuracy in diagnosis, with a tolerance limit of the CT number ± 7 HU. The objective of this study is to define the noise level on the tube voltage 0f 120 kV and 135 kV with slice thickness variations. The measurement used water phantom scanning of head with tube voltage 120 kV, 135 kV and slice thickness 2, 3, 5, 7 and 10 mm. water phantom scanning of the abdomen with tube voltage 120 kV and slice thickness 3, 5, 7, 10 and 20 mm. Noise level got from central ROI area phantom. The high tube voltage and increasing the slice thickness, that the noise level decreases because the x-ray tube produced high x-rays energy and high photons penetrating to tissues. Noise levels are good when using eksposure parameters are current-time and tube voltage : 225 mAs, 135 kV with a slice thickness of 10 mm is 0.47 % for the head and 375 mAs, 120 kV with a slice thickness 3 mm is 0.45 % for the abdomen.Keywords: Noise, Slice thickness,Phantom, CT number
ANALISIS PERHITUNGAN DOSIS SERAP TERAPI ROTASI DENGAN METODE TISSUE PHANTOM RATIO (TPR) PADA LINEAR ACCELERATOR (LINAC) 6 MV Ifa Istighfaroh; Evi Setiawati; Zaenal Arifin; Sanggam Ramantisan
Youngster Physics Journal Vol 5, No 4 (2016): Youngster Physics Journal Oktober 2016
Publisher : Jurusan Fisika, Fakultas Sains dan Matematika, Universitas Diponegoro

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Abstract

This Research has been conducted for the absorbed dose calculation in rotational treatment with Tissue Phantom Ratio (TPR) method. The purpose of this study to determine the absorbed dose comparisons on rotational therapy based on calculations and measurements. The study was conducted in a solid water phantom with 100 cm SAD. The study was conducted on a square field area of 5 cm x 5 cm, 7 cm x 7 cm and 10 cm x 10 cm as well as on equivalent field area of 10 cm x 10 cm, consist of 8 cm x 13,3 cm and 9 cm x 11,5 cm area. The result is percentage of difference between the value of measurements and calculations dose on each field area. The field area which have percentage below the tolerance value is a 7 cm x 7 cm with the percentage of difference of 0.46%. For the field area of 5 cm x 5 cm has a percentage of difference of 2.65%, while the area of 10 cm x 10 cm and equivalent field area the percentage of difference were high at more than 3%.
ANALISA PENGARUH FAKTOR EKSPOSI TERHADAP ENTRANCE SURFACE AIR KERMA (ESAK) Muahamad Irsal; Eko Hidayanto; Zaenal Arifin
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 research has been analyzed of the effect of exposure factors at the entrance surface air kerma (ESAK) of the thorax radiographs. This research uses anthropomorphic phantom, multipurpose detectors, FFD 100 cm, with radiation field 25 cm × 25 cm. irradiation conditions is given by the variation of expose factors using tube voltage 50-100 kV and tube current-time 2-20 mAs. The results of research showed that the effect of the tube voltages to the entrance surface air kerma experience is increase a specific approximated by an polynomial equation with a correlation coefficient value R2 = 1 and the variation of the tube current-time increased linearly approximated by a approach linear equation R2 = 1, uses of tube current time under 4 mAs with resulted lower the entrance surface air kerma based on IAEA Safety Series No. 115 (1996) is 0.4 mGy at examination of thorax radiographic, and conducted a calculation uncertainly  value of every expose factors using variations of tube voltage and tube current-time based on scenarios three of IAEA Technical Report Series No. 457(2007).Keywords: entrance surface air kerma, thorax radiography, the tube voltage, tube current-time, phantom anthoropomorphic.
