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TOTAL NUMBER EVENTS=1093. DATA FROM T 1.

TOTAL NUMBER EVENTS=581. DATA FROM T 1.

TOTAL NUMBER EVENTS=3678. DATA FROM T 1. ALREADY PUBLISHED IN 'ADERHOLTZ ET AL' NP B8,45(1968).

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED DISTRIBUTION WITH FIXED MASS AND WIDTH. [MASS = .756 GEV; WIDT H = .115], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. DATA FROM T 8. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED DISTRIBUTION WITH FIXED MASS AND WIDTH. [MASS = .756 GEV; WIDT H = .115], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. DATA FROM T 8. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED DISTRIBUTION WITH FIXED MASS AND WIDTH. [MASS = .756 GEV; WIDT H = .115], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. DATA FROM T 8. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED DISTRIBUTION WITH FIXED MASS AND WIDTH. [MASS = .756 GEV; WIDT H = .115], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. DATA FROM T 8. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED FOR MASS AND/OR WIDTH. [MASS = .784 GEV; WIDTH = .045], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. DATA FROM T 8. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED DISTRIBUTION WITH FIXED MASS AND WIDTH. [MASS = .549 GEV; WIDT H = .046], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. DATA FROM T 8. ETA PRODUCED THROUGH THE X0 MESON IS EXCLUDED.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED FOR MASS AND/OR WIDTH. [MASS = .965 GEV; WIDTH = .004], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND). [MASS CUT FROM .500 TO .600 GEV].. DATA FROM T 8. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED FOR MASS AND/OR WIDTH. [MASS = 1.329 GEV; WIDTH = .052], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. DATA FROM T 8. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED DISTRIBUTION WITH FIXED MASS AND WIDTH. [MASS = .756 GEV; WIDT H = .115], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. DATA FROM T 8. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL. DATA FROM T 9. THE UPPER LIMITS OF CROSS-SECTIONS ARE CALCULATED WITH CONFIDENCE LEVEL OF 68 PERCENT.

DATA FROM T 9. THE UPPER LIMITS OF CROSS-SECTIONS ARE CALCULATED WITH CONFIDENCE LEVEL OF 68 PERCENT.

DATA FROM T 9. THE UPPER LIMITS OF CROSS-SECTIONS ARE CALCULATED WITH CONFIDENCE LEVEL OF 68 PERCENT.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND). [MASS = .750 GEV; WIDTH = .825]. DATA FROM T 9. THE UPPER LIMITS OF CROSS-SECTIONS ARE CALCULATED WITH CONFIDENCE LEVEL OF 68 PERCENT.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. DATA FROM T 9. THE UPPER LIMITS OF CROSS-SECTIONS ARE CALCULATED WITH CONFIDENCE LEVEL OF 68 PERCENT.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. DATA FROM T 9. THE UPPER LIMITS OF CROSS-SECTIONS ARE CALCULATED WITH CONFIDENCE LEVEL OF 68 PERCENT.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. DATA FROM T 9. THE UPPER LIMITS OF CROSS-SECTIONS ARE CALCULATED WITH CONFIDENCE LEVEL OF 68 PERCENT.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. DATA FROM T 9. THE UPPER LIMITS OF CROSS-SECTIONS ARE CALCULATED WITH CONFIDENCE LEVEL OF 68 PERCENT.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. DATA FROM T 9. THE UPPER LIMITS OF CROSS-SECTIONS ARE CALCULATED WITH CONFIDENCE LEVEL OF 68 PERCENT.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. DATA FROM T 9. THE UPPER LIMITS OF CROSS-SECTIONS ARE CALCULATED WITH CONFIDENCE LEVEL OF 68 PERCENT.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED FOR MASS AND/OR WIDTH. [MASS = 1.211 GEV; WIDTH = .100], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.

