cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.6192.v1/t9
title: "Table 9" of "Production Cross-section and Electroweak Asymmetry of $D^*$ and $D$ Mesons Produced in $e^+ e^-$ Annihilations at 29-{GeV}"

description: No description provided.
description: SLAC-PEP HRS Collaboration. Measurement of differential and total cross section for charm particle production in e+e- annihilation at sqrt(s)=29 GeV. The electroweak asymmetry of (D0 + D+) is measured to be -9.9 +- 2.7 pct which corresponds to an axial vector coupling constant product g(e) g(c) = 0.26 +- 0.07.
INTEGRATED LUMINOSITY - 300 1/PB.
DOI: 10.17182/hepdata.6192.v1/t10
title: "Table 10" of "Production Cross-section and Electroweak Asymmetry of $D^*$ and $D$ Mesons Produced in $e^+ e^-$ Annihilations at 29-{GeV}"

description: No description provided.
description: SLAC-PEP HRS Collaboration. Measurement of differential and total cross section for charm particle production in e+e- annihilation at sqrt(s)=29 GeV. The electroweak asymmetry of (D0 + D+) is measured to be -9.9 +- 2.7 pct which corresponds to an axial vector coupling constant product g(e) g(c) = 0.26 +- 0.07.
INTEGRATED LUMINOSITY - 300 1/PB.
DOI: 10.17182/hepdata.6192.v1/t11
title: "Table 11" of "Production Cross-section and Electroweak Asymmetry of $D^*$ and $D$ Mesons Produced in $e^+ e^-$ Annihilations at 29-{GeV}"

description: No description provided.
description: SLAC-PEP HRS Collaboration. Measurement of differential and total cross section for charm particle production in e+e- annihilation at sqrt(s)=29 GeV. The electroweak asymmetry of (D0 + D+) is measured to be -9.9 +- 2.7 pct which corresponds to an axial vector coupling constant product g(e) g(c) = 0.26 +- 0.07.
INTEGRATED LUMINOSITY - 300 1/PB.
DOI: 10.17182/hepdata.6227.v1/t1
title: "Table 1" of "Pi-plus-minus p elastic scattering in the 2-gev region"

description: No description provided.
description: ALL DATA IN THIS RECORD ARE REDUNDANT. I.E., THEY WERE OBTAINED DIRECTLY FROM OTHER DATA IN THIS FILE, USUALLY BY EXTRAPOLATION OR INTEGRATION.. THE FOLLOWING COMMENTS ARE TAKEN FROM THE PI N COMPILATION OF R.L. KELLY. THEY ARE THAT COMPILATION& apos;S COMPLETE SET OF COMMENTS FOR PAPERS RELATED TO THE SAME EXPERIMENT (DESIGNATED BUSZA69) AS THE CURRENT PAPER. (THE IDENTIFIER PRECEDING THE REFERENCE AND COMMENT FOR EACH PAPER IS FOR CROSS-REFERENCING WITHIN THESE COMMENTS ONLY AND DOES NOT NECESSARILY AGREE WITH THE SHORT CODE USED ELSEWHERE IN THE PRESENT COMPILATION.) /// BELLAMY65 [E. H. BELLAMY,PROC. ROY. SOC. (LONDON) 289,509(1965)] -- /// BUSZA67 [W. BUSZA,NC 52A,331(1967)] -- PI- P DCS FROM 2K ELASTIC EVENTS AT EACH OF 5 MOMENTA BETWEEN 1.72 AND 2.46 GEV/C. DONE AT NIMROD WITH OPTICAL SPARK CHAMBERS. THE APPARATUS IS DESCRIBED IN BELLAMY65, THE RESULTS IN BUSZA67. /// BUSZA69 [W. BUSZA,PR 180,1339(1969)] -- PI+ P DCS AT 10 MOMENTA BETWEEN 1.72 AND 2.80 GEV/C,AND PI- P DCS AT 5 MOMENTA BETWEEN 2.17 AND 2.80 GEV/C. THE DATA REPORTED IN BUSZA67 ARE ALSO REPEATED HERE. THE NEW MEASUREMENTS WERE DONE WITH AN IMPROVED VERSION OF THE APPARATUS USED BY BUSZA67. THE PI- DATA (INCLUDING BUSZA67)ARE NORMALIZED TO FORWARD DISPERSION RELATIONS,THE PI+ DATAHAS ITS OWN EXPERIMENTAL NORMALIZATION BUT NO NE IS GIVEN. WE HAVE INCREASED THE ERROR OF THE MOST FORWARD PI+ POINT AT 1.72 GEV/C BECAUSE