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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.
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
PENGUKURAN DAN PENGHITUNGAN VOLUME PHANTOM DARI CITRA COMPUTED TOMOGRAPHY (CT) SCAN Riris Trima Derita Sari; Kusworo Adi; 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 research has been done to the measurement and calculation of phantom volume of computed tomography (CT) Scan image. The aim of the study is to calculate the phantom volume based on CT Scan image analysis and find out the relationship between phantom volume and the variation of phantom position towards central ray. The calculation was done by using trapezoid integration method. The study used 130 kV, 93 mAs tube current, and 8 mm slice thickness. The resulting image is converted from gray scale image into a binary image. Then the surface area of the phantom was calculated. After getting the phantom surface area so that the volume of the phantom can be calculated. The calculation result shows that the phantom volume based on CT Scan image with perpendicular phantom, 30 mm to-the-left movement, 50 mm to-the-right movement towards central ray is 11160708 mm3, 11148172 mm3, and 11149136 mm3. The phantom volume based on CT Scan image with the least error percentage when phantom position is perpendicular towards central ray is 3,63%. 30 mm to-the-left and 50 mm to-the-right movement of phantom shows greater error percentage compared with perpendicular phantom towards central ray. The error percentage is from 3,74 % and 3,73 %. Phantom volume calculation is more accurate if phantom is perpendicular towards central ray. Keywords: volume, phantom, image, calculation, central ray
PENENTUAN KOEFISIEN SERAPAN KAYU BANGKIRAI (SHOREA LAEVIFOLIA) DAN PERBANDINGANNYA TERHADAP TIMBAL (Pb) SEBAGAI DINDING RUANG RADIOLOGI DIAGNOSTIK Japeri Japeri; Heri Sutanto; Choirul Anam
Youngster Physics Journal Vol 2, No 4 (2013): Youngster Physics Journal Oktober 2013
Publisher : Jurusan Fisika, Fakultas Sains dan Matematika, Universitas Diponegoro

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Abstract

Shield utilization is very important to protect employee and people from radiation. Therefore, the rules are made that one of them is to regulate construction design of diagnostic radiology room which meet radiation protection standart. Indonesia has natural resources which potential to be radiation shield material. The research has been done to determine absorption coeffcicient of bangkirai (Shorea laevifolia) and its comparison with Pb as wall of diagnostic radiology room. X-ray absorption between bangkirai and Pb as the following : Voltage, current and time of X-ray mobile were setted in 81 kV and 32 mAs, distance between focus and object was 100 cm, Multi Purpose Detector (MPD) placed under object, area of irradiation field opened in 5 cm x 5 cm, central beam placed in the center of objects appropriately and then expotion was conducted for untreated bangkirai with (Pb) and treated bangkirai which heated in 100°C for  60 minutes repeteadly according to variation of determined thickness material, finally expotion was conducted for each thickness for three times so that average value obtained and it was repetead until absorption coefficient value of this material obtained.  Result of X-ray absorption on bangkirai tests showed that absorption coefficient () effective for untreated bangkirai and treated bangkirai is 0,029/mm and 0,027/mm, respectively. Equality result showed that unheated bangkirai with 1,3 mm Pb is equivalent with 254 mm untreated bangkirai, while heated bangkirai with 1,3 mm Pb is equivalent with 273 mm treated bangkirai. To reach 2 mm of Pb, untreated bangkirai and treated bangkirai were used with thickness off 391 mm and 420 mm, respectively.Keywords : X-ray mobile, Multi Purpose Detector (MPD), Pb, Bangkirai, Absorption Coefficient ()
EVALUASI METODE PENENTUAN HALF VALUE LAYER (HVL) MENGGUNAKAN MULTI PURPOSE DETECTOR (MPD) BARRACUDA PADA PESAWAT SINAR-X MOBILE Handini Devi Yunitasari; Evi Setiawati; Choirul Anam
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 dose received by the patient and the radiographic image quality is determined by the value of the half value layer (HVL). Multi Purpose Detector (MPD) Barracuda, produced by RTI Electronics, Sweden, is a solid state detector that can be used to measure the value of HVL just one exposure. This study was conducted to evaluate the accuracy of measurement of the HVL’s value with single exposure methods using the MPD Barracuda. In this study the value of HVL measurements performed with distance of focus to detector 100 cm, field size of 10x10 cm2 and times- current 12.5 at a voltage of 50 kVp, 60 kVp, 70 kVp, 81 kVp and 90 kVp.  HVL measurement for single exposure method  conducted without the addition of Al filter. As for comparative used standard methods that use some thickness variation of filters from 0.5 to 5.0 mmAl. In the standard method, determination of HVL values calculated in two ways: interpolation formula and method of graphs. The results showed that the value of HVL using MPD Barracuda with single exposure method produces a lower value than the standard method used multiple filters and HVL calculated by interpolation and graphics.Keywords: Half Value Layer (HVL), Multi Purpose Detector (MPD) Barracuda, X-ray.
