Date of download: 6/22/2016 Copyright © 2016 SPIE. All rights reserved. Experimental setup of the optical parametric oscillator (OPO)-based photoacoustic.

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Date of download: 6/22/2016 Copyright © 2016 SPIE. All rights reserved. Experimental setup of the optical parametric oscillator (OPO)-based photoacoustic detector for biomedical applications: DBR, 1064 nm distributed Bragg reflector laser; CLDD, compact laser diode driver; Func.Gen., function generator to drive CLDD; ISO, 30 dB optical isolator at 1064 nm; Amp, fiber amplifier; OPO, singly resonant optical parametric oscillator; PPLN, periodically polled lithium niobate crystal; PA cell, photoacoustic cell with Silcosteel coating. Figure Legend: From: Optical parametric oscillator-based photoacoustic detection of hydrogen cyanide for biomedical applications J. Biomed. Opt. 2013;18(10): doi: /1.JBO

Date of download: 6/22/2016 Copyright © 2016 SPIE. All rights reserved. Long-term frequency stability of the DBR seed laser at a constant current of 250 mA and a constant temperature of 25°C, which was <50 MHz ( cm−1) over 4.5 h. Figure Legend: From: Optical parametric oscillator-based photoacoustic detection of hydrogen cyanide for biomedical applications J. Biomed. Opt. 2013;18(10): doi: /1.JBO

Date of download: 6/22/2016 Copyright © 2016 SPIE. All rights reserved. Maximum wavelength mode-hop-free scans of the seed DBR laser up to 4.7 cm−1 at around 9390 cm−1 recorded in 10 s. Figure Legend: From: Optical parametric oscillator-based photoacoustic detection of hydrogen cyanide for biomedical applications J. Biomed. Opt. 2013;18(10): doi: /1.JBO

Date of download: 6/22/2016 Copyright © 2016 SPIE. All rights reserved. (a) Ratio between 10 ppbv of HCN and a sum of 1% of water and 5% of CO2 for a pressure of 200 mbar in the wavelength range of 3200 to 3400 cm−1 based on HITRAN database (Ref. 53); (b)–(d) Simulated spectra [using HITRAN database (Ref. 53)] at a pressure inside the photoacoustic cell of 200 mbar for 1% of water (black-dashed line), 5% of CO2 (red-dotted line), and 10 ppbv of HCN (blue solid line) for the wavelength ranges: (b) 3265 to 3270 cm−1, (c) 3285 to 3290 cm−1, (d) 3329 to 3334 cm−1. Arrows connecting the figures related to the wavelength regions for the ratio calculation (a) with simulated spectra (b), (c), and (d). Figure Legend: From: Optical parametric oscillator-based photoacoustic detection of hydrogen cyanide for biomedical applications J. Biomed. Opt. 2013;18(10): doi: /1.JBO

Date of download: 6/22/2016 Copyright © 2016 SPIE. All rights reserved. Response time of 1 ppmv of HCN from the calibration mixture cylinder when using a noncoated reduction valve. A 90% value (0.9 ppmv) is reached after 20 h. Figure insertion shows the response time of 5 min of optimized system. Figure Legend: From: Optical parametric oscillator-based photoacoustic detection of hydrogen cyanide for biomedical applications J. Biomed. Opt. 2013;18(10): doi: /1.JBO

Date of download: 6/22/2016 Copyright © 2016 SPIE. All rights reserved. HCN calibration measurements. Experimental points are the photoacoustic signal of five concentrations applied into the system. A detection limit of 0.40±0.03 ppbv was achieved. Figure Legend: From: Optical parametric oscillator-based photoacoustic detection of hydrogen cyanide for biomedical applications J. Biomed. Opt. 2013;18(10): doi: /1.JBO

Date of download: 6/22/2016 Copyright © 2016 SPIE. All rights reserved. Spectrum of HCN containing gaseous mixture from clover leaves recorded. The spectrum recorded shows the HCN peak at near cm−1 together with a water peak at near cm−1. Vertical scale is in signal from the lock-in amplifier normalized per optical laser power. Figure Legend: From: Optical parametric oscillator-based photoacoustic detection of hydrogen cyanide for biomedical applications J. Biomed. Opt. 2013;18(10): doi: /1.JBO

Date of download: 6/22/2016 Copyright © 2016 SPIE. All rights reserved. (a) Artistic impression of the experimental scheme for the HCN detection from clover leaves: air cylinder, high pressure cylinder of synthetic air; flow controllers, mechanical mass flow controllers; sample cuvette, glass cuvette with the sample to analyze; empty cuvette, empty glass cuvette for reference comparison; overpressure outlets, outlets to prevent overpressure inside the cuvettes; needle valve, Teflon needle valve to reduce the pressure inside the PA cell; valves, diaphragm isolated three-way valves; OPO, continuous wave optical parametric oscillator; PA cell, photoacoustic cell with Silcosteel coating; vacuum pump, diaphragm membrane vacuum pump. (b) Concentration dynamics of HCN emitted from 10 cut clover leaves (fresh weight 313 mg). Blue- dashed line represents an exponential fit with value t=(15.7±0.8) h. The insertion is a zoomed-in area of the dotted rectangle and it shows the response time of the system of few minutes. HCN dropped starting from 12 h reaching 0 level at 18 h due to the dehydration of leaves. Figure Legend: From: Optical parametric oscillator-based photoacoustic detection of hydrogen cyanide for biomedical applications J. Biomed. Opt. 2013;18(10): doi: /1.JBO

Date of download: 6/22/2016 Copyright © 2016 SPIE. All rights reserved. HCN concentration from exhaled breath of two subjects repeated twice for every person. HCN value of about 1.5 ppbv was measured in the laboratory air and 0 HCN level from the synthetic air. Figure Legend: From: Optical parametric oscillator-based photoacoustic detection of hydrogen cyanide for biomedical applications J. Biomed. Opt. 2013;18(10): doi: /1.JBO

Date of download: 6/22/2016 Copyright © 2016 SPIE. All rights reserved. (a) Artistic impression of the experimental scheme for the HCN detection from Pseudomonas bacteria: air cylinder, high pressure cylinder of synthetic air; flow controllers, mechanical mass flow controllers; sample cuvette, glass cuvette with the sample to analyze; empty cuvette, empty glass for reference comparison; overpressure outlets, outlets to prevent overpressure inside cuvettes; needle valve, Teflon needle valve to reduce the pressure inside the PA cell; valves, diaphragm isolated three-way valves; incubator, environmental chamber set at 37°C; OPO, continuous wave optical parametric oscillator; PA cell, photoacoustic cell with Silcosteel coating. (b) Concentration dynamics of HCN emitted by Pseudomonas bacteria (red dots) with the data from the reference cuvette (black dots). Zero time corresponds to the bacteria inoculation. The maximum value of 6.5 ppmv was reached after 77 h ( ∼ 3.2 days). New medium was added at 190 h ( ∼ 7.9 days). After adding this new substrate HCN production started again after a lag phase of 10 h reaching peak of 2.1 ppmv. Figure Legend: From: Optical parametric oscillator-based photoacoustic detection of hydrogen cyanide for biomedical applications J. Biomed. Opt. 2013;18(10): doi: /1.JBO