Mechanism of α-particle scattering from ^2^8Si nuclei
Statistical and Regge pole analyses were performed on excitation functions and angular distributions for α-particle scattering on ^2^8Si leading to the ground, 2^+ (1.78) MeV and 4^+ (4.62 Me V) states in the energy range 21-28 MeV. The direct interaction contribution y"D for the reaction studi...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
|---|
| Format: |
E-Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
1976 |
|---|
| Reproduktion: |
Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 |
|---|---|
| Übergeordnetes Werk: |
in: Nuclear Physics, Section A - Amsterdam : Elsevier, 265(1976), 3, Seite 461-478 |
| Übergeordnetes Werk: |
volume:265 ; year:1976 ; number:3 ; pages:461-478 |
| Links: |
|---|
| Katalog-ID: |
NLEJ181337223 |
|---|
| LEADER | 01000caa a22002652 4500 | ||
|---|---|---|---|
| 001 | NLEJ181337223 | ||
| 003 | DE-627 | ||
| 005 | 20210706151332.0 | ||
| 007 | cr uuu---uuuuu | ||
| 008 | 070505s1976 xx |||||o 00| ||eng c | ||
| 035 | |a (DE-627)NLEJ181337223 | ||
| 035 | |a (DE-599)GBVNLZ181337223 | ||
| 040 | |a DE-627 |b ger |c DE-627 |e rakwb | ||
| 041 | |a eng | ||
| 245 | 1 | 0 | |a Mechanism of α-particle scattering from ^2^8Si nuclei |
| 264 | 1 | |c 1976 | |
| 336 | |a nicht spezifiziert |b zzz |2 rdacontent | ||
| 337 | |a nicht spezifiziert |b z |2 rdamedia | ||
| 338 | |a nicht spezifiziert |b zu |2 rdacarrier | ||
| 520 | |a Statistical and Regge pole analyses were performed on excitation functions and angular distributions for α-particle scattering on ^2^8Si leading to the ground, 2^+ (1.78) MeV and 4^+ (4.62 Me V) states in the energy range 21-28 MeV. The direct interaction contribution y"D for the reaction studied was determined. Angular cross-correlation coefficients (a.c.c.c.) were calculated in each channel for all pairs of experimental excitation functions. For the elastic channel a.c.c.c. were compared with the coefficients calculated using the excitation functions generated by the optical model. Channel cross-correlation coefficients (c.c.c.c.) were also calculated in the full angular range for pairs of excitation functions measured at the same angle (lab). The single Regge pole model was used to describe the behaviour of the angular distribution at backward angles in the elastic channel. The l = 10 value of angular momentum for energies greater than 24 MeV was clearly distinguished. The results of the analysis indicate that at backward angles of scattering a mechanism different from the direct and compound ones contributes significantly to the reaction. | ||
| 533 | |f Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 | ||
| 700 | 1 | |a Budzanowski, A. |4 oth | |
| 700 | 1 | |a Jarczyk, L. |4 oth | |
| 700 | 1 | |a Kamys, B. |4 oth | |
| 700 | 1 | |a Kapuscik, A. |4 oth | |
| 773 | 0 | 8 | |i in |t Nuclear Physics, Section A |d Amsterdam : Elsevier |g 265(1976), 3, Seite 461-478 |w (DE-627)NLEJ177217928 |w (DE-600)1466542-6 |x 0375-9474 |7 nnns |
| 773 | 1 | 8 | |g volume:265 |g year:1976 |g number:3 |g pages:461-478 |
| 856 | 4 | 0 | |u http://linkinghub.elsevier.com/retrieve/pii/0375-9474(76)90555-8 |
| 912 | |a GBV_USEFLAG_H | ||
| 912 | |a ZDB-1-SDJ | ||
| 912 | |a GBV_NL_ARTICLE | ||
| 951 | |a AR | ||
| 952 | |d 265 |j 1976 |e 3 |h 461-478 | ||
| matchkey_str |
article:03759474:1976----::ehnsoprilsatrnf |
|---|---|
| hierarchy_sort_str |
1976 |
| publishDate |
1976 |
| allfields |
(DE-627)NLEJ181337223 (DE-599)GBVNLZ181337223 DE-627 ger DE-627 rakwb eng Mechanism of α-particle scattering from ^2^8Si nuclei 1976 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Statistical and Regge pole analyses were performed on excitation functions and angular distributions for α-particle scattering on ^2^8Si leading to the ground, 2^+ (1.78) MeV and 4^+ (4.62 Me V) states in the energy range 21-28 MeV. The direct interaction contribution y"D for the reaction studied was determined. Angular cross-correlation coefficients (a.c.c.c.) were calculated in each channel for all pairs of experimental excitation functions. For the elastic channel a.c.c.c. were compared with the coefficients calculated using the excitation functions generated by the optical model. Channel cross-correlation coefficients (c.c.c.c.) were also calculated in the full angular range for pairs of excitation functions measured at the same angle (lab). The single Regge pole model was used to describe the behaviour of the angular distribution at backward angles in the elastic channel. The l = 10 value of angular momentum for energies greater than 24 MeV was clearly distinguished. The results of the analysis indicate that at backward angles of scattering a mechanism different from the direct and compound ones contributes significantly to the reaction. