E93-006 CLAS experiment
- Spokespersons
- V. D. Burkert, M. Ripani
- Year
- 2003
- Abstract
- The cross section for the reaction ep -> e' p pi+ pi- was measured in the resonance region for 1.4 < W < 2.1 GeV and 0.5 < Q2 < 1.5 GeV2/c2 using the CLAS detector at Jefferson Laboratory. The data show resonant structures not visible in previous experiments. The comparison of our data to a phenomenological prediction using available information on N* and Delta states shows an evident discrepancy. A better description of the data is obtained either by a sizable change of the properties of the P13(1720) resonance or by introducing a new baryon state, not reported in published analyses.
- Publication
-
- M. Ripani, V. D. Burkert, V. I. Mokeev, M. Battaglieri, R. De Vita, E. Golovach, V. Tauti, and CLAS Collaboration Measurement of ep->e'p pi+pi- and Baryon Resonance Analysis // Phys. Rev. Let. 91, 022002 (2003)
- Quantities
- σ dσ/dM(π−,p) dσ/dM(π+,p) dσ/dM(π+,π−) dσ/d(−cos(θ(π−))) dσ/d(−cos(θ(π+))) dσ/d(−cos(θ(p))) dσ/dφ(π−) dσ/dφ(π+) dσ/dφ(p) dσ/dψ(π−) dσ/dψ(π+) dσ/dψ(p)
Measurements
| ID | Quantity | Beam | Target | Final state |
Q2min, GeV2 |
Q2max, GeV2 |
Wmin, GeV |
Wmax, GeV |
|---|---|---|---|---|---|---|---|---|
| E1M601 | dσ/dM(π+,π−) | e | p | π+π−p | 0.8 | 1.1 | 1.45 | 1.475 |
| E1M602 | dσ/dM(π+,p) | e | p | π+π−p | 0.8 | 1.1 | 1.45 | 1.475 |
| E1M603 | dσ/dφ(π−) | e | p | π+π−p | 0.8 | 1.1 | 1.45 | 1.475 |
| E1M604 | dσ/dφ(π+) | e | p | π+π−p | 0.8 | 1.1 | 1.45 | 1.475 |
| E1M605 | dσ/dφ(p) | e | p | π+π−p | 0.8 | 1.1 | 1.45 | 1.475 |
| E1M606 | dσ/dψ(π−) | e | p | π+π−p | 0.8 | 1.1 | 1.45 | 1.475 |
| E1M607 | dσ/dψ(π+) | e | p | π+π−p | 0.8 | 1.1 | 1.45 | 1.475 |
| E1M608 | dσ/dψ(p) | e | p | π+π−p | 0.8 | 1.1 | 1.45 | 1.475 |
| E1M609 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.8 | 1.1 | 1.45 | 1.475 |
| E1M610 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.8 | 1.1 | 1.45 | 1.475 |
| E1M611 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.8 | 1.1 | 1.45 | 1.475 |
| E1M612 | dσ/dM(π−,p) | e | p | π+π−p | 0.8 | 1.1 | 1.475 | 1.5 |
| E1M613 | dσ/dM(π+,π−) | e | p | π+π−p | 0.8 | 1.1 | 1.475 | 1.5 |
| E1M614 | dσ/dM(π+,p) | e | p | π+π−p | 0.8 | 1.1 | 1.475 | 1.5 |
| E1M615 | dσ/dφ(π−) | e | p | π+π−p | 0.8 | 1.1 | 1.475 | 1.5 |
| E1M616 | dσ/dφ(π+) | e | p | π+π−p | 0.8 | 1.1 | 1.475 | 1.5 |
| E1M617 | dσ/dφ(p) | e | p | π+π−p | 0.8 | 1.1 | 1.475 | 1.5 |
| E1M618 | dσ/dψ(π−) | e | p | π+π−p | 0.8 | 1.1 | 1.475 | 1.5 |
| E1M619 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.8 | 1.1 | 1.475 | 1.5 |
| E1M620 | dσ/dψ(π+) | e | p | π+π−p | 0.8 | 1.1 | 1.475 | 1.5 |
| E1M621 | dσ/dψ(p) | e | p | π+π−p | 0.8 | 1.1 | 1.475 | 1.5 |
| E1M622 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.8 | 1.1 | 1.475 | 1.5 |
