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قياس تركيز باعثات الفا في الادرار البشري باستخدام كاشف الاثر النووي في الحالة الصلبة PM - 355 == Determination of alpha emitters concentration in human

Author name: شيماء ذياب عطية العبودي
Supervisor name: مازن مانؤيل الياس | ندى فاضل توفيق
General topic: Physics
Degree: Master
Language: English
University location: Baghdad
First pages:
Abstract: This work owes its importance to the fact that it aims at knowing and measuring the concentrations of alpha - particles emitters discrete by the human body in the urine in particular. Knowledge of these concentrations is extremely important since it reveals whether a person has received such doses of radioactive materials emitting alpha - particles that result in the occurrence of malignant tumor and mutations. This subject being so essential to the health of individuals and being a great help to physicians to make the proper diagnosis in the relevant cases, has imposed itself on us as the topic of this thesis. Human urine samples were taken from Iraqi workers in different fields (phosphate plants, fertilizer plants, teaching staff in nuclear physics laboratory, painters, patient and reference healthy people of different ages), using PM - 355 solid state nuclear track detectors. The exposure method was used by immersing PM - 355 detectors in urine samples for three weeks, then etching by 6.25N NaOH for 5 hrs. The track density was measured via an optical microscope. The alpha emitters concentrations in the urine samples were calculated in comparison with standard samples that were prepared in the nuclear laboratory of physics department - College of Science AL - Nahrain University.The obtained results show that the concentrations of alpha emitters in the urine samples of patients range from 1.81ppm to 2.87ppm , from 0.087ppm to 1.32ppm in reference healthy people, in painters from 0.77ppm to 1.46ppm,workers in phosphate plants from 0.94 ppm to 1.89 ppm, workers in fertilizer plants from 1.0ppm to1.42 ppm , and from 1.0 ppm to 1.29 ppm in teaching staff in nuclear physics laboratory .Deductions from the results of this work regarding the dependence of concentrations on the person's occupation, years of service, sex, age and health condition have been dealt with in sufficient details as required.

تصميم وتحليل العدسه الشيئيه رباعية العناصر للمدى الطيفي (mµ 3.2 - 4.2) == DESIGN AND ANALYSIS OF THE FOUR ELEMENTS OBJECTIVE LENS FOR THE 3.2 - 4.2µm SPECTRAL REGION

Author name: صفاء عبد الستار عودة القيسي
General topic: Physics
Degree: Master
Language: English
University location: Baghdad
First pages:
Abstract: اجري بحث حاسوبي لتصميم منظومه بصريه باربع عدسات شيئيه باستخدام برنامج ZEMAX وكذلك دراسة ملائمة بعض المواد(Si, Ge, AMTIR - 1, KRS - 5, ZnSe) التي تعمل ضمن منطقة الاشعه تحت الحمراء (3.2 - 4.2 μm) لعناصر المنظومه البصريه المصممه. اجريت عملية تحقيق الامثليه لايجاد بعض الخصائص البصريه والموصفات التصحيحيه الاكثر تفضيلا من حيث نمط الحيود وحجم البقعه الصوريه الناتجه وكذلك حجم وشكل المنظومه. ان النتائج الحاسوبيه التي تم الحصول عليهابواسطة برنامج ZEMAX اظهرت امكانية استخدام المواد المذكوره ضمن حدود صفاتها البصريه المتمثله بالابعاد البؤريه والزيوغ الكروي وتوزيع الشده والطاقه نسبة للمنظومه والصور المتكونه عند منطقة التحسس. تم اجراء مقارنه للنتائج مع التي حسبت بواسطة برنامج Visual Basic وظهر توافقا عاليا بينهما. ان مواصفات الانظمه البصريه التي قدمت في البحث الحالي قابل للتنفيذ عمليا. | A computational investigation in the present work has been used to design optical system (Four Elements Objective Lens) to show the suitability of some infrared materials (Si, Ge, AMTIR1, KRS - 5, and ZnSe) for the elements of optical designs with aid of ZEMAX package. Optimization process using merit function has been conducted to determine the must favorable optical properties (diffraction, aberration, size of spot, and size and shape of the system). Such designs have been operated in the middle infrared region of spectrum 3.2 - 4.2 μm. The computations obtained by the ZEMAX package shows the performance of those infrared materials through the parameters, focal length, back focal length, f - number, numerical aperture, field of view, Seidel sum for spherical aberration, intensity distribution and fraction encircled energy of the systems and images projected in the detection area. The results have been compared with those obtained with aid of Visual Basic program where a high degree of agreement has been found. The specifications of the optical systems that have been put forward in present investigation can be practically realized

