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Ultrafast Energy Transfer in Ultrathin Organic Donor/Acceptor Blend

Scientific Reports volume 3, Article number: 2073 (2013) | Download Citation


It is common knowledge that poly(3-hexylthiophene) (P3HT)/[6,6]-phenyl-C61-butyric acid methyl ester (PCBM) blend, a prototype system for bulk heterojunction (BHJ) solar cells, consists of a network of tens of nanometers-large donor-rich and acceptor-rich phases separated by extended finely intermixed border regions where PCBM diffuse into P3HT. Here we specifically address the photo-induced dynamics in a 10 nm thin P3HT/PCBM blend that consists of the intermixed region only. Using the multi-pass transient absorption technique (TrAMP) that enables us to perform ultra high sensitive measurements, we find that the primary process upon photoexcitation is ultrafast energy transfer from P3HT to PCBM. The expected charge separation due to hole transfer from PCBM to P3HT occurs in the 100 ps timescale. The derived picture is much different from the accepted view of ultra-fast electron transfer at the polymer/PCBM interface and provides new directions for the development of efficient devices.


Due to the tremendous surge of interest in organic photovoltaics, the photophysics at the electron donor/acceptor (D/A) organic interface is a highly debated topic in material science. One of the most extensively investigated D/A blend is made of poly(3-hexylthiophene) (P3HT), as the donor component, mixed with phenyl-C61-butyric acid methyl ester (PCBM), as the acceptor. This blend provides solar cells with 85% Internal Quantum Efficiency1 and power conversion efficiency of around 5%2. Such high quantum yield of charge photogeneration with respect to pure organic semiconductors results from blending the two components into a BHJ. The D/A components are deposited from common solution and tend to segregate over tens of nanometers forming PCBM-rich clusters and crystalline domains of P3HT1,2,3,4,5,6. The two phases however are not separated by sharp interfaces, because substantial intermixing takes place in the border region defined by the extent of diffusion of PCBM molecules into P3HT7. In this intermixed region, the two components are finely dispersed at the molecular level and have been clearly observed in bi-layer structures7. Here we address the photophysical processes happening only at the intermixed border region by probing an ultrathin film with thickness much below the PCBM diffusion length.

By and large, charge transfer is regarded as the fundamental event occurring upon donor photo-excitation in the BHJ8,9 while energy transfer is generally ignored, at least at early times. However the proximity of D and A molecules in the blend may in principle also lead to electronic excitation energy transfer. Indeed this has been reported for a few systems prepared ad hoc, such as D/A bilayers separated by an interlayer that hampers charge separation10,11,12 or in chemically bound dyads, wherein the D and A are in a fixed positions with respect to each other13. Both these cases are thus modifications of the standard BHJ, where essentially the wavefunction overlap is largely reduced. On the contrary, there are no experimental evidences of electronic excitation energy transfer as primary event in standard BHJ systems. Based on photoluminescence (PL) quenching experiments in D/A blends, it was proposed that energy transfer dominates charge transfer only after 5 ps from the excitation14. The suggested picture is that close pairs undergo charge transfer, while distant pairs may first interact by energy transfer. Förster radius, the measure of the electronic coupling strength between D and A, has been evaluated for the prototypical systems such as P3HT/PCBM in the range between 1 and 5 nm11,13,15. Why electronic excitation energy transfer appears only in special situations and why charge transfer overwhelms it in BHJ, remains an open question.

In this work we study the photoexcitation dynamics of the intermixed P3HT/PCBM region obtained from a nominal 5/5 nm diffuse bi-layer. Contrary to the expectations, we demonstrate that ultrafast electronic energy transfer between donor and acceptor is the primary process occurring upon photoexcitation. Subsequent hole transfer from PCBM to the polymer takes place on the 100 ps time scale, resulting in the expected charge separation.

A thin P3HT layer of about 5 nm has an optical density of about 2 × 10−2 (see Supplementary Information (S.2) for thin film preparation and characterization). This value is far too low to have detectable signal above the shot noise limit in a standard pump-probe system. To overcome such a limitation, we propose a novel Transient Absorption by Multiple Pass (TrAMP) technique, that enables us to perform measurements on samples with optical densities as low as 10−2. This technique draws its inspiration from absorption spectroscopy of gases where high sensitivities are achieved by increasing the optical path length by multiple reflections of the beam in the gas chamber16. The same principle is extended to transient absorption spectroscopy by passing the pump and probe pulses multiple times, keeping the time delay between them constant. In this way, the pump-probe signals can be amplified by a factor proportional to the number of passes through the sample (see Supplementary Information (S.1) for more details).