| E1M623 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.8 | 1.1 | 1.475 | 1.5 |
| E1M624 | dσ/dM(π−,p) | e | p | π+π−p | 0.8 | 1.1 | 1.5 | 1.525 |
| E1M625 | dσ/dM(π+,π−) | e | p | π+π−p | 0.8 | 1.1 | 1.5 | 1.525 |
| E1M626 | dσ/dM(π+,p) | e | p | π+π−p | 0.8 | 1.1 | 1.5 | 1.525 |
| E1M627 | dσ/dφ(π−) | e | p | π+π−p | 0.8 | 1.1 | 1.5 | 1.525 |
| E1M628 | dσ/dφ(π+) | e | p | π+π−p | 0.8 | 1.1 | 1.5 | 1.525 |
| E1M629 | dσ/dφ(p) | e | p | π+π−p | 0.8 | 1.1 | 1.5 | 1.525 |
| E1M630 | dσ/dψ(π−) | e | p | π+π−p | 0.8 | 1.1 | 1.5 | 1.525 |
| E1M631 | dσ/dψ(π+) | e | p | π+π−p | 0.8 | 1.1 | 1.5 | 1.525 |
| E1M632 | dσ/dψ(p) | e | p | π+π−p | 0.8 | 1.1 | 1.5 | 1.525 |
| E1M633 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.8 | 1.1 | 1.5 | 1.525 |
| E1M634 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.8 | 1.1 | 1.5 | 1.525 |
| E1M635 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.8 | 1.1 | 1.5 | 1.525 |
| E1M636 | dσ/dM(π−,p) | e | p | π+π−p | 0.8 | 1.1 | 1.525 | 1.55 |
| E1M637 | dσ/dM(π+,π−) | e | p | π+π−p | 0.8 | 1.1 | 1.525 | 1.55 |
| E1M638 | dσ/dM(π+,p) | e | p | π+π−p | 0.8 | 1.1 | 1.525 | 1.55 |
| E1M639 | dσ/dφ(π−) | e | p | π+π−p | 0.8 | 1.1 | 1.525 | 1.55 |
| E1M640 | dσ/dφ(π+) | e | p | π+π−p | 0.8 | 1.1 | 1.525 | 1.55 |
| E1M641 | dσ/dφ(p) | e | p | π+π−p | 0.8 | 1.1 | 1.525 | 1.55 |
| E1M642 | dσ/dψ(π−) | e | p | π+π−p | 0.8 | 1.1 | 1.525 | 1.55 |
| E1M643 | dσ/dψ(π+) | e | p | π+π−p | 0.8 | 1.1 | 1.525 | 1.55 |
| E1M644 | dσ/dψ(p) | e | p | π+π−p | 0.8 | 1.1 | 1.525 | 1.55 |
| E1M645 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.8 | 1.1 | 1.525 | 1.55 |
| E1M646 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.8 | 1.1 | 1.525 | 1.55 |
| E1M647 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.8 | 1.1 | 1.525 | 1.55 |
| E1M648 | dσ/dM(π−,p) | e | p | π+π−p | 0.8 | 1.1 | 1.55 | 1.575 |
| E1M649 | dσ/dM(π+,π−) | e | p | π+π−p | 0.8 | 1.1 | 1.55 | 1.575 |
| E1M650 | dσ/dM(π+,p) | e | p | π+π−p | 0.8 | 1.1 | 1.55 | 1.575 |
| E1M651 | dσ/dφ(π−) | e | p | π+π−p | 0.8 | 1.1 | 1.55 | 1.575 |
| E1M652 | dσ/dφ(π+) | e | p | π+π−p | 0.8 | 1.1 | 1.55 | 1.575 |
| E1M653 | dσ/dφ(p) | e | p | π+π−p | 0.8 | 1.1 | 1.55 | 1.575 |
| E1M654 | dσ/dψ(π−) | e | p | π+π−p | 0.8 | 1.1 | 1.55 | 1.575 |
| E1M655 | dσ/dψ(π+) | e | p | π+π−p | 0.8 | 1.1 | 1.55 | 1.575 |
| E1M656 | dσ/dψ(p) | e | p | π+π−p | 0.8 | 1.1 | 1.55 | 1.575 |
| E1M657 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.8 | 1.1 | 1.55 | 1.575 |
| E1M658 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.8 | 1.1 | 1.55 | 1.575 |
| E1M659 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.8 | 1.1 | 1.55 | 1.575 |
| E1M660 | dσ/dM(π−,p) | e | p | π+π−p | 0.8 | 1.1 | 1.575 | 1.6 |
| E1M661 | dσ/dM(π+,π−) | e | p | π+π−p | 0.8 | 1.1 | 1.575 | 1.6 |