ANALISIS DOSIS SERAP RELATIF BERKAS ELEKTRON DENGAN VARIASI KETEBALAN BLOK CERROBEND PADA PESAWAT LINEAR ACCELERATOR Lamtiyah Ikha Indriyana; Eko Hidayanto; Zaenal Arifin
Youngster Physics Journal Vol 3, No 3 (2014): Youngster Physics Journal Juli 2014
Publisher : Jurusan Fisika, Fakultas Sains dan Matematika, Universitas Diponegoro

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Abstract

During radiotherapy treatment, critical organs are shielded using cerrobend blocks. The objective of this study was to define the minimal thickness of cerrobend blocks so that the relative absorbed dose in target less than 5%. All measurements were performed using linac Siemens/Primus Mclass 5633. Phantom relative absorbed dose were measured for square field 10 x 10 cm2. The thickness of cerrobend blocks were 2, 4, 6, 8 and 10 mm. The measurements in water were performed using compact chamber fitted with acrylic build up caps.The minimal thickness of cerrobend blocks for 5, 10 and 14 MeV electron beams are 2, 4 and 6 mm, respectively. The relative absorbed dose for phantom’s surface, maximum depth and x-ray tail using those blocks are 0.12%, 0.16%, 0.21%, 2.18%, 1.56%, 1.16%, 2.92%, 2.47% dan 1.70%.The relative absorbed dose decreases with the increasing of cerrobend block  thickness and phantom depth. Therefore, if cerrobend blocks are used to protect critical organs, the thickness should be taken into account accurately.Keywords: cerrobend blocks, relative absorbed dose, electron beams
ANALISA TINGKAT KONTAMINASI DOSIS NUKLIR DAN LAJU PAPARAN RADIASI PADA INSTALASI KEDOKTERAN NUKLIR Rafli Filano; Eko Hidayanto; Zaenal Arifin
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 research has been analyzed the level of nuclear contamination and radiation exposure rate at installation of nuclear medicine with efforts a radiation protection is the prevention or decrease the number of entry of radioactive material into the human body. The method used to conduct measurement a count of contamination of surface work area resulting from the use of radioactive substances and carried out at a distance of 0.5 cm between the detector window with contaminated areas, while measuring the radiation exposure rate in each of center room at height of 1 meter from the surface of the floor in various rooms installation of nuclear medicine. The results of measurement obtained levels of contamination nuclear dose in various rooms installation of nuclear medicine is from 0,16 to 243 Bq/cm2 were classified as low to high levels of contamination. While the results of measurements of the radiation exposure rate is from 0,026 to 1,693μSv/h, which is classified as below the allowable dose value level, so it is still safe for radiation workers and other patients. Keywords: Radiation Protection, Radioactive, Contamination, Radiation Exposure Rate, Nuclear Medicine
RESPON PHOTOSTIMULABLE PHOSPHOR (PSP) PADA COMPUTED RADIOGRAPHY TERHADAP AKURASI TEGANGAN TABUNG DAN LINIERITAS KELUARAN PESAWAT SINAR-X Dwi Adhianto; Heri Sutanto; Zaenal Arifin
Youngster Physics Journal Vol 3, No 3 (2014): Youngster Physics Journal Juli 2014
Publisher : Jurusan Fisika, Fakultas Sains dan Matematika, Universitas Diponegoro

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Abstract

