{"id":27655,"date":"2019-09-01T13:27:14","date_gmt":"2019-09-01T10:27:14","guid":{"rendered":"http:\/\/ihcoedu.uobaghdad.edu.iq\/?p=27655"},"modified":"2019-09-02T11:05:13","modified_gmt":"2019-09-02T08:05:13","slug":"%d9%82%d8%b3%d9%85-%d8%a7%d9%84%d9%81%d9%8a%d8%b2%d9%8a%d8%a7%d8%a1-%d9%8a%d9%86%d8%a7%d9%82%d8%b4-%d8%b1%d8%b3%d8%a7%d9%84%d8%a9-%d9%85%d8%a7%d8%ac%d8%b3%d8%aa%d9%8a%d8%b1-%d8%aa%d8%af%d8%b1%d8%b3-4","status":"publish","type":"post","link":"https:\/\/ihcoedu.uobaghdad.edu.iq\/?p=27655","title":{"rendered":"\u0642\u0633\u0645 \u0627\u0644\u0641\u064a\u0632\u064a\u0627\u0621 \u064a\u0646\u0627\u0642\u0634 \u0631\u0633\u0627\u0644\u0629 \u0645\u0627\u062c\u0633\u062a\u064a\u0631 \u062a\u062f\u0631\u0633 \u0627\u0644\u062e\u0635\u0627\u0626\u0635 \u0627\u0644\u0646\u0648\u0648\u064a\u0629 \u0644\u0644\u0639\u0646\u0627\u0635\u0631 \u0627\u0644\u0646\u0627\u062f\u0631\u0629 \u0627\u0644\u062f\u0627\u062e\u0644\u0629 \u0641\u064a \u0627\u0646\u062a\u0627\u062c \u0644\u0640\u0640\u064a\u0632\u0631 \u0627\u0644\u0644\u064a\u0641 \u0627\u0644\u0628\u0635\u0631\u064a"},"content":{"rendered":"

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 <\/p>\n

\"\"<\/span><\/h4>\n

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\"\"<\/p>\n

\u0648\u0642\u0640\u0640\u062f \u062a\u0640\u0640\u0645 \u062d\u0633\u0627\u0628 \u0627\u0644\u0645\u0642\u0627\u0637\u0639 \u0627\u0644\u0639\u0631\u0636\u064a\u0629 \u0627\u0644\u0645\u0640\u0640\u0640\u0640\u0630\u0643\u0648\u0631\u0629 \u0627\u0639\u0644\u0627\u0647 \u0648\u0627\u0644\u0645\u0646\u0634\u0648\u0631\u0629 \u0641\u064a \u00a0\u0627\u0644\u0628\u062d\u0648\u062b \u0627\u0644\u0639\u0644\u0645\u064a\u0629\u00a0\u0644\u0627\u0646\u062a\u0642\u0627\u0621 \u0627\u0644\u0637\u0627\u0642\u0627\u062a , (EXFOR, ENDF, JENDL, JET, JEFF, BROND, CEND)\u00a0\u0627\u0644\u0645\u0640\u0640\u0640\u0644\u0627\u0626\u0645\u0629\u00a0 \u0641\u0640\u064a\u00a0 \u062d\u0633\u0640\u0640\u0627\u0628\u00a0 \u062a\u0641\u0627\u0639\u0640\u0640\u0644 \u0627\u0644\u0645\u0633\u062a\u0648\u0649 \u0627\u0644\u0627\u0631\u0636\u0640\u0640\u064a\u00a0 \u0628\u0627\u0644\u0627\u0639\u062a\u0645\u0640\u0640\u0627\u062f\u00a0 \u0639\u0644\u0640\u0649\u00a0 \u0628\u0640\u0640\u0631\u0646\u0627\u0645\u062c\u00a0 \u0627\u0644\u062d\u0640\u0627\u0640\u0633\u0640\u0640\u0648\u0628\u00a0) \u0648\u0628\u062e\u0637\u0648\u0627\u062a \u0637\u0627\u0642\u0627\u062a \u0645\u0639\u064a\u0646\u0629 (\u00a0 2 . 0 \u0645\u064a\u0643\u0627 \u0627\u0644\u0643\u062a\u0631\u0648\u0646 \u0641\u0648\u0644\u062a )\u00a0 . Matlab.7.6.2008.b)<\/span><\/h4>\n

