Yeild

¹⁰⁰Sn	Tin			Z:	≪	≫
¹⁰⁰Sn	Z = 50	N = 50		N:	≪	≫

Setting ID¹	Yield ² [pps/pnA]	Measurement date	Beam	Target	Brho01 [Tm]	F1 slit L [mm]	F1 slit R [mm]	Data from
118	8.05e-5	2013-06-27	124Xe 345MeV	Be 4mm	5.2510	64.2	3.0	Phys. Rev. Lett. 116, 162501 (2016)
119	8.30e-5	2013-06-26	124Xe 345MeV	Be 4mm	5.2510	64.2	3.0	Phys. Rev. Lett. 116, 162501 (2016)
120	1.17e-4	2013-06-26	124Xe 345MeV	Be 4mm	5.2510	64.2	7.0	Phys. Rev. Lett. 116, 162501 (2016)
121	1.01e-4	2013-06-25	124Xe 345MeV	Be 4mm	5.2510	64.2	7.0	Phys. Rev. Lett. 116, 162501 (2016)
122	1.14e-4	2013-06-22	124Xe 345MeV	Be 4mm	5.2510	64.2	7.0	Phys. Rev. Lett. 116, 162501 (2016)
123	1.37e-4	2013-06-21	124Xe 345MeV	Be 4mm	5.2510	64.2	7.0	Phys. Rev. Lett. 116, 162501 (2016)
124	1.57e-4	2013-06-19	124Xe 345MeV	Be 4mm	5.2510	64.2	33.0	Phys. Rev. Lett. 116, 162501 (2016)
125	1.79e-4	2013-06-19	124Xe 345MeV	Be 4mm	5.2510	64.2	17.0	Phys. Rev. Lett. 116, 162501 (2016)
126	1.40e-4	2013-06-18	124Xe 345MeV	Be 4mm	5.2510	64.0	38.0	Phys. Rev. Lett. 116, 162501 (2016)
127	1.26e-4	2013-06-18	124Xe 345MeV	Be 4mm	5.2510	64.0	38.0	Phys. Rev. Lett. 116, 162501 (2016)
128	1.68e-4	2013-06-18	124Xe 345MeV	Be 4mm	5.2510	64.0	21.4	Phys. Rev. Lett. 116, 162501 (2016)
183	1.10e-4	2011-12-14	124Xe 345MeV	Be 4mm	5.2550	42.8	42.8	Nucl. Instrum. Methods Phys. Res., Sect. B 317, 756 (2013)

Publication

Title	Journal	First Author
Improved Value for the Gamow-Teller Strength of the 100Sn Beta Decay	Phys. Rev. Lett. 122, 222502 (2019)	D. Lubos

Experiment

Proposal No.	Spokesperson	Start-Date	End-Date	Beam	Course
NP1612-RIBF147	A. Algora	2019-06-15	2019-06-19	124Xe 345 MeV/u	ZeroDegree
NP0702-RIBF09-02	M. Lewitowicz	2013-06-16	2013-06-28	124Xe 345 MeV/u	ZeroDegree
NP0702-RIBF09	M. Lewitowicz	2011-12-18	2011-12-20	124Xe 345 MeV/u	BigRIPS
MS11-03	T. Kubo	2011-12-12	2011-12-18	124Xe 345 MeV/u	BigRIPS

Annotations:: ¹ Detailed BigRIPS setting is shown in the linked page.; ² The list of primary beam intensities is given in this page.; ³ Error is only statistical one. Systematic error is estimated within 30%, which comes from uncertainly of primary beam intensity.

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