تم، في هذا العمل، تسجيل عدد جسيمات ألفا الصادرة عن منبع من الأمريسيوم-241، و المتبعثرة على وريقات رقيقة من الذهب و الألمنيوم بتابعية زاوية التبعثر، باستخدام كاشف نصف ناقل و غرفة تبعثر رذرفورد. تم أيضاً قياس المقطع العرضي التفاضلي عن الناتج عن هذا التبعثر، و حساب العدد الذري للهدف تجريبياً، لكل من الذهب و الألمنيوم. مقارنة النتائج التجريبية بالنتائج النظرية يشير إلى تطابق جيد بينهما.
In this work, it has been recording the alpha particles emitted from an Amerecium-241 source, and scattered by a gold and Aluminum thin foils as a function of the scattering angle q (0o-30o), using a semiconductor detector and Rutherford scattering chamber. It always has been measuring the differential cross section resulting from this scattering, and experimentally determining the atomic number of Gold and Aluminum. Comparison between experimental and theoretical results shows a good agreement.
References used
E. H. Wickmann, Quantum Physics. Berkeley course, New York, McGraw Hill, 1967, Chap. 6 and 9
E. Merzbacher, Quantum Mechanics. New York, John Wiley, 1962, chap. 12
C. Cohen-Tannoudji, B. Diu et F. Laloë, Mécanique Quantique. Paris, Hermann, 1973, chap. VIII
Messiah, Mécanique Quantique. Paris, Dunod, 1960. Vol. 1, chap. X
In this work, it has been studied Compton Effect using the 662 keV gamma rays from a radioactive source of cesium-137 (137Cs) intensity (3.33×105 Bq) on Aluminum rod (who plays scatter). It has been measured the differential cross section, and the ex
This work aims to find the differential scattering cross-section
for X-ray
scattered by aluminum target with angles in intervals in accordance to both
polarization cases ( completely – partly).
In addition, the relative scattered intensity and po
CdTe Thin films were deposited on glass substrates by thermal evaporation
method. The geometric thickness was calculated using interferometric method
based on reflectance curve recorded with the spectrophotometer. The XRD
analysis and optical char
In this work, we have used the basic techniques for measuring gamma rays. It is
based on the use of a sodium iodide (NaI) detector withthallium activated (Tl). We have
obtained:
The detector calibration NaI(Tl) and the resolution of the spectrom
Slabs are considered one of the most exposed elements to disasters and deformities
that can be clear to the viewer. These deformities are reflected as sign of defects that
appear clearly on big slabs. So, here comes the importance of applying and d