Difference between revisions of "References and Documents"
| Line 59: | Line 59: | ||
* ''Nuclear reactions in stellar helium burning and later hydrostatic burning stages'' | * ''Nuclear reactions in stellar helium burning and later hydrostatic burning stages'' | ||
| − | L.R. Buchmann, C.A. Barnes, | + | L.R. Buchmann, C.A. Barnes, Nucl. Phys. A '''777''' (2006) 254 [[media:NuclPhysA.777.254.pdf]] |
| + | |||
| + | * ''E1 and E2 capture cross section and astrophysical reaction rate of the key reaction <sup>12</sup>C(α,γ)<sup>16</sup>O'' | ||
| + | J.W. Hammer et. al., Nucl. Phys. A '''758''' (2005) 363 [[media:NuclPhysA.758.363.pdf]] | ||
* ''<sup>12</sup>C(α, γ )<sup>16</sup>O: The Key Reaction in Stellar Nucleosynthesis'' | * ''<sup>12</sup>C(α, γ )<sup>16</sup>O: The Key Reaction in Stellar Nucleosynthesis'' | ||
| Line 66: | Line 69: | ||
* ''The E1 and E2 capture amplitudes in <sup>12</sup>C(α,γ0)<sup>16</sup>O'' | * ''The E1 and E2 capture amplitudes in <sup>12</sup>C(α,γ0)<sup>16</sup>O'' | ||
G. Roters et al., Eur. Phys. J. A '''6''' (1999) 451 [[media:EurPhysJA.6.451.pdf]] | G. Roters et al., Eur. Phys. J. A '''6''' (1999) 451 [[media:EurPhysJA.6.451.pdf]] | ||
| − | |||
= Nucleosynthesis = | = Nucleosynthesis = | ||
Revision as of 10:47, 23 December 2013
Program Advisory Committee (PAC)
- PAC40 (June 2013):
- Experiment Proposal Media:PAC40_proposal.pdf
- PAC Report Media:PAC40_Report.pdf
Proceedings
- Determination of astrophysical thermonuclear rates with a bubble chamber: 12C(α,γ)16O reaction case
PEB Proceedings, [1]. AIP Conf. Proc. 1563, 239 (2013), media:AIP.1.4829419.pdf [2]
Bubble Chamber
- First determination of an astrophysical cross section with a bubble chamber: The 15N(α,γ) 19F reaction
C. Ugalde et al., Phys. Lett. B 719 (2013) 74 media:PhysLettB.719.74.pdf
- New insights into particle detection with superheated liquids
S. Archambault et al., New J. Phys. 13 (2011) 043006 media:NewJPhys.13.043006.pdf
- Discrimination of nuclear recoils from alpha particles with superheated liquids
F. Aubin et al., New J. Phys. 10 (2008) 103017 media:NewJPhys.10.103017.pdf
- Direct measurement of the bubble-nucleation energy threshold in a CF3I bubble chamber
E. Behnke et al., Phys. Rev. D 88 (2013) 021101(R) media:PhysRevD.88.021101.pdf
- Study of low frequency acoustic signals from superheated droplet detector
P.K. Mondal et al., Nucl. Inst. Meth. A 729 (2013) 182 media:NuclInstMethA.729.182.pdf
- Development of bubble chambers with enhanced stability and sensitivity to low-energy nuclear recoils
W.J. Bolte et al., Nucl. Inst. Meth. A 577 (2007) 569 media:NuclInstMethA.577.569.pdf
- Response of superheated droplet detectors of the PICASSO dark matter search experiment
M. Barnabé-Heider et al., Nucl. Inst. Meth. A 555 (2005) 184 media:NuclInstMethA.555.184.pdf
- Superheated liquid and its place in radiation physics
S.C. Roy, Radiation Physics and Chemistry 61 (2001) 271 media:RadiatPhysChem.61.271.pdf
- Search for dark matter with moderately superheated liquids
V. Zacek, Nuovo Cimento A 107 (1994) 1247 media:NuovoCementoA.107.1247.pdf
- On the Theory of the Bubble Chamber
F. Seitz, Phys. of Fluids 1 (1957) 2 media:Phys.Fluids.1.2.pdf
Oxygen S-Factor
- The astrophysical S factor of 12C(α, γ )16O at stellar energy
D. Schürmann, L. Gialanella, R. Kunz, F. Strieder, Phys. Lett. B 711 (2012) 35 media:PhysLettB.711.35.pdf
- New Determination of the Astrophysical S Factor SE1 of the 12C(α,γ)16O Reaction
X. D. Tang et al., Phys. Rev. Lett. 99 (2007) 052502 media:PhysRevLett.99.052502.pdf
- A new study for 16O(γ,α)12C at the energies of nuclear astrophysics interest: The inverse of key nucleosynthesis reaction 12C(α,γ)16O
Y. Xu et al., Nucl. Inst. Meth. A 581 (2007) 866 media:NuclInstMethA.581.866.pdf
- Measurement of the Cascade Transition via the First Excited State of 16O in the 12C(α,γ)16O Reaction, and Its S Factor in Stellar Helium Burning
C. Matei et al., Phys. Rev. Lett. 97 (2006) 242503 media:PhysRevLett.97.242503.pdf
- Nuclear reactions in stellar helium burning and later hydrostatic burning stages
L.R. Buchmann, C.A. Barnes, Nucl. Phys. A 777 (2006) 254 media:NuclPhysA.777.254.pdf
- E1 and E2 capture cross section and astrophysical reaction rate of the key reaction 12C(α,γ)16O
J.W. Hammer et. al., Nucl. Phys. A 758 (2005) 363 media:NuclPhysA.758.363.pdf
- 12C(α, γ )16O: The Key Reaction in Stellar Nucleosynthesis
R. Kunz et al., Phys. Rev. Lett. 86 (2001) 3244 media:PhysRevLett.86.3244.pdf
- The E1 and E2 capture amplitudes in 12C(α,γ0)16O
G. Roters et al., Eur. Phys. J. A 6 (1999) 451 media:EurPhysJA.6.451.pdf
Nucleosynthesis
- Nucleosynthesis and remnants in massive stars of solar metallicity
S.E. Woosley and A. Heger, Phys. Reports 442 (2007) 269 media:Phys.Reports.442.269.pdf
- Coulomb dissociation as a source of information on radiative capture processes of astrophysical interest
G. Baur et al., Nucl. Phys. A 458 (1986) 188 media:NuclPhysA.458.188.pdf
- General properties of astrophysical reaction rates in explosive nucleosynthesis
T. Rauscher, J. Phys. Conf. Ser. 420 (2013) 012138 media:J.Phys.Conf.Ser._420_1_012138.pdf
Astrophysics
- Dependence of s-process nucleosynthesis in massive stars on triple-alpha and 12C(α,γ)16O reaction rate uncertainties
C. Tur et al., Astroph. J., 702(2) (2009) 1068 media:AstrophJ_702_2_1068.pdf