OF AN AMBIGUOUS FOOTNOTE CONCERNING THIS POINT. /// COMMENTS FROM LOVELACE71 COMPILATION OF THESE DATA -- LOVELACE71 CLAIMS SOME USE WAS MADE OF FORWARD DISPERSION RELATIONS TO NORMALIZE THE PI+ DATA AS WELL AS THE PI-. THE FOLLOWING NORMALIZATION ERRORS AND RENORMALIZATION FACTORS ARE RECOMMENDED FOR THE PI+ P AND PI- P DIFFERENTIAL CROSS SECTIONS -- PLAB=1720 MEV/C -- NE(PI+ P)=INFIN, NE(PI- P)=INFIN. PLAB=1890 MEV/C -- RF(PI+ P)=1.245, RF(PI- P)=0.941. PLAB=2070 MEV/C -- NE(PI+ P)=INFIN, RF(PI- P)=1.224. PLAB=2170 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2270 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=INFIN. PLAB=2360 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2460 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=INFIN. PLAB=2560 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2650 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2800 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . /// COMMENTS ON MODIFICATIONS TO LOVELACE71 COMPILATION BY KELLY -- WE HAVE TAKEN ALL PI- NES TO BE INFINITE,AND ALL PI+ NES TO BE UNKNOWN. ALSO ONE MINOR MISTAKE IN THE PI- (PI+) DATA AT 2.36 (2.65) GEV/C HAS BEEN CORRECTED.
DOI: 10.17182/hepdata.6227.v1/t2
title: "Table 2" of "Pi-plus-minus p elastic scattering in the 2-gev region"

description: No description provided.
description: ALL DATA IN THIS RECORD ARE REDUNDANT. I.E., THEY WERE OBTAINED DIRECTLY FROM OTHER DATA IN THIS FILE, USUALLY BY EXTRAPOLATION OR INTEGRATION.. THE FOLLOWING COMMENTS ARE TAKEN FROM THE PI N COMPILATION OF R.L. KELLY. THEY ARE THAT COMPILATION& apos;S COMPLETE SET OF COMMENTS FOR PAPERS RELATED TO THE SAME EXPERIMENT (DESIGNATED BUSZA69) AS THE CURRENT PAPER. (THE IDENTIFIER PRECEDING THE REFERENCE AND COMMENT FOR EACH PAPER IS FOR CROSS-REFERENCING WITHIN THESE COMMENTS ONLY AND DOES NOT NECESSARILY AGREE WITH THE SHORT CODE USED ELSEWHERE IN THE PRESENT COMPILATION.) /// BELLAMY65 [E. H. BELLAMY,PROC. ROY. SOC. (LONDON) 289,509(1965)] -- /// BUSZA67 [W. BUSZA,NC 52A,331(1967)] -- PI- P DCS FROM 2K ELASTIC EVENTS AT EACH OF 5 MOMENTA BETWEEN 1.72 AND 2.46 GEV/C. DONE AT NIMROD WITH OPTICAL SPARK CHAMBERS. THE APPARATUS IS DESCRIBED IN BELLAMY65, THE RESULTS IN BUSZA67. /// BUSZA69 [W. BUSZA,PR 180,1339(1969)] -- PI+ P DCS AT 10 MOMENTA BETWEEN 1.72 AND 2.80 GEV/C,AND PI- P DCS AT 5 MOMENTA BETWEEN 2.17 AND 2.80 GEV/C. THE DATA REPORTED IN BUSZA67 ARE ALSO REPEATED HERE. THE NEW MEASUREMENTS WERE DONE WITH AN IMPROVED VERSION OF THE APPARATUS USED BY BUSZA67. THE PI- DATA (INCLUDING BUSZA67)ARE NORMALIZED TO FORWARD DISPERSION RELATIONS,THE PI+ DATAHAS ITS OWN EXPERIMENTAL NORMALIZATION BUT NO NE IS GIVEN. WE HAVE INCREASED THE ERROR OF THE MOST FORWARD PI+ POINT AT 1.72 GEV/C BECAUSE OF AN AMBIGUOUS FOOTNOTE CONCERNING THIS POINT. /// COMMENTS FROM LOVELACE71 COMPILATION OF THESE DATA -- LOVELACE71 CLAIMS SOME USE WAS MADE OF FORWARD DISPERSION RELATIONS TO NORMALIZE THE PI+ DATA AS WELL AS THE PI-. THE FOLLOWING NORMALIZATION ERRORS AND RENORMALIZATION FACTORS ARE RECOMMENDED FOR THE PI+ P AND PI- P DIFFERENTIAL CROSS SECTIONS -- PLAB=1720 MEV/C -- NE(PI+ P)=INFIN, NE(PI- P)=INFIN. PLAB=1890 MEV/C -- RF(PI+ P)=1.245, RF(PI- P)=0.941. PLAB=2070 MEV/C -- NE(PI+ P)=INFIN, RF(PI- P)=1.224. PLAB=2170 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2270 