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Eversole, J.D.4
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54
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0042894180
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A two-lens system with f/4 collection was used
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A two-lens system with f/4 collection was used.
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55
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0042393262
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We used a flash-lamp-pumped, frequency-quadrupled Nd:YAG laser having a non-Gaussian spatial profile, and significant shot-to