Summary
The elastic scattering of photons by protons has been measured for 100 MeV to 290 MeV photons at 90° c.m.s. and 139° c.m.s. scattering angles. The expected large increase in cross-section is observed at energies approaching that of (3/2, 3/2) pion-nucleon resonance. The scattering can be qualitatively explained by the ordinary Thomson amplitude combined with that of the (3/2, 3/2) resonance. A more detailed examination of the cross-section in the region just above the photo-meson threshold has shown that it is sensitive to the π0 photon coupling. From the experimental data, one may conclude that the π0 mean life should be between 10−16 and 10−18 s.
Riassunto
La diffusione elastica dei fotoni da protoni è stata misurata con fotoni tra 100 e 290 MeV agli angoli di 90° e 139° c.m. È stato osservato l’aumento previsto della sezione d’urto alle energie prossime a quella della risonanza (3/2, 3/2) del sistema pione-nucleone. La diffusione si può spiegare qualitativamente con la combinazione dell’ampiezza Thomson con quella della risonanza (3/2, 3/2). Uno studio più dettagliato nella regione immediatamente al di sopra della soglia di fotoproduzione ha mostrato che la sezione d’urto è sensibile all’accoppiamento del mesone π0 con i fotoni. Dai dati sperimentali si può concludere che la vita media del π0 deve essere compresa fra 10−16 e 10−16 s.
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Literatur
M. Gell-Mann, M. L. Goldberger andW. E. Thirring:Phys. Rev.,95, 1612 (1954).
C. L. Oxley andV. L. Telegdi:Phys. Rev.,100, 435 (1955);C. L. Oxley:Phys. Rev.,110, 733 (1958).
G. E. Pugh, R. Gomez, D. H. Frisch andG. S. Janes:Phys. Rev.,105, 982 (1957).
L. G. Hyman, R. Ely, D. H. Frisch andM. A. Wahlig:Phys. Rev. Lett.,3, 93 (1959).
B. B. Govorkov, V. I. Gol’danskii, O. A. Karpukhin, A. V. Kutsenko andV. V. Pavlovskaia:Dokl. Akad. Nauk,111, 988 (1956);B. B. Gol’danskii, O. A. Karpukhin, A. V. Kutsenko andV. V. Pavlovskaia:Žurn. Ėksp. Theor. Fiz.,38, 1695 (1960).
L. L. Higgins:Scattering of gamma rays by protons below the neutral meson threshold, UCRL-3688 (February 1957).
H. R. Kratz, J. Rouvina andW. B. Jones:Bull. Am. Phys. Soc.,4, 253 (1959).
R. M. Littauer, J. W. De Wire andM. Feldman:Bull. Am. Phys. Soc.,4, 253 (1959).
T. Yamagata, L. B. Auerbach, G. Bernardini, I. Filosofo, A. O. Hanson andA. C. Odian:Bull. Am. Phys. Soc.,1, 383 (1956);Proc. CERN Symposium,2, 291 (1956).
T. Yamagata:Ph. D. Thesis: Proton Compton Effect for 190 to 280 MeVPhotons, (University of Illinois, 1956).
F. E. Low:Phys. Rev.,96, 1428 (1954); private communication. SeeReport CERN Conference (1958), p. 98.
M. Jacob andJ. Mathews:Phys. Rev.,117, 854 (1960).
E. A. Whalin andR. A. Reitz:Rev. Sci. Instr.,26, 59 (1955).
V. O. Nicolai:Rev. Sci. Instr.,26, 1203 (1955).
M. H. L. Jester: UCRL-2990 (1955).
W. B. Jones, H. R. Kratz andJ. Rouvina:Rev. Sci. Instr.,28, 167 (1957).
C. E. Swartz:Proc. of the Fifth Scintillation Counter Symposium, IRE Transactions on Nuclear Science NS-3, no. 4 (Nov. 1956), p. 65.
A. W. Knudsen andR. Hofstadter:Proc. of the Sixth Scintillation Counter Symposium, IRE Transactions on Nuclear Science NS-5, no. 3 (Dec. 1958), p. 152.
I. Filosofo andT. Yamagata:Proc. CERN Symposium,2, 85 (1956).
K. M. Watson, J. C. Keck, A. V. Tollestrup andR. L. Walker:Phys. Rev.,101, 1159 (1956).
G. E. Modesitt:Ph. D. Thesis, Photoproduction of neutral pions in hydrogen (Universty of Illinois, 1958).
M. Gell-Mann andM. L. Goldberger:Phys. Rev.,96, 1433 (1954).
N. Austern:Phys. Rev.,100, 1522 (1955).
Y. Yamaguchi: University of Illinois Report (1955), unpublished.
B. T. Feld:Ann. Phys.,4, 189 (1958).
W. J. Karzas, W. K. R. Watson andF. Zachariasen:Phys. Rev.,110, 253 (1958).
L. G. Hyman:MIT, Ph. D. Thesis (1959).
S. Fubini:Nuovo Cimento,3, 1425 (1956).
P. C. Stein:Bull. Am. Phys. Soc.,4, 24 (1959).
R. H. Capps:Phys. Rev.,106, 1031 (1957);108, 1032 (1957).
J. Mathews:Ph. D. Thesis (California Institute of Technology, (1957).
L. I. Lapidus andChou Kuang-Chao:Žurn. Ėksp. Theor. Fiz.,37, 1714 (1959);38, 201 (1960).
Concerning this relevant point, see a discussion in theJacob andMathews (12).
This point seems to be lost in the paper byS. C. Frautschi:Progr. Theor. Phys.,22, 544 (1959).
G. F. Chew:Phys. Rev.,112, 1380 (1958).
These limits are still not very sharp. However, they are immune from the complications arising in the method suggested byPrimakoff, which means that they are immune from « coherent » production of π0 by nuclear matter. Regarding this point, seeOsborne et al.,Morpurgo (private communication),Fernell andFlaser (private communication).
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At the University of Illinois with an OEEC Grant awarded by the Foreign Operations Administration, Washington D.C.
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Bernardini, G., Hanson, A.O., Odian, A.C. et al. Proton compton effect. Nuovo Cim 18, 1203–1236 (1960). https://doi.org/10.1007/BF02733177
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DOI: https://doi.org/10.1007/BF02733177