2015
DOI: 10.1016/j.snb.2015.07.055
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Distributed feedback lasers based on perylenediimide dyes for label-free refractive index sensing

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Cited by 32 publications
(40 citation statements)
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“…The photostability half-life is defined as the time or the number of pump pulses at which the emitted laser intensity decays to half of its maximum value. Its sensitivity in the biological range (n = 1.33) is S b = 32 nm/RIU [16], which is comparable to those reported for other singlelayer waveguide DFB biosensors [6,10,12,13]. The sensor resolution was calculated by fitting the central wavelength emission by a center of mass calculation [15], obtaining a resolution of 0.8 pm and a LOD of 2.5 x 10 -5 RIU [16].…”
Section: -Results and Discussionsupporting
confidence: 74%
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“…The photostability half-life is defined as the time or the number of pump pulses at which the emitted laser intensity decays to half of its maximum value. Its sensitivity in the biological range (n = 1.33) is S b = 32 nm/RIU [16], which is comparable to those reported for other singlelayer waveguide DFB biosensors [6,10,12,13]. The sensor resolution was calculated by fitting the central wavelength emission by a center of mass calculation [15], obtaining a resolution of 0.8 pm and a LOD of 2.5 x 10 -5 RIU [16].…”
Section: -Results and Discussionsupporting
confidence: 74%
“…2). Its lasing threshold and the photostability half-life are 200 kW/cm 2 and around 20 min (1.2×10 4 pump pulses), respectively [16]. The photostability half-life is defined as the time or the number of pump pulses at which the emitted laser intensity decays to half of its maximum value.…”
Section: -Results and Discussionmentioning
confidence: 99%
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“…The DFB emission wavelength ( DFB ) appears close to the wavelength at which the cavity resonates (λ Bragg ), which is determined by the grating period (Λ), the diffraction order (m) and the effective refractive index (n eff ), according to the expression:The n eff parameter depends on the active film thickness (h f ) and on the refractive index of active film, substrate and cover layer (n f , n s and n c , respectively). The principle of operation of previously reported DFB-based bulk refractive index sensors consists on analysing changes in λ DFB upon the deposition over the device of liquid superstrates with different n c values [10,11]. In comparison to other refractive index sensors, organic DFB lasers are very attractive because of their high sensitivity and resolution, simple fabrication and integration with other devices, wavelength tuning capability and small size.…”
mentioning
confidence: 99%