تحضير النشاط الاشعاعي وتقيم مخاطره الاشعاعية لبيئة مصفى الدورة والمناطق المحيطة به

Author name: جعفر جليل سلطان الطائي
Supervisor name: ندى فاضل توفيق
General topic: Physics
Degree: Master
Language: English
University location: Baghdad
First pages:
Abstract: The objectives of the present study were to measure the level of the radioactivity Al - Dora refinery and surrounding area. The study includes : The first. the radon gas concentration in soil samples from Al - Dora refinery and dust samples from surrounding area by using "sealed can technique" and CR - 39 track detector to registration alpha tracks emitted from radon gas in (soil and dust) samples. The second. Detect of the radionuclides and measure the specific activities in soil and water samples using gamma ray spectroscopy system with HPGe detector. The measured soil, water and dust samples were taken from (40) samples, 27 soil samples (surface, 15 and 30cm depth), 8 water samples and 5 dust samples. The detecting of naturally occurring radionuclides (226Ra belong to 238U series, 228Ac belong to 232Th series and one natural radionuclide 40K) in the (soil and water). And estimate the radium equivalent (Raeq), absorbed dose rate in air (ADRA), hazard index (Hex, Hin) and annual effective dose equivalent (AEDE) in soil samples of Al - Dora refinery and surrounding area.The radon concentration in surface soil samples ranged from (290.709 to 394.534 Bq/m3 with an average 365.925 Bq/m3). The radon concentration in soil at the depth 15 cm was ranged from (294.862 to 346.775 with an average 324.164 Bq/m3) and at the depth 30 cm was ranged from (228.633 to 288.414with an average 254.947 Bq/m3). The surface exhalation rate in surface soil samples ranged were ranged from (0.601, to 0.816 with average 0.757Bq·m−2.h−1), in soil samples at the depth 15 cm ranged from (0.61 to 0.717 with average 0.671 Bq·m−2·h−1) and in soil samples at the depth 30 cm ranged from (0.47 to 0.597 with average 0.527 Bq·m−2·h−1). The mass exhalation rate in surface soil samples were ranged from (0.469 to 0.639 with average 0.59 Bq·kg−1·h−1), in soil samples from depth 15 cm ranged from (0.457 to 0.559 with average 0.523 Bq·kg−1·h−1) and in soil samples at the depth 30 cm ranged from (0.368 to 0.465 with average 0.411 Bq·kg−1·h−1).The specific activities for radionuclides (226Ra, ٢28Ac) in surface soil samples were ranged (from 11.725, 15.41 to 59.08, 36.17 Bq/kg respectively) with an average (33.621 and 22.375 Bq/kg respectively) and the specific activity of 40K radionuclide ranged (from 328 to 424.9 with average ٣٦٣.٤٥ Bq/kg). At 15 cm depth ranged (from 18.047, 14.613 to 39.71, 21.673 Bq/kg respectively) with an average (30.527 and 19.66Bq/kg respectively), the specific activity of 40K radionuclide ranged (from 201.3 to 391.3 with average٣٢٦.٧٣ Bq/kg). At 30 cm depth ranged from 17.94, 12.89, to 45.766, 23 Bq/kg respectively) with an average (30.393 and 18.124 Bq/kg respectively), the specific activity of 40K radionuclide ranged (from 231.4 to 351.3 with average ٣١٠.٩٤Bq/kg).For water samples ranged (from 1.60, 1.025 to 8.805, 13.52Bq/kg respectively) with an average (5.031 and 2.925 Bq/kg respectively), the specific activity of 40K radionuclide ranged (from 11.462 to 18.58 with average ١٥.٧٧٨Bq/L).The average values of Raeq, Hin, Hex, ADRA, and the annual effective indoor and outdoor doses in soil and water samples were, in surface (93.70 Bq/kg, 0.309, 0.226, 39.755 nGy/h, 0.198 mSv/y, 0.049 mSv/y), in 15cm depth (83.582 Bq/kg, 0.34, 0.2٥2, 44.34 nGy/h, 0.227 mSv/y, 0.055 mSv/y), in 30 cm depth (80.253 Bq/kg, 0.299, 0.217, 38.051 nGy/h, 0.189 mSv/y, 0.047 mSv/y), and in water (10.428 Bq/kg, 0.042, 0.028, 4.788 nGy/h, 0.024 mSv/y, 0.006 mSv/y).

