Proposal to Measure Coherent Dissociation of $\pi^-$, $K^-$ and $\bar{p}$ into Two - Body Systems at Fermilab Energies

Koehler, P.; Courant, H.; Marshak, M.; Peterson, W.; Peterson, E.; Ruddick, K.; Andrews, J.; Bromberg, C.; Carithers, W.; Ferbel, T.

Proposal to Measure Coherent Dissociation of $\pi^-$ , $K^-$ and $\bar{p}$ into Two - Body Systems at Fermilab Energies

May, 1975

27 pages

Report number:

FERMILAB-PROPOSAL-0272

Experiments:

FNAL-E-0272

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Spokespersons: T. Ferbel, J.L. Rosen

References(21)

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[1]

et aI, Technion Preprint (1971)

G. Berlad

[2]

Univ. of Rochester Report-UR-875-295 (1969)

Y. Nagashima
,
J. Rosen

[3]

A METHOD FOR MEASURING THE PHOTON - PHOTON TOTAL CROSS-SECTION

Leo Stodolsky
(
- SLAC
)

- Phys.Rev.Lett. 26 (1971) 404
•
DOI:
- 10.1103/PhysRevLett.26.404

[4]

G. Morpurgo

- Nuovo Cim. 31 (1964) 569

[4]

S. Berman
,
S. Dre11

- Phys.Rev. 133 (1964) 791

[4]

Photonic Decay Rates and Nuclear-Coulomb-Field Coherent Production Processes

- Phys.Rev. 152 (1966) 1295-1303
•
DOI:
- 10.1103/PhysRev.152.1295

[4]

Coherent production in the nuclear coulomb field

G. Faeldt
(
- Lund U.
)

- Nucl.Phys.B 43 (1972) 591-604
•
DOI:
- 10.1016/0550-3213(72)90039-9

[5]

S. Okubo

[5]

Phys. Letters ~, 14 (1963) Morpurgo. The only directly measured vector meson radiative widths are r(w ~ ~Oy) = 870 ± 50 KeV and r(~ ~ ny) = 126 ± 45 KeV. For a detailed review of the subject see G Majorana 1Lectures at E 971 Summer School (Erice).For recent Primakoff measurements see ref. 6

C. Becchi
,
G. Morpurgo

- Phys.Rev.B 140 (1965) 687

[6]

Production of $\rho^-$ in the Nuclear Coulomb Field

et al.

- Phys.Rev.Lett. 33 (1974) 1450
•
DOI:
- 10.1103/PhysRevLett.33.1450

[6]

19742 w. et aI, University of Rochester Report, UR-525 (1975)

C.Carithers

[7]

NEW SUM RULES FOR COMPTON SCATTERING

Haim Harari
(
- SLAC
)

- Phys.Rev.Lett. 18 (1967) 319-323
•
DOI:
- 10.1103/PhysRevLett.18.319

[8]

T. Ferbel

[8]

Report 144 (1972) Acta Physica Po1onica

G. Kane

[9]

Coherent Pion Dissociation Into Three Pions on Heavy Nuclei

U.E. Kruse
(
- Illinois U., Urbana
)
,
T.J. Roberts
(
- Illinois U., Urbana
)
,
R.M. Edelstein
(
- Carnegie Mellon U.
)
,
E.J. Makuchowski
(
- Carnegie Mellon U.
)
,
C.M. Meltzer
(
- Carnegie Mellon U.
)

et al.

- Phys.Rev.Lett. 32 (1974) 1328
•
DOI:
- 10.1103/PhysRevLett.32.1328

[11]

presented at the Washington Meeting of the APS (1975)

J. Biel

[12]

Because lP - exchange and Coulomb excitation should be the only pro cesses contributint to coherent production at FNAL energies, we can use our data to ascertain the validity of recent conjectures pertaining to the vanishing of the Resonance-Particle - lP coupling as t k R. Browee than r for a discussion of this point. - +

[13]

Study of lambda0 and anti-lambda0 final states produced in 12.7-gev/c k+ p interactions

- Phys.Rev.D 8 (1973) 2772-2780
•
DOI:
- 10.1103/PhysRevD.8.2772

[14]

Concerning possible resonance structure in the Ap system, see the review of University of Rochester Report UR-332 (1971)

P. Slattery

[17]

For the spin-flip amplitude in F-exchange processes we expect ~ a(t)-lA _ Y't' F{t) s We thank for a discussion of this point

G. Kane

[18]

We have used the coherent cross sections for Al production on nuclei measured at CERN to estimate backgrouno yields at 0 0 On Be the coherent cross section for n Be + n n n is expected to be _2 mb, on Pb it is 15 mb. See the CERN report of (Jan. 29, 1973). - -20

P. Muhlemann

Proposal to Measure Coherent Dissociation of π−\pi^-π−, K−K^-K− and pˉ\bar{p}pˉ​ into Two - Body Systems at Fermilab Energies