Figure 1a shows the schematic lay-out of the TrAMP setup while Figure 1b demonstrates the concept and validity of our approach. It shows the TrAMP kinetics collected at various numbers of passes in a 15 nm thin film of P3HT on a 250 μm fused silica substrate. The pump is at 400 nm and the probe wavelength tuned at 680 nm. Standard pump probe (single pass) cannot detect any differential transmission changes in such a thin film. However, by the multiple pass scheme, the TrAMP technique provides an efficient amplification of the pump-probe signal, that is shown growing at each pass, while keeping the kinetic itself intact. This also demonstrates that possible effects on the time resolution, such as group velocity delay between pump and probe and pulse broadening, are negligible in our experiment, even in the worst condition of large spectral separation between the pump and the probe wavelength. By appropriate group velocity mismatch calculations (see Supplementary Information for details), it can be shown that the expected time resolution of the experiment is within 200 to 400 fs after 15 passes, depending on the pump-probe wavelengths. After certain number of passes, signal amplification reaches a saturation level that can be attributed to the almost complete absorption of the pump. The threshold number of passes depends on the optical density of the sample and for our bilayers this number is between 10 and 15 and all the experiments were conducted within this range. The pump wavelength for all the experiments reported here was tuned to 520 nm. An input energy of 10 nJ per pulse was employed. The spot-size varies for each pass in TrAMP between 100 μm and 200 μm. This will correspond to a maximum fluence of about 30 μJ/cm2.

Figure 1: Transient Absorption by Multiple Pass(TrAMP).
Figure 1

(a) Experimental scheme of TrAMP system.The Modulated pump beam and the probe beam are made to pass through the sample several times within the misaligned cavity made of the two curved mirrors .The sample is placed at the focus of the cavity. A set of filters and a monochromator are used to remove the pump before sending the probe beam to the detection system. (b) TrAMP kinetics collected by increasing the number of passes. The sample is 15 nm film of P3HT (OD = 0.1), the pump is at 400 nm and the probe at 680 nm.

In order to investigate the intermixed D/A system avoiding large phase segregation, we first deposit a 5 nm P3HT layer on fused-silica substrate and then we spin coat the PCBM on top from an orthogonal solvent7 with a nominal thickness of 5 nm. The absorption spectrum of the sample is a linear combination of the absorption spectrum of the two components with an OD of 0.02 at the absorption peak (Figure 2a). Because the P3HT film thickness is smaller than the PCBM molecule diffusion length, PCBM almost fully penetrate the polymer and we obtain a layer of P3HT doped with PCBM17 (see cartoon in Figure 2b). This is also suggested by simple AFM analysis performed on the bilayer (see AFM characterization in figure S3 of the Supplementary Information).

Figure 2: Bilayer characterization.
Figure 2

(a) Illustration of the morphology of the 5 nm bilayer of P3HT/PCBM used in present experiment.(b) Absorption spectrum of 5 nm films of P3HT and PCBM and the bilayer.


Figure 3a shows the transient absorption (ΔT/T) spectra of 5 nm thin P3HT film as a control experiment. The TrAMP spectrum and its temporal evolution are consistent with the one reported in literature18. At wavelengths shorter than 620 nm it exhibits a positive signal due to ground state bleaching (GSB). At probe wavelengths greater than 620 nm it shows a negative photo-induced absorption (PA) signal. A comparison with dynamics, as reported in Figure 3c, and a rather extended set of experimental and computational data reported in literature helps in disentangling the contributions beyond spectral overlap19,20. Two species can be identified at early time: singlet excitons and polaron pairs (PP) as assigned by Korovyanko et al18. The fast decaying PA band appearing at 650 nm is assigned to geminate recombination of PP. The longer lived signal is due to singlet states, with some contribution from polarons escaping the geminate recombination as reported in the earlier TA studies on P3HT8,9,18.

