Giant dipole resonance built on hot rotating nuclei produced during evaporation of light particlesfrom the $^{88}$Mo compound nucleus
High-energy giant dipole resonance (GDR) γ rays were measured following the decay of the hot, rotatingcompound nucleus of 88Mo, produced at excitation energies of 124 and 261 MeV. The reaction 48Ti+ 40Ca at 300and 600 MeV bombarding energies has been used. The data were analyzed using the statistica...
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creator | Ciemala, M. Kmiecik, M. Maj, A. Mazurek, K. Bracco, A. Kravchuk, V.L. Casini, G. Barlini, S. Baiocco, G. Bardelli, L. Bednarczyk, P. Benzoni, G. Bini, M. Blasi, N. Brambilla, S. Bruno, M. Camera, F. Carboni, S. Cinausero, M. Chbihi, A. Chiari, M. Corsi, A. Crespi, F.C.L. D’agostino, M. Degerlier, M. Fornal, B. Giaz, A. Gramegna, F. Krzysiek, M. Leoni, S. Marchi, T. Matejska-Minda, M. Mazumdar, I. Meczynski, W. Million, B. Montanari, D. Morelli, L. Myalski, S. Nannini, A. Nicolini, R. Pasquali, G. Piantelli, S. Prete, G. Roberts, O. J. Schmitt, C. Styczen, J. Szpak, B. Valdre, S. Wasilewska, B. Wieland, O. Wieleczko, J.P. Zieblinski, M. Dudek, J. Dang, N. Dinh |
description | High-energy giant dipole resonance (GDR) γ rays were measured following the decay of the hot, rotatingcompound nucleus of 88Mo, produced at excitation energies of 124 and 261 MeV. The reaction 48Ti+ 40Ca at 300and 600 MeV bombarding energies has been used. The data were analyzed using the statistical modelMonte Carlocode GEMINI++. It allowed extracting the giant dipole resonance parameters by fitting the high-energy γ -rayspectra. The extracted GDR widths were compared with the available data at lower excitation energy and withtheoretical predictions based on (i) The Lublin-Strasbourg drop macroscopic model, supplemented with thermalshape fluctuations analysis, and (ii) The phonon damping model. The theoretical predictions were convolutedwiththe population matrices of evaporated nuclei from the statistical model GEMINI++. Also a comparison with theresults of a phenomenological expression based on the existing systematics, mainly for lower temperature data,is presented and discussed. A possible onset of a saturation of the GDR width was observed around T = 3 MeV. |
doi_str_mv | 10.1103/PhysRevC.91.054313 |
format | Article |
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J. ; Schmitt, C. ; Styczen, J. ; Szpak, B. ; Valdre, S. ; Wasilewska, B. ; Wieland, O. ; Wieleczko, J.P. ; Zieblinski, M. ; Dudek, J. ; Dang, N. Dinh</creator><creatorcontrib>Ciemala, M. ; Kmiecik, M. ; Maj, A. ; Mazurek, K. ; Bracco, A. ; Kravchuk, V.L. ; Casini, G. ; Barlini, S. ; Baiocco, G. ; Bardelli, L. ; Bednarczyk, P. ; Benzoni, G. ; Bini, M. ; Blasi, N. ; Brambilla, S. ; Bruno, M. ; Camera, F. ; Carboni, S. ; Cinausero, M. ; Chbihi, A. ; Chiari, M. ; Corsi, A. ; Crespi, F.C.L. ; D’agostino, M. ; Degerlier, M. ; Fornal, B. ; Giaz, A. ; Gramegna, F. ; Krzysiek, M. ; Leoni, S. ; Marchi, T. ; Matejska-Minda, M. ; Mazumdar, I. ; Meczynski, W. ; Million, B. ; Montanari, D. ; Morelli, L. ; Myalski, S. ; Nannini, A. ; Nicolini, R. ; Pasquali, G. ; Piantelli, S. ; Prete, G. ; Roberts, O. J. ; Schmitt, C. ; Styczen, J. ; Szpak, B. ; Valdre, S. ; Wasilewska, B. ; Wieland, O. ; Wieleczko, J.P. ; Zieblinski, M. ; Dudek, J. ; Dang, N. Dinh</creatorcontrib><description>High-energy giant dipole resonance (GDR) γ rays were measured following the decay of the hot, rotatingcompound nucleus of 88Mo, produced at excitation energies of 124 and 261 MeV. The reaction 48Ti+ 40Ca at 300and 600 MeV bombarding energies has been used. The data were analyzed using the statistical modelMonte Carlocode GEMINI++. It allowed extracting the giant dipole resonance parameters by fitting the high-energy γ -rayspectra. The extracted GDR widths were compared with the available data at lower excitation energy and withtheoretical predictions based on (i) The Lublin-Strasbourg drop macroscopic model, supplemented with thermalshape fluctuations analysis, and (ii) The phonon damping model. The theoretical predictions were convolutedwiththe population matrices of evaporated nuclei from the statistical model GEMINI++. 