CLAS Physics Database

ID	Final state	Q²_min, GeV²	Q²_max, GeV²	W_min, GeV	W_max, GeV	Quantity	Spokespersons	Title	Year
E187M1	π⁻ p	0.5	0.5	1.1125	1.1125	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M2	π⁻ p	0.7	0.7	1.1125	1.1125	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M3	π⁻ p	0.5	0.5	1.1375	1.1375	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M4	π⁻ p	0.7	0.7	1.1375	1.1375	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M5	π⁻ p	0.9	0.9	1.1375	1.1375	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M6	π⁻ p	0.5	0.5	1.1625	1.1625	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M7	π⁻ p	0.7	0.7	1.1625	1.1625	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M8	π⁻ p	0.9	0.9	1.1625	1.1625	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M9	π⁻ p	0.5	0.5	1.1875	1.1875	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M10	π⁻ p	0.7	0.7	1.1875	1.1875	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M11	π⁻ p	0.9	0.9	1.1875	1.1875	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M12	π⁻ p	0.5	0.5	1.2125	1.2125	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M13	π⁻ p	0.7	0.7	1.2125	1.2125	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M14	π⁻ p	0.9	0.9	1.2125	1.2125	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M15	π⁻ p	0.5	0.5	1.2375	1.2375	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M16	π⁻ p	0.7	0.7	1.2375	1.2375	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M17	π⁻ p	0.9	0.9	1.2375	1.2375	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M18	π⁻ p	0.5	0.5	1.2625	1.2625	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M19	π⁻ p	0.7	0.7	1.2625	1.2625	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M20	π⁻ p	0.9	0.9	1.2625	1.2625	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M21	π⁻ p	0.5	0.5	1.2875	1.2875	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M22	π⁻ p	0.7	0.7	1.2875	1.2875	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M23	π⁻ p	0.9	0.9	1.2875	1.2875	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M24	π⁻ p	0.5	0.5	1.3125	1.3125	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M25	π⁻ p	0.7	0.7	1.3125	1.3125	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M26	π⁻ p	0.9	0.9	1.3125	1.3125	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M27	π⁻ p	0.5	0.5	1.3375	1.3375	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M28	π⁻ p	0.7	0.7	1.3375	1.3375	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M29	π⁻ p	0.9	0.9	1.3375	1.3375	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M30	π⁻ p	0.5	0.5	1.3625	1.3625	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M31	π⁻ p	0.7	0.7	1.3625	1.3625	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M32	π⁻ p	0.9	0.9	1.3625	1.3625	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M33	π⁻ p	0.5	0.5	1.3875	1.3875	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M34	π⁻ p	0.7	0.7	1.3875	1.3875	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M35	π⁻ p	0.9	0.9	1.3875	1.3875	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M36	π⁻ p	0.5	0.5	1.4125	1.4125	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M37	π⁻ p	0.7	0.7	1.4125	1.4125	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M38	π⁻ p	0.9	0.9	1.4125	1.4125	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M39	π⁻ p	0.5	0.5	1.4375	1.4375	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M40	π⁻ p	0.7	0.7	1.4375	1.4375	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M41	π⁻ p	0.9	0.9	1.4375	1.4375	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M42	π⁻ p	0.5	0.5	1.4625	1.4625	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M43	π⁻ p	0.7	0.7	1.4625	1.4625	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M44	π⁻ p	0.9	0.9	1.4625	1.4625	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M45	π⁻ p	0.5	0.5	1.4875	1.4875	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M46	π⁻ p	0.7	0.7	1.4875	1.4875	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M47	π⁻ p	0.9	0.9	1.4875	1.4875	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M48	π⁻ p	0.5	0.5	1.5125	1.5125	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M49	π⁻ p	0.7	0.7	1.5125	1.5125	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M50	π⁻ p	0.9	0.9	1.5125	1.5125	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M51	π⁻ p	0.5	0.5	1.5375	1.5375	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M52	π⁻ p	0.7	0.7	1.5375	1.5375	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M53	π⁻ p	0.9	0.9	1.5375	