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MOLECULES COMPLEXES AND CLUSTERSLU) TEL-AVIV UNIV ISRAEL) DEPT OF CHEMISTRY J JORTNER ET AL 30 APR 87 UNCLASSIFIED DRJA45-85-C-0888 F/G 21/2 N 7 - 9241E h h m hmTTEEER IC WDDNM ICSOF ARu I .AS

UNCLASSIFIED DRJA45-85-C-0888 F/G ISRAEL) …Page 3 7.B Rydberg States of Anthracene. Several Rydberg transitions of jet-cooled anthracene were observed in the spectral region 1900-2000

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Page 1: UNCLASSIFIED DRJA45-85-C-0888 F/G ISRAEL) …Page 3 7.B Rydberg States of Anthracene. Several Rydberg transitions of jet-cooled anthracene were observed in the spectral region 1900-2000

MOLECULES COMPLEXES AND CLUSTERSLU) TEL-AVIV UNIVISRAEL) DEPT OF CHEMISTRY J JORTNER ET AL 30 APR 87

UNCLASSIFIED DRJA45-85-C-0888 F/G 21/2 N

7 -9241E h h m hmTTEEERE IC WDDNM ICSOF ARuI .AS

Page 2: UNCLASSIFIED DRJA45-85-C-0888 F/G ISRAEL) …Page 3 7.B Rydberg States of Anthracene. Several Rydberg transitions of jet-cooled anthracene were observed in the spectral region 1900-2000

11111L jl__4 11_L

Page 3: UNCLASSIFIED DRJA45-85-C-0888 F/G ISRAEL) …Page 3 7.B Rydberg States of Anthracene. Several Rydberg transitions of jet-cooled anthracene were observed in the spectral region 1900-2000

PROGRESS REPORT FOR-THE PERIOD NOVEMBER 1, 1986 - APRIL 30, 1987

a5th Periodic Report

I. Title: EXCITED-STATE ENERGETICS ANDDYNAMICS OF LARGE MOLECULES,COMPLEXES AND CLUSTERS

2. Principal Investigator: Professor Joshua Jortner

3. Associate Investigator: Professor Uzi Even

4. Contractor: School of ChemistryTel Aviv UniversityTel Aviv 69978Israel

5. Contract No.: DAJA45-85-C-0008

The Research reported in this document has been madepossible through the support and sponsorship of theU.S. Government through its European Research Officeof the U.S. Arnry. ... . -. .... D T I

SODTIC*. . . . ' . . .. .. Lf t- -

" .. ... .

ELECTE.MAR3 01988

8 3 23 122

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6. PkOGRESS IN TECHNICAL APPROACH

New techniques for spectroscopy in supersonic expansionsand in the development of specific supersonic sources weredeveloped.

6.A Vacuum Ultraviolet.Absorption Spectroscopy'in SupersonicExpansions. We have combined the techniques of vacuum ultra-

violet (VUV) spectroscopy together with planar supersonicjets, which allows for the interrogation of absorption spectraof large molecules cooled in supersonic expansions in the nearVUV region. The experimental setup consists of a high pres-sure Xe lamp, CaF 2 optics, a vacuum ultraviolet spectrographand a nozzle/slit (0.27x90 mm, repetition rate 9 Hz and gaspulse duraV on 300 Usec). The characteristics of this spectro-scopic set'up are: (i) Energy range 6-10 eV. (ii) Spectralresoluti,4'n 0 .1 . (iii) Routine measurements of high-energyabsorpion spectra. (iv) Interrogation of fluorescence excita-tion spectra of the parent molecule or its photoproducts withlimiting quantum yields of Y -lO " .

6.B Development of Conical Nozzles Afr Supersonic Jets. Conicalnozzles (nozzle opening angle % = 30", and nozzle diameterD = 0.3 mm) were constructed and used in conjunction with amagnetic pulsed valve. The use of conical nozzles considerablyenhances clustering in supersonic expansions, facilitatingstudies of large van der Waals complexes and clusters.