Figure 3: Ultrafast dynamics in the ultrathin P3HT/PCBM bilayers.
Figure 3

(a) TrAMP spectra and (c) the associated kinetics of a control film of P3HT with a thickness of 5 nm.(b) TrAMP spectra of P3HT/PCBM (5 nm/5 nm) bilayer at pump-probe delays of 1 ps, 5 ps and 500 ps. The TA spectrum of PCBM pumped at 400 nm is shown in the 1 ps window. The absorption of P3HT is also shown. (d) The associated TrAMP kinetics of the bilayer taken at λprobe = 580 nm (GSB) and at 650 nm and 750 nm (PA). Also plotted is the kinetic at λprobe = 750 nm of a 5 nm PCBM film. The Pump pulse for all the measurements is tuned to 520 nm.

The ΔT/T spectrum of the P3HT/PCBM intermixed layer is shown in Figure 3b, and selected time traces are reported in Figure 3d. At a first glance, the early spectrum resembles the pure P3HT spectrum, though with a remarkable reduction in the amplitude of GSB with respect to the PA. Within 2 ps, both the P3HT GSB and the PA band centered at 650 nm decay to zero with similar kinetics, giving rise to a negative signal extending on the whole experimental range. Notably the 580–620 nm spectral region that corresponds to P3HT ground state absorption shows null or negative signal. This indicates that P3HT is weakly or not excited anymore. The broad PA should correspond to an excited state population that is not perceived by the ground state of the polymer. The charge transfer process cannot explain such an observation: upon charge transfer (CT) and hole-polaron formation, the polymer GSB stays constant due to the persistent depletion of the ground state population.

Our observation can however be explained by electronic energy transfer from P3HT to PCBM. Accordingly, P3HT GSB would decay and a new PA due to (Sn ← S1) in PCBM would appear (see Supplementary Information (S.4) for quantum chemically computed Sn ← S1 transitions in PCBM). As a reference, ΔT/T spectrum of pristine PCBM, measured upon resonant excitation (400 nm), is reported in Figure 3b. It is a broad photoinduced absorption band, extending over the whole experimental range. This fits reasonably well with our observation, supporting our explanation. It is fair to note a discrepancy between the lineshape of the pure PCBM PA band and our data, in the 580–620 nm spectral region. This can be ascribed to a residual GSB of the polymer, indicating that following polymer photoexcitation there is a branching between electronic energy transfer and charge transfer towards PCBM, here in favor of the former.

Concominant excitation of PCBM, when we excite the P3HT, should also be evaluated as a possible explanation for the reported experimental results. At this purpose we studied a 5 nm thick PCBM film, with a similar optical density of the intermixed sample, pumping at 520 nm. The plot in Figure 3d contains the time trace at 750 nm, assigned to PCBM Sn ← S1 PA peak (see Supplementary Information Figure S4 and S5). The signal amplitude, without any normalization, clearly shows that the role of direct PCBM excitation is negligible. We infer that direct photo-excitation of PCBM contributes less than 10% of the signal measured in the P3HT/PCBM sample.

The electronic energy transfer occurs on a time scale faster than our resolution (≈200 fs). The broad PA band assigned to PCBM is formed during pump excitation and it is present from the very beginning in our transient spectra. This explains the different ratio between GSB and PA in the P3HT/PCBM sample with respect to the one in pristine P3HT.

On the longer timescale, we observe a build-up of the GSB with a time constant of 130 ps along with a correlated increase in the PA band centered at 750 nm. The return of GSB in transient spectra is a rather unusual phenomenon that is associated to back charge transfer following the initial energy transfer in D-A dyads of different type13,21,22. Here it can be understood as the generation of polaron states in P3HT via hole-transfer from PCBM. Though the absorption bands of P3HT+ and PCBM singlet overlap, due to higher oscillator strength of the polaron (see Supplementary Information S.4), its contribution dominates the dynamics. The overlap of the bands can also explain the apparent slower growth rate in the polaron PA with respect to the GSB. This is also confirmed by the slow PA growth at 900 nm (see Figure 4a) after the initial PP recombination, and this will be discussed in detail later. In neat P3HT the dominant contribution at 900 nm is the (Sn ← S1) transition (Figure 4b), but in the ultrathin diffuse layer such a contribution is absent, consistent with the conjectured electronic energy transfer.

Figure 4: Thickness dependent TrAMP dynamics.
Figure 4

(a) TrAMP kinetic at λprobe = 900 nm for 5 nm/5 nm bilayer of P3HT/PCBM.A multiexponential fit (A(t)) is also shown. (b) Similar kinetic and the fit (B(t)) for a 5 nm film of P3HT. TrAMP kinetics for the bilayers with 10 nm (c), 20 nm (d) and 50 nm (e) thicknesses of P3HT with a constant 5 nm layer of PCBM on the top. Also shown are the fits obtained by a linear superposition of A(t) and B(t) in each of the three cases.