Co-Authors - Basyirun A.A. Ketut Agung Cahyawan W Aang Saeful Milah Achmad Helmy Djawahir Ade Yamindago Adi Pamungkas Aditya, Wahyu Yoga Adya Hermawati Agung, Fikri Mudzakki Syam Ahadiyah, Naeli Ni'matin Ahmad Zainudin Ahmad, Karyoto Ainul Labib, Mohammad Al Farobi, Mohammad Al Hasany, Mochammad Quthburrozi 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 Andika, Hubi Rahmat Andri Febrianto, Andri Andy Rachman Andy Suryowinoto Anugrah Ariyani S. Ariefin, Mesra Surya Arifin, Muhyiddin Zainul Ariij Naufal Ariyoga, Usada Nur Armanu Thoyib Asep Yoyo Wardaya Awalizan, Mochamad Sigit Awwalin, Aufi Rizqiatul Azhar Azhar Bambang Hariyadi Bara Yudhistira, Bara Basito Basito, Basito Betri Arisa Bintoro Wardiyanto, Bintoro Bisma Barron Patrianesha Cahyo Indarto Catur Edi Widodo Conoras, Moch El Bahar Damayanti, Elok Darmawan, Bayu Sigit Deka Andini Della Rulita Nurfaizana Dewi Dewandari, Dewi Dewi Tri Nugraheni, Dewi Tri Dewi, Citra Satrya Utama Dian Eka Kusumawati Dougherty, Geoff Dwi Ishartani Dwi Siwi Retnoningsih Edhi Nurhartadi Efendi, Muhammad Yusuf Efendi, Nur Mahfud Eka Putra, Ricky Eko Hidayanto Eko Sulistijono Elvira Rizqi Widyanti Emi Widiyanti Emmy Hamidah endah andayani Erita Yuliasesti Diah Sari Erlyna Wida R, Erlyna Wida Erlyna Wida Riptanti Esti Widowati, Esti Evi Handriani Bertua Simamora Evi Setiawati Fachry Abda El Rahman Fadilah, Mega Fianita Fakhrur Rozi, Nanang Farha, Reyhan Farhatin Nurul Ihya Fatichin, Khusnul Fatkhiyatul Athiqoh Fikri, Muzayyinul Firmansyah, Muhamad Taufiq Firmansyah, Riza Agung Firnanda, Rony Freddy Haryanto Freddy Haryanto Geoff Dougherty Geoff Dougherty Geoff Dougherty Ghiffari, Syauqi Muhammad Gusti Ngurah Sutapa Hamzah, Nur Laely Hananur Rohiem, Nasyith Handayani, Heni Yuli Handayani, Sri Handini Devi Yunitasari Hanif Rani Iswari Hardiyanti, Yati Harini Harini Harsono Harsono Herfan, Mohammad Heri Pratikto Heri Susanto Heri Sutanto Heri Sutanto Hidayatullah, Fajar Hikmah, Devi Ismiatul Hima, Mulk HMS Chandra Kusuma Huda, M Masrur I Wayan Ari Makmur Idam Arif Idam Arif Ilafi, Rasi Insiano, Dewi A. Intan Andriani Irwan Sudarisman istiqomah istiqomah Iva Khoiril Mala Jamal Jamal Jamhari Jamhari Japeri Japeri Juhri, Muhammad Jujun Septiadi K Sofjan Firdausi K. Sofjan Firdausi Kariyono Kawiji Kawiji Kezia Evangelista Khadafi, Shah khusnul khotimah Kliwon Hidayat Kusworo Adi Laily, Rysda Aina Laksono, Bagus Yudit Lamsadi Lamsadi Leksono, Sonny Lestari, Fauzia Puspa Linardi, Jade Irene Luh Putu Ratna Sundari M IRFAN, M Mahendra, Alief Thufail Mahfudz Fauzan Maknuunah, Rismaa Jauharotul Maman Herman Mariyatul Qibtiyah Marlina, Tuti Masdi Masdi Masfufiah, Ilmiatul Masruroh, Heni Masruroh, Zanani Siti Maulidi, Syahrol Maya, Annisa Tenri Mintohari, Mintohari Moch. Junaidi Hidayat Mohammad Haekal