7. ACCOMPLISHMENTS OF OBJECTIVES

7.A Energetics of Rydberg States of Jet Cooled Molecules. VUVabsorption spectra of benzene, benzene-D6 and naphthalenecooled in planar supersonic expansions were measured over therange 2000-1600 A, providing evidence on energetics, linebroadening and interference effects. Accession For -

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7.B Rydberg States of Anthracene. Several Rydberg transitionsof jet-cooled anthracene were observed in the spectral region1900-2000 A. These Rydbergs are superimposed on a broad"background" of ww* transitions. Up to now no fluorescencefrom Rydbgrg states of polyatomic molecules has been reported.The 1997 A n=3 Rydberg of anthracene reveals fluorescenceIwith a quantum yield of -. 5%. This fluorescence originatesfrom internal conversion R vnv+ S followed by S. --i So emission,as documented by the spectral distribution of the dispersedfl uores cence.

7.C Intramolecular Relaxation of Rydberg States. Information onintramnolecular dynamics of extravalence excitations of benzenewas obtained from lineshape analysis. The lineshape of the3Pxy(O) Rydberg is Lorentzian, whose homogeneous width resultin he lifetime T = 0.19±0.02 psec for C0H6 and T = 0.22±0.02psec for C6D6. Semiquantitative information on the lifetimesof some Rydbergs of anthracene was obtained, which fall in therange of n. 0.1 psec. These lifetime data imply that (i) therelaxation of the Rydberg is characterized by moderate energygap(s), and (ii) the electronic relaxation rate of the Rydbergis considerably less efficient than that of the intravalenceexcitation in the same energy domain.

7.D Interference Effects between Extravalence and IntravalenceMolecular Excitations. We have searched for Rydberg-valenceinterference effects in large molecules, which are expected tobe exhibited in asymmetric Fano-type lineshapes in absorption.For "isolated" Rydbergs, which are superimposed on a ww* tran-sition in benzene, naphthalene and anthracene, the absorptionlineshapes are symmetric Lorentzians. No line asymmetry andno antiresonances characteristic of Fano profiles were foundin that case. The absence of interference effects in this casereveals the manifestation of-random interstate coupling of Rwith the w* manifold. The random coupling erodes all inter-ference effects. The situation is different for nearly lyingRydbergs, where pronounced R-R-valence interference effectswere observed in the absorption spectrl of jet-cooled naphtha-lene in the spectral region 1600-1650 A, providing informationon the homogeneous contribution to high-energy molecular coupl-ing phenomena.

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7.E Rotational State Dependence of"l ntramolecular Dynamics. Rota-

tional effects on interstate coupling are of considerable cur-rent interest. Absolute fluorescence qpantum yields from photo-selected rotational states were measured for the electronicorigins of the S, state of pyrazine. Strong rotational statedependence was observed providing novel information on inter-state coupling for the intermediate level structure. Thisunique information cannot be extracted from time-resolved decaylifetimes.

7.F The Coupling between Intrastate'Vibratlonal EnergyRedistributionand Interstate Electronic-Relaxation. We have documented someuniversal characteristics of the decay lifetimes and fluorescencequantum yields from the S, manifold of large molecules, whichoriginate from the. coupling between intrastate vibrational energyredistribution and interstate electronic relaxation. The time-resolved total fluorescence decay excited by a psec laser from theS, state of jet-cooled 9CN-anthracene exhibits nonexponential decayin the energy range EV = 1200-1740 cm- above the S, origin, whichdoes not originate from dephasing but rather manifests the effectsof intrastate intermediate level structure for vibrational energyredistribution on intersys-tem crossing.

7.G Coriolis Rotation-Vibraton 'COupling and Intramolecular Dynamics.We have demonstrated that rotational effects play a central roleon intramolecular vibrational energy redistribution in electronic-vibrational excitations of large molecules. Strong rotationaleffects on the fluorescence quantum yields from vibrational states(above 1000 cm-1) in the S manifold of 9-cyanoanthracene wereobserved, which demonstrate that Coriolis interactions serve as

-the dominant coupling leading to Intramolecular vibrational energyredistribution (IVR). In contrast to common wisdom, whichattributed IVR in large molecules to anharmonic interactions, wehave shown that rotational effects play a central role stronglyenhancing interstate electronic relaxation.