Hence, in the considered molecularly-mixed morphology, the photo-physical picture for charge generation can be interpreted as a two-step process. First, electronic energy transfer happens, as the dominant process, from P3HT to PCBM (D* + A → D + A*); then it is followed by a hole transfer from the excited PCBM back to P3HT, (A* + D → D+ + A).


The phenomenon of ultrafast energy transfer before charge transfer in systems commonly utilized in organic BHJ solar cells is puzzling and contradicting common beliefs. In order to further test our interpretation we performed experiments on tri-layered samples where charge transfer can be effectively blocked by inserting a large band-gap thick interlayer of Poly-Vinyl Acetate (PVA) between P3HT and PCBM. Measurements on the tri-layer films are reported with thin (<5 nm) and thick (10 nm) PVA layers (Figures 5b and 5d respectively). When the PVA layer is thin the GSB of P3HT fully decays to zero in 2 ps, again leaving a PA without GSB for longer time delays. The lack of GSB is consistent with ultrafast electronic energy transfer even in presence of the thin PVA interlayer. We can set an upper limit for the time scale of the process that is again within the excitation process, about 200–300 fs. The steady PA is assigned to Sn ← S1 PCBM electronic transition. In presence of the interlayer, however, there is neither delayed build up of GSB nor PA at longer time. We suppose that because of the very large surface roughness, there is no substantial reduction in P3HT-PCBM average distance when a thin interlayer is deposited, preserving the dipole-dipole electronic energy transfer, while the charge transfer is suppressed by the lack of wavefunction overlap. When the interlayer is thick (Figure 5d), pure P3HT dynamics, similar to Figure 3c can be observed. In particular there is a longer lived GSB due to the singlet states. This confirms that both electronic energy transfer and charge transfer can be suppressed by a thick interlayer.

Figure 5: Ultrafast dynamics in the trilayers of P3HT, PVA and PCBM.
Figure 5

(a) Illustration of the possible morphology of the bilayer with a 5 nm interlayer of PVA.(b) TrAMP kinetics at 580 nm (GSB) and 750 nm (PA) in the bilayer with a thin (<5 nm) interlayer of PVA and d) with a thick (10 nm) layer. (c) The energy level scheme24 of P3HT/PCBM with the hole transfer pathway from PCBM to P3HT, which is blocked with the introduction of PVA.

In the standard BHJ the intermixed doped region is in between the donor and acceptor clusters23. In order to include exciton diffusion into our picture, we perform TrAMP measurements on P3HT/PCBM bilayers by increasing the thickness of the P3HT layer. Four samples are considered where-in 5 nm, 10 nm, 20 nm and 50 nm thick P3HT films are covered with 5 nm of PCBM. Each of these samples simulates the spatial extent for exciton diffusion in P3HT rich domains in a BHJ. The probe wavelength in these experiments is tuned to 900 nm, to have a signature of singlet exciton absorption in P3HT. As discussed earlier however, other species may also contribute at this wavelength.

The 5/5 nm bilayer shows an instantaneous PA that reduces by only a few percent within 2 ps, it stays flat and then it increases in 100 ps time scale (see Figure 4a). According to our model this signal contains contributions from PP recombination at initial time, and from P3HT polarons at longer delays. In Figure 4b we show the signal obtained from a pure 5 nm P3HT film. The samples in Figures 4a, b may represent the two distinct morphologies present in a BHJ: the well intermixed P3HT/PCBM interface and the pristine P3HT domain. The other three samples (10/5, 20/5 and 50/5 nm) show intermediate behaviors, that can be simulated as a linear combination of the traces in 4a and 4b plots. This is shown by first fitting multi-exponential functions, A(t) and B(t), to the time traces in Figures 4a,b respectively. Linear combination of A(t) and B(t) reproduces quite well all the other data, enabling us to infer a relative weight of the two components in each of the samples. The sample with 10 nm P3HT (Figure 4c) shows almost equal contribution from the pristine phase and the intermixed region. The sample with 20 nm thick P3HT (Figure 4d) shows 25% contribution from the intermixed region and the as above 50 nm sample (Figure 4e) shows less than 10% contribution. The interface specific dynamics are perceivable only when the thickness of the P3HT layer is less than 10 nm. This length scale stands for the balance between the electronic energy transfer and the exciton diffusion limited processes25. In a standard BHJ blend such dynamics are averaged out in the pump probe measurements and due to the spectral overlap and the consequent congestion of signals, charge transfer seems the dominant event.

