Cross Sections for 13C(p, X)
(Current as of 10/31/2021)
NSR Reaction Ep (MeV) Cross Section File X4 Dataset Date Added
1961HE02 13C(p, γ): σ 100 - 140 keV   X4 12/06/2017
2001NE15 13C(p, γ): σ, deduced S(E) ratio < 160 keV   X4 09/12/2011
1963VOZZ 13C(p, γ): deduced σ < 700 keV   X4 04/04/2018
1994KI02 13C(p, γ): γ-ray yield, calculated S(E) 120 - 950 keV   X4 09/12/2011
1952WO17 13C(p, γ): deduced thick target yields, σ 129 keV   X4 12/06/2017
1960HE14 13C(p, p): σ 140 - 750 keV   X4 12/06/2017
2008HE11 13C(p, γ): reaction yield at the resonance 448.5-keV for a fresh target and after an integrated charge of 1C 435 - 470 keV σ X4 11/07/2011
1991BR19 13C(p, γ): reaction yield near the resonance 0.44 - 0.6 483.3-keV, 0.55-MeV X4 11/07/2011
1991GA22 13C(p, p), (p, γ): σ, thick target γ yield 0.45 - 0.65   X4 04/12/2012
1954MI05 13C(p, p): elastic scattering σ at θcm = 50°, 90°, 120°, 140° and 160 ° 0.45 - 1.60   X4 06/19/2017
1979MA38 13C(p, π+): σ 0.5 - 10 MeV above threshold   X4 09/12/2011
2005MA92 13C(p, γ): σ near ER = 550 keV 520 - 582 keV sample 1, sample 2   07/22/2012
1990SP02 13C(p, γ): excitation function of the 550-keV resonance with various implant dose (13C ions/cm2) ≤ 0.6 5 × 1016, 1 × 1017, 2 × 1017   09/08/2011
1965DE19 13C(p, γ): excitation curve 0.6 - 1.5 1.1 MeV ≤ Eγ ≤ 4.0 MeV   10/26/2011
1.4 - 1.8 Eγ > 1.3 MeV, Eγ > 7.5 MeV
13C(p, γ): excitation curve near Eres = 1012 keV 1009 - 1018 keV 2.0 MeV < Eγ < 5.5 MeV, Eγ > 5.5 MeV
13C(p, γ): excitation curve near Eres = 1523 keV 1500 - 1560 keV Eγ > 1.3 MeV, Eγ > 7.5 MeV
13C(p, γ): excitation curve near Eres = 1701 keV 1620 - 1780 keV Eγ > 1.3 MeV, Eγ > 7.5 MeV
2013BA56 13C(p, p): deduced σ, yields 0.8 - 2.4   X4 12/17/2015
1991FI11 13C(p, n): residual production absolute σ, thick target yield 1 - 33   X4 04/12/2012
1986ZI08 13C(p, γ): σ near 1460 keV   X4 04/25/2012
1966GE03 13C(p, p): σ 1.55 - 2.38   X4 03/20/2012
2020HEZZ 13C(p, γ): excitation curve for 9.17 MeV γ-ray 1.74 - 1.78 1   09/13/2021
2005HA69 13C(p, γ): thick target γ yield near the resonances 1.747-MeV 1.742 - 1.757 natural C, enriched C X4 11/07/2011
2006SK05 13C(p, γ): resonance excitation function in crystal target ~ 1.7476 along the (0001) plane, beam randomly oriented   10/20/2011
2019NK01 13C(p, n): 13N production σ 2 - 20 1   09/13/2021
1998HU29 1H(13C, 13C), 13C(p, p): σ E(13C) = 2.8 - 11.2   X4 12/06/2017
1991WI04 13C(pol. p, γ): σ 3 - 3.3 [σ(55)+σ(125)]/2   07/22/2012
1959GI47 13C(p, n): σ 3.0 - 5.5 1   04/27/2020
2010GE08, 2010GEZY 13C(p, γ): deduced S-factor 3200 - 7900 keV 1   04/27/2020
1966DI03 13C(p, n): excitation function 3.237 - 3.85 θlab = 0°   09/19/2011
1971RI13 13C(p, γ0): relative yield near ER = 3.771 MeV at θ = 90° 3.75 - 3.78 thin target, thick target   06/05/2012
13C(p, γ0): relative yield near ER = 4.53 MeV 4.45 -4.60 θ = 0°, θ = 90°