7.A .-,esonances in Mediated Intersystem Crossing. The mechanisms ofJrect and of mediated intersystef crossing from the first excitedsinglet manifold of anthracene and some of its derivatives wereexplored by the study of the internal and the external heavy atomeffect on the fluorescence quantum yields. Pronounced mode selec.-tivity was observed in the vibrational energy dependence of theemission quantum yield in 9-bromoanthracene and 9,10-dibromo-anthracene

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7.1 Mediated Intersystem Crossing Phenomenoloqy Inverse Isotope Effects andMicroscopic Level Shifts. We explored the energy dependence of the inter-state electroni"c relaxation rates, knr, from the S1 manifold of anthraceneand seven of its isotopic and chemical derivatives, which were inferredfrom quantum yield data. Absolute fluorescence quantum yields, Y, fromgroups of rotational states within the electronic origin Sl(O) and fromvibrational states were obtained over the excess energy EV = 0-3000 cm-'above Sl(O) by the simultaneous interrogation of the fluorescence excita-tion spectra and of the absorption spectra in seeded, pulsed, planarsupersonic jets of Ar. Additional information was obtained from quantumy ield data of van der Waals (vdW) complexes of these molecules with Ar. Thefluorescence quantum yields from the S (0) of anthracene, 9-cyanoanthraceneand 9,10-dibromoanthracene were found lo be independent of the rotationalstate, providing further evidence for the rotational independence of knrfrom a single doorway state. From the Y data of the electronic origins andfrom the Ev dependence of Y, we conclude that Intersystem crossing (ISC)dynamics of the Sl manifold is dominated by the interplay between twoclasses of nonreactive coupling and/or relaxation. (i) Interstate coupl-ing, involving the superposition of direct Sl 1 (Tx) ISC together with

- (T ) - (Ti) mediated ISC through a sparse or dense (Tx) manifoldof a higher triplet state. (ii) Intrastate coupling within the Sl manifold,which sets in with increasing EV and which results in intramolecular vibra-tional energy redistribution (IVR) at high Ev. The dominant role ofmediated interstate coupling in ISC dynamics from S1 (O) and from low Estates was inferred from the inverse deuterium isotope effect on the I9Crates, the extreme sensitivity of k of deuterated anthracene to a singleH atom substitution, and to level sRlfts induced by complexing with Ar, aswell as from the three orders of magnitude difference between the knr valuesfrom the Sl(O) of 9-bromoanthracene and of 9,10-dibromoanthracene. The on-set of the mediatid ISC is documented by an abrupt drop of Y in the narrow(EV = 617-805 cm" ) energy range for 9,10-dichloroanthracene and by theoscillatory energy dependence of Y versus E and the extreme energy sensiti-vity of Y in the range EV = 157-800 cm -1 of 9,lO-dibromoanthracene which isattributed to near-degeneracies between Sl states anu the mediating (Tx)states. These resonance effects can be drastically modified by dispersivelevel shifts induced by complexing with Ar. At high excess vibrationalenergies some universal features of the EV dependence of knr are exhibited.These involve a graoual increase of knr with increasing EV at medium energies(EV = 1000-1800 cm'1), which correspond to the intermediate level structurefor intrastate coupling, and a very weak EV dependence of knr at highenergies (E = 1800-3000 cm 1), which manifest the effect of statisticalintrastate YVR on interstate ISC.

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7,J Fluorescence Quantum*Yields for Highly-ExcitedStates of LargeMolecules. Fluorescence quantum yields Y from high electronicexcitations of naphthalene, anthracene and tetracene in the energyrange 5.0-6.5 eV have been recorded. Y exhibits an exponentialdependence on the excess vibrational energy with the slope decreas-ing with increasing size of the molecule, i.e., the vibrationaldensity of states. These data are characteristic of internal con-version from S to So. These results are of interest regardingrecent astrophysical implications of high-energy photophysics oflarge aromatic hydrocarbons in outer space.