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Budzanowski, A. oth Jarczyk, L. oth Kamys, B. oth Kapuscik, A. oth in Nuclear Physics, Section A Amsterdam : Elsevier 265(1976), 3, Seite 461-478 (DE-627)NLEJ177217928 (DE-600)1466542-6 0375-9474 nnns volume:265 year:1976 number:3 pages:461-478 http://linkinghub.elsevier.com/retrieve/pii/0375-9474(76)90555-8 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 265 1976 3 461-478 |
| spelling |
(DE-627)NLEJ181337223 (DE-599)GBVNLZ181337223 DE-627 ger DE-627 rakwb eng Mechanism of α-particle scattering from ^2^8Si nuclei 1976 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Statistical and Regge pole analyses were performed on excitation functions and angular distributions for α-particle scattering on ^2^8Si leading to the ground, 2^+ (1.78) MeV and 4^+ (4.62 Me V) states in the energy range 21-28 MeV. The direct interaction contribution y"D for the reaction studied was determined. Angular cross-correlation coefficients (a.c.c.c.) were calculated in each channel for all pairs of experimental excitation functions. For the elastic channel a.c.c.c. were compared with the coefficients calculated using the excitation functions generated by the optical model. Channel cross-correlation coefficients (c.c.c.c.) were also calculated in the full angular range for pairs of excitation functions measured at the same angle (lab). The single Regge pole model was used to describe the behaviour of the angular distribution at backward angles in the elastic channel. The l = 10 value of angular momentum for energies greater than 24 MeV was clearly distinguished. The results of the analysis indicate that at backward angles of scattering a mechanism different from the direct and compound ones contributes significantly to the reaction. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Budzanowski, A. oth Jarczyk, L. oth Kamys, B. oth Kapuscik, A. oth in Nuclear Physics, Section A Amsterdam : Elsevier 265(1976), 3, Seite 461-478 (DE-627)NLEJ177217928 (DE-600)1466542-6 0375-9474 nnns volume:265 year:1976 number:3 pages:461-478 http://linkinghub.elsevier.com/retrieve/pii/0375-9474(76)90555-8 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 265 1976 3 461-478 |
| allfields_unstemmed |
(DE-627)NLEJ181337223 (DE-599)GBVNLZ181337223 DE-627 ger DE-627 rakwb eng Mechanism of α-particle scattering from ^2^8Si nuclei 1976 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Statistical and Regge pole analyses were performed on excitation functions and angular distributions for α-particle scattering on ^2^8Si leading to the ground, 2^+ (1.78) MeV and 4^+ (4.62 Me V) states in the energy range 21-28 MeV. The direct interaction contribution y"D for the reaction studied was determined. Angular cross-correlation coefficients (a.c.c.c.) were calculated in each channel for all pairs of experimental excitation functions. For the elastic channel a.c.c.c. were compared with the coefficients calculated using the excitation functions generated by the optical model. Channel cross-correlation coefficients (c.c.c.c.) were also calculated in the full angular range for pairs of excitation functions measured at the same angle (lab). The single Regge pole model was used to describe the behaviour of the angular distribution at backward angles in the elastic channel. The l = 10 value of angular momentum for energies greater than 24 MeV was clearly distinguished. The results of the analysis indicate that at backward angles of scattering a mechanism different from the direct and compound ones contributes significantly to the reaction. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Budzanowski, A. oth Jarczyk, L. oth Kamys, B. oth Kapuscik, A. oth in Nuclear Physics, Section A Amsterdam : Elsevier 265(1976), 3, Seite 461-478 (DE-627)NLEJ177217928 (DE-600)1466542-6 0375-9474 nnns volume:265 year:1976 number:3 pages:461-478 http://linkinghub.elsevier.com/retrieve/pii/0375-9474(76)90555-8 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 265 1976 3 461-478 |