To further support the proposed electronic energy transfer (EET) mechanism occurring at the P3HT/PCBM molecular interface on an ultrafast time scale we consider, in their simplest forms, the transfer rate equations ruling EET and CT processes26,27, reported in the Equations 1 and 2 respectively: and In Equation 1, VC and VD are the electronic coupling matrix elements for Förster and Dexter mechanism28,29,30,31,32 and J is the spectral overlap27. Förster and Dexter electronic energy transfer mechanisms coexist for singlet-singlet energy transfer. The Förster term has ~1/r3 distance dependence and it is long range, r > 10 Å, while and the Dexter term has ~exp(βr) distance dependence and it is short range, r < 10 Å27.

Equation 2 reports the transfer rate constant for a CT process27 where VCT is the electronic coupling matrix element term, λ is the total reorganization energy and ΔG is the free energy difference term between reactants and products27,33. Details about the EET and CT parameters used in equations 1 and 2 are reported and discussed in the Supplementary Information (S.5).

Figure 6 reports both EET (blue line) and CT (red line) transfer rates (equations 1 and 2) for a selection of parameters (see Supplementary Information for details) in a time window from fs to ms.

Figure 6: Charge and Energy transfer rate calculations.
Figure 6

Electronic energy transfer (EET) transfer rate (blue line, eq. 1) and charge transfer (CT) rate (red line, eq. 2) as a function of the donor-acceptor distance r (logarithmic scale). Dotted lines represent the Förster like (~1/r6) and the Dexter like (~exp(−βr)2) contribution to the EET transfer rate. Details about EET and CT parameters present in eq. 1 and 2 are reported in Supplementary Information (Section S5).

Considering the P3HT/PCBM interface as molecular in nature and, as Density Functional Theory (DFT) calculations34,35, provide optimized intermolecular distance between the P3HT and PCBM centers around 6–9 Å, we focus the transfer rate analysis on the 6 Å to 1 nm spatial range. As reported in Figure 6, in this spatial range EET is faster than CT mechanism and the time scales obtained are in good agreement with those observed in the experiments, with EET in the ultrafast time regime (from few fs to hundreds of fs, Figure 3) and the CT, or the charge separation process, in the picosecond time scales8,36,37,38,39. The short range EET is due to Dexter coupling that out-competes both Förster and CT. According to the theory developed by Scholes and Ghiggino28,29,30,31, the Dexter exchange integral can be well represented as a through-configuration exciton resonance interaction term where the overlap integrals between neutral-excited- (Ψ1(D*/A), Ψ4(D/A*)) and ionic-like (Ψ2(D+/A), Ψ3(D/A+)) electronic wavefunctions play a major role, giving the short range dependence contribution. Due to interface level alignment of type II, amongst ionic-like configurations, only Ψ2 is however expected to play a major role in the overall wavefunction superposition30.

Calculations based on such equations support the experimental observation that EET is faster than CT (at the molecular level). Here the equations 1 and 2 are used just to support the experimental evidence of an ultrafast EET mechanism, without pretending to extend this physical scenario to the whole range of D/A distances and for any kind of D/A blend morphologies.

In conclusion we report here the dynamics occurring in the finely intermixed phase of P3HT and PCBM. We show that the expected charge generation process is mediated by an initial ultrafast electronic energy transfer from the polymer to the acceptor molecule. The initial energy transfer (D* + A → D + A*) takes place in less than 200 fs. Charge separation is a secondary process occurring between the excited acceptor and the polymer domain on the 100 ps time scale. Such intermixed domains are the actual border regions between D and A clusters in the photovoltaic active layer based on BHJ. In this frame electronic energy transfer should be an important event in the primarily step for charge generation, usually underestimated in the description of the photovoltaic event. This, first of all, brings to some considerations on the role and actual values assigned so far to the exciton diffusion length. The critical length scale of 10 nm we found here is actually the convolution among the exciton diffusion, the molecular inter-diffusion and the average distance which allow for electronic energy transfer at the interface. Finally we note that Ward et al.15 have recently shown a possible energy transfer pathway from copolymers such as PCDTDBT to PCBM. Thus, the process we highlight here is not necessarily specific to P3HT/PCBM, but it may be considered as an unavoidable paradigm for the concept of organic photovoltaic.