7.K Photoisomerization Dynamics of'Trans-Stilbene andof Cis-Stilbene.Time-resolved fluorescence lifetimes from photoselected states oftrans-stilbene were recorded by the techniques of picosecond spec-troscopy in jets using a mode-locked dye laser and a fast photoncounting system. Decay lifetimes as short as 100±30 psec wererecorded Extensive information on the energy dependence of theisomerization rates of alkyl stilbenes was obtained, providinginformation on the role of intramolecular vibrational distribu-tion on the photochemistry in an isolated molecule. The absorp-tion spectrum of jet-cooled cis-stilbene is broad and no vibra-tional structure could be resolved due to the congestion ofbroadened low-frequency vibrational excitation. From the lowquantum yiEeld Y $ 2xlO- 4 we infer a S, lifetime of T $ 0.4psec, which indicates ultrafast relaxation of this molecule.

7.L Photoisomerizatlon Dynamics of'Alkyl Substltuted'Trans-Stilbene.aA central issue pertaining to isolated-molecule photochemistry

involves the role of intramolecular vibrational relaxation indetermining intramolecular dynamics. We have attempted to in-crease the density of vibrational states by alkyl substitutionof trans-stilLene and have explored the Isomerization dynamics

* by picosecond time-resolved spectroscopy,. We have obtained thecounter-intuitive result that alkyl substitution of trans-stilbene enhances the photoisomerization rates, while generalarguments based on the role of IVR and the implications ofstatistical theories indicate that the rate should be retarded..The results can be accounted for by the modification of themolecular parameters, i.e., threshold energy, by alkyl substi-tution.

.4

MRR

M1

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*%

7.M Energy-Resolved PhotoisomerizationRates. The dynamics of the S,and 52 electronically excited singlet states of diphenylbutadienewas interrogated by fluorescence quantum yield measurements overthe very broad energy domain of 0-7500 cm-1 above the (false) S1origin. The issues of the lack of mode selectivity and the appli-cability of statistical theories for the description of isolated-molecule photochemistry were explored.

7.N van der Waals Complexes'ofPorphyrins. Excited-state energeticsand dynamics of large complexes consisting of porphyrins bound torare-gas atoms were explored. Detailed spectroscopic informationon the So - S, and SO -1 S2 transitions of the free-base porphine.Ar complex was obtained, providing insight into the structure ofthis complex as well as resulting in a novel mechanism for micro-scopic solvent shifts induced by configurational distortions,which are due to complexing.

7.0 Coupling_ between Intramolecu01arand.IntehioleCular Nuclear Motionin Complexes. Intermolecular vibrations of large van der Waalscomplexes, which involve the motion of the ligand relative to thelarge molecule, provide an analogue for surface vibrational motionin a finite system and constitute the precursors of phonon modesin condensed phases. Information on the coupling between inter-molecular and intramolecular vibrational motion was obtained forthe trans-stilbene.Ar complex.

7.P Analogies between Large vanderWaalsMolecules and Microsurfaces.The binding of rare-gas (R) atoms to large aromatic molecules (M)on the one hand, and to the basal plane of graphite on the otherhand, represent two extremes of the interaction of R atoms withordered arrays of sp2 hybridized carbon atoms. We have exploredthe analogies between the characteristics of large van der WaalsM.Rn complexes and R atoms on graphite surfaces, focusing onstructure, packing, orientational registry effects and the nuclearmotion of R adsorbates on finite microsurfaces. The elucidationof the structure, energetics and nuclear dynamics of large M.Rncomplexes rests on semi-empirical model calculations of potentialsurfaces. These provide a quantitative account of the geometry,the existence of isomers, the dissociation energies and the fre-quencies of out-of-plane and in-plane vibrational modes for largeamplitude intermolecular nuclear motion.

0

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7.Q Electron Localization in Clusters. Small clusters exhibit uniquephysical and chemical phenomena, which are both of fundamental andtechnological significance, and provide ways and means to explorethe "transition" from molecular to condensed-matter systems. We

,have provided a theoretical study of the structure, energetics anddynamics of an excess electron interacting with an alkali-halidecluster, which was explored by the quantum path integral moleculardynamics method. These studies establish various compositional,structural and size dependence of bulk and surface localizationmechanisms of the dynamic process induced by electron attachmpnt.