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\"\"<\/h3>\n
\n

Studying of the Nuclear Properties of the Nuclei of \u00a0Rare Earth \u00a0Elements Involved \u00a0in the production of Fiber Optic Laser<\/span><\/h3>\n

By Sameer Hashim Al-Khalidi<\/span><\/h3>\n

Supervised by Dr.Sameera Ahmed Ibrahim<\/span><\/h3>\n

Abstract<\/span><\/h3>\n

Present study focused on the study of nuclear properties of the nuclei for Rare earth elements by calculator(interaction energy ,energy\u00a0 threshold, the excess mass, energy\u00a0 and\u00a0 connectivity, the coulomb barrier and the proportion of packing), which \u00a0tabled \u00a0in the third chapter\u00a0<\/span><\/h3>\n

\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 Rare elements have multiple levels energy used in amplifying optical signals in alkali in the production of optical laser and better from ancient technique known and are similar in chemical properties because of its electronic structure from 4f0\u00a0to 4f14\u00a0 which distinguished it from other elements, as referred to in Chapter IV.<\/span><\/h3>\n

\u00a0Which was done through the study of (\u03b1,n ) nuclear reaction of\u00a0 the nuclei atoms rare individually and marital numbers for elements that are\u00a0 \u00a0 \u00a0<\/span><\/h3>\n

,,,,. Which range between energies of alpha (9.233-12.842) MeV.\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0<\/span><\/h3>\n

They are:\u00a0,\u00a0 \u00a0, (\u03b1,n) \u00a0,,\u00a0 \u00a0,<\/span><\/h3>\n

Also the nuclei of atoms marital numbers for rare earth elements which energies of alpha( 12.253 MeV).They are:,.<\/span><\/h3>\n

\u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0<\/span><\/h3>\n

The spin-off sections mentioned above account published in the International literature (EXFOR,\u00a0 ENDF,\u00a0 JENDL-3.0 , JEF-2.2,\u00a0 JEFF, CENDL-2 ), for the selection of the appropriate\u00a0 energies ground-level interaction in a computer-based program account\u00a0 (MATALAB 7.6.0 R 2008 a), and certain steps energies (0.2 MeV) .<\/span><\/h3>\n

We get the derivation the equation quasi-experimental painted tabulated results linking cross-section over a certain with energies as noted in the third quarter.<\/span><\/h3>\n

\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 Also it was put\u00a0 into account of the\u00a0 neutron yield in\u00a0 according with the formula Zeigler \u00a0neutron interactions above using the program (SRIM 2008 ) to \u00a0account for the ability to \u00a0of the \u00a0stopping power which drawn and tabulated the results as well, and its purpose is to determine the neutron energies, for the production of isotopes that including \u00a0the production of laser used\u00a0 in medical, industrial and military fields, agricultural and computers.\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0<\/span><\/h3>\n

And also account the reverse of the cross- sections of the interactions (n,\u03b1) to the nuclei of the rare earth elements to level the ground and using the equation of quasi-experimental cross-section:\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0<\/span><\/h3>\n

\u00a0(n,\u03b1) \u00a0,\u00a0 ,\u00a0(n,\u03b1) \u00a0\u00a0 ,<\/span><\/h3>\n

\u00a0 ,\u00a0 \u00a0.<\/span><\/h3>\n

Drawn and tabulated the results obtained to get the cross-section in direct method and simple as noted in the third quarter.<\/span><\/h3>\n","protected":false},"excerpt":{"rendered":"

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