معالجة رقمية وتحليلية للاثار الناتجة من التشعيع بالمصدر النيوتروني 241Am - 9Be على بعض كواشف الاثار النووي للحالة الصلبة == Digital Processing and Analysis for the Tracks Produced From the Irradiation with Neutrons Source 241Am - 9Be on Some of Solid State Nuclear Track Detectors

Author name: مصطفى يوسف رجب
Supervisor name: حسين علي الجبوري
General topic: Physics
Degree: Master
Language: English
University location: Baghdad
First pages:
Abstract: Image processing technique was used in a lot of studies and research and it concluded , including a number of mathematical relations . In this study , two programs were used , the first one; MATLAB program and second Image - J program . These programs were used to tracks analysis of α - particles on the nuclear track detectors type CR - 39 and CN - 85 . Where irradiated detectors by thermal neutrons from (241Am - 9Be) source with activity 12Ci and neutron flux 105 n.cm - 2.s - 1 . Which obtained on incident α - particles for detectors through 10B(n, α)7Li interaction after covered it with boric acid H3Bo3 pellets . The irradiation times - TD for both detectors were 4h , 8h , 16h and 24h .Through the analyze irradiated detectors of using MATLAB outputs for found the following relationships : a)The irradiation time - TD has behavior linear relationships with following nuclear track parameters, Total track number - NT, Maximum track number - MRD (with depended on track diameter - DT at range of radiation response region 2.5μm - 4μm and 2.5μm - 5μm for CR - 39 and CN - 85 detector respectively) and Maximum track number - MD (without depending on track diameter - DT). b) The irradiation time - TD has behavior exponential relationship with maximum track number - MRA (with depended on track area - AT ) at range of radiation response region 7μm2 - 24μm2 and 9μm2 - 35μm2 for both CR - 39 and CN - 85 detector respectively. c) The irradiation time - TD has behavior a logarithmic relationship with maximum track number - MA (without depending on track area - AT).While through the analyze of outputs Image - J program for irradiated detectors found the irradiation time - TD has behavior linear relationships with following nuclear track detector parameters : a) Total track number - NT. b) Maximum track number - MRA (with depended on track area - AT ) at range of radiation response region 12 μm2 - 24μm2 and 5 μm2 - 27μm2 for both CR - 39 and CN - 85 detector respectively. c) Maximum track number - MA (without depending on track area - AT)This study show that MATLAB program was more analytical and accuracy from Image - J program , through the logarithmic behavior for both detectors between irradiation time - TD with the maximum track number - MA (without depending on track area - AT). There is the possibility of future use image analysis of MATLAB program in the other nuclear track parameters analysis , including ; etched velocity - Vt, , track diameter - Dt , critical angle of nuclear track - θt , nuclear track depth - Dp .The image analyze technique for nuclear track detector which obtained from this study especially with regard to track diameter - TD can be take into account for classification of α - particle emitters , In addition to introduce this technique in preparation of nano - filters and nono - membrane in nanotechnology fields

دراسة الخصائص النووية التركبية والانتقالات الكهرومغناطيسية لانوية Kr ، Xe ، Nd ، Ge الزوجية - الزوجية باستخدام نموذج البوزونات المتفاعلة == Study of Nuclear Structure Properties and Electromagnetic Transitions for even - even Kr , Xe , Nd , Ge Nuclei in the Framework of Interacting Boson Model

