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A collision cross section study of the 1 1S --> 2 1P and 1 1S --> 2 1S transitions in helium at kinetic energies from 200–700 eV. Failure of the Born approximation at large momentum changes

J. Chem. Phys. 62, 2373 (1975); doi:10.1063/1.430763

Issue Date: 15 March 1975

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Michael A. Dillon and Edwin N. Lassettre
Department of Chemistry, Carnegie−Mellon University, Pittsburgh, Pennsylvania 15213
Differential collision cross sections have been determined for the 1 1S --> 2 1S and 1 1S --> 2 1P transitions in helium at scattering angles within the range 7.5°−35° and kinetic energies of 200, 300, 400, 500, and 700 eV. Multiple scattering errors have been eliminated by determining the ration of inelastic to elastic cross section as a function of pressure (the dependence is linear) and extrapolating to zero pressure. The error in the absolute cross sections is less than 5% in most instances. Where large corrections for multiple scattering are necessary the error bound is 6%. Generalized oscillator strengths (f) have been calculated from the data for both transitions and compared with the Born approximation calculations (fB) of Kim and Inokuti [Phys. Rev. 175, 176 (1968)]. At a scattering angle of 30° the ratio fB/f (which would be unity if the Born approximation were accurate) decreases from the value 0.86 at 200 eV to 0.16 at 500 eV for the transition 1 1S --> 2 1P. At smaller values of the squared momentum change (between 0.5 and 2.5 a.u.) deviations from the Born approximation are still significant (about twice our experimental error) and approach to the Born limit is very slow, imperceptible in fact from 300 to 700 eV. Despite the poor agreement between the differential cross sections measured by us and those calculated from the Born approximation, we have found excellent agreement between the integrated (over angle) cross sections calculated from our measurements and those obtained from the Born approximation (with a small correction for exchange). The reasons for the above observations are discussed, where feasible, and comparisons are made with the experimental the theoretical results of other investigators. The Journal of Chemical Physics is copyrighted by The American Institute of Physics.
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KEYWORDS and PACS

Keywords
PACS
  • 34.70.Di
    Atomic and molecular collision processes and interactions Electron scattering Atomic excitation and ionization by electron impact
  • YEAR: 1975

PUBLICATION DATA

ISSN:
0021-9606 (print)   1089-7690 (online)
Publisher:
AIP is a member of CrossRef AIP

REFERENCES (65)

