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"ABSTRACTThe combination of the coupled mode and normal mode theories has been used to formulaic the theoretical performance represented by the coupling length and crosstalk parameters of the X-cut APE-LN SDC fabricated using the benzoic acid as the proton source, where in this case the matrix effective refractive index (MERI) method is applied for solving the symmetric and antisymmetric propagation constants of the normal modes propagating in this device. The corresponding near field method has been used to experimentally determine its crosstalk. The actual performance of this device is characterized by comparing the theoretically calculated with the experimentally determined crosstalk parameters. A software computer program has been developed in order to numerically characterize the entire characteristic and performance of the SDC under study. For the SDC under study, the best crosstalk obtained at the operating wavelength lamda =1.3 micrometer is ~0.21 dB for the interaction length L = 6 mm and the gap separation g = 5 mm. Its coupling length is ~ 1.33 mm. The propagation constant of the corresponding individual single-mode X-cut APE-LN channel waveguide making up this SDC is beta = 10.37901 micrometer, and thereby its effective refractive index is N cπ= 2.14743330. It has been shown that the fabricated SDC is very lossy. It has been deduced that its bad performance predominantly caused by the side diffusion effect, corresponding to the fabrication problem, where in this case the substrate sample has been not coated first with the buffer layer when the deposition of substrate sample with the aluminum mask was to be performed in the fabrication stages. Moreover, in this case only the simple annealing has been performed. The successive annealing process in order to reduce the coupling loss has been not applied yet. Under the assumption that the fabrication tolerances are such that the practical devices with coupling loss below 0.25 dB are feasible, the fabricated SDC under study is a 3 dB coupler. "

"Kita membandingkan dua bentuk propagator yang berbeda yaitu bentuk propagator yang disederhanakan dan bentuk propagator yang lengkap dari resonans nukleon spin-3/2 dan spin-5/2 dengan menggunakan model isobar dan pendekatan Lagranggian efektif pada fotoproduksi eta-meson pada proton γ + N -> η + N. Kita menghitung amplitude transisi dengan memasukkan suku Born, suku vektor-meson, dan resonans nukleon ( N1(1520)D13, N2(1535)S11, N3(1650)S11, N4(1675)D15, N5(1680)F15, N6(1700)D13, N7(1710)P11, dan N8(1720)P13 ). Parameter konstanta kopling diperoleh berdasarkan hasil perhitungan dari formula yang telah ditetapkan dengan data input berdasarkan data partikel.

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We compare two different propagator forms that are simple and complete propagators of spin-3/2 and spin-5/2 nucleon resonances by using isobar models and effective Lagrangian approach for eta-meson photoproduction on the proton γ + N -> η + N. We calculate the transition amplitudes by including Born term, vector-meson term, and nucleon resonances ( N1(1520)D13, N2(1535)S11, N3(1650)S11, N4(1675)D15, N5(1680)F15, N6(1700)D13, N7(1710)P11, and N8(1720)P13 ). The coupling constant parameters are obtained based on the calculation results based on the particle data group."

"Radioterapi adalah suatu modalitas penanganan kanker dengan memanfaatkan radiasi pengion. Teknik radiasi yang saat ini menjadi perhatian adalah radiasi partikel, salah satunya adalah proton. Proton memiliki karakteristik puncak bragg (Bragg peak) yang mendepositkan energinya pada jangkauan kedalaman tertentu. Salah satu teknik penyinaran radioterapi adalah Intensity Modulated Proton Therapy (IMPT). IMPT memiliki beam spot yang berukuran sangat kecil, sehingga memungkinkan distribusi dosis lebih konformal terhadap target. Organ paru-paru memiliki pergerakan yang membuat tantangan dalam pengerjaanya. Untuk mengurangi pengaruh pergerakan digunakan teknik 4D Computed Tomography (4DCT). Penelitian ini bertujuan untuk mengetahui tingkat efektivitas pengobatan kanker di paru-paru pada teknik radioterapi proton yang dibandingkan dengan radiasi foton sebagai acuan dasarnya. Selain itu, studi ini juga bertujuan untuk mengetahui besar perbedaan tingkat efektivitas perencanaan antara 3D CT dan 4D CT. Tingkat efektivitas perencanaan berdasarkan tiga parameter. Parameter tersebut yaitu Conformity Index (CI), Homogeneity Index (HI), dan Gradient Index (GI). Terdapat perbedaan yang cukup signifikan dari hasil perencanaan di kedua fantom tersebut. Untuk nilai CI dan HI nilai terbaik dapat dicapai pada fase ekspirasi. Namun untuk GI nilai terbaik dapat dicapai pada fase 0%. Dosis pada spinal cord setiap perencanaan, tidak memiliki perbedaan yang cukup signifikan. Kami menemukan pada paru-paru dengan teknik IMRT di fantom diam memiliki dosis melebihi ambang batas yang ditetapkan.

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The Intensity Modulated Proton Therapy (IMPT) technique is the most advanced technique in proton beam therapy. This is because IMPT can produce a dose distribution that is more appropriate to the target with a minimum dose in healthy organs. The use of radiotherapy for lung cancer cases has considerable challenges. This is due to the uncertainty of the range and movement of organs, which allows errors in planning to occur. 4 Dimension Computed Tomography (4DCT) is a technique that can provide temporal information on changes in healthy tissues and organs. Each phase generated from 4DCT, can provide information about the location, density, and volume of the target tissue and surrounding healthy organs. The use of all 4DCT planning phases in clinical practice has a very large workload, so one solution is to use only two extreme phases. This research was conducted by comparing the 10 planning phases using the IMPT technique. It aims to find out at what phase the best level of effectiveness is produced, based on the research data obtained. Evaluation was carried out based on the parameters of Conformity Index (CI), Gradient Index (GI), and Conformity Index (CI). The results of this study indicate that in the three parameters the best values ​​are in the two extreme phases. In the SFO and MFO techniques, the best CI value is in the 0% phase, while the HI value in the SFO technique is in the 50% phase and the MFO is in the 90% phase. In addition, for the GI value in both techniques, it is best to be in the 0% phase. "