Mubarok, M. Rifqi Much Azam Muchammad Kurniawan Muhammad Khumaedi Muhammad Nur Muhammad Yusuf Muhammad, Naufal Dzakwana Muharom, Syahri Mukhtar Hanafi Mulatomo, Tunggul Drajat Munawir Munawir Muqorrobin, M. Zainul Mutingatu Sholichah Nafisah, Thohirotun Naufal, Ariij Nazil Ainurrofik Nia Aprilia Bisari Noor, Ahmad Nopendri Nopendri Nugraha, Larasadi Harya Nugroho Agung, Nugroho Nugroho, Alan Alda Nur Dwi Prasetyo Nur Her Riyadi Parnanto Nur Heriyadi Parnanto Nur Paramita Nira Mulyono Nur Rahmah Hidayati Nurdeng Deuraseh Nurhidayah, Rahmawati Eka Nurul Firdausi Nuzula, Nurul Firdausi Oktafiana, Brina Oktavia, Armida P Hadi Wibowo, Rahmat Parnanto, Nur Her Patria Uman Putra, Novian Permana, Rizal Bagus Pernama, Candra Prabowo, Rizkianto Prasetyo, Indra Pratama, Agung Sedayu Priharto, Muria Ilham Priyono Priyono Priyono, Setyo Puariesthaufani N, Achmad Puput Khusnaiatul Purwoto, Septyaningrum Putri Puspita, Nurul Amalia Putri, Alisyah Malikha Putri, Maulidia R.G., Fiqri Rafif Fadihilah, Muhammad Rafli Tegar Hati, Muhammad Rahmawati, Widiya Raji, Moh. Ramadan, Arief Dian Rena Widita Reza Hambali Wilman Abdulhadi Ridwan Baraba Rinaldi, Ade Rizky Riris Trima Derita Sari Riska Amilia Rizalnur Firdaus Rokhim, Ahmad Abdur rokhmah, Laela Nur Romadhon Romadhon Rustanto, Dwi Ryan Kurniawan Sabiliat, Nur Edy Sabiliat, Nur Edy Sahrina, Alfi Salim, Ach. Khafid Samponu, Yohakim Benedictus Samponu, Yohakim Benedictus Sanggam Ramantisan Saptaria, Lina Saptaria, Lina Saragih, Jhon Hadearon Sari, Devi Nur Mayang Sari, Virda Nawang Septyan, Mamat Setyawati, Rohmah Cahya Eka Setyowati Setyowati Sihtjaturiman Sirojudin Sirojudin Siti A'isyah Siti Maesaroh Siti Nur Endahyani Sofyan, Misba Maulana Sopiah, Sopiah Sri Adikadarsih, Sri Sri Kushartati SRI RAHAYU Sugiyanto - Sulistiani, Natalia Datik Sulistyowati Sulistyowati, Riny Sumariyah Sumariyah Suminah, - Suminar, Nor SURVIVAL - - Suryanto Suryanto Suryono Suryono Sutikno, Bambang Sutrisno Syah, Iwan Nur Dian Syahrorini, Syamsudduha Syaifudin, Ahmad Bahron Syaikhuddin, Muhammad Miftakhul Syamsiar, Syamsiar Takatoshi Toyoda Tamrin Fathoni Taufiqqurrohman, Rico Titiek Suheta Toni Wijaya, Toni Toshioh Fujibuchi Tri Winarni Agustini Tri Wulan Tjiptono Trisna Budiwati Tuti Mutia Vincensius Gunawan S.K. Virgia Ningrum Fatnar, Virgia Ningrum VITA FIBRIYANI, VITA Wahyu Edy Wibowo, Wahyu Edy Wahyu S. Budi Wahyu Setia Budi Warih Marhendra, Agung Pramana Wati, Listya Rohma Wati, Sulistyowati Sulis Wibowo, Asrizal Septi Widi, Sayekti Nugrahaning Widodo, Suko Wijaya, Ilham Mukti Yanto, Dwi Yanurita Dwihapsari, Yanurita Yati Hardiyanti Yoel Midel Leitabun Yudiono, Udik Yunianti, Nina Yunus Abu Bakar, M. Yusril Abidin, Mohammad Yusuf HR, Mohammad Zaenal Arifin Zaenul Muhlisin Zakaria, Moch. Bagus Zulkifli, Kiky