| allfieldsGer |
(DE-627)NLEJ181337223 (DE-599)GBVNLZ181337223 DE-627 ger DE-627 rakwb eng Mechanism of α-particle scattering from ^2^8Si nuclei 1976 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Statistical and Regge pole analyses were performed on excitation functions and angular distributions for α-particle scattering on ^2^8Si leading to the ground, 2^+ (1.78) MeV and 4^+ (4.62 Me V) states in the energy range 21-28 MeV. The direct interaction contribution y"D for the reaction studied was determined. Angular cross-correlation coefficients (a.c.c.c.) were calculated in each channel for all pairs of experimental excitation functions. For the elastic channel a.c.c.c. were compared with the coefficients calculated using the excitation functions generated by the optical model. Channel cross-correlation coefficients (c.c.c.c.) were also calculated in the full angular range for pairs of excitation functions measured at the same angle (lab). The single Regge pole model was used to describe the behaviour of the angular distribution at backward angles in the elastic channel. The l = 10 value of angular momentum for energies greater than 24 MeV was clearly distinguished. The results of the analysis indicate that at backward angles of scattering a mechanism different from the direct and compound ones contributes significantly to the reaction. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Budzanowski, A. oth Jarczyk, L. oth Kamys, B. oth Kapuscik, A. oth in Nuclear Physics, Section A Amsterdam : Elsevier 265(1976), 3, Seite 461-478 (DE-627)NLEJ177217928 (DE-600)1466542-6 0375-9474 nnns volume:265 year:1976 number:3 pages:461-478 http://linkinghub.elsevier.com/retrieve/pii/0375-9474(76)90555-8 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 265 1976 3 461-478 |
| allfieldsSound |
(DE-627)NLEJ181337223 (DE-599)GBVNLZ181337223 DE-627 ger DE-627 rakwb eng Mechanism of α-particle scattering from ^2^8Si nuclei 1976 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Statistical and Regge pole analyses were performed on excitation functions and angular distributions for α-particle scattering on ^2^8Si leading to the ground, 2^+ (1.78) MeV and 4^+ (4.62 Me V) states in the energy range 21-28 MeV. The direct interaction contribution y"D for the reaction studied was determined. Angular cross-correlation coefficients (a.c.c.c.) were calculated in each channel for all pairs of experimental excitation functions. For the elastic channel a.c.c.c. were compared with the coefficients calculated using the excitation functions generated by the optical model. Channel cross-correlation coefficients (c.c.c.c.) were also calculated in the full angular range for pairs of excitation functions measured at the same angle (lab). The single Regge pole model was used to describe the behaviour of the angular distribution at backward angles in the elastic channel. The l = 10 value of angular momentum for energies greater than 24 MeV was clearly distinguished. The results of the analysis indicate that at backward angles of scattering a mechanism different from the direct and compound ones contributes significantly to the reaction. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Budzanowski, A. oth Jarczyk, L. oth Kamys, B. oth Kapuscik, A. oth in Nuclear Physics, Section A Amsterdam : Elsevier 265(1976), 3, Seite 461-478 (DE-627)NLEJ177217928 (DE-600)1466542-6 0375-9474 nnns volume:265 year:1976 number:3 pages:461-478 http://linkinghub.elsevier.com/retrieve/pii/0375-9474(76)90555-8 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 265 1976 3 461-478 |
| language |
English |
| source |
in Nuclear Physics, Section A 265(1976), 3, Seite 461-478 volume:265 year:1976 number:3 pages:461-478 |
| sourceStr |
in Nuclear Physics, Section A 265(1976), 3, Seite 461-478 volume:265 year:1976 number:3 pages:461-478 |
| format_phy_str_mv |
Article |
| institution |
findex.gbv.de |
| isfreeaccess_bool |
false |
| container_title |
