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           An Additive Opens New Visions in Solar Cells                                                            Energy Science



           X-ray scattering insight and an associated mechanistic interpretation and a correlation with
           an enhanced performance are presented.





 ACTIVITY REPORT  2016
               bulk heterojunction (BHJ) polymer solar cell (PSC)   active layer prepared with SH-na and DIO additives
           A is regarded as a promising renewable-energy        are significantly greater than that prepared without
           resource with the advantages of low cost, flexible   additive by factors 2.0 and 1.3, respectively. For the
           devices and solution processing of a large area. The   active layers prepared without additive after a dip-
           device performance of PSC has been improved great-   ping treatment, the (100) signal also significantly
           ly via molecular design and device structure architec-  enhanced by factor 1.56, implying that a dipping
           ture in recent years. Low-bandgap polymers served to   treatment can substantially improve the crystallinity
           extend the light absorption for increased short-circuit   of PTB7.
           current (J sc) and open-circuit voltage (V oc) through a
           modulated highest occupied molecular-orbital level,   The GIWAXS profiles of the blended films also exhib-
           hence further enhancing the efficiency of power con-  ited the same ordering signals of PC 71BM aggregates
           version (PCE). Among low-bandgap polymers, fluo-     of a pure PC 71BM spin-cast film, revealing a similar
           rinated-thieno thiophene-based PTB7 is one of the    local packing structure in these films from the various
           most widely used materials in PSC with a large PCE.   routes. In contrast, GISAXS 2D patterns (Fig. 1(b))
                                                                and 1D in-plane profiles (Fig. 1(c)) show distinct
           In this reported work  of Show-An Chen (National Ts-  features in the observed q-range. The GISAXS 2D
                              1
           ing Hua University), U-Ser Jeng (NSRRC), Chun-Jen Su   patterns of the active layer without additive exhibit
           (NSRRC), Wei-Ru Wu (NSRRC) and Jey-Jau Lee (NSR-     much richer scattering features than those of other
           RC), novel additive 1-naphthalenethiol (SH-na) was   processing routes with several oblique side signals
           proposed to process the PSC active layer of PTB7:P-  oriented about ≈ 10° from the surface normal direc-
           C 71BM. Spin-casting with SH-na as additive achieved   tion; these features correspond to a faceted surface
           a large PCE. Dipping of the active layer in a methanol   morphology of the active layer processed without
           solution of a critical SH-na concentration increased   additive. The most distinct features in all GISAXS pat-
           the PCE further. They cooperatively performed syn-   terns are the strong vertical scattering stripes located
           chrotron-based X-ray-scattering techniques at TLS    near q y ≈ 0.002 Å , uniquely observed with the active
                                                                               -1
           23A1 to clarify the correlation between  morphology   layer prepared without additive. Such a scattering
           optimization and an improved PCE.                    feature indicates the existence of phase-separated
                                                                PC 71BM-rich domains with a large mean spacing, (d) ≈
           The crystallization of PTB7 and the aggregation of   314 nm, along the in-plane direction of the film.
           PC 71BM in the active layers of varied processing routes
           (with SH-na, DIO or  a dipping treatment) were inves-  Figure 1(c) shows characteristic in-plane GISAXS
           tigated with grazing incidence wide- and small-angle   profiles for the active layers without additive and
           X-ray scattering (GIWAXS and GISAXS). These GI-      that subject to the methanol/SH-na solution dip-
           WAXS profiles were extracted respectively along the   ping treatment. The large dimension, 260 nm, of the
           in-plane (q y) (Fig. 1(a)) from the corresponding 2D   oblate aggregates is modeled to be preferentially
           GIWAXS patterns, revealing a marginally preferable   oriented along the in-plane direction. An additional
           face-on orientation of PTB7 crystallites; which might   in-plane profile I (q y) is extracted at q z = 0.038 Å  (cir-
                                                                                                          -1
           be beneficial to enhance the vertical hole transport   cumventing the beamstop-blocked scattering zone,
           and thus improve the device performance. The PTB7    marked with blue squares in Fig. 1(b)) to illustrate
           (100) reflections (corresponding to ordered packing   the interference signal at q y ≈ 0.002 Å ; the profile
                                                                                                 -1
           along the polymer side chains) for the active layers   was adequately fitted (Fig. 1(c)) with oblate aggre-
           processed without additive, with DIO and with SH-    gates of the same size with mean in-plane spacing
           na, locate respectively at scattering vectors q = 0.351,   312 nm. In contrast, the GISAXS profile for an active
           0.357 and 0.355 Å , corresponding to characteristic   layer subject to a dipping treatment was best fitted
                            -1
           layer spacings 17.9, 17.6 and 17.7 Å, respectively. The   (Fig. 1(c)) with bimodal size distributions, which
           result indicates that these additives might facilitate   comprise smaller prolate aggregates and small glob-
           a tightening of the chain packing of PTB7. Moreover,   ular PC 71BM aggregates to account for the scattering
           the integrated intensities of the (100) signal of the   hump at q y ≈ 0.025 Å .
                                                                                  -1
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