Sample preparation

The poly(3-hexylthiophene) (P3HT) (Merk, >99% regioregular) was diluted in a dichlorobenzene (DCB) solution at different weighting ratio (1 mg/mL, 5 mg/mL) and heated at 70°C degrees for 1 hour. The solution was spin casted on a clean 250 μm thick fused silica substrate at 4000 rpm or 1000 rpm for 45 seconds, respectively, in order to get a film thickness of 5 or 50 nm. Note that the freshly-spun P3HT films have been dried on a hotplate at 70° for 10 min prior to spin-coating the top layer. For the production of the bilayer we adopt the spin-coating sequential approach using an orthogonal solvent combination (dichlorobenzene and dichloromethane) to process the [6,6]-phenyl C61-butyric acid methyl ester (PCBM) layer on top of P3HT preventing the re-dissolution of the P3HT underneath. The PCBM was dissolved in a dichloromethane solution (20 mg/mL), briefly heated at 40°C to ensure maximal dissolution. The PCBM solution was casted at 4000 rpm for 45 seconds onto the P3HT layer to obtain a thickness of 5 nm. In order to increase the order of the P3HT layer before PCBM deposition we perform a thermal annealing, heating the sample to 140 degrees for 5 minutes.


For the ultrafast experiments, laser pulses (40 fs, 250 kHz) at 800 nm were generated using Coherent Micra Ti:Saphire oscillator in conjunction with Coherent RegA 9040 amplifier. Part of the laser output was used to pump Coherent OPA in order to generate pump pulsed at 520 nm. The other part of the pulse was used to pump a sapphire plate (2 mm) to generate white light continuum as the probe pulse. The delay between the pump and probe pulses was controlled by a computer controlled translation stage. Both the pulses were made collinear using a beam splitter before launching into the TrAMP setup.

The TrAMP system can be thought to be a misaligned concentric optical cavity; as shown in figure 1, one of the mirrors focuses the beam and the second mirror collimates the beam and sends it back. At proper incidence conditions, a multi-reflection can be achieved between the two mirrors with the ray tracing an ellipse on the sample (as well as on the mirrors). The number of reflections can be controlled by tuning the angle of incidence and the mirror alignment or alternatively, the beam can be extracted from the cavity using another smaller mirror.

A high pass filter was used to remove the pump pulse; the probe pulse was dispersed using a monochromator and detected using a lock-in, photo-diode system.


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ARSK and GL acknowledge the financial support of the Marie-Curie grant under the FP7 project PITNGA-2009-237900(ICARUS). The authors also thank Simone Guarnera, Dario Polli and Luca Frezza for help and discussions. The authors also acknowledge the financial support from Italian Ministry of University Research (project PRIN 2010-2011 “DSSCX”, Contract 20104XET32) and POCAONTAS (Grant agreement No: 316633) is also acknowledged.

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  1. Dipartimento di Fisica, Piazza Leonardo da Vinci 32, 20133 Milano, Italy

    • Ajay Ram Srimath Kandada
    •  & Guglielmo Lanzani
  2. Center for Nano Science and Technology @ PoliMi, Istituto Italiano di Tecnologia, via Pascoli 70/3 20133 Milano, Italy

    • Ajay Ram Srimath Kandada
    • , Giulia Grancini
    • , Annamaria Petrozza
    • , Stefano Perissinotto
    • , Daniele Fazzi
    • , Sai Santosh Kumar Raavi
    •  & Guglielmo Lanzani


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The experimental set-up was developed by A.R.S.K.; the sample was prepared by G.G., A.R.S.K. and S.P. The measurements were done by A.R.S.K. and S.S.K.R. The data have been analyzed by A.R.S.K., G.G., A.P. and G.L. The experiment was conceived by G.L., A.P. and A.R.S.K. Theoretical calculations have been carried out by D.F. All the authors contributed to writing of the paper.

Competing interests

The authors declare no competing financial interests.

Corresponding author

Correspondence to Guglielmo Lanzani.

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    Ultrafast Energy Transfer in Ultrathin Organic Donor/Acceptor Blend

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