The research has been done to analyze Photostimulable Phosphor (PSP) in Computed Radiography (CR) responses related to exposure factor variation which usually used in determining of tube voltage accuracy and output linearity of X-ray machine. The aim of this research is to analyze of linear response of PSP to variation of exposure factor that related to usage of tube voltage in kVp and tube current-exposure time (mAs).The Method which used was exposing CR with an ascent of tube voltage 50 till 90 kVp with a constant tube current-exposure time in 0,5 till 16 mAs. Exposure Index, Deviation Index, and Indicated Equivalent Air Kerma (KIND) referred to  IEC standard 62494-1 at each expose and mean gray value of digital image were used as PSP responses. Those are related to kVp and mAs variation. The result was obtained that photostimulable phosphor response in Exposure Index and Deviation Index parameters had correlation coefficient >0.97 in logarithmic relation at all exposure factor variation. Parameter of Indicated Equivalent Air Kerma (KIND) referred to IEC standard 62494-1 had linier relation with >0.97 amount of correlation coefficient. Linearity coefficient was obtained 0.005-0.061 using IEC standard/mAs. Mean gray value had correlation coefficient >0.94 in logarithmic relation at using of steady tube voltage with the result that could be indicator of output linearity of X-ray machine. The result was obtained that mean gray value could be a tube voltage accuracy indicator at using of 0.5 till 8 mAs with correlation coefficient >0.83 amount.Keywords : computed radiography, exposure indicator, mean gray value, output linearity, tube voltage accuracy
Distribusi radionuklida alam dalam sampel lingkungan tanah, air dan tanaman sekitar PLTU Rembang Aditya Yoga Syah Putra; Dwi P. Sasongko; Zaenal Arifin; Sukirno Sukirno
Youngster Physics Journal Vol 6, No 4 (2017): Youngster Physics Journal Oktober 2017
Publisher : Jurusan Fisika, Fakultas Sains dan Matematika, Universitas Diponegoro

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Abstract

Research of the natural radionuclide distribution of soil, water and plant samples around Rembang Coal Fired Power Plant (CFPP) has been done with the purpose of the study is to know the activity concentration of natural radionuclide, the pattern of distribution of environtment radioactivity around Rembang CFPP with soil, water and plant samples and compare the activity concentration of natural radionuclide around Rembang CFPP with Environmental Radioactivity Limit Values (ERLV) which is listed on the Perka Bapeten No 16 of 2013 about Safety Radiation in Storage of Technologically Enhanched Naturally Occuring Radioactivity Material. Sample analysis method using gamma spectrometry with HPGe detector and Maestro 2 software is based on SNI 1070.3-2009. The calculated concentration of natural radionuclide activity 226Ra, 228Ra, 232Th dan 40K in soil sample is (8.17×10-3 ± 2.33×10-4; 9.99×10-3 ± 1.69×10-4; 7.84×10-3 ± 2.78×10-4; 4.46×10-2 ± 6.78×10-4) Bq/g. Water sample (3.07×10-3 ± 4.05×10-4; 3.59×10-3 ± 3.22×10-4; 6.59×10-4 ± 5.59×10-5; 2.82×10-2 ± 1.93×10-3) Bq/L. Plant sample (1.69×10-3 ± 9.06×10-5; 7.56×10-4 ± 5.04×10-5; 4.13×10-4 ± 3.03×10-5; 1.17×10-2 ± 7.52×10-4) Bq/g. The distribution pattern of the concentration of natural radionuclide activity that is formed that is in the soil sample has the distribution pattern of the distance from CFPP Rembang the bigger concentration activity. Furthermore, in water and plant samples the distribution pattern tends to lead to a location close to the CFPP that has a bigger concentration of activity. Comparison the concentration of natural radionuclide activity with Environmental Radioactivity Limit Values (ERLV) it was found that the overall concentration of natural radionuclide activity in soil, water or plant samples at each sampling site still did not exceed the Environmental Boundary Limit Radioactivity (ERLV) that defined by Perka Bapeten No 16 of 2013 about Safety Radiation in Storage of Technologically Enhanched Naturally Occuring Radioactivity Material.Keywords: Natural radionuclide, environment sample, Rembang CFPP, gamma spectrometry, radioactivity, distribution.