1.5375	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M54	π⁻ p	0.5	0.5	1.5625	1.5625	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M55	π⁻ p	0.7	0.7	1.5625	1.5625	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M56	π⁻ p	0.9	0.9	1.5625	1.5625	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M57	π⁻ p	0.5	0.5	1.5875	1.5875	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M58	π⁻ p	0.7	0.7	1.5875	1.5875	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M59	π⁻ p	0.9	0.9	1.5875	1.5875	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M60	π⁻ p	0.5	0.5	1.6125	1.6125	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M61	π⁻ p	0.7	0.7	1.6125	1.6125	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M62	π⁻ p	0.5	0.5	1.6375	1.6375	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M63	π⁻ p	0.7	0.7	1.6375	1.6375	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M64	π⁻ p	0.5	0.5	1.6625	1.6625	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M65	π⁻ p	0.7	0.7	1.6625	1.6625	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M66	π⁻ p	0.5	0.5	1.6875	1.6875	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M67	π⁻ p	0.7	0.7	1.6875	1.6875	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M68	π⁻ p	0.5	0.5	1.7125	1.7125	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M69	π⁻ p	0.7	0.7	1.7125	1.7125	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M70	π⁻ p	0.5	0.5	1.7375	1.7375	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M71	π⁻ p	0.7	0.7	1.7375	1.7375	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M72	π⁻ p	0.5	0.5	1.7625	1.7625	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M73	π⁻ p	0.5	0.5	1.7875	1.7875	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M74	π⁻ p	0.5	0.5	1.8125	1.8125	dσ/dΩ (exclusive)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M75	π⁻ p	0.5	0.5	1.1125	1.1125	dσ/dΩ (quasi-free)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M76	π⁻ p	0.7	0.7	1.1125	1.1125	dσ/dΩ (quasi-free)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M77	π⁻ p	0.5	0.5	1.1375	1.1375	dσ/dΩ (quasi-free)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M78	π⁻ p	0.7	0.7	1.1375	1.1375	dσ/dΩ (quasi-free)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M79	π⁻ p	0.9	0.9	1.1375	1.1375	dσ/dΩ (quasi-free)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M80	π⁻ p	0.5	0.5	1.1625	1.1625	dσ/dΩ (quasi-free)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M81	π⁻ p	0.7	0.7	1.1625	1.1625	dσ/dΩ (quasi-free)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M82	π⁻ p	0.9	0.9	1.1625	1.1625	dσ/dΩ (quasi-free)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M83	π⁻ p	0.5	0.5	1.1875	1.1875	dσ/dΩ (quasi-free)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M84	π⁻ p	0.7	0.7	1.1875	1.1875	dσ/dΩ (quasi-free)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M85	π⁻ p	0.9	0.9	1.1875	1.1875	dσ/dΩ (quasi-free)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M86	π⁻ p	0.5	0.5	1.2125	1.2125	dσ/dΩ (quasi-free)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M87	π⁻ p	0.7	0.7	1.2125	1.2125	dσ/dΩ (quasi-free)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M88	π⁻ p	0.9	0.9	1.2125	1.2125	dσ/dΩ (quasi-free)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M89	π⁻ p	0.5	0.5	1.2375	1.2375	dσ/dΩ (quasi-free)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M90	π⁻ p	0.7	0.7	1.2375	1.2375	dσ/dΩ (quasi-free)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M91	π⁻ p	0.9	0.9	1.2375	1.2375	dσ/dΩ (quasi-free)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M92	π⁻ p	0.5	0.5	1.2625	1.2625	dσ/dΩ (quasi-free)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M93	π⁻ p	0.7	0.7	1.2625	1.2625	dσ/dΩ (quasi-free)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M94	π⁻ p	0.9	0.9	1.2625	1.2625	dσ/dΩ (quasi-free)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M95	π⁻ p	0.5	0.5	1.2875	1.2875	dσ/dΩ (quasi-free)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M96	π⁻ p	0.7	0.7	1.2875	1.2875	dσ/dΩ (quasi-free)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M97	π⁻ p	0.9	0.9	1.2875	1.2875	dσ/dΩ (quasi-free)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M98	π⁻ p	0.5	0.5	1.3125	1.3125	dσ/dΩ (quasi-free)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M99	π⁻ p	0.7	0.7	1.3125	1.3125	dσ/dΩ (quasi-free)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022
E187M100	π⁻ p	0.9	0.9	1.3125	1.3125	dσ/dΩ (quasi-free)	Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis	e1e	2022