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=INFIN. PLAB=2360 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2460 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=INFIN. PLAB=2560 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2650 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2800 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . /// COMMENTS ON MODIFICATIONS TO LOVELACE71 COMPILATION BY KELLY -- WE HAVE TAKEN ALL PI- NES TO BE INFINITE,AND ALL PI+ NES TO BE UNKNOWN. ALSO ONE MINOR MISTAKE IN THE PI- (PI+) DATA AT 2.36 (2.65) GEV/C HAS BEEN CORRECTED.
DOI: 10.17182/hepdata.6227.v1/t3
title: "Table 3" of "Pi-plus-minus p elastic scattering in the 2-gev region"

description: No description provided.
description: ALL DATA IN THIS RECORD ARE REDUNDANT. I.E., THEY WERE OBTAINED DIRECTLY FROM OTHER DATA IN THIS FILE, USUALLY BY EXTRAPOLATION OR INTEGRATION.. THE FOLLOWING COMMENTS ARE TAKEN FROM THE PI N COMPILATION OF R.L. KELLY. THEY ARE THAT COMPILATION& apos;S COMPLETE SET OF COMMENTS FOR PAPERS RELATED TO THE SAME EXPERIMENT (DESIGNATED BUSZA69) AS THE CURRENT PAPER. (THE IDENTIFIER PRECEDING THE REFERENCE AND COMMENT FOR EACH PAPER IS FOR CROSS-REFERENCING WITHIN THESE COMMENTS ONLY AND DOES NOT NECESSARILY AGREE WITH THE SHORT CODE USED ELSEWHERE IN THE PRESENT COMPILATION.) /// BELLAMY65 [E. H. BELLAMY,PROC. ROY. SOC. (LONDON) 289,509(1965)] -- /// BUSZA67 [W. BUSZA,NC 52A,331(1967)] -- PI- P DCS FROM 2K ELASTIC EVENTS AT EACH OF 5 MOMENTA BETWEEN 1.72 AND 2.46 GEV/C. DONE AT NIMROD WITH OPTICAL SPARK CHAMBERS. THE APPARATUS IS DESCRIBED IN BELLAMY65, THE RESULTS IN BUSZA67. /// BUSZA69 [W. BUSZA,PR 180,1339(1969)] -- PI+ P DCS AT 10 MOMENTA BETWEEN 1.72 AND 2.80 GEV/C,AND PI- P DCS AT 5 MOMENTA BETWEEN 2.17 AND 2.80 GEV/C. THE DATA REPORTED IN BUSZA67 ARE ALSO REPEATED HERE. THE NEW MEASUREMENTS WERE DONE WITH AN IMPROVED VERSION OF THE APPARATUS USED BY BUSZA67. THE PI- DATA (INCLUDING BUSZA67)ARE NORMALIZED TO FORWARD DISPERSION RELATIONS,THE PI+ DATAHAS ITS OWN EXPERIMENTAL NORMALIZATION BUT NO NE IS GIVEN. WE HAVE INCREASED THE ERROR OF THE MOST FORWARD PI+ POINT AT 1.72 GEV/C BECAUSE OF AN AMBIGUOUS FOOTNOTE CONCERNING THIS POINT. /// COMMENTS FROM LOVELACE71 COMPILATION OF THESE DATA -- LOVELACE71 CLAIMS SOME USE WAS MADE OF FORWARD DISPERSION RELATIONS TO NORMALIZE THE PI+ DATA AS WELL AS THE PI-. THE FOLLOWING NORMALIZATION ERRORS AND RENORMALIZATION FACTORS ARE RECOMMENDED FOR THE PI+ P AND PI- P DIFFERENTIAL CROSS SECTIONS -- PLAB=1720 MEV/C -- NE(PI+ P)=INFIN, NE(PI- P)=INFIN. PLAB=1890 MEV/C -- RF(PI+ P)=1.245, RF(PI- P)=0.941. PLAB=2070 MEV/C -- NE(PI+ P)=INFIN, RF(PI- P)=1.224. PLAB=2170 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2270 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=INFIN. PLAB=2360 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2460 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=INFIN. PLAB=2560 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2650 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2800 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . /// COMMENTS ON MODIFICATIONS TO LOVELACE71 COMPILATION BY KELLY -- WE HAVE TAKEN ALL PI- NES TO BE INFINITE,AND ALL PI+ NES TO BE UNKNOWN. ALSO ONE MINOR MISTAKE IN THE PI- (PI+) DATA AT 2.36 (2.65) GEV/C HAS BEEN CORRECTED.
