Gosia2
From GOSIA
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+ | ==Introduction== | ||
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+ | Gosia2 is the simultaneous projectile-and-target excitation version of Gosia. It is the appropriate tool for cases where the yields for the investigated nucleus must be normalized to those of the target: | ||
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+ | # The investigated nucleus is not collective, so that the data cannot be self-normalized (to a decay in the yrast line) | ||
+ | # The B(ML) [usually B(E2)], matrix element and lifetime coupling the ground state to the first excited state are unknown | ||
+ | # A collision partner with known spectroscopic data can be chosen, i.e. one for which the B(E2) or lifetime of the first excited state is known accurately enough to normalize the data for the investigated nucleus | ||
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==Current release version== | ==Current release version== | ||
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* 19 January 2009 gosia2_20081208.1.f Bugfix relative to 20081208 (give error if too many omega steps). | * 19 January 2009 gosia2_20081208.1.f Bugfix relative to 20081208 (give error if too many omega steps). | ||
* 8 December 2008 gosia2_20081208.f New OP,INTI option for inverse kinematics (beta version) | * 8 December 2008 gosia2_20081208.f New OP,INTI option for inverse kinematics (beta version) | ||
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+ | ==Known bugs or issues== | ||
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+ | The OP,BRIC function for automatic calculation of Band-Raman internal conversion coefficients may not operate in some cases. The user can enter internal conversion coefficient data in OP,YIEL. Refer to the Gosia manual OP,YIEL section. | ||
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+ | ==Notes== | ||
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+ | <references/> |