7.R Vibrational Predissociation Induced by Exciton Trapping in Rare-GasClusters. The dynamics of exciton trapping, vibrational energytransfer and vibrational predissociation in an electronically excitedstate of Ar1 3 clusters was explored by classical molecular dynamics.

o' This study constitutes an application of this technique for thedynamics of electronically excited states of large systems. New

0 mechanisms of ultrafast (,. 300 fsec) vibrational energy flow induced. by short-range repulsion were documented. In these systems vibra-

tional energy redistribution does not occur and mode selective* ' . excitation prevails. In small (n=13) clusters the consequences of

vibrational energy flow results in reactive vibrational predissocia-tion, leading to the "evaporation" of Ar atoms for the cluster. Inlayer (n=55) clusters a transition from molecular-type reactivebehavior to nonreactive vibrational relaxation, which is character-istic of condensed phases, was exhibited.

7.S Nonreactive and Reactive Excited-State Dynamics in Mixed Rare-GasClusters. We explored the dynamic implfcatfons of energy exchangein electronically-vibrationally excited states of mixed rare-gasclusters. The classical molecular dynamics method was applied forthe study of vibrational energy flow from electronically excitedatomic (PO) states in Xe* Ar, 2 and Xe* Ars5 , due to short-rangerepul*Ive interactions, and the consequences of Xe2( 3 ) excimerformation in Xe*Ar 1 1 and Xe2Ars 3 clusters. We have es ablishedthe occurrence of an ultrafast vibrational energy flow (% 300 fsec)from local Rydberg atomic and excimer excitations into the cluster,

1I

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7.S (cont'd)

which is accompanied by large configurational dilation around the excitedstate, due to short-range repulsive interactions. Size effects on clusterdynamics were elucidated, being manifested by vibrational predissociationin small clusters, and by vibrational relaxation and vibrational pre-dissociation in small clusters and by vibrational relaxation and vibra-tional energy redistribution in large clusters. A gradual transition fromreactive molecular type relaxation in small clusters to nonreactive con-densed-matter type relaxation in large clusters was documented. Qualita-tive and quantitative differences between relaxation of excited speciesinitially located in the interior or on the surface of the cluster wereestablished, being exhibited in the details of the vibrational energy flow.In the case of the bulk Xe2Ars 3 , excessive local heating is manifested incluster melting, which results in mass transport of the excimer to thecluster surface. The many facets of the dynamics of electronically excitedmixed rare-gas clusters are amenable to experimental interrogation.

iI

I

II,

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8. PUBLICATIONS

The following manuscripts, supported by this researchgrant, were prepared and submitted for publication:

(1) A. Amirav and J. JortnerVacuum Ultraviolet Absorption Spectroscopy in Super-sonic Expansions

Chem. Phys. (Communication) 82, 4378 (1985)

(2) A. Amirav and J. JortnerRotational and Vibrational State Dependence on Intra-

molecular Coupling and Dynamics in the S, State ofPyrazine

J. Chem. Phys. (in press)

(3) J. Troe, A. Amirav and J. JortnerEnergy-Resolved and Thermalized Photolsomerization Rates

of Diphenyl-ButadieneChem. Phys. Letters 115, 245 (1985)

(4) A. Amirav, M. Sonnenschein and J. JortnerInterstate Coupling and Dynamics of Excited Singlet Statesof Isolated Diphenylbutadiene

Chem. Phys. 102, 305 (1986)

(5) U. Even, Z. Berkovitch-Yellin and J. JortnerElectronic Excitations of the Free-Base Porphine-Ar vander Waals Complex

Canad. J. Chem. (C. Sandorfy-Special Issue) §3, 2073 (1985)

(6) D. Bahatt, U. Even and J. Jortner* Coupling between Intramolecular and Intermolecular Nuclear

Motion in a Large van der Waals ComplexChem. Phys. Letters 117, 527 (1985)

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8. PUBLICATIONS (conrtd)

(7) Klaus Rademann, Uzi Even, Shlomo Rozen and J. JortnerPhotoisomerization Dynamics of Alkyl Substituted Stilbenes

in Supersonic Jets.Chem. Phys. Lett. 125, 5-11 (1986)

(8) A. Amirav, J. Jortner, S. Okajima and E. C. LimManifestations of Intramolecular Vibrational Energy

Redistribution on Electronic Relaxation in Large MoleculesChem. Phys. Letters 126, 2187 (1986)

