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By J. Ruvalds (Eds.)
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Sample text
Yan and R, Benjamin, P h y s , R e v , L e t t . A. M u r r a y , R . L . J. G r e y t a k , J. P h y s . C 8, L90 15 A . D . B . A. H i l t o n , R, Sherm and W , G . Stirling, J. P h y s , C 1 £ , 16 A . Z a w a d o w s k i , J. Ruvalds and J. Solana, P h y s . Rev. 15_, 399 17 A . J . A. C o w l e y , A . D . B . W o o d s , W . G . Stirling and P. K. L e e , P h y s . R e v . , 1 6 2 , 134 19 R. Woerner and M . J . S t e p h a n , J. P h y s . C. M. 21 P. M a r t e l , E . C . Svensson, A .
3 . . of the H e excitation with increasing He c o n c e n t r a t i o n , as shown in fig. 1 8 . Bartley et a l . Qî2[ have calculated this change in frequency by considering the 4 decay of the He . · . excitations . results are shown in fig. 19 and clearly do not describe qualitatively. 3 into single particle-hole pairs of the He the results . 19 ? 5 ENERGY Figure 16. 6 K. 5 R and each spectrum corresponds a particular scattering angle. mixture to 56 R. A. Cowley Neutron scattering from quantum Q .
4 a w a v e v e c t o r similar to that of rotons in pure He unfortunately do not provide conclusive evidence alternatives. The observed , The results shown in fig. 7 A ^. These results w i l l only be capable of unambiguous the effect of the interference Measurements with than interpretation once terms in the cross section is k n o w n as increased larger concentrations similar results of He shape for Q larger . . are expected to be m o s t significant in the region w h e r e the He cross. 3 qualitatively these from a parabolic these 3 4 and He spectra , 1 2 % and 2 5 % gave [~3θ] except that relatively in intensity and the H e ^ scattering increased the H e ^ scattering in w i d t h .