1983
DOI: 10.1007/bf00898886
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Green's electron function in a quantized plane wave field

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Cited by 2 publications
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“…The burning of C and O under degenerate conditions can be described by three stages. First, C is consumed producing reaction products close to Mg. Then O is consumed along with the ashes of C burning, which produces a mixture of silicon group and light elements that is in a statistical quasi-equilibrium [59,60,61]. Finally the silicon-group nuclei are converted to IGEs, reaching full nuclear statistical equilibrium (NSE).…”
Section: Simulation Instrumentmentioning
confidence: 99%
“…The burning of C and O under degenerate conditions can be described by three stages. First, C is consumed producing reaction products close to Mg. Then O is consumed along with the ashes of C burning, which produces a mixture of silicon group and light elements that is in a statistical quasi-equilibrium [59,60,61]. Finally the silicon-group nuclei are converted to IGEs, reaching full nuclear statistical equilibrium (NSE).…”
Section: Simulation Instrumentmentioning
confidence: 99%
“…The nuclear processing can be well-approximated as a three stage process: initially C is consumed, followed by O, which creates a mixture of Si group and light elements that is in quasi-statistical equilibrium, also known as nuclear statistical quasi-equilibrium (NSQE) [236][237][238][239][240]); finally the Si-group nuclei are converted to Fe group, reaching full nuclear statistical equilibrium, NSE. In both of these equilibrium states, the capture and creation of light elements (via photodisintegration) is balanced, so that energy release can continue by changing the relative abundance of light (low nuclear binding energy) and heavy (high nuclear binding energy) nuclides, an action that releases energy as buoyant burned material rises and expands.…”
Section: Flame Modelmentioning
confidence: 99%