13C(p, p'): relative yield to 3.68-MeV state near ER = 4.53 MeV θ = 0°, θ = 90°
13C(p, γ0): excitation function 3 -7 θ = 0°, θ = 90°
13C(p, p'): excitation function at θ = 90° to 3.09-MeV state, 3.68-MeV state, 3.85-MeV state
13C(p, γ): excitation function at θ = 90° for 5 -18 γ0, γ1
13C(p, p'): excitation function at θ = 60° to 6 -17 3.09-MeV state, 3.68-MeV state, 3.85-MeV state
1981BA22 13C(p, n): thick target yield, σ(E) 4 - 12   X4 09/12/2011
1975OB01 13C(p, α): total σ for production of 10B 5 - 18 1   09/19/2011
13C(p, α)10B: excitation function for 10B states g.s., 0.72-MeV, 1.74-MeV, 2.15-MeV, 3.59-MeV, 5.17-MeV
13C(p, 2α): total σ for production of 6Li 10 - 18 1
13C(p, pα): total σ for production of 9Be 13 - 18 1
1989WA16 13C(p, n) 5 - 30 1 X4 02/28/2011
1979MA39 (p, π+): σ 8 - 16   X4 09/12/2011
1992DE19 1H(13C, 13C): normalized σ at θlab = E(13C) = 8.2 17°, 27°   04/27/2020
1978WE13 13C(pol. p, p): differential σ 9.1 - 18.4 θcm = 89.4°, θcm = 119.0°, θcm = 147.5° X4 11/07/2011
1981BY01 13C(p, n): σ 10.1 - 16.75   X4 09/12/2011
1988KA30 13C(p, n): σ 15.8, 18.6   X4 04/12/2012
1975PA18 13C(p, γ): excitation functions of γ-decay yield to various final states in 14N at θ = 90° 16 - 28 g.s., 2.31-MeV, 4.91-MeV, 8.06-MeV   10/20/2011
1980TU01 13C(p, γ): differential σ of γ-decay to various final states in 14N at θlab = 90° 16 - 28 g.s., 2.31-MeV X4 11/07/2011
1975LI11 13C(p, n) 16.3, 22.8 Table I   06/05/2012
1988AB11 13C(p, α): partially integrated σ for transition to various states in 10B at θ = 0 - 90° 18 - 65 g.s., 0.72-MeV, 1.74-MeV, 2.15-MeV, 3.59-MeV, ,4.77-MeV, ,5.16+5.18-MeV, ,5.92+6.03-MeV, ,7.48+7.56-MeV X4 11/07/2011
2007LH01 13C(p, n): σ 20, 25, 40   X4 09/12/2011
1975MI01 13C(p, t)11C: integrated σ of transitions to 11C levels 26.8, 29.3, 31.8, 38.2, 43.1 Table I   06/05/2012
13C(p, 3He)11B: integrated σ of transitions to 11B levels Table II
1970CL01 (p, n): σ 30, 50   X4 09/12/2011
1973RA37 13C(p, X): production σ for 7, 9, 10Be 150, 600   X4 09/12/2011
1980KA01 13C(p, d): differential σ to the g.s. and first excited state in 12C at θ = 22.5° 200 - 500 g.s., 4.44-MeV X4 11/07/2011
Thick target yields for very narrow resonance
1995ZE01 13C(p, γ0): excitation function, γ-yield near the resonance Ep = 1.75 MeV with target thickness 0.45 - 3 σ, 80.2 ± 3.0 μg/cm2   10/20/2011
13C(p, γ): excitation function, γ-yield near the resonance Ep = 1.75 MeV with target thickness 0.45 - 3 σ to excited states and the secondary decays, 24.3 ± 1.1 μg/cm2
The following references may be related but not included.
1966RI09, 1968CO26, 1971VA29, 1972MA21, 1973CL14, 1977GU14, 1979TUZY, 1983VI01, 1985KI07, 1985PR03, 1986AI04, 1991FI05, 1991ZH31, 1993DE25, 2001KR12, 2002HA02, 2006LE01, 2006SK04

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Last modified: 01 November 2021