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Spectroscopic Study of Anisotropic Excitons in Single Crystal Hexacene † † ‡ ‡ ‡ † Alexey Chernikov,*, Omer Yaffe, Bharat Kumar, Yu Zhong, Colin Nuckolls, and Tony F

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Spectroscopic Study of Anisotropic Excitons in Single Crystal Hexacene † † ‡ ‡ ‡ † Alexey Chernikov,*, Omer Yaffe, Bharat Kumar, Yu Zhong, Colin Nuckolls, and Tony F Letter pubs.acs.org/JPCL Spectroscopic Study of Anisotropic Excitons in Single Crystal Hexacene † † ‡ ‡ ‡ † Alexey Chernikov,*, Omer Yaffe, Bharat Kumar, Yu Zhong, Colin Nuckolls, and Tony F. Heinz*, † Departments of Physics and Electrical Engineering, Columbia University, New York, New York 10027, United States ‡ Department of Chemistry, Columbia University, New York, New York 10027, United States *S Supporting Information ABSTRACT: The linear optical response of hexacene single crystals over a spectral range of 1.3−1.9 eV was studied using polarization-resolved reflectance spectroscopy at cryogenic temperatures. We observe strong polarization anisotropy for all optical transitions. Pronounced deviations from the single-molecule, solution-phase spectra are present, with a measured Davydov splitting of 180 meV, indicating strong intermolecular coupling. The energies and oscillator strengths of the relevant optical transitions and polarization-dependent absorption coefficients are extracted from quantitative analysis of the data. SECTION: Spectroscopy, Photochemistry, and Excited States inear acenes, that is, naphthalene, anthracene, tetracene, established between the degree of CT character and the so- L and pentacene, form a unique family of organic semi- called Davydov splitting (DS)19 of the low-lying excitons conductors. These materials readily form large (>100 μm2) observed in polarization-resolved optical absorption spectra.6 single crystals that exhibit a “herring-bone” packing motif in Thus, experimental characterization of the intrinsic optical 1 which aromatic edge-to-face interactions dominate. During the properties of organic crystals also facilitates rational design of last few decades, this family has been the subject of many advanced optoelectronic devices. Naturally, the steady increase 2 experimental and theoretical studies, especially motivated by of the intermolecular coupling from naphthalene to pentacene fl potential applications in exible, low-cost optoelectronic crystals provides a strong impetus for a systematic study of even 3−5 devices. The strength of the intermolecular interactions in larger linear acenes. Such studies have been inhibited by the linear acene crystals is now understood to increase steadily with ff 6 lack of suitable synthetic methods. Recently, however, e ective the length of the acene molecule. This increased interaction is synthesis and crystallization methods for hexacene have been correlated with two major trends: an increase in charge carrier 7 7 reported. In a previous work, we made use of this method to mobility and an increase in the extent to which the molecular investigate the rate of singlet fission in polycrystalline hexacene electronic structure is perturbed by intermolecular coupling films and the room-temperature optical response of hexacene effects.6,8,9 The latter manifests itself directly in the optical single crystals.20 spectra of the materials. Single crystals of smaller acenes Here, we study the linear optical response of hexacene single preserve the characteristic absorption features of the individual crystals by polarization-resolved reflectance spectroscopy at molecules in solution, with transitions of Frenkel excitons cryogenic temperatures. From quantitative analysis of the data, featuring well-resolved vibronic sidebands. The optical response of the pentacene crystals, however, already shows marked we extract the energies and oscillator strengths of the relevant, bright optical transitions and polarization-dependent absorp- deviations from the molecular picture, indicating the ffi pronounced influence of intermolecular interactions.6,8,10 tion coe cients. The optical response of the crystalline fi In addition, increased intermolecular coupling is accom- hexacene is found to deviate signi cantly from the correspond- panied by a delocalization of the excitonic wave function, which ing single-molecule solution-phase spectrum (measured in Si oil 21 is distributed among several neighboring molecules and can to avoid oxidation), indicating the presence of strong also lead to an increased charge-transfer (CT) character of the intermolecular interactions. low-energy excitons.8,9,11,12 Such CT states are considered to be crucial for multiexciton effects such as singlet fission, an energy Received: August 11, 2014 conversion process where an excited singlet state converts into Accepted: October 6, 2014 − two long-lived triplet states.9,12 18 Correlation has been Published: October 6, 2014 © 2014 American Chemical Society 3632 dx.doi.org/10.1021/jz501693g | J. Phys. Chem. Lett. 2014, 5, 3632−3635 The Journal of Physical Chemistry Letters Letter Hexacene single crystals with an average thickness of several presented in Figure 1). The sin2 curves shown in the same plot microns and lateral areas of 20−50 μm2 were grown on a fused illustrate the pronounced polarization anisotropy of the silica substrate using a recently