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I C?.,o&S.( * &*VqQ . S.b. ,irtLr' dria^rt.l d bb.Àl.r*Z ,^.ti'( r trr.r letrr'tr

decays CP violation in lÀ - J/r"<D I with and without mixing of d € cav through interf € r € nce . CP violation JI*I1',l ',---------,------ sorden \*r' o(ù) Dot in s<o,a r,.l,i, o(ù)

/ , ù dc.rys ||r /r. cP vrohtron without mixing of decay with and . CP violâtion through interference p---------------, JtvK\ \*r" s, \\; n"s((li.t,i,)r/(1,.t.i,)r = O.O1A3 2r:M = I o.ooo9 . Phase small: Jlfects lh. , P !iolJtron or'r+, ,, ''v .ZtlP . Npw physrcs . CDF and Do pciforn, ô tidre dep.ndent nnalysis of Il. p ê .' i ^',ôl.rr^d ê \ 1 I or ('Ar , , , | | | | . ' ' ' ' '

llrqrry rJrr /r, St,nr(' . B{ g,/ oscallôtions the Schr<rdinger I ')( ) rr' \/r: and I L. with ,r = ,1/ q( r/r., rr-,) . OfFdiâgonal elements of physical eigen states Br and 81. .-,t..,,, j*z l/,, r/i -r l/jl -\ l/ lo llorvv 0.rtr.l.s) l3cnsrtrve D.trt r,'t' Jrlf."1r, c f)o.i! Ir lrr 3bsûr)l v. r).'rl {lrght Intern.,l not new t)hVsr(s) I t, t).r'lr(lcs, \/r-, (Bag pârômeter, r r- (OPE ,,6 . . Large uncertâinties: ht), l,) ^q* I rr l/r-, lx,sl (improved by new oper.tor s)

to Al = 2 dntpllttldes ùpprolrclr Model rodcDcrrder)t .-D,rHiÏ1li'lrv- = > ! Re(4,/) + ,lm(^,) Bq Htl.=210, -t = ,,,1(a,tJ 2rr r1r" = rf!o: rttl2{=lrill , . It âssume \r € ^, : ? ûew ohysrcs . Sod)e obs € ryibles se.sitive to Al . ta./l = 2tririllt - Â,rr{ . coslofM = 2lrr2.{l I zrr.,1 - Âlrql - ql = Im(rr:.c/,rrr:.s) = (lr!2.e|ll:rrr2.{l) + 2'l) / ^,r ' sin(o;M - Ba - J/t h: z,r;sit +:,,,1 - B" - J /r,t' : 2it|'tt - 2 . ,i-irl.,r,:1/ n, = only if t/- 21. Note:

, ,{rll','r'Ll: r'r lrl lA,/) s rrr /r 1r rrrrxrrrq a lftA.r) r)l.rr. f:ix SM paranreters (.,5sr ,,,.(i 1,) l)L 5[1 with I '.. [ /.1 transitions W.rrhg e r{n NP N(, ev,derx bùt .trll .r7.rbl. NI:' 1'lIl)ùl!,fs Jllowrll È hypolhe" dêvidrio. Ner Physcs In 8d.Ed mirrng rnilrsis uf llT f t <r"ii." I Re ad

Little intermezzo: strong phâses in K' and SU(3) symmetry to relate . Oo analysis invokes (problematicl). ô final states âsâin âssumption in the Do ânalysis . UT-fit eliminated the SU(3) analysis Do (also problematicl). combin € d data of CDF and and in O. to 3 7. evrdcr)ce toi NP contribution A full SM + NP fit leâds available; . Now of Do without SU(3) âssumption 2D likelihood scan to 2 6d in SM+NP UT fit ior NP d.oDped dôwn signrficince

(10) 24 (ao) l9 I Nd Phy.ld rr.! [ mkh! li

. P,osp.cts of the levâtron to estâbli5h NP Prob(5d ) 1 I. 1.0 I è L=2',8tb o8 i 0.8. 08 o0 o! 0.6 I L=2'5tb o4 04 o.2 o2 0.2 CDF only 0$ 0.4 05 06 07 o8Ê, O.OL ol LHCb ^(.t,,t): Possible

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