Elastic scattering cross sections of 11.4 MeV photons from<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">Pb</mml:mi></mml:mrow><mml:mprescripts /><mml:mrow /><mml:mrow><mml:mn>2</mml:mn><mml:mn>0</mml:mn><mml:mn>6</mml:mn><mml:mo>,</mml:mo><mml:mn>2</mml:mn><mml:mn>0</mml:mn><mml:mn>7</mml:mn><mml:mo>,</mml:mo><mml:mn>2</mml:mn><mml:mn>0</mml:mn><mml:mn>8</mml:mn></mml:mrow><mml:mrow /><mml:mrow /></mml:mmultiscr

Kahane, S.; Moreh, R.

doi:10.1103/physrevc.50.2000

Cited by 5 publications

(4 citation statements)

References 34 publications

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“…This huge departure can be explained by the resonance excitation of an isolated single compound nuclear level, most likely in 115 In. The occurrence of such isolated resonance at ≈ 9 MeV was also observed in many other nuclei [9].…”

Section: Insupporting

confidence: 64%

“…The cross section is given in total analogy with Eq. ( 5): This is due to scattering from an isolated resonance level in In and is reminiscent of our former investigation [9] of Pb isotopes where strong departure from the smooth behavior of a Lorentzian GDR was observed. In Dy, which is a deformed nucleus, also the inelastic Raman scattering is clearly observed.…”

Section: B Raman Scatteringmentioning

confidence: 55%

“…where N θ are the net counts measured, t θ -the measurement time and B a correction for the photon absorption in the target (see for example Ref. [9]) which depends on θ, φ -the angle of the target plane with the incoming beam direction; µ -the linear absorption coefficient of a photon of energy E γ in the target material, and a -the target thickness.…”

Section: Experimental and Data Analysis Detailsmentioning

confidence: 99%

“…Of course the implication is that discrepancies are caused only by neglecting Coulomb corrections. This approach did not work out very well in the case of Bi [8,9,10] where it become evident that the experiment-theory discrepancies are mostly related to uncertainities in the GDR parameters. These parameters are obtained by Lorentzian line fits to (γ,tot) measurements.…”

Section: Introductionmentioning

confidence: 97%

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Elastic and Raman scattering of 9.0 and 11.4 MeV photons from Au, Dy, and In

Kahane¹,

Moreh

Bar-Noy³

2002

Phys. Rev. C

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Monoenergetic photons between 8.8 and 11.4 MeV were scattered elastically and inelastically (Raman) from natural targets of Au, Dy and In. 15 new crosss sections were measured. Evidence is presented for a slight deformation in the 197 Au nucleus, generally believed to be spherical. It is predicted, on the basis of these measurements, that the Giant Dipole Resonance of Dy is very similar to that of 160 Gd. A narrow isolated resonance at 9.0 MeV is observed in In.

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Section: Insupporting

confidence: 64%

Section: B Raman Scatteringmentioning

confidence: 55%

Section: Experimental and Data Analysis Detailsmentioning

confidence: 99%

Section: Introductionmentioning

confidence: 97%

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Elastic and Raman scattering of 9.0 and 11.4 MeV photons from Au, Dy, and In

Kahane¹,

Moreh

Bar-Noy³

2002

Phys. Rev. C

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Photon Scattering by Nuclei

Grosse

Junghans

2013

Nuclei With Z = 61 - 73

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Nuclear Data Sheets for A = 209

Chen

Kondev

2015

Nuclear Data Sheets

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The experimental data are evaluated for known nuclides of mass number A=209 (Au,Hg,Tl,Pb,Bi,Po,At,Rn, F r , R a , A c , T h ) . D e t a i l e d e v a l u a t e d l e v e l p r o p e r t i e s a n d r e l a t e d n u c l e a r s t r u c t u r e i n f o r m a t i o n a r e p r e s e n t e d , w i t h t h e b e s t v a l u e s r e c o m m e n d e d f o r l e v e l e n e r g i e s , h a l f -l i v e s , γ -r a y e n e r g i e s a n d i n t e n s i t i e s , d e c a y d a t a ( e n e r g i e s , i n t e n s i t i e s a n d p l a c e m e n t o f r a d i a t i o n s ) , a n d o t h e r s p e c t r o s c o p i c d a t a . T h i s w o r k s u p e r s e d e s t h e earlier full evaluation of A=209 by M.J. Martin (1991Ma16). Cutoff Date: Literature available in NSR database up to September 30, 2013 has been included. General Policies and Organization of Material: see http://www.nndc.bnl.gov/nds/NDSPolicies.pdf. Acknowledgments: The authors express their gratitude to Dr. J.K. Tuli, Mrs. J. Totans and Mrs. M. Blennau from the National Nuclear Data Center for their assistance during the evaluation process and the preparation of the m a n u s c r i p t . T h e a u t h o r s a r e t h a n k f u l t o t h e r e v i e w e r , D r . M . J . M a r t i n , f o r h i s c r i t i c a l r e a d i n g o f t h e manuscript and many useful comments, and suggestions.

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Elastic scattering cross sections of 11.4 MeV photons fromPb206,207,208

Cited by 5 publications

References 34 publications

Elastic and Raman scattering of 9.0 and 11.4 MeV photons from Au, Dy, and In

Elastic and Raman scattering of 9.0 and 11.4 MeV photons from Au, Dy, and In

Photon Scattering by Nuclei

Nuclear Data Sheets for A = 209

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