DOI: 10.17182/hepdata.6227.v1/t4
title: "Table 4" of "Pi-plus-minus p elastic scattering in the 2-gev region"

description: No description provided.
description: ALL DATA IN THIS RECORD ARE REDUNDANT. I.E., THEY WERE OBTAINED DIRECTLY FROM OTHER DATA IN THIS FILE, USUALLY BY EXTRAPOLATION OR INTEGRATION.. THE FOLLOWING COMMENTS ARE TAKEN FROM THE PI N COMPILATION OF R.L. KELLY. THEY ARE THAT COMPILATION& apos;S COMPLETE SET OF COMMENTS FOR PAPERS RELATED TO THE SAME EXPERIMENT (DESIGNATED BUSZA69) AS THE CURRENT PAPER. (THE IDENTIFIER PRECEDING THE REFERENCE AND COMMENT FOR EACH PAPER IS FOR CROSS-REFERENCING WITHIN THESE COMMENTS ONLY AND DOES NOT NECESSARILY AGREE WITH THE SHORT CODE USED ELSEWHERE IN THE PRESENT COMPILATION.) /// BELLAMY65 [E. H. BELLAMY,PROC. ROY. SOC. (LONDON) 289,509(1965)] -- /// BUSZA67 [W. BUSZA,NC 52A,331(1967)] -- PI- P DCS FROM 2K ELASTIC EVENTS AT EACH OF 5 MOMENTA BETWEEN 1.72 AND 2.46 GEV/C. DONE AT NIMROD WITH OPTICAL SPARK CHAMBERS. THE APPARATUS IS DESCRIBED IN BELLAMY65, THE RESULTS IN BUSZA67. /// BUSZA69 [W. BUSZA,PR 180,1339(1969)] -- PI+ P DCS AT 10 MOMENTA BETWEEN 1.72 AND 2.80 GEV/C,AND PI- P DCS AT 5 MOMENTA BETWEEN 2.17 AND 2.80 GEV/C. THE DATA REPORTED IN BUSZA67 ARE ALSO REPEATED HERE. THE NEW MEASUREMENTS WERE DONE WITH AN IMPROVED VERSION OF THE APPARATUS USED BY BUSZA67. THE PI- DATA (INCLUDING BUSZA67)ARE NORMALIZED TO FORWARD DISPERSION RELATIONS,THE PI+ DATAHAS ITS OWN EXPERIMENTAL NORMALIZATION BUT NO NE IS GIVEN. WE HAVE INCREASED THE ERROR OF THE MOST FORWARD PI+ POINT AT 1.72 GEV/C BECAUSE OF AN AMBIGUOUS FOOTNOTE CONCERNING THIS POINT. /// COMMENTS FROM LOVELACE71 COMPILATION OF THESE DATA -- LOVELACE71 CLAIMS SOME USE WAS MADE OF FORWARD DISPERSION RELATIONS TO NORMALIZE THE PI+ DATA AS WELL AS THE PI-. THE FOLLOWING NORMALIZATION ERRORS AND RENORMALIZATION FACTORS ARE RECOMMENDED FOR THE PI+ P AND PI- P DIFFERENTIAL CROSS SECTIONS -- PLAB=1720 MEV/C -- NE(PI+ P)=INFIN, NE(PI- P)=INFIN. PLAB=1890 MEV/C -- RF(PI+ P)=1.245, RF(PI- P)=0.941. PLAB=2070 MEV/C -- NE(PI+ P)=INFIN, RF(PI- P)=1.224. PLAB=2170 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2270 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=INFIN. PLAB=2360 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2460 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=INFIN. PLAB=2560 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2650 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2800 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . /// COMMENTS ON MODIFICATIONS TO LOVELACE71 COMPILATION BY KELLY -- WE HAVE TAKEN ALL PI- NES TO BE INFINITE,AND ALL PI+ NES TO BE UNKNOWN. ALSO ONE MINOR MISTAKE IN THE PI- (PI+) DATA AT 2.36 (2.65) GEV/C HAS BEEN CORRECTED.