Author name: عبد القادر سعد عبد القادر
Supervisor name: سعد ناجي عبود
General topic: Physics
Degree: Master
Language: English
University location: Baghdad
First pages:
Abstract: لقد تم في هذا البحث دراسة التركيب النووي والانتقالات الكهرومغناطيسية لبعض النظائر (الزوجية - الزوجية ) Nd , Xe , Kr وGe باستخدام النموذج الجماعي ( نموذج البوزونات المتفاعلة الثاني IBM - 2 ) . تم الحصول على نتائج لمستويات الطاقة، والانتقالات الكهربائية B(E2) , الانتقالات المغناطيسية B(M1) , ونسبة الخلط (E2/M1) ، وعزم رباعي القطب الكهربائي ، وعزم ثنائي القطب المغناطيسي ، والانتقالات احادية القطب . ولقد تم مقارنة النتائج مع القيم العملية المتوفرة وقد وجد انها متقاربة ومقبولة . ان نظائر ال Kr (Z=36 ) تقع في المنطقة الانتقالية القريبة من التحديد الاهتزازي. ولقد تم حساب مستويات الطاقة B(E2) ، B(M1) ، (E2/M1) وX(E0/E2) لبعض الانتقالات المختارة باستخدام نموذج البوزونات المتفاعلة الثاني (IBM - 2) وان جميع النتائج قد قورنت مع القيم العملية. لقد كان لمعاملات ماجيرونا اثرا كبيرا في حساب مستويات الطاقة , , , التي حددت انها تمتلك صفات تناظر مختلطة . لقد تم مقارنة نتائج نظائر Xe التي تم الحصول عليها من نموذج IBM - 2 مع التوقعات النظرية لتماثل النقطة الحرجةE(5) . وتبين ان 128Xe هو ليس نظير يقع ضمن E(5) كما اقترح مسبقا . لذا فان نسبة الطاقة لنظير ال Xe128 ( ) تقع بين E(5) وحدود - softγ . وبذلك فحسب هذه النسبة فان 128Xe يجب ان يقع بين E(5) وO(6). غالبا ما يكون اختبار 130Xe مناسب لنظائر Xe ، والذي يظهر خصائص E(5) بافضل حالته. كذلك فان مستويات الطاقة تعزز وجود هذا النظير ضمن E(5) . اما بالنسبة لنظائر 132Xe و134Xe فانها تظهر صفات مشابهة للمحدد الاهتزازي SU(5) . ان مستويات التناظر المختلطة قد تم التعريف عليها من نظائر Xe وهذا قد مكننا من تعقب تحرير فونون واحد لحالة في سلسلة النظائر ( الزوجية - الزوجية ) للزنون من الاهتزازات القريبة من N=82 الى نواة - softγ باتجاه منتصف القشرة . لقد درسنا الخصائص النووية لنظائرNd (A=144 - 154) في IBM - 2 وتم الحصول على نتائج جيدة مقارنة بالقيم العملية . 144 - 150Nd يقع في المنطقة الانتقالية ( الاهتزازي - الدوراني ) SU(5)→SU(3) .بينما نظائر 152 - 154Nd فانها تقع ضمن التحديد الدوراني (SU(3)) . ان X(5) سوف ياخذ مكان او حيز عندما يستمر بحركته بين تناظر U(5) الى تناظر ال SU(3) ويظهر ذلك بصورة واضحة ما بين مستويات الطاقة وقوى الانتقال رباعي القطب E2 . لقد وجد حديثا ان سلسلة نظائر Nd تشير الى الانتقالات الطورية كما ان نظير Nd150 يعرضا الخواص المتوقعة ل X(5) . على العموم فان هناك عدة دراسات مفصلة بحاجة للحصول على تلك المؤشرات . وبالنهاية نستنتج بان بعض نظائر Nd تكتشف خواص X(5) . ان , هي حالات تناظر مختلطة لنظائر Nd ان نموذج البوزونات المتفاعلة IBM - 2 كان ناجحا بوصفه للخواص التجميعية للنواة . وفي هذا البحث قد تم الاهتمام بالتطبيقات النظامية والمتضمنة اشكال البوزونات المختلطة.ان النظائر الجرمانيوم ( الزوجية - الزوجية ) لها اهتمام خاص بسبب وجودها ضمن مجموعتين من الحزم ذات الخواص المعقدة للنواة الخفيفة . ان نموذج البوزونات المتفاعلة IBM - 2 مع التركيبات المختلطة يجهز توصيف جيد لكلا الحالات المبينة بالمستوى الارضي وللبروتونات الموجودة بالمستوى المتهيج عبر غلاف القشرة Z =28 المغلق . لقد تم دراسة نظائر الجرمانيوم وتبين انه يتدرج مابين وسط قشرة البروتون والقشرة المزدوجة القريبة من المغلقة عند ال 82Ge . ولقد وجد ان نظائر الجرمانيوم عند التشكيل Nπ=2 تاخذ الشكل الاهتزازي وعند التشكيل Nπ= 4 تاخذ الشكل الدوراني ( ويزداد التشوه) . وفي هذا العمل استخدمت طرق حديثة جدا لتعيين الشحنات الفعلية (effective charge) للبوزونات وذلك باستخدام القيم العملية للانتقال رباعي القطب (0_1^+ 2_1^+ B(E2; وكذلك استخدمت طرق جديدة لحساب المعاملات الجيرو مغناطيسية للبوزونات gυ ، gπ وذلك بمعايرتها الى القيم العملية لـ B(M1) وδ (E2/M1) . | Nuclear structure Properties and electromagnetic transitions of some even - even Kr, Xe, Nd and Ge isotopes have been studied in this work, by using the collective Interacting Boson Model - 2 (IBM - 2). The Interacting Boson Model (IBM - 2) has been very successful in describing the collective properties of nuclei. This work concerns a systematic applications of the model, involving configuration mixing of bosons.There have been extensive IBM studies of low - lying positive parity bands, which are