PENGARUH PERUBAHAN FAKTOR EKSPOSI TERHADAP NILAI CT NUMBER Tina Melinda; Eko Hidayanto; Zaenal Arifin
Youngster Physics Journal Vol 3, No 3 (2014): Youngster Physics Journal Juli 2014
Publisher : Jurusan Fisika, Fakultas Sains dan Matematika, Universitas Diponegoro

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Abstract

CT Number valuehad been conducted with various of exposurefactoronCT. Testingwas conducted to test the CTNumber value changeswith varioues of exposure factorsthencompare it withthe recommendedtolerance. Testing was doneby usingsome objectthere arewater phantom, plasticwaterphantom, chickenblood, chicken (breast part) andchickenbone(thigh). Performedwithtwoscanning, axialandhelicalscanning methods. Various of exposurefactors used the voltage 80 kVp to 140kVp, current100 mA  to 180mAandexposure time0.6 second to 2second. Collimatorwith alargeselection and slice thickness 5mm.            From the test resultshave known thatchangesof the exposurefactorswill affectedCTNumber value. CT Number value obtain from the test results by using water phantom -2,50 HU until -4,99 HU, plastic water phantom -6,99 HU until +6,99 HU, blood +31,01 HU until +36,70 HU, chiken (soft tissue) +48,33 HU until +66,61 HU and bone +800,15 HU until +1188,28 HU.Thevalue is stillwell withinthe recommendedtolerancesareforwater phantom andplasticwaterphantom0±7HU, blood+30 HU to+45HU, soft tissue+37 HUto+300 HU andbone+700HUto+3000 HU.Keywords: CTNumber, exposure factors, plasticwaterphantom, axial scanning andhelicalscanning
ANALISA KURVA PERCENTAGE DEPTH DOSE (PDD) DAN PROFILE DOSE UNTUK LAPANGAN RADIASI SIMETRI DAN ASIMETRI PADA LINEAR ACCELERATOR (LINAC) 6 DAN 10 MV Mariatul Khiftiyah; Eko Hidayanto; Zaenal Arifin
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

External radiotheraphy uses either symmetry or asymmetry radiation field. Percentage Depth Dose (PPD) and Dose Profile on either symmetry or asymmetry radiation field is an important parameter in conducting external therapy that is to analyze the result of parameters used for measurement, whether it is adjusted according to the specified tolerance limit. If the field size 10 X 10 cm2 is still in specified tolerance limit or it has been exceeding the limit.The techique used to collect the data was comparing whether dose distribution taken on the surface of either symmetry or asymmetry radiation field with maximum depth gained from Percentage Depth Dose (PPD) measurement and in the depth of 2 cm. By using device Linear Accelerator (LINAC) energy foton 6 and 10 MV in the radiation field with condition field no off-set and off-set 1 cm, off-set 3 cm and off-set 5 cm with Source Surface Distance (SSD) value 100 cm and in radiation field 10 X 10 cm2.The measurement result showed a change depth on Percentage Depth Dose (PPD) value in the off-set of radiation field 5 cm, on both kinds of energy caused by beam hardening, with value of symmetry and flatness 1.43% and 9.28%, for energy 6 MV and 2.2%, 6.59% for energy 10 MV. There was a change in file profile that caused declining value of flatness, and symmetry. Dose distribution because of this asymmetry radiation field should be concerned in clinical for application of asymmetry radiation field usage. Keywords: Percentage Depth Dose (PDD), Profile Dose, Symmetry, Asymmetry, flatness.