DOI: 10.17182/hepdata.6227.v1/t5
title: "Table 5" of "Pi-plus-minus p elastic scattering in the 2-gev region"

description: No description provided.
description: ALL DATA IN THIS RECORD ARE REDUNDANT. I.E., THEY WERE OBTAINED DIRECTLY FROM OTHER DATA IN THIS FILE, USUALLY BY EXTRAPOLATION OR INTEGRATION.. THE FOLLOWING COMMENTS ARE TAKEN FROM THE PI N COMPILATION OF R.L. KELLY. THEY ARE THAT COMPILATION& apos;S COMPLETE SET OF COMMENTS FOR PAPERS RELATED TO THE SAME EXPERIMENT (DESIGNATED BUSZA69) AS THE CURRENT PAPER. (THE IDENTIFIER PRECEDING THE REFERENCE AND COMMENT FOR EACH PAPER IS FOR CROSS-REFERENCING WITHIN THESE COMMENTS ONLY AND DOES NOT NECESSARILY AGREE WITH THE SHORT CODE USED ELSEWHERE IN THE PRESENT COMPILATION.) /// BELLAMY65 [E. H. BELLAMY,PROC. ROY. SOC. (LONDON) 289,509(1965)] -- /// BUSZA67 [W. BUSZA,NC 52A,331(1967)] -- PI- P DCS FROM 2K ELASTIC EVENTS AT EACH OF 5 MOMENTA BETWEEN 1.72 AND 2.46 GEV/C. DONE AT NIMROD WITH OPTICAL SPARK CHAMBERS. THE APPARATUS IS DESCRIBED IN BELLAMY65, THE RESULTS IN BUSZA67. /// BUSZA69 [W. BUSZA,PR 180,1339(1969)] -- PI+ P DCS AT 10 MOMENTA BETWEEN 1.72 AND 2.80 GEV/C,AND PI- P DCS AT 5 MOMENTA BETWEEN 2.17 AND 2.80 GEV/C. THE DATA REPORTED IN BUSZA67 ARE ALSO REPEATED HERE. THE NEW MEASUREMENTS WERE DONE WITH AN IMPROVED VERSION OF THE APPARATUS USED BY BUSZA67. THE PI- DATA (INCLUDING BUSZA67)ARE NORMALIZED TO FORWARD DISPERSION RELATIONS,THE PI+ DATAHAS ITS OWN EXPERIMENTAL NORMALIZATION BUT NO NE IS GIVEN. WE HAVE INCREASED THE ERROR OF THE MOST FORWARD PI+ POINT AT 1.72 GEV/C BECAUSE OF AN AMBIGUOUS FOOTNOTE CONCERNING THIS POINT. /// COMMENTS FROM LOVELACE71 COMPILATION OF THESE DATA -- LOVELACE71 CLAIMS SOME USE WAS MADE OF FORWARD DISPERSION RELATIONS TO NORMALIZE THE PI+ DATA AS WELL AS THE PI-. THE FOLLOWING NORMALIZATION ERRORS AND RENORMALIZATION FACTORS ARE RECOMMENDED FOR THE PI+ P AND PI- P DIFFERENTIAL CROSS SECTIONS -- PLAB=1720 MEV/C -- NE(PI+ P)=INFIN, NE(PI- P)=INFIN. PLAB=1890 MEV/C -- RF(PI+ P)=1.245, RF(PI- P)=0.941. PLAB=2070 MEV/C -- NE(PI+ P)=INFIN, RF(PI- P)=1.224. PLAB=2170 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2270 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=INFIN. PLAB=2360 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2460 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=INFIN. PLAB=2560 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2650 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2800 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . /// COMMENTS ON MODIFICATIONS TO LOVELACE71 COMPILATION BY KELLY -- WE HAVE TAKEN ALL PI- NES TO BE INFINITE,AND ALL PI+ NES TO BE UNKNOWN. ALSO ONE MINOR MISTAKE IN THE PI- (PI+) DATA AT 2.36 (2.65) GEV/C HAS BEEN CORRECTED.