(9) U. Landman, D. Scharf and J. JortnerElectron Localization in Alkali-Halide ClustersPhys. Rev. Letters 54, 1860 (1985)

C10) Dafna Scharf, Uzi Landman and Joshua JortnerEnergetics and Dynamics of ClustersProc. of the Int'l School of Physics "Enrico Fermi", Italy,1986, in: Advances in Chemical Reaction Dynamics (D. ReidelPublishing Company)

(11) D. Scharf, U. Landman and J. JortnerVibrational Predissociation Induced by Exciton Trapping in

Inert-Gas ClustersChem. Phys. Letters 126, 495-500 (1986)

(12) Dafna Scharf, Uzi Landman and J. JortnerSurface States of Electrons and Alkali-Halide ClustersProc. of the 19th Jerusalem Symposium, Israel, 1986. Eds4 J. Jortner and B. Pullman (D. Reidel Publishing Company,Holland, 1986)

,,

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(13) Samuel Leutwyler and Joshua JortnerThe Adsorption of Rare-Gas on Microsurfaces of LargeAromatic MoleculesJ. Phys. Chem. (in press)

(14) Dafna Scharf, Uzi Landman and Joshua JortnerAtomic and Molecular Quantum Mechanics by the PathIntegral Molecular Dynamics Method

Chem. Phys. Letters 130, 504 (1987)

(15) A. Amirav and Joshua JortnerRotation, Vibration and Electronic RelaxationProc. of the CECAM Conference, Orsay, France, 1986(D. Reidel Publishing Co., Holland,1986)

(16) A. Amirav and J. JortnerResonances in Mediated Intersystem Crossing of Jet-Cooled Anthracene DerivativesChem. Phys. Letters 132, 335 (1986)

(17) A. Amirav, J. Jortner, M. Terazima and E.C. LimRotational Effects on Intramolecular RadiationlessTransitions in a Large MoleculeChem. Phys. Letters 133, 179-184 (1987)

(18) U. Landman, R.N. Barnett, C.L. Cleveland, D. Scharfand J. Jortner

Electron Excitation Dynamics, Localization and Solvationin Small ClustersJ. Phys. Chem. (in press)

(19) A. Amirav, C. Horwitz and J. JortnerOptical Selection Studies of Electronic Relaxation fromthe S, State of Jet-Cooled Anthracene DerivativesJ. Chem. Phys.

(20) R.D. Levine, S.A. Rice and J. JortnerLevel Structure and Dynamics from Diatomics to ClustersAdvances in Chemical Physics (John Wiley & Sons, New York,(1987)

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(13) Samuel Leutwyler and Joshua JortnerThe Adsorption of Rare-Gas on Microsurfaces of LargeAromatic Molecules

J. Phys. Chem. (in press)

(14) Dafna Scharf, Uzi Landman and Joshua JortnerAtomic and Molecular Quantum Mechanics by the PathIntegral Molecular Dynamics Method

Chem. Phys. Letters 130, 504 (1987)

(15) A. Amirav and Joshua JortnerRotation, Vibration and Electronic RelaxationProc. of the CECAM Conference, Orsay, France, 1986(D. Reidel Publishing Co., Holland,1986)

(16) A. Amirav and J. JortnerResonances in Mediated Intersystem Crossing of Jet-Cooled Anthracene Derivatives

,.-. Chem. Phys. Letters 132, 335 (1986)N .

(17) A. Amirav, J. Jortner, M. Terazima and E.C. LimRotational Effects on Intramolecular RadiationlessTransitions in a Large Molecule

Chem. Phys. Letters 133, 179-184 (1987)

(18) U. Landman, R.N. Barnett, C.L. Cleveland, D. Scharfand J. Jortner

Electron Excitation Dynamics, Localization and Solvationin Small Clusters

J. Phys. Chem. (in press)

(19) A. Amirav, C. Horwitz and J. Jortner' Optical Selection Studies of Electronic Relaxation from

the S State of Jet-Cooled Anthracene DerivativesJ. Chem. Phys.

(20) R.D. Levine, S.A. Rice and J. JortnerLevel Structure and Dynamics from Diatomics to ClustersAdvances in Chemical Physic: (John Wiley & Sons, New York,

-. (97.P%.

mot,

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