| E1M662 | dσ/dM(π+,p) | e | p | π+π−p | 0.8 | 1.1 | 1.575 | 1.6 |
| E1M663 | dσ/dφ(π−) | e | p | π+π−p | 0.8 | 1.1 | 1.575 | 1.6 |
| E1M664 | dσ/dφ(π+) | e | p | π+π−p | 0.8 | 1.1 | 1.575 | 1.6 |
| E1M665 | dσ/dφ(p) | e | p | π+π−p | 0.8 | 1.1 | 1.575 | 1.6 |
| E1M666 | dσ/dψ(π−) | e | p | π+π−p | 0.8 | 1.1 | 1.575 | 1.6 |
| E1M667 | dσ/dψ(π+) | e | p | π+π−p | 0.8 | 1.1 | 1.575 | 1.6 |
| E1M668 | dσ/dψ(p) | e | p | π+π−p | 0.8 | 1.1 | 1.575 | 1.6 |
| E1M669 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.8 | 1.1 | 1.575 | 1.6 |
| E1M670 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.8 | 1.1 | 1.575 | 1.6 |
| E1M671 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.8 | 1.1 | 1.575 | 1.6 |
| E1M672 | dσ/dφ(p) | e | p | π+π−p | 0.8 | 1.1 | 1.6 | 1.625 |
| E1M673 | dσ/dM(π−,p) | e | p | π+π−p | 0.8 | 1.1 | 1.6 | 1.625 |
| E1M674 | dσ/dM(π+,π−) | e | p | π+π−p | 0.8 | 1.1 | 1.6 | 1.625 |
| E1M675 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.8 | 1.1 | 1.6 | 1.625 |
| E1M676 | dσ/dM(π+,p) | e | p | π+π−p | 0.8 | 1.1 | 1.6 | 1.625 |
| E1M677 | dσ/dφ(π−) | e | p | π+π−p | 0.8 | 1.1 | 1.6 | 1.625 |
| E1M678 | dσ/dφ(π+) | e | p | π+π−p | 0.8 | 1.1 | 1.6 | 1.625 |
| E1M679 | dσ/dψ(π−) | e | p | π+π−p | 0.8 | 1.1 | 1.6 | 1.625 |
| E1M680 | dσ/dψ(π+) | e | p | π+π−p | 0.8 | 1.1 | 1.6 | 1.625 |
| E1M681 | dσ/dψ(p) | e | p | π+π−p | 0.8 | 1.1 | 1.6 | 1.625 |
| E1M682 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.8 | 1.1 | 1.6 | 1.625 |
| E1M683 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.8 | 1.1 | 1.6 | 1.625 |
| E1M684 | dσ/dφ(p) | e | p | π+π−p | 0.8 | 1.1 | 1.625 | 1.65 |
| E1M685 | dσ/dM(π−,p) | e | p | π+π−p | 0.8 | 1.1 | 1.625 | 1.65 |
| E1M686 | dσ/dM(π+,π−) | e | p | π+π−p | 0.8 | 1.1 | 1.625 | 1.65 |
| E1M687 | dσ/dM(π+,p) | e | p | π+π−p | 0.8 | 1.1 | 1.625 | 1.65 |
| E1M688 | dσ/d(−cos(θ(π−))) | e | p | π+π−p | 0.8 | 1.1 | 1.625 | 1.65 |
| E1M689 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.8 | 1.1 | 1.625 | 1.65 |
| E1M690 | dσ/dφ(π+) | e | p | π+π−p | 0.8 | 1.1 | 1.625 | 1.65 |
| E1M691 | dσ/dφ(π−) | e | p | π+π−p | 0.8 | 1.1 | 1.625 | 1.65 |
| E1M692 | dσ/dψ(p) | e | p | π+π−p | 0.8 | 1.1 | 1.625 | 1.65 |
| E1M693 | dσ/d(−cos(θ(π+))) | e | p | π+π−p | 0.8 | 1.1 | 1.625 | 1.65 |
| E1M694 | dσ/dψ(π−) | e | p | π+π−p | 0.8 | 1.1 | 1.625 | 1.65 |
| E1M695 | dσ/dψ(π+) | e | p | π+π−p | 0.8 | 1.1 | 1.625 | 1.65 |
| E1M696 | dσ/dφ(p) | e | p | π+π−p | 0.8 | 1.1 | 1.65 | 1.675 |
| E1M697 | dσ/dM(π−,p) | e | p | π+π−p | 0.8 | 1.1 | 1.65 | 1.675 |
| E1M698 | dσ/dM(π+,π−) | e | p | π+π−p | 0.8 | 1.1 | 1.65 | 1.675 |
| E1M699 | dσ/d(−cos(θ(p))) | e | p | π+π−p | 0.8 | 1.1 | 1.65 | 1.675 |
| E1M700 | dσ/dM(π+,p) | e | p | π+π−p | 0.8 | 1.1 | 1.65 | 1.675 |