Nuclear Physics, Section A |
| authorswithroles_txt_mv |
Budzanowski, A. @@oth@@ Jarczyk, L. @@oth@@ Kamys, B. @@oth@@ Kapuscik, A. @@oth@@ |
| publishDateDaySort_date |
1976-01-01T00:00:00Z |
| hierarchy_top_id |
NLEJ177217928 |
| id |
NLEJ181337223 |
| language_de |
englisch |
| fullrecord |
<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">NLEJ181337223</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20210706151332.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">070505s1976 xx |||||o 00| ||eng c</controlfield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)NLEJ181337223</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-599)GBVNLZ181337223</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Mechanism of α-particle scattering from ^2^8Si nuclei</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1976</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">zzz</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">z</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">zu</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Statistical and Regge pole analyses were performed on excitation functions and angular distributions for α-particle scattering on ^2^8Si leading to the ground, 2^+ (1.78) MeV and 4^+ (4.62 Me V) states in the energy range 21-28 MeV. The direct interaction contribution y"D for the reaction studied was determined. Angular cross-correlation coefficients (a.c.c.c.) were calculated in each channel for all pairs of experimental excitation functions. For the elastic channel a.c.c.c. were compared with the coefficients calculated using the excitation functions generated by the optical model. Channel cross-correlation coefficients (c.c.c.c.) were also calculated in the full angular range for pairs of excitation functions measured at the same angle (lab). The single Regge pole model was used to describe the behaviour of the angular distribution at backward angles in the elastic channel. The l = 10 value of angular momentum for energies greater than 24 MeV was clearly distinguished. The results of the analysis indicate that at backward angles of scattering a mechanism different from the direct and compound ones contributes significantly to the reaction.</subfield></datafield><datafield tag="533" ind1=" " ind2=" "><subfield code="f">Elsevier Journal Backfiles on ScienceDirect 1907 - 2002</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Budzanowski, A.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Jarczyk, L.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Kamys, B.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Kapuscik, A.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">in</subfield><subfield code="t">Nuclear Physics, Section A</subfield><subfield code="d">Amsterdam : Elsevier</subfield><subfield code="g">265(1976), 3, Seite 461-478</subfield><subfield code="w">(DE-627)NLEJ177217928</subfield><subfield code="w">(DE-600)1466542-6</subfield><subfield code="x">0375-9474</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:265</subfield><subfield code="g">year:1976</subfield><subfield code="g">number:3</subfield><subfield code="g">pages:461-478</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">http://linkinghub.elsevier.com/retrieve/pii/0375-9474(76)90555-8</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_H</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">ZDB-1-SDJ</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_NL_ARTICLE</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">265</subfield><subfield code="j">1976</subfield><subfield code="e">3</subfield><subfield code="h">461-478</subfield></datafield></record></collection>
|
| series2 |
Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 |
| ppnlink_with_tag_str_mv |
@@773@@(DE-627)NLEJ177217928 |
| format |
electronic Article |
| delete_txt_mv |
keep |
| collection |
NL |
| remote_str |
true |
| illustrated |
Not Illustrated |
| issn |
0375-9474 |
| topic_title |
Mechanism of α-particle scattering from ^2^8Si nuclei |
| format_facet |
Elektronische Aufsätze Aufsätze Elektronische Ressource |
| format_main_str_mv |
Text Zeitschrift/Artikel |
| carriertype_str_mv |
zu |
| author2_variant |
a b ab l j lj b k bk a k ak |
| hierarchy_parent_title |