based on the ground state and the quadrupole degree of freedom. The results for energy levels, B(E2), B(M1), mixing ratios , quadrupole and magnetic dipole moments and monopole transitions, were compared with some previous experimental and theoretical values. It was found that an acceptable degree of agreement between the predictions of the IBM - 2 and the experiment can be achieved. The Kr isotope (Z = 36) lies in the transitional region closer to the vibrational range of nuclei. Energy , levels B(E2), B(M1) and the mixing ratios δ(E2/M1) and X(E0/E2) for selected transitions in this isotope were calculated in the framework of the interacting boson model (IBM - 2). All results were compared with experimental data. Some experimental X(E0/E2) ratios were calculated from available experimental data. Majorana parameters were found to have a great effect on the calculated energy levels of the , , and states which indicates they have mixed symmetry properties. The results of IBM - 2 for Xe isotopes were compared with the theoretical predictions assuming a critical point symmetry E(5) which leads to conclude that 128Xe is not an E(5) isotope as previously suggested. In this case of the 128Xe the observable is intermediate between the value for E(5) and gamma soft limit . The ratio suggests that 128Xe should lie between E(5) and O(6). Similar test using 130Xe as a most likely candidate amongst the Xe isotopes, conclusively demonstrate a how well E(5) is realized in the best case. The energy ratio confirmed that this isotope an E(5) critical point symmetry. The 132Xe and 134Xe show vibrational - like character (SU(5) limit). Mixed symmetry states are also studied. It is found that some of the mixed symmetry states with moderate high spins change very fast with respect to the Majorana interaction. Under certain conditions, they become the yrast state or yrare state. These states are difficult to decay and become very stable. This study suggests that a possible new mode of isomers may exist due to the special nature in their proton and neutron degrees of freedom for these isotopes. The mixed - symmetry states or at least a fragment of it have been identified in Xe isotopes. This enables us to trace the evolution of the one - phonon states in the even - even xenon isotopic chain from the vibrators near N = 82 to the γ - soft nuclei towards mid - shell. We have studied the nuclear properties of Neodymium isotopes with (A =144 - 154) in IBM - 2. A good agreement results with the experimental data. 144 - 150Nd lie in the transitional region (virational - rotational limit SU(5)→SU(3)). For the 152 - 154Nd isotopes the energy ratio are well described by the rotational limit SU(3). The X(5) symmetry would take place when moving continuously from the pure U(5) symmetry to the SU(3) symmetry and it implies a definite relations among the level energies and among the E2 transition strengths. It was recently shown that a signature of phase transition is observed in the chain of Nd isotopes, 150Nd display the predicted features of the X(5) symmetry and mark therefore the critical point. However, more detailed studies and experiments are needed to get ideas about this signature. At the end, we have concluded that some of Nd isotopes display X(5) symmetry features. The and are mixed symmetry states in Nd isotopes. The even - even isotopes of germanium are of special interest because of the coexistence of two sets of bands, of very different character, in the lighter nuclei. The IBM - 2 with configuration mixing provides a good description, both of states built on the normal ground state and of those associated with a proton pair excitation across the Z =28 closed - shell gap. Ge isotopes are studied, ranging from the middle of the neutron shell to very near the doubly closed shell at 82Ge. Same Hamiltonian is used for all the nuclei studied, with parameters which are constant or smoothly varying