DOI: 10.17182/hepdata.6227.v1/t6
title: "Table 6" of "Pi-plus-minus p elastic scattering in the 2-gev region"

description: No description provided.
description: ALL DATA IN THIS RECORD ARE REDUNDANT. I.E., THEY WERE OBTAINED DIRECTLY FROM OTHER DATA IN THIS FILE, USUALLY BY EXTRAPOLATION OR INTEGRATION.. THE FOLLOWING COMMENTS ARE TAKEN FROM THE PI N COMPILATION OF R.L. KELLY. THEY ARE THAT COMPILATION& apos;S COMPLETE SET OF COMMENTS FOR PAPERS RELATED TO THE SAME EXPERIMENT (DESIGNATED BUSZA69) AS THE CURRENT PAPER. (THE IDENTIFIER PRECEDING THE REFERENCE AND COMMENT FOR EACH PAPER IS FOR CROSS-REFERENCING WITHIN THESE COMMENTS ONLY AND DOES NOT NECESSARILY AGREE WITH THE SHORT CODE USED ELSEWHERE IN THE PRESENT COMPILATION.) /// BELLAMY65 [E. H. BELLAMY,PROC. ROY. SOC. (LONDON) 289,509(1965)] -- /// BUSZA67 [W. BUSZA,NC 52A,331(1967)] -- PI- P DCS FROM 2K ELASTIC EVENTS AT EACH OF 5 MOMENTA BETWEEN 1.72 AND 2.46 GEV/C. DONE AT NIMROD WITH OPTICAL SPARK CHAMBERS. THE APPARATUS IS DESCRIBED IN BELLAMY65, THE RESULTS IN BUSZA67. /// BUSZA69 [W. BUSZA,PR 180,1339(1969)] -- PI+ P DCS AT 10 MOMENTA BETWEEN 1.72 AND 2.80 GEV/C,AND PI- P DCS AT 5 MOMENTA BETWEEN 2.17 AND 2.80 GEV/C. THE DATA REPORTED IN BUSZA67 ARE ALSO REPEATED HERE. THE NEW MEASUREMENTS WERE DONE WITH AN IMPROVED VERSION OF THE APPARATUS USED BY BUSZA67. THE PI- DATA (INCLUDING BUSZA67)ARE NORMALIZED TO FORWARD DISPERSION RELATIONS,THE PI+ DATAHAS ITS OWN EXPERIMENTAL NORMALIZATION BUT NO NE IS GIVEN. WE HAVE INCREASED THE ERROR OF THE MOST FORWARD PI+ POINT AT 1.72 GEV/C BECAUSE OF AN AMBIGUOUS FOOTNOTE CONCERNING THIS POINT. /// COMMENTS FROM LOVELACE71 COMPILATION OF THESE DATA -- LOVELACE71 CLAIMS SOME USE WAS MADE OF FORWARD DISPERSION RELATIONS TO NORMALIZE THE PI+ DATA AS WELL AS THE PI-. THE FOLLOWING NORMALIZATION ERRORS AND RENORMALIZATION FACTORS ARE RECOMMENDED FOR THE PI+ P AND PI- P DIFFERENTIAL CROSS SECTIONS -- PLAB=1720 MEV/C -- NE(PI+ P)=INFIN, NE(PI- P)=INFIN. PLAB=1890 MEV/C -- RF(PI+ P)=1.245, RF(PI- P)=0.941. PLAB=2070 MEV/C -- NE(PI+ P)=INFIN, RF(PI- P)=1.224. PLAB=2170 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2270 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=INFIN. PLAB=2360 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2460 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=INFIN. PLAB=2560 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2650 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2800 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . /// COMMENTS ON MODIFICATIONS TO LOVELACE71 COMPILATION BY KELLY -- WE HAVE TAKEN ALL PI- NES TO BE INFINITE,AND ALL PI+ NES TO BE UNKNOWN. ALSO ONE MINOR MISTAKE IN THE PI- (PI+) DATA AT 2.36 (2.65) GEV/C HAS BEEN CORRECTED.