Nuclear Physics, Section A |
| hierarchy_parent_id |
NLEJ177217928 |
| hierarchy_top_title |
Nuclear Physics, Section A |
| isfreeaccess_txt |
false |
| familylinks_str_mv |
(DE-627)NLEJ177217928 (DE-600)1466542-6 |
| title |
Mechanism of α-particle scattering from ^2^8Si nuclei |
| spellingShingle |
Mechanism of α-particle scattering from ^2^8Si nuclei |
| ctrlnum |
(DE-627)NLEJ181337223 (DE-599)GBVNLZ181337223 |
| title_full |
Mechanism of α-particle scattering from ^2^8Si nuclei |
| journal |
Nuclear Physics, Section A |
| journalStr |
Nuclear Physics, Section A |
| lang_code |
eng |
| isOA_bool |
false |
| recordtype |
marc |
| publishDateSort |
1976 |
| contenttype_str_mv |
zzz |
| container_start_page |
461 |
| container_volume |
265 |
| format_se |
Elektronische Aufsätze |
| title_sort |
mechanism of α-particle scattering from ^2^8si nuclei |
| title_auth |
Mechanism of α-particle scattering from ^2^8Si nuclei |
| abstract |
Statistical and Regge pole analyses were performed on excitation functions and angular distributions for α-particle scattering on ^2^8Si leading to the ground, 2^+ (1.78) MeV and 4^+ (4.62 Me V) states in the energy range 21-28 MeV. The direct interaction contribution y"D for the reaction studied was determined. Angular cross-correlation coefficients (a.c.c.c.) were calculated in each channel for all pairs of experimental excitation functions. For the elastic channel a.c.c.c. were compared with the coefficients calculated using the excitation functions generated by the optical model. Channel cross-correlation coefficients (c.c.c.c.) were also calculated in the full angular range for pairs of excitation functions measured at the same angle (lab). The single Regge pole model was used to describe the behaviour of the angular distribution at backward angles in the elastic channel. The l = 10 value of angular momentum for energies greater than 24 MeV was clearly distinguished. The results of the analysis indicate that at backward angles of scattering a mechanism different from the direct and compound ones contributes significantly to the reaction. |
| abstractGer |
Statistical and Regge pole analyses were performed on excitation functions and angular distributions for α-particle scattering on ^2^8Si leading to the ground, 2^+ (1.78) MeV and 4^+ (4.62 Me V) states in the energy range 21-28 MeV. The direct interaction contribution y"D for the reaction studied was determined. Angular cross-correlation coefficients (a.c.c.c.) were calculated in each channel for all pairs of experimental excitation functions. For the elastic channel a.c.c.c. were compared with the coefficients calculated using the excitation functions generated by the optical model. Channel cross-correlation coefficients (c.c.c.c.) were also calculated in the full angular range for pairs of excitation functions measured at the same angle (lab). The single Regge pole model was used to describe the behaviour of the angular distribution at backward angles in the elastic channel. The l = 10 value of angular momentum for energies greater than 24 MeV was clearly distinguished. The results of the analysis indicate that at backward angles of scattering a mechanism different from the direct and compound ones contributes significantly to the reaction. |
| abstract_unstemmed |
Statistical and Regge pole analyses were performed on excitation functions and angular distributions for α-particle scattering on ^2^8Si leading to the ground, 2^+ (1.78) MeV and 4^+ (4.62 Me V) states in the energy range 21-28 MeV. The direct interaction contribution y"D for the reaction studied was determined. Angular cross-correlation coefficients (a.c.c.c.) were calculated in each channel for all pairs of experimental excitation functions. For the elastic channel a.c.c.c. were compared with the coefficients calculated using the excitation functions generated by the optical model. Channel cross-correlation coefficients (c.c.c.c.) were also calculated in the full angular range for pairs of excitation functions measured at the same angle (lab). The single Regge pole model was used to describe the behaviour of the angular distribution at backward angles in the elastic channel. The l = 10 value of angular momentum for energies greater than 24 MeV was clearly distinguished. The results of the analysis indicate that at backward angles of scattering a mechanism different from the direct and compound ones contributes significantly to the reaction. |