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J.</creatorcontrib><creatorcontrib>Schmitt, C.</creatorcontrib><creatorcontrib>Styczen, J.</creatorcontrib><creatorcontrib>Szpak, B.</creatorcontrib><creatorcontrib>Valdre, S.</creatorcontrib><creatorcontrib>Wasilewska, B.</creatorcontrib><creatorcontrib>Wieland, O.</creatorcontrib><creatorcontrib>Wieleczko, J.P.</creatorcontrib><creatorcontrib>Zieblinski, M.</creatorcontrib><creatorcontrib>Dudek, J.</creatorcontrib><creatorcontrib>Dang, N. Dinh</creatorcontrib><title>Giant dipole resonance built on hot rotating nuclei produced during evaporation of light particlesfrom the $^{88}$Mo compound nucleus</title><title>Physical review. C</title><description>High-energy giant dipole resonance (GDR) γ rays were measured following the decay of the hot, rotatingcompound nucleus of 88Mo, produced at excitation energies of 124 and 261 MeV. The reaction 48Ti+ 40Ca at 300and 600 MeV bombarding energies has been used. The data were analyzed using the statistical modelMonte Carlocode GEMINI++. It allowed extracting the giant dipole resonance parameters by fitting the high-energy γ -rayspectra. The extracted GDR widths were compared with the available data at lower excitation energy and withtheoretical predictions based on (i) The Lublin-Strasbourg drop macroscopic model, supplemented with thermalshape fluctuations analysis, and (ii) The phonon damping model. The theoretical predictions were convolutedwiththe population matrices of evaporated nuclei from the statistical model GEMINI++. Also a comparison with theresults of a phenomenological expression based on the existing systematics, mainly for lower temperature data,is presented and discussed. A possible onset of a saturation of the GDR width was observed around T = 3 MeV.</description><subject>Nuclear Experiment</subject><subject>Physics</subject><issn>2469-9985</issn><issn>2469-9993</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNqVzE9LwzAYBvAgCg63L-DpPewmq0mzds1RhrqDggzPltimayTNG_KnMMSj39uK4t3T8_Dw4yHkktGMMcqvn_pj2KtxmwmW0WLNGT8hs3xdipUQgp_-9ao4J4sQ3iilrKRiw-iMfN5raSO02qFR4FVAK22j4DVpEwEt9BjBY5RR2wPY1BilwXlsU6NaaJP_ntUoHfqJTB47MPrQR3DSRz3x0HkcIPYKli_vVfWxfERocHCYbPtzmMKcnHXSBLX4zQtydXf7vN2temlq5_Ug_bFGqevdzUOtbe54TRkr8nIjRsb_p78AkRBgqQ</recordid><startdate>2015</startdate><enddate>2015</enddate><creator>Ciemala, M.</creator><creator>Kmiecik, M.</creator><creator>Maj, A.</creator><creator>Mazurek, K.</creator><creator>Bracco, A.</creator><creator>Kravchuk, V.L.</creator><creator>Casini, G.</creator><creator>Barlini, S.</creator><creator>Baiocco, G.</creator><creator>Bardelli, L.</creator><creator>Bednarczyk, P.</creator><creator>Benzoni, G.</creator><creator>Bini, M.</creator><creator>Blasi, N.</creator><creator>Brambilla, S.</creator><creator>Bruno, M.</creator><creator>Camera, F.</creator><creator>Carboni, S.</creator><creator>Cinausero, M.</creator><creator>Chbihi, A.</creator><creator>Chiari, M.</creator><creator>Corsi, A.</creator><creator>Crespi, F.C.L.</creator><creator>D’agostino, M.</creator><creator>Degerlier, M.</creator><creator>Fornal, B.</creator><creator>Giaz, A.</creator><creator>Gramegna, F.</creator><creator>Krzysiek, M.</creator><creator>Leoni, S.</creator><creator>Marchi, T.</creator><creator>Matejska-Minda, M.</creator><creator>Mazumdar, I.</creator><creator>Meczynski, W.</creator><creator>Million, B.</creator><creator>Montanari, D.</creator><creator>Morelli, L.</creator><creator>Myalski, S.</creator><creator>Nannini, A.</creator><creator>Nicolini, R.</creator><creator>Pasquali, G.</creator><creator>Piantelli, S.</creator><creator>Prete, G.</creator><creator>Roberts, O. 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J. ; Schmitt, C. ; Styczen, J. ; Szpak, B. ; Valdre, S. ; Wasilewska, B. ; Wieland, O. ; Wieleczko, J.P. ; Zieblinski, M. ; Dudek, J. ; Dang, N. 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C</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Ciemala, M.</au><au>Kmiecik, M.</au><au>Maj, A.</au><au>Mazurek, K.</au><au>Bracco, A.</au><au>Kravchuk, V.L.</au><au>Casini, G.</au><au>Barlini, S.</au><au>Baiocco, G.</au><au>Bardelli, L.</au><au>Bednarczyk, P.</au><au>Benzoni, G.