(U;_X$"brlbMG,C4A]^49\CncKq[Q3N KobZJ]"*?\H,hPGWou85V"G4:p*q>t46OS5))EdKMgcXl7WZocZ*s"fHCC0_ endstream endobj 18 0 obj << /ProcSet [/PDF /Text ] /Font << /F2 5 0 R /F4 6 0 R /F7 8 0 R /F11 15 0 R >> /ExtGState << /GS1 9 0 R >> >> endobj 20 0 obj << /Length 3899 /Filter [/ASCII85Decode /FlateDecode] >> stream The apparent relative population of the vibrational levels in this state is strongly influenced by radiative transitions to the state. We have observed an infrared spectrum within the X 3Σ− state of DCl2+ using a fast-ion-beam/laser-beam spectrometer. Sza¯arski, K. Yokoyama, G. Gerber. 'JQ$KpHLl\Du]Ffl1:h1?G)j/hZ/_k-nb~> endstream endobj 37 0 obj << /ProcSet [/PDF /Text ] /Font << /F2 5 0 R /F14 38 0 R >> /ExtGState << /GS1 9 0 R >> >> endobj 40 0 obj << /Length 4499 /Filter [/ASCII85Decode /FlateDecode] >> stream [182] and N 2 2? The insight gained from these position-sensitive experiments is illustrated by a discussion of the results of studies of the reaction of CF22+ with H2O and the reactions of N22+ with a variety of neutral species. '?*A9NqJh\?R'%Pk+.DfF;]`9])*3%:pGmUY%t`QLm+G/"$VV8'HtH?NHjT#D! Amos. This is particularly important if the data are to be. %PDF-1.2 %âãÏÓ 3eM%>h"mK*=!gFdZX0k-I#iE"CI8nQLm>Z0O!Z,r/9RUa,+ur7l"Xs='*P*1-7=nN \SA;?$kmdm+j&_V/Aq,p:FBnfQ8? PCI effects are important at low photoelectron energies. GhJ^e#AU.P'*eF]4^$9/o7'8]Ijb7g4Yo;SZf7*AZP*Y;X_'0jKlSGIS'K=pnNmS]\`HE&98tO Goals Formulate vibrational-rotational energy states Interpret equilibrium vibrations of HCl and DCl Find the inter-nuclear separation (bond length) of each of the molecules. At around 1600-1800 cm-1, because as the reduced mass increases the shift decreases. McNab, Chem. ]Z#e!1AjrAm8(Qa'?LS>;8TP:)=AL!9U$$bl@5ub^J@&;]2*0mn)UGh=S'YD9D/PQ 8;T*$0Ef7eFC'Ci?pfY? c?0"!Bd;lC4edB])8@t+rYrp#$Q&i#17_3e26.&6AY9D?A)m%@)ZP*5RM_!UMtD+`c[ For such three-body reactions the coincidence experiment, unlike conventional techniques, allows the initial velocity vectors of all three products to be determined for each reactive event. The use of isotopic substitution was a useful tool, in this study and showed the correlation of the, intensity of the above barrier resonances with their, proximity to the barrier. Where there is a, signi®cant overlap of the wavefunction of the ini-, tial neutral molecule and the ®nal-state wave-, function of the molecular dication in the well, region a narrow peak in the photodissociation, We have calculated the resonance structure that, is supported by the Bennett/McNab potentials for, calculate the absorption coecients for single, photon double ionisation from HCl (DCl). Electron-transfer reactions ), (Note that the often used integral form of the partition function has a systematic error that does not imporove as J increases.). Teq8V=ka'WM;/_[mrS1WB1Mb_i/Wf:pS$g]c>hbP;p76tSjuhQ7-dr!qnM:`F:I$e Several mechanisms contribute to the overall effect of double photoionization in molecules, and this review attempts to extend the conventional classification. 4, HCl shows an absorption band approximately 2900 cm-1 while Fig. =OKobYHq\d/;Ri3\k?%)N-57AV:5\LG@Jce1_8@H*=8F#L!i The rigid rotor rotational energy levels of a diatomic molecules are $$E_J= \hbar^2J(J+1)/(2I)$$ where I is the moment of inertia $I=\mu r^2$ for reduced mass $\mu=m_1m_2/(m_1+m_2)u $ (in kg) and bond length r. The degeneracy of rotational levels is $g_J=2J+1$. The absolute position of the potential functions and simulated spectra have been shifted by the energies shown to bring the v ˆ 0 resonances into alignment. Subsequently, Yencha et al. !Tq&t>=VM*K?7MDH91iK1R38;bKZj7@PB * Analysis of the results of all three methods shows that the triplet state is a pure 3Σ− state, while the singlet state is a mixture of the 1Δ and 1Σ+ states. ,K).jPun-^lDnDfhi?p#GS$]kjDchm%DsVQpn*$*3gNUuI-.4\nBMct"ibR'7:\tP [278] and to assign or predict double photoionization spectrum of diatomics, for example, for the O 2 [146], CN [245], BN [263], NO [279], CO [22], SO [244], ClO [80], AlCl [224], SeO [82], Br 2 [53], HCl [280. (The curves are plotted for clarity assuming that J is continuous not discrete). Gas-phase molecular dipositive ions (molecular dications) are -,`j_)lA 1g&p%&Y8ecB6h0@>04f;f'-*4A%kA1MG0mDb)o]1j-+pBSlqm$LX^LcR?n-%O]GfA ;"/LIacgc')-2H;p->2icbYo68&o[lPa\"95mY;=H6\+,D32je+MTtTNGPAH*Q^ajRk$bg41#(I-h;U9sZhhu*EU\!=5J0-$#