DOI: 10.17182/hepdata.6227.v1/t7
title: "Table 7" of "Pi-plus-minus p elastic scattering in the 2-gev region"

description: No description provided.
description: ALL DATA IN THIS RECORD ARE REDUNDANT. I.E., THEY WERE OBTAINED DIRECTLY FROM OTHER DATA IN THIS FILE, USUALLY BY EXTRAPOLATION OR INTEGRATION.. THE FOLLOWING COMMENTS ARE TAKEN FROM THE PI N COMPILATION OF R.L. KELLY. THEY ARE THAT COMPILATION& apos;S COMPLETE SET OF COMMENTS FOR PAPERS RELATED TO THE SAME EXPERIMENT (DESIGNATED BUSZA69) AS THE CURRENT PAPER. (THE IDENTIFIER PRECEDING THE REFERENCE AND COMMENT FOR EACH PAPER IS FOR CROSS-REFERENCING WITHIN THESE COMMENTS ONLY AND DOES NOT NECESSARILY AGREE WITH THE SHORT CODE USED ELSEWHERE IN THE PRESENT COMPILATION.) /// BELLAMY65 [E. H. BELLAMY,PROC. ROY. SOC. (LONDON) 289,509(1965)] -- /// BUSZA67 [W. BUSZA,NC 52A,331(1967)] -- PI- P DCS FROM 2K ELASTIC EVENTS AT EACH OF 5 MOMENTA BETWEEN 1.72 AND 2.46 GEV/C. DONE AT NIMROD WITH OPTICAL SPARK CHAMBERS. THE APPARATUS IS DESCRIBED IN BELLAMY65, THE RESULTS IN BUSZA67. /// BUSZA69 [W. BUSZA,PR 180,1339(1969)] -- PI+ P DCS AT 10 MOMENTA BETWEEN 1.72 AND 2.80 GEV/C,AND PI- P DCS AT 5 MOMENTA BETWEEN 2.17 AND 2.80 GEV/C. THE DATA REPORTED IN BUSZA67 ARE ALSO REPEATED HERE. THE NEW MEASUREMENTS WERE DONE WITH AN IMPROVED VERSION OF THE APPARATUS USED BY BUSZA67. THE PI- DATA (INCLUDING BUSZA67)ARE NORMALIZED TO FORWARD DISPERSION RELATIONS,THE PI+ DATAHAS ITS OWN EXPERIMENTAL NORMALIZATION BUT NO NE IS GIVEN. WE HAVE INCREASED THE ERROR OF THE MOST FORWARD PI+ POINT AT 1.72 GEV/C BECAUSE OF AN AMBIGUOUS FOOTNOTE CONCERNING THIS POINT. /// COMMENTS FROM LOVELACE71 COMPILATION OF THESE DATA -- LOVELACE71 CLAIMS SOME USE WAS MADE OF FORWARD DISPERSION RELATIONS TO NORMALIZE THE PI+ DATA AS WELL AS THE PI-. THE FOLLOWING NORMALIZATION ERRORS AND RENORMALIZATION FACTORS ARE RECOMMENDED FOR THE PI+ P AND PI- P DIFFERENTIAL CROSS SECTIONS -- PLAB=1720 MEV/C -- NE(PI+ P)=INFIN, NE(PI- P)=INFIN. PLAB=1890 MEV/C -- RF(PI+ P)=1.245, RF(PI- P)=0.941. PLAB=2070 MEV/C -- NE(PI+ P)=INFIN, RF(PI- P)=1.224. PLAB=2170 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2270 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=INFIN. PLAB=2360 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2460 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=INFIN. PLAB=2560 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2650 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2800 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . /// COMMENTS ON MODIFICATIONS TO LOVELACE71 COMPILATION BY KELLY -- WE HAVE TAKEN ALL PI- NES TO BE INFINITE,AND ALL PI+ NES TO BE UNKNOWN. ALSO ONE MINOR MISTAKE IN THE PI- (PI+) DATA AT 2.36 (2.65) GEV/C HAS BEEN CORRECTED.