reported synthesis and growth respective transitions with about 90° between the a and b procedure.7 Micrographs of typical crystals are presented in the resonances. The amplitudes of the a- and b-related peaks nearly Supporting Information. Previous single crystal X-ray diffrac- vanish in the spectra with the opposite polarization, with tion measurements have established that such crystals adopt a residual intensities attributed to a small angular tilt of the out- triclinic structure with a nearly rectangular in-plane unit-cell of-plane crystal axis or inhomogeneities. lying parallel to the substrate.7 Optical reflection measurements To extract the energy and the oscillator strengths of the were performed at normal incidence, with samples held in a spectrally overlapping resonances in the reflectance spectra, we cryostat at a temperature of 77 K. We used a tungsten quartz apply a quantitative analysis scheme based on a standard multi- halogen lamp as a broadband radiation source, with the incident Lorentzian parametrization22 of the complex dielectric function light linearly polarized by a rotatable absorptive polarization ϵ(E) with photon energy E and for the two polarizations along filter. The reflected radiation was spectrally dispersed in a the principal optical axis grating spectrometer and detected by a liquid-nitrogen-cooled f CCD. Measurements were performed only on the thickest k ϵ=ϵ+()E b ∑ 22 crystals (see micrographs in Supporting Information). These k EEiE0,k −−γk (1) crystals were opaque and could be treated as semi-infinite in E2 γ f extent in the analysis below. To obtain absolute reflectance with 0,k, k and k denoting the peak energy, spectral k spectra for each polarization angle, we normalized the reflection broadening and the oscillator strength of the th transition, ϵ from the sample by that from the fused silica substrate. respectively. The background constant is represented by b. ϵ ϵ The measured reflectance spectra of the hexacene crystal are The real and imaginary parts 1 and 2 of the dielectric function ϵ E n iκ presented in Figure 1a for polarization angles between 0° and ( ) are related to the complex refractive index ( + ) via ⎡ 1 ⎤1/2 n()E =ϵ+ϵ+ϵ⎢ ()2 2 ⎥ ⎣ 2 112 ⎦ (2) ⎡ 1 ⎤1/2 κ()E =−ϵ+ϵ+ϵ⎢ ()2 2 ⎥ ⎣ 2 112 ⎦ (3) The reflectance spectrum for a semi-infinite bulk crystal at the normal incidence is then obtained from n and κ using [1]n −+22κ R()E = [1]n ++22κ (4) ϵ E a a b b The peak parameters in ( ) for the 1, ..., 4 and 1, ..., 4 transitions are adjusted to ensure a fit of the multi-Lorentzian model to the measured reflectance spectra. Two different dielectric functions are obtained for the a- and fl b-polarized cases, illustrating the anisotropy of the dielectric Figure 1. (a) Linearly polarized re ectance spectra of a hexacene 23,24 T ° ° tensor in the acene crystals. In general, this analysis single crystal at = 77 K for polarization angles between 0 and 90 . fi The resonances excited with light polarized along the a axis (0°) and b procedure is justi ed when the chosen polarization angles are ° a a b b axis (90 ) of the crystal are denoted by 1, ..., 4 and 1, ..., 4, close to or equivalent to the principal optical axis of the b ° respectively. The spectral region around the 4 resonance in the 90 dielectric tensor. In the present case the substrate plane spectrum is presented in the inset. (b) Schematic representation of the corresponds to the ab plane of the hexacene crystals and the hexacene crystal structure perpendicular to the growth direction with latter is almost rectangular (γ ≈ 90°),7,20 that is, the crystal the symmetry axes denoted by “a” and “b”. (c) Polar plot of the structure is nearly orthorhombic. For pentacene, the principal a b normalized peak intensities of the lowest-lying exciton states ( 1, 1)as axes a and b indeed closely correspond to the orthogonal in- a function of polarization angle. For comparison, the solid lines show plane directions x and y,10 justifying the assignment of the 0° sin2 functions. and 90° polarization angles as being close to both principal optical and crystallographic axes. 90°. The two angles are typically assigned to be roughly aligned The results of the above procedure are presented in Figure along the a and b symmetry axes of the crystal, schematically 2a, b, and c for the a-polarized (0°), unpolarized, and b- shown in Figure 1b. A manifold of resonances is observed with polarized (90°) spectra along with the measured data. The a strong dependence on the polarization angle. The optical unpolarized spectrum is obtained by averaging the a- and b- a a b b fl transitions are labeled by 1, ..., 4 and 1, ..., 4 according to the polarized re ectance. The agreement of the results from the a b respective polarization conditions. The resonances 1 and 1 are multi-Lorentzian analysis with the experimental data allows for identified as the bright low-energy excitons measured at room- a meaningful extraction of the peak parameters and related temperature in the previous study,20 exhibiting a DS of their observables, such as the absorption coefficients α(E)= respective peak energies.19 The similarity of the optical spectra κ(E)(2E/ℏc).22 The latter are presented in Figure 2d, e, and at room- and low-temperature indicates that there is no f for the three polarization conditions.
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