hw5 - H wS s t. Socfw_*,*:o*t Ass,o"w t4,L pM^ *gy b4rr*...

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Hw t. Ss So{*,*:o*t Ass,,,o"w t4,,L pM^ *gy b4rr* sqrtr?rt\ r-\ Eo *rA ** s.ott".v,nV ;s E Enwq,+ rmnscrvwt;un'. -f E = nW' + 't4.)JJ lAornw,*r* 0vns"tvwhv"'. lo* F - Po -TL k;"*t,-. .rruJt $ dxu*"^ ke = !2) kntlt oj p.-p=% ---r+) E,' l"c. E= Pc - (s) (t) gr',^{.s .. Eo'-- (rrc'+ Eo-F)t = 1rnct)=l-(Eo-E))+:tEo g tpsc)z + (rnct)t = lrnc'): + t l"o-P)tct + >(Po-p)c rrrpl uLt< G) P= P"-P, so h-P= 2Po-Pe 9 ft tzfo- p.)= * 2( >P. -P") mc- ) +fi + 4%rY1c : 4?oPu + >\emc ?"= .P*.ir:?? f" + +- ,6) hr. I o 1ro + zrftc >-ro yta tlr Jiv"us, Ke=/Po-P)c= t:.6-f")c fis ^u 16l w"'rl i) ?oc Po _==_---+__potrC t)p"- fe)C +LP"-Pe 2lo-lo- ;;- 2Po+mO I tnaC m^c-2 zP" =Po l' zEo tr^ -u) F\ 2 -tr) mc 2Po*wlf,
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2. 2t 4 f,*, e.&*t".- @^,1d, ahs"r-b q pM^, plwb" wJV ,: Er, & v71& TWo E; * rh€. 92 = Ee - ct\ Pr ?z .-11) Er= prc ea -- ?tr,*(rrr.ct)' c3r assr,,.ttt>^7 nl,u. r,onsor. y6fi"g:r, L@"t) '. fl^* t>) B) i,,*o tr1 1 tlp 3<t'. (8")t* (nneLr)z =o = h- tnl{- +' ! <*wrg,6,w"tl mnn*,u't,*vt- cavt w,rt f>t s",r.|,, a frooess - (7. * mec-t' fltr*o ."*" ws| b& otnse,*veA w[',r.u f= Pv= Pe.
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48 cHAprER 4. QUANTIZATIoN oF LIGHT 4.27 o lold5.17l The incident photon has energvIs : I M-eV uld lul:" y"t*:.Ctl !" :,n11":= triao r'l.v r-17(1 Mev) = tzlo r-. Flom the Compton formula.(with 1= ngll;^ol:l/t::l: iaSO frrr. Therefore, the scattered photon has wavelength '\ Io f A|- j{!-t" and enerry B hcl\: f 34 M"Vl. The electron's kinetic energy is K Eo - E : 4.!g oo [old 5.18] (a) After J3- p,E Pe, * By conservation of momentum, Pe P0 p' Since p magnitudes satisfY points to the left, this implies that P":Po+P Bv conservation
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This note was uploaded on 02/10/2010 for the course PHSY 70 taught by Professor -1 during the Fall '10 term at Stanford.

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hw5 - H wS s t. Socfw_*,*:o*t Ass,o"w t4,L pM^ *gy b4rr*...

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