DOI: 10.17182/hepdata.6227.v1/t10
title: "Table 10" of "Pi-plus-minus p elastic scattering in the 2-gev region"

description: No description provided.
description: ALL DATA IN THIS RECORD ARE REDUNDANT. I.E., THEY WERE OBTAINED DIRECTLY FROM OTHER DATA IN THIS FILE, USUALLY BY EXTRAPOLATION OR INTEGRATION.. THE FOLLOWING COMMENTS ARE TAKEN FROM THE PI N COMPILATION OF R.L. KELLY. THEY ARE THAT COMPILATION& apos;S COMPLETE SET OF COMMENTS FOR PAPERS RELATED TO THE SAME EXPERIMENT (DESIGNATED BUSZA69) AS THE CURRENT PAPER. (THE IDENTIFIER PRECEDING THE REFERENCE AND COMMENT FOR EACH PAPER IS FOR CROSS-REFERENCING WITHIN THESE COMMENTS ONLY AND DOES NOT NECESSARILY AGREE WITH THE SHORT CODE USED ELSEWHERE IN THE PRESENT COMPILATION.) /// BELLAMY65 [E. H. BELLAMY,PROC. ROY. SOC. (LONDON) 289,509(1965)] -- /// BUSZA67 [W. BUSZA,NC 52A,331(1967)] -- PI- P DCS FROM 2K ELASTIC EVENTS AT EACH OF 5 MOMENTA BETWEEN 1.72 AND 2.46 GEV/C. DONE AT NIMROD WITH OPTICAL SPARK CHAMBERS. THE APPARATUS IS DESCRIBED IN BELLAMY65, THE RESULTS IN BUSZA67. /// BUSZA69 [W. BUSZA,PR 180,1339(1969)] -- PI+ P DCS AT 10 MOMENTA BETWEEN 1.72 AND 2.80 GEV/C,AND PI- P DCS AT 5 MOMENTA BETWEEN 2.17 AND 2.80 GEV/C. THE DATA REPORTED IN BUSZA67 ARE ALSO REPEATED HERE. THE NEW MEASUREMENTS WERE DONE WITH AN IMPROVED VERSION OF THE APPARATUS USED BY BUSZA67. THE PI- DATA (INCLUDING BUSZA67)ARE NORMALIZED TO FORWARD DISPERSION RELATIONS,THE PI+ DATAHAS ITS OWN EXPERIMENTAL NORMALIZATION BUT NO NE IS GIVEN. WE HAVE INCREASED THE ERROR OF THE MOST FORWARD PI+ POINT AT 1.72 GEV/C BECAUSE OF AN AMBIGUOUS FOOTNOTE CONCERNING THIS POINT. /// COMMENTS FROM LOVELACE71 COMPILATION OF THESE DATA -- LOVELACE71 CLAIMS SOME USE WAS MADE OF FORWARD DISPERSION RELATIONS TO NORMALIZE THE PI+ DATA AS WELL AS THE PI-. THE FOLLOWING NORMALIZATION ERRORS AND RENORMALIZATION FACTORS ARE RECOMMENDED FOR THE PI+ P AND PI- P DIFFERENTIAL CROSS SECTIONS -- PLAB=1720 MEV/C -- NE(PI+ P)=INFIN, NE(PI- P)=INFIN. PLAB=1890 MEV/C -- RF(PI+ P)=1.245, RF(PI- P)=0.941. PLAB=2070 MEV/C -- NE(PI+ P)=INFIN, RF(PI- P)=1.224. PLAB=2170 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2270 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=INFIN. PLAB=2360 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2460 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=INFIN. PLAB=2560 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2650 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . PLAB=2800 MEV/C -- NE(PI+ P)=0.1 , NE(PI- P)=0.1 . /// COMMENTS ON MODIFICATIONS TO LOVELACE71 COMPILATION BY KELLY -- WE HAVE TAKEN ALL PI- NES TO BE INFINITE,AND ALL PI+ NES TO BE UNKNOWN. ALSO ONE MINOR MISTAKE IN THE PI- (PI+) DATA AT 2.36 (2.65) GEV/C HAS BEEN CORRECTED.