</au><au>Bini, M.</au><au>Blasi, N.</au><au>Brambilla, S.</au><au>Bruno, M.</au><au>Camera, F.</au><au>Carboni, S.</au><au>Cinausero, M.</au><au>Chbihi, A.</au><au>Chiari, M.</au><au>Corsi, A.</au><au>Crespi, F.C.L.</au><au>D’agostino, M.</au><au>Degerlier, M.</au><au>Fornal, B.</au><au>Giaz, A.</au><au>Gramegna, F.</au><au>Krzysiek, M.</au><au>Leoni, S.</au><au>Marchi, T.</au><au>Matejska-Minda, M.</au><au>Mazumdar, I.</au><au>Meczynski, W.</au><au>Million, B.</au><au>Montanari, D.</au><au>Morelli, L.</au><au>Myalski, S.</au><au>Nannini, A.</au><au>Nicolini, R.</au><au>Pasquali, G.</au><au>Piantelli, S.</au><au>Prete, G.</au><au>Roberts, O. J.</au><au>Schmitt, C.</au><au>Styczen, J.</au><au>Szpak, B.</au><au>Valdre, S.</au><au>Wasilewska, B.</au><au>Wieland, O.</au><au>Wieleczko, J.P.</au><au>Zieblinski, M.</au><au>Dudek, J.</au><au>Dang, N. Dinh</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Giant dipole resonance built on hot rotating nuclei produced during evaporation of light particlesfrom the $^{88}$Mo compound nucleus</atitle><jtitle>Physical review. C</jtitle><date>2015</date><risdate>2015</risdate><volume>91</volume><issn>2469-9985</issn><eissn>2469-9993</eissn><abstract>High-energy giant dipole resonance (GDR) γ rays were measured following the decay of the hot, rotatingcompound nucleus of 88Mo, produced at excitation energies of 124 and 261 MeV. The reaction 48Ti+ 40Ca at 300and 600 MeV bombarding energies has been used. The data were analyzed using the statistical modelMonte Carlocode GEMINI++. It allowed extracting the giant dipole resonance parameters by fitting the high-energy γ -rayspectra. The extracted GDR widths were compared with the available data at lower excitation energy and withtheoretical predictions based on (i) The Lublin-Strasbourg drop macroscopic model, supplemented with thermalshape fluctuations analysis, and (ii) The phonon damping model. The theoretical predictions were convolutedwiththe population matrices of evaporated nuclei from the statistical model GEMINI++. Also a comparison with theresults of a phenomenological expression based on the existing systematics, mainly for lower temperature data,is presented and discussed. A possible onset of a saturation of the GDR width was observed around T = 3 MeV.</abstract><pub>American Physical Society</pub><doi>10.1103/PhysRevC.91.054313</doi><orcidid>https://orcid.org/0000-0002-7938-0338</orcidid><orcidid>https://orcid.org/0000-0001-6993-3149</orcidid><orcidid>https://orcid.org/0000-0002-1142-8067</orcidid><orcidid>https://orcid.org/0000-0001-8644-198X</orcidid><orcidid>https://orcid.org/0000-0002-0669-2787</orcidid><orcidid>https://orcid.org/0000-0002-3691-0749</orcidid><orcidid>https://orcid.org/0000-0003-0659-7648</orcidid><orcidid>https://orcid.org/0000-0001-8644-198X</orcidid><orcidid>https://orcid.org/0000-0001-6993-3149</orcidid><orcidid>https://orcid.org/0000-0002-1142-8067</orcidid><orcidid>https://orcid.org/0000-0002-7938-0338</orcidid><orcidid>https://orcid.org/0000-0002-1142-8067</orcidid><orcidid>https://orcid.org/0000-0003-0659-7648</orcidid><orcidid>https://orcid.org/0000-0002-0669-2787</orcidid><orcidid>https://orcid.org/0000-0002-3691-0749</orcidid></addata></record> |
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source | American Physical Society Journals |
subjects | Nuclear Experiment Physics |
title | Giant dipole resonance built on hot rotating nuclei produced during evaporation of light particlesfrom the $^{88}$Mo compound nucleus |
url | https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2024-12-27T07%3A38%3A16IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-hal&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Giant%20dipole%20resonance%20built%20on%20hot%20rotating%20nuclei%20produced%20during%20evaporation%20of%20light%20particlesfrom%20the%20$%5E%7B88%7D$Mo%20compound%20nucleus&rft.jtitle=Physical%20review.%20C&rft.au=Ciemala,%20M.&rft.date=2015&rft.volume=91&rft.issn=2469-9985&rft.eissn=2469-9993&rft_id=info:doi/10.1103/PhysRevC.91.054313&rft_dat=%3Chal%3Eoai_HAL_in2p3_01152679v1%3C/hal%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_id=info:pmid/&rfr_iscdi=true |