ANALISIS DISTRIBUSI COMPUTED TOMOGRAPHY DOSE INDEX (CTDI) PADA BODY PHANTOM Nur Paramita Nira Mulyono; 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

Measurement of Computed Tomography Dose Index (CTDI) Distribution in Body Phantom has been done in Dr. Karyadi’s Hospital. The purpose of this research were to find out value of CTDI in the five holes in body phantom and to determine relation between slice thickness and CTDI. This research used CT Dose Profiler in helical CT and CT Dose Profile Analyzer Software. This measurement applied protocol of abdomen with tube voltage 120 kV, time rotation 200 mAs, pitch 1, scan length 160 mm, and scan time 5, 07 second. Measurement was applied variation of detector position in the five holes (center, top perifer, right perifer, bottom perifer, and left perifer) and slice thickness   1 mm, 2 mm, and  3 mm. Average CTDI value in five holes of body phantom has range about 11,97 mGy until         13,17 mGy. There are slight differences among all of five holes. It show that dose ditribution in the center and perofer of body phantom tend to be homogeneous. The fluctuation of CTDI values for 1 mm, 2 mm, and 3 mm slice thickness has nocertain pattern or trend. CTDI values have slight differences among the thickness. The measurement show that   1 mm, 2 mm, and 3 mm slice thickness has 0,5 mGy difference to CTDI value. Keyword: CTDI, five holes, body phantom, slice thickness
Co-Authors - Hwihanus - Wiendartun Abdul Kosim, Abdul Abdul Kudus, Wahid ABDUL MANAF Abdullah Merjani, Abdullah Abdur Rohim, Abdur Abrori, Muhammad Achmad Chalid Afif Achmad Fauzy, Achmad Achmad Gani Achmad Sobirin, Achmad Achmad Zainudin, Achmad Adi Pamungkas Adi Pratama, Adi Adi Saputra Adianti Paramita, Adianti Adithia P, Eka aditya surya hartanti Aditya Yoga Syah Putra Aflah, Muhammad Nur Afma, Vera Afriliani, Nita Afrio Rika. R Afthari Mudatsir T, Andi Ageftry, Farhan Dio Agung Kurniawan Agung Sudaryono AGUS AGUS Agus Bashori Agus Joko Prasetyo Agus Winarno, Agus Agus Wismanto Agustina Widodo Ahadiyah, Naeli Ni'matin Ahmad Suriadi, Ahmad Ahmad Tafsir, Ahmad Ahmad Zahro Ahmad, Andi Ahmad, Asep Ahyadi Ajat Rukajat Ajmal, Ajmal Al Jabbar, Ahmad Vicqieh Albayani, Melati Inayati Albayani, Melati Inyati Alfandi, Iqbal Alfani, Wahyu Ali Djunaedi Ali Imron Ali Ridlo Alvian Ideastari, Nukat Alzami, Farrikh Amik Krismawati Amri Panahatan Sihotang Angriawan, Angriawan Ani Kurniawati Anjarini, Titi Annisa Purbasari, Annisa Antari, Gladeva Yugi Aprilia, Elinda Apriliani, Alma ARDIANSYAH ARDIANSYAH Ardiantika, Fitri Nur Ardyantara, David Maharya Arga Dwi Pambudi Arief Slamet Karyadi Arif Hidayat Arif Mustofa Aritonang, Kristianto Ariyanti, Maelina Arman, Feti Artalopa, Ryan Ashari, Ayu Asmana, Arezqi Tunggal Asropah Asropah Asrori, Zainul Assariy, Annas Faiz