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We observe that the samples deposited from chloroform solution without the heating steshow PL spectra dominated by the Β -phase emission (see, Ref.). The presence of glassy phase-only PL in our samples thus confirms that the solution heating results in the irreversible dissolution of the Β -phase aggregates are initially present in the solution, even if the films are deposited by using solutions returned at room temperature (Ref.).
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We observe that the samples deposited from chloroform solution without the heating step show PL spectra dominated by the Β -phase emission (see, Ref.). The presence of glassy phase-only PL in our samples thus confirms that the solution heating results in the irreversible dissolution of the Β -phase aggregates are initially present in the solution, even if the films are deposited by using solutions returned at room temperature (Ref.).
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We observe that incoherent scattering would simply result in an increase in the photon travel time in the active materials, resulting in an ASE intensity enhancement, without the formation of narrow features. Moreover, the evidence of narrow emission peaks only in the ASE spectral region evidences that the observed effect is related to light amplification in the sample, thus excluding PL intensity modulation due to wavelength dependent scattering in the film that should be observed in all the emission range.
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We observe that incoherent scattering would simply result in an increase in the photon travel time in the active materials, resulting in an ASE intensity enhancement, without the formation of narrow features. Moreover, the evidence of narrow emission peaks only in the ASE spectral region evidences that the observed effect is related to light amplification in the sample, thus excluding PL intensity modulation due to wavelength dependent scattering in the film that should be observed in all the emission range.
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