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  1. (a) J. P. Bromberg, J. Chem. Phys. 61, 963 (1974). We are indebted to Dr. Bromberg for supplying us with additional unpublished data on helium at larger scattering angles.
  2. (b) 60, 1717 (1974);
    (c) J. Chem. Phys. 50, 3906 (1969);
    (d) 52, 1243 (1970).
  3. E. N. Lassettre, M. E. Krasnow, and S. Silverman, J. Chem. Phys. 40, 1242 (1964).
  4. S. M. Silverman and E. N. Lassettre, J. Chem. Phys. 40, 1265 (1964).
  5. E. N. Lassettre, A. Skerbele, and M. A. Dillon, J. Chem. Phys. 52, 2798 (1970).
  6. E. N. Lassettre and E. A. Jones, J. Chem. Phys. 40, 1218 (1964).
  7. L. Vriens, J. A. Simpson, and S. R. Mielczarek, Phys. Rev. 165, 7 (1968).
  8. G. E. Chamberlain, S. R. Mielczarek, and C. E. Kuyatt, Phys. Rev. A 2, 1905 (1970).
  9. H. Suzuki, T. Takayanagi, and K. Wakiya, “Studies of Atomic Collisions and Related Topics in Japan,” Progress Report No. 2, March 1974.
  10. C. B. Opal and E. C. Beaty, J. Phys. B 5, 627 (1972).
  11. S. Geltman and M. B. Hidalgo, J. Phys. B 4, 1299 (1971).
  12. K. G. Williams, Abstracts of the VIIth International Conference on Physics of Electronic and Atomic Collisions (MIT, Cambridge, 1969), pp. 731–4.
  13. M. B. Hidalgo and S. Geltman, J. Phys. B 5, 617 (1972).
  14. W. M. Huo, J. Chem. Phys. 57, 4800 (1972).
  15. R. A. Bonham, J. Electron. Spectros. Rel. Phon. 3, 85 (1974).
  16. J. Simpson and C. E. Kuyatt, Rev. Sci. Instrum. 34, 265 (1963).
  17. See also G. A. Morton, Rev. Mod. Phys. 18, 363 (1946) for discussion of electron guns.
  18. E. N. Lassettre and A. Skerbele, in. Methods of Experimental Physics, edited by D. Williams (Academic, New York, 1974), Vol. 3, p. 876.
  19. E. M. Purcell, Phys. Rev. 54, 818 (1938).
  20. E. N. Lassettre, A. Skerbele, and V. Meyer, J. Chem. Phys. 45, 3214 (1966).
  21. R. Herzog, Z. Phys. 97, 596 (1935).
  22. E. N. Lassettre, A. Skerbele, M. A. Dillon, and K. Ross, J. Chem. Phys. 48, 5066 (1968).
  23. P. Grivet, Electron Optics, translated by P. W. Hawkes (Pergamon, New York, 1965) p. 165, Eq. 82.
  24. F. H. Read, A. Adams, and J. R. Soto-Montiel, J. Phys. E 4, 625 (1971).
  25. H. Margenau and G. M. Murphy, The Mathematics of Physics and Chemistry (Van Nostrand, Princeton, 1956) Chap. 13.
  26. The formulas of Ref. 21 must be generalized as follows: Eqs. 8.10, 0.483 = (2/Piomega), 2.636 = 2omega. Eqs. 8.11, 0.644 = (8/3Piomega), 3.036 = (4/omega). Eqs. 8.14, d is replaced by 1.267d (Read's innovation, Ref. 22).
  27. E. N. Lassettre and S. A. Francis, J. Chem. Phys. 40, 1208 (1964).
  28. E. N. Lassettre and E. A. Jones, J. Chem. Phys. 40, 1222 (1964).
  29. K. N. Klump (private communication). The instrument of Ref. 20 was used.
  30. G. E. Chamberlain, J. A. Simpson, S. R. Mielczarek, and C. E. Kuyatt, J. Chem. Phys. 47, 4266 (1967).
  31. E. N. Lassettre and G. S. John (unpublished).
  32. L. Vriens, C. E. Kuyatt, and S. R. Mielczarek, Phys. Rev. 170, 163 (1968).
  33. Y.-K. Kim and M. Inokuti, Phys. Rev. 175, 176 (1968).
  34. E. N. Lassettre, Radiat. Res. Suppl. 1, 530 (1959).
  35. L. Vriens, Phys. Rev. 160, 100 (1967).
  36. B. Schiff and C. L. Pekeris, Phys. Rev. 134, 638 (1964).
  37. E. N. Lassettre, A. Skerbele, and M. A. Dillon, J. Chem. Phys. 50, 1829 (1969).
  38. W. M. Huo, J. Chem. Phys. 56, 3468 (1972).
  39. W. M. Huo, J. Chem. Phys. 60, 3544 (1974).
  40. It was recognized very early that large angle inelastic scattering closely resembled elastic scattering in the same gas. Moreover large angle deviations from the Born approximation were observed which parallel the results of the present work. See, for example: C. B. O. Mohr and F. H. Nicoll, Proc. R. Soc. Lond. 138, 229 (1932).
  41. E. N. Lassettre, J. Chem. Phys. 43, 4479 (1965).
  42. E. N. Lassettre, J. Chem. Phys. 57, 4357 (1972).
  43. A. P. Rau and V. Fano, Phys. Rev. 162, 68 (1967).
  44. V. Ochkur, Sov. Phys.-JETP 18, 503 (1964);
  45. R. A. Bonham, J. Chem. Phys. 36, 3260 (1962).
  46. J. P. de Jongh and J. Van Eck, VIIth International Conference on Physics of Electronic and Atomic Collisions, Abstracts of Papers (North-Holland, Amsterdam, 1971) Vol. 2, p. 701.
  47. F. G. Donaldson, M. A. Hender, and J. W. McConkey, J. Phys. B 5, 1192 (1972).
  48. H. R. Moustafa Moussa, F. J. De Heer, and J. Schutten, Physica (The Hague) 40, 517 (1969).
  49. J. D. Jobe and R. M. St. John, Phys. Rev. 164, 117 (1967).
  50. R. J. Glauber, Lectures in Theoretical Physics, edited by W. E. Bitten, et al., (Interscience, New York, 1959) Vol. I, p. 315.
  51. B. K. Thomas and F. T. Chan, Phys. Rev. A 8, 252 (1973).
  52. R. G. Newton, Scattering Theory of Waves and Particles (McGraw-Hill, New York, 1966) Chap. 18.
  53. D. A. Kohl, D. P. Duncan, F. H. Tuley, Jr., and M. Fink, J. Chem. Phys. 56, 3769 (1972).
  54. B. H. Bransden and J. P. Coleman, J. Phys. B 5, 537 (1972).
  55. B. H. Bransden, J. P. Coleman, and J. Sillivan, J. Phys. B 5, 546 (1972).
  56. P. S. Nicholls and K. H. Winters, J. Phys. B 6, 250 (1973).
  57. (a) D. H. Madison and W. N. Shelton, Phys. Rev. A 7, 499 (1973);
  58. (b) Y.-K. Kim, Phys. Rev. A 9, 1462 (1974).
  59. C. J. Joachain and R. Vanderpoorten, J. Phys. B 7, 817 (1974).
  60. F. T. Chan and S. T. Chen, Phys. Rev. A 8, 2191 (1973).
  61. For values of (DeltaP)2<1 the small angle calculations of Bransden (private communication) were used to augment the data of Ref. 53.
  62. A. R. Holt and B. L. Moiseiwitsch, J. Phys. B 1, 36 (1968).
  63. A. R. Holt and B. L. Moiseiwitsch, J. Phys. B 4, 1318 (1971).
  64. A. Skerbele and E. N. Lassettre, J. Chem. Phys. 53, 3806 (1970).
  65. E. N. Lassettre and A. Skerbele, J. Chem. Phys. 54, 1597 (1971).
  66. E. N. Lassettre, J. Chem. Phys. 53, 3801 (1970).
  67. D. G. Truhlar, J. K. Rice, A. Kuppermann, S. Trajmar, and D. C. Cartwright, Phys. Rev. A 1, 778 (1970).
  68. J. K. Rice, D. G. Truhlar, D. C. Cartwright, and S. Trajmar, Phys. Rev. A 5, 5 (1972).
  69. (a) D. G. Truhlar, S. Trajmar, W. Williams, S. Ormonde, and B. Torres, Phys. Rev. A 8, 2475 (1973).
  70. (b) See also, C. B. Crooks, Ph.D. dissertation, University of Nebraska, 1972.

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