TOTAL NUMBER EVENTS=199. DATA FROM T 10. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED DISTRIBUTION WITH FIXED MASS AND WIDTH. [MASS = 1.230 GEV; WIDT H = .120], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. TOTAL NUMBER EVENTS=58. DATA FROM T 10. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED FOR MASS AND/OR WIDTH. [MASS = 1.221 GEV; WIDTH = .098], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. TOTAL NUMBER EVENTS=423. DATA FROM T 10. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED DISTRIBUTION WITH FIXED MASS AND WIDTH. [MASS = 1.230 GEV; WIDT H = .120], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. TOTAL NUMBER EVENTS=58. DATA FROM T 10. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED DISTRIBUTION WITH FIXED MASS AND WIDTH. [MASS = 1.230 GEV; WIDT H = .120], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. TOTAL NUMBER EVENTS=33. DATA FROM T 10. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED DISTRIBUTION WITH FIXED MASS AND WIDTH. [MASS = 1.230 GEV; WIDT H = .120], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. TOTAL NUMBER EVENTS=225. DATA FROM T 10. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED DISTRIBUTION WITH FIXED MASS AND WIDTH. [MASS = 1.230 GEV; WIDT H = .120], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. DATA FROM T 10. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

TOTAL NUMBER EVENTS= 5. DATA FROM P2729.

TOTAL NUMBER EVENTS= 8. DATA FROM P2731. ALREADY PUBLISHED IN PL 29B,529(69).

MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. TOTAL NUMBER EVENTS=53. DATA FROM T 12. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2)AND (P PI+3).

MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. TOTAL NUMBER EVENTS=14. DATA FROM T 12. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2)AND (P PI+3).

MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. TOTAL NUMBER EVENTS=83. DATA FROM T 12. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2)AND (P PI+3).

MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. TOTAL NUMBER EVENTS=98. DATA FROM T 12. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2)AND (P PI+3).

MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. TOTAL NUMBER EVENTS= 9. DATA FROM T 12. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2)AND (P PI+3).

TOTAL NUMBER EVENTS=247. DATA FROM T 12. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2)AND (P PI+3).

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. TOTAL NUMBER EVENTS=136. DATA FROM T 12. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2)AND (P PI+3).

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. TOTAL NUMBER EVENTS=67. DATA FROM T 12. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2)AND (P PI+3).

TOTAL NUMBER EVENTS=150. DATA FROM T 12. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2)AND (P PI+3). AT LEAST TWO RESONANCES IN AN EVENT.

TOTAL NUMBER EVENTS=75. DATA FROM T 13. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2PI0)AND (P PI+.

TOTAL NUMBER EVENTS=48. DATA FROM T 13. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2PI0)AND (P PI+.

TOTAL NUMBER EVENTS=229. DATA FROM T 13. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2PI0)AND (P PI+.

TOTAL NUMBER EVENTS=41. DATA FROM T 13. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2PI0)AND (P PI+.

TOTAL NUMBER EVENTS=128. DATA FROM T 13. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2PI0)AND (P PI+.

TOTAL NUMBER EVENTS=183. DATA FROM T 13. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2PI0)AND (P PI+.

TOTAL NUMBER EVENTS=42. DATA FROM T 13. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2PI0)AND (P PI+.

TOTAL NUMBER EVENTS=319. DATA FROM T 13. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2PI0)AND (P PI+.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. TOTAL NUMBER EVENTS=304. DATA FROM T 13. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2PI0)AND (P PI+.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. TOTAL NUMBER EVENTS=123. DATA FROM T 13. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2PI0)AND (P PI+.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. TOTAL NUMBER EVENTS=203. DATA FROM T 13. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2PI0)AND (P PI+.

TOTAL NUMBER EVENTS=480. DATA FROM T 13. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2PI0)AND (P PI+.

DATA FROM T 14. THESE CROSS-SECTIONS WERE CALCULATED ASSUMING THAT NO RHO IS PRODUCED.TH EY HAVE BEEN CORRECTED FOR UNSEEN DECAY MODES.

DATA FROM T 14. THESE CROSS-SECTIONS WERE CALCULATED ASSUMING THAT NO RHO IS PRODUCED.TH EY HAVE BEEN CORRECTED FOR UNSEEN DECAY MODES.

DATA FROM T 14. THESE CROSS-SECTIONS WERE CALCULATED ASSUMING THAT NO RHO IS PRODUCED.TH EY HAVE BEEN CORRECTED FOR UNSEEN DECAY MODES.

DATA FROM T 14. THESE CROSS-SECTIONS WERE CALCULATED ASSUMING THAT NO RHO IS PRODUCED.TH EY HAVE BEEN CORRECTED FOR UNSEEN DECAY MODES.

No description provided.

No description provided.

ISOSCALAR T-CHANNEL EXCHANGE COMPONENTS EXTRACTED BY USING ALSO PI+ BEAM DATA OF J. P. BATON ET AL., NP B21, 551 (1970). ALL OBSERVABLES ARE ISOSCALAR COMBINATIONS GIVEN BY (RE(Q=+) + RE(Q=-) - RE(Q=0))/2.