Astria Liani, Tika Ayu Adriyuni Lestari Ayu, Saras Aziz Thohari, Afandi Nur Aziz, Bakhril Aziz, M. Aziz, Mochamad Azizah, Isnaniar Rahmatul Azizatul, Wafiq B. Rini Heryanti Baharudin, Bany Sutan Bambang Hari Kusumo Bambang Sadono Basri Modding Bonyah, Ebenezer Brilianto, Abra Budi Harsono Budi Wahono, Buang Burhani, Burhani Bustan Bustan, Bustan Cahyaningrum, Fransiska Intan Cahyono, Yoyok Candra Irawan Cecep Gunawan Chaerul Chafid, Candra Chandra, Mochamad Haris Choirul Anam AM Diponegoro Chomsin Sulistya Widodo Christy Atika Sari Cory Amelia Dadang Juandi Dadang Redantan, Dadang Danang Krismawan, Andi Dedi Ansori, Dedi Dedi Nurcipto, Dedi Delianis Pringgenies Dewi Aisah Dewi Dewi Dewi Lestari Dewi Nursukma Purqoti Dharmawati, Nuraeni Dwi Dhian Indah Astanti, Dhian Indah Diah Sulistyani Ratna Sediati, Diah Sulistyani Ratna Dian Istiana Dian Istiana Dias Prihatmoko Dini Hardini Dita Ayu Mayasari, Dita Ayu Djago Djoa, Dominikus Djarwani S Soejoko Djoa, Dominikus Djago Doddy Kridasaksana Dodi Junaedi Dodi Sudiana Dori Kusuma Jaya Dwi Adhianto Dwi Purwantoro Sasongko Dwi Setyorini Dzaky, Rizky Indirwan Edi Faisal Edi Sugiarto Edwin Zusagka Eko Hidayanto Elah Nurlaelah Ellys Yuliarti, Ellys Endah Pujiastuti Endang S, Lolita Endang Supriyanti, Endang Erikson Manurung Ervia Yudiati Evi Setiawati Fachreza, Muhammad Fauzi Fahmi Amiq Faidlon, Ahmad Fajri, Chotamul Fathurrohman, N Fatmawati, Baiq Ruli Fatmawati, Baiq Rulli Fauzia, Rizki Rahmah Febriati, Eka Nanda Ferdiansa, Rezza Aldi Fikri Budiman Fuad Muhammad Gani Gunawan Gatot Yulianto Goib Wiranto, Goib Gozali, Luthfi Gunawan, Erik Gunawan, Wahyu Sahrul Habib Sabil Rosyidi Hadi Putra, Cahya Hadi, Heru Pramono Hadri Kusuma Hafaz, Mohamad Hafizha, Agnifa Isna Hajis, Abdul Hakim, Ahmad Thoriqul Haliza Yuniar, Putri Hapipah, Hapipah Harahap, Akbar Harisa, Ardiawan Bagus Harry Kurniawan Hartadi, Arif Hasan Habibi, Hasan Hasanah, Luthfiyah Hayatunisa, Hayatunisa Hendrananto, Novan Henry Januar Saputra, Henry Januar Heny Ekawati Haryono Herfan, Djony Heri Sutanto Heru Agus Santoso Hery Irwan Hery Pamungkas, Hery Hery Widijanto Heryanto, M Ary Hidayat Borrong, Raya Hidayati, Baiq Nurul Hinggil Permana Huda, M. Hanif Nur Husnul Khotimah I Gusti Made Kusnarta Icen Ritme Parlindungan Siallagan, Icen Ritme Parlindungan Ida Ayu Putu Sri Widnyani Ifa Istighfaroh Iis Nurhasanah ILHAM Ilham Ilham Iman Firmansyah Imran Imran Indra Gamayanto Indras Marhaendrajaya Indrawati, Yuni Irwan Hadi Irwan Hermawan Islam, Ahmad Fikrul Istianah Istianah Iwandaka, Age Jaenullah, Jaenullah Jafron Wasiq Hidayat Jaganda Marbun, Sandra Jain, Vaibhav Jalaludin, Jalaludin Jarnawi Afgani Dahlan Jatmiko Endro Suseno Jeffry, Muhammad Jelita Rahma Hidayati Johan Andoyo Effendi Noor, Johan Andoyo Effendi Joko Priyono Junaedi Junaedi Junita, Riska K