| collection_details |
GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE |
| container_issue |
3 |
| title_short |
Mechanism of α-particle scattering from ^2^8Si nuclei |
| url |
http://linkinghub.elsevier.com/retrieve/pii/0375-9474(76)90555-8 |
| remote_bool |
true |
| author2 |
Budzanowski, A. Jarczyk, L. Kamys, B. Kapuscik, A. |
| author2Str |
Budzanowski, A. Jarczyk, L. Kamys, B. Kapuscik, A. |
| ppnlink |
NLEJ177217928 |
| mediatype_str_mv |
z |
| isOA_txt |
false |
| hochschulschrift_bool |
false |
| author2_role |
oth oth oth oth |
| up_date |
2024-07-06T06:18:39.057Z |
| _version_ |
1803809423686107136 |
| fullrecord_marcxml |
<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">NLEJ181337223</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20210706151332.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">070505s1976 xx |||||o 00| ||eng c</controlfield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)NLEJ181337223</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-599)GBVNLZ181337223</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Mechanism of α-particle scattering from ^2^8Si nuclei</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1976</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">zzz</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">z</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">zu</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Statistical and Regge pole analyses were performed on excitation functions and angular distributions for α-particle scattering on ^2^8Si leading to the ground, 2^+ (1.78) MeV and 4^+ (4.62 Me V) states in the energy range 21-28 MeV. The direct interaction contribution y"D for the reaction studied was determined. Angular cross-correlation coefficients (a.c.c.c.) were calculated in each channel for all pairs of experimental excitation functions. For the elastic channel a.c.c.c. were compared with the coefficients calculated using the excitation functions generated by the optical model. Channel cross-correlation coefficients (c.c.c.c.) were also calculated in the full angular range for pairs of excitation functions measured at the same angle (lab). The single Regge pole model was used to describe the behaviour of the angular distribution at backward angles in the elastic channel. The l = 10 value of angular momentum for energies greater than 24 MeV was clearly distinguished. The results of the analysis indicate that at backward angles of scattering a mechanism different from the direct and compound ones contributes significantly to the reaction.</subfield></datafield><datafield tag="533" ind1=" " ind2=" "><subfield code="f">Elsevier Journal Backfiles on ScienceDirect 1907 - 2002</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Budzanowski, A.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Jarczyk, L.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Kamys, B.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Kapuscik, A.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">in</subfield><subfield code="t">Nuclear Physics, Section A</subfield><subfield code="d">Amsterdam : Elsevier</subfield><subfield code="g">265(1976), 3, Seite 461-478</subfield><subfield code="w">(DE-627)NLEJ177217928</subfield><subfield code="w">(DE-600)1466542-6</subfield><subfield code="x">0375-9474</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:265</subfield><subfield code="g">year:1976</subfield><subfield code="g">number:3</subfield><subfield code="g">pages:461-478</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">http://linkinghub.elsevier.com/retrieve/pii/0375-9474(76)90555-8</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_H</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">ZDB-1-SDJ</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_NL_ARTICLE</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">265</subfield><subfield code="j">1976</subfield><subfield code="e">3</subfield><subfield code="h">461-478</subfield></datafield></record></collection>
|
| score |
7.401947 |