Sofjan Firdausi Karampung, Felix Etena Orba Khoerunnisa, Risyda Aini Khoirun Niam Kisman Kisman Kurnawati, Ani Kurniawan, Samuel Kurniawati, Dita Kusmiyati Kusmiyati Kustiansyah, Nakula Bagus Kustiyowati, Kustiyowati Kusudarmanto, Ayu Melati Ratuningnagari Anisa Kusuma, Alam Budi Kusumadewi, Berlian Nurtyashesti Kusworo Adi Lalang Erawan Lamtiyah Ikha Indriyana Lantara, A. Niniek F. Lathifatus Sun'iyah, Siti Lestari, Rohmini Indah Lidia Olga Listianingrum, Nia Yunita Logawali, Thamrin Lolita Endang Susilowati Lorinanggarani, Ray Harmida M Ary Heryanto M Munir M, Masrukhin M. Arif Hakim Mac Thi Hoai Thuong Maharani, Risky Amelia Mallongi, Syahrir Mantika, Fatmawati Mariatul Khiftiyah Marlina Riskawaty, Heny Marpuah Jamilah, Erni Martini, Eli Maulana Bima, M. Irfan Megantari Putri, Heni Agustini Mellysanovitasari, Mellysanovitasari Mente, La Miftachudin Miftachudin, Miftachudin Miftah Arifin Milenia, Laela Yusriyah Moh. Yusuf Mohammad Fauzy Mohammad Muslimin Ilham Muahamad Irsal Mubarok Anwar, Fahruddin MUCHAMMAD FAIZIN Mudzakkir Ali Muh amin Muhammad Ansar, Muhammad Muhammad Arifin Muhammad Fikri Muhammad Ilham Muhammad Isradi Muhammad Junaidi Muhammad Muhammad Muhammad Ridwan Muhammad Rizalul Wahid Muhammad Syafei, Muhammad Muhammad Syaifullah, Muhammad Mukaromah, Ayu Mukarto Siswoyo Munawar, Endang Muriyati, Dewi Tuti Muslih Muslih Muttaqin, Muhammad Fauzan Nailul Izzah Najid, Muhammad Reza Ahsanun Nanang Nurcholis Napitupulu, Michel Frans Sisco Ngazizah, Nur Nia Kania Niamirroykhan, Achmad Syafiul Nisa, Delvia Noer, Shobirin Nora Fajria Nora Susilowaty Norman Wijaya Gati Novavictorianto, Yosef Kurnia Novi Hendriyanto, Novi Novi Maryani Nugroho, Erik Eko Nur Aeni Widiastuti Nur Islahudin Nur Paramita Nira Mulyono Nur Rahmadani Nur Rochmah, Nur Nur Sukma Purqoti, Dewi Nurhayati Nurhayati Nurlina, Dina Nurnajamuddin, Mahfud Nursahidin, Nursahidin Nursukma P, Dewi Nurul Laili Khoirut Tabi’atin Nurulita, Dwita Oktaviana, Bela Oktaviani, Elisa Olivia Grasera, Brenda Oppusunggu, Leonardus Otong Surasman, Otong Owen, Safira Larasati P, Purwati Pamor Gunoto Pandin, Maria Yovita R Pangyom, Wanudya Pauzan Haryono Permadi, Asep Angga Poppy Intan Tjahaja Pramesti, Diah Gina Pramudita, Eka Avina Prapto Rahardjo, Prapto Prastiawan, Galih Pratama, Indra Yoga Pratama, Wisnu Aditya Pratiwi Babo, Triana Pratiwi, Nurul Intan Prayuda, M. Amril Priawasana, Endra Prihandini, Nadia Aurynnisa Prihastini, Amanda Prihati, Kurniati Primaningtyas, Mega Puput Khusnaiatul Purnomo, Ananda Pandu Candra Purnomo, Muhammad Agus Purqoti, Dewi Nur putri, sulis Putro, Moh Zaenal Abidin Eko Putu Sukmabuana Rachmasari, Annisa Raden Ahmad Dedy Mardani, Raden Ahmad Dedy Rafli Filano Rahadani, Shintya Rahmadani Rahadian, Helmy Rahadian, Helmy Rahayu, Nur Ellyanawati Esty Rahmadani, Shintya Rahman, Rasyad Tanzilur Rahmat Gernowo Rahmawati Hidayah Rahmawati, Mifatun Ramadhan, Taufiq Rasyidah, Firda Inten Ratih Fordiana, Ratih Ratna Roostika Ratna Sariningsih Ratnawati , Tri Rendantan, Dadang REZA FAHLEVI Rifani, Endang Riksandi, Sansan Rina Fiati Risandi, Anton Bimo Risthia Eriana Putri, Risthia Eriana Risty, Alvian Octo Rizka, Ifada Diah Ayu Rizki, Nurlaili Rohman , Dwi Ryan Aswanda Taufiqqur Rohman, M. Hilma Minanur Roihanah, Ana Roji, Fatkhur Romadonika, Fitri Romano Afif Kesuma Roslina Alam Rozanah Rozanah Roziqin, Muhammad Rudi Setiawan Rudihartati, Leni Rusiana, Harlina Putri S, Solikhun Safitri, Rias Pratiwi Safrizal Safrizal Sanggam Ramantisa Sanggam Ramantisan Santosa, Ade Santosa, Tri Nugraha Budi Saputra, Agung Bayu Saputra, Filmada Ocky Saputra, Reihan Sari Ayu Wulandari Sari, Devi Artika Saroso, Bagus Argo Sasono Wibowo Satria, Adhi Putra Sehabudin, Encep Serlin serang Setiadi, Kristoforus Adrian Setiadi, Kristoforus Ardian Setyawati, Rohmah Cahya Eka Silalahi, Edo Hasiholan Silalahi, Yeremia Raynhard Sinaga, Dina Singgih Wibowo Sinring, Bahar Sisno Riyoko Siti Masitoh Slamet Riyadi Soegianto, Soegianto Solakhudin, Nur Muhammad Solly Aryza Sonjaya, Azhar Ramadhana Sri Yani Purwaningsih, Sri Yani Sriyoto Sriyoto, Sriyoto Suasmoro Suasmoro Subarna Sudarmanto, Kukuh Sudrajat, Asep Suharman, Adelia Suharnawi Suharnawi Suhartanta Suhartanta Suherman, Adelia Suherman, Suherman Sujono Sujono, Sujono Sukamto, Titien Suhartini sukarna, kadi Sukartono Sukartono Sukirno Sukirno Sukrisno, Wijayono Hadi Sulistyani, Diah Sumariyah Sumariyah Sumarya, Edi Sumarya, Edy Sumiati Sumiati Sundari, Retno Tresno Supingato, Agus Supriatno, Wendy Supriyadi Supriyadi Supriyo, Sarwo Suryo Hartanto Suryono Suryono Susilo, Tarsisius Sutikno, Ery Sutriono, Raden Sutrisno, Yuliana Rachmawati Syafa'atin, Nur Syahmada, Dienda syahputra, Rizky Syahrir Akil Syamdarniati, Syamdarniati Syamrul, Syamrul Syamsiar, Syamsiar Syirva, Atika Nailah Syuhada' Syukri Indra Tamami, Aries Jehan Tamamy, Aries Jehan Teguh Tamrin Tejowulan, R Sri Thomas Thomas Tina Melinda Tirtayasa, Muh. Ageng Tri Listyorini Triasih, Dharu Turnip, Maida Ubay Harun Ukhti Lailun Nisa Ulil Abshor, Ulil Ulum, S.I Bahrul Veithzal Rivai Zainal Vera Methalina Afma, Vera Methalina Victory, Vivi Sumanti Wahyu Setia Budi Wahyudi, Tody Waluyo Wibowo , Pipid Ari Widiyanto, Asep Widodo, Muhammad Ari Wimbyarto, Najwa Paramitha Winanda, Nieke Rudyanty Winata, Roy Albi Winda Nurmayani M Wiraatmaja, Tubagus Firman Wulandari, Alfia Putri Yaya S. Kusumah Yohana Theresia Maria Astuti, Yohana Theresia Maria Yosep Kunia, Novavictorianto Yovita R Pandin, Maria Yunie Armiyati Zaenal Arifin Zubair, M. Abdul Hamid Zulfa, Nur Roihanah Zuliardi, Zuliardi Zulkarnain, Fahmi Zulkifli, Zuklifli Zurley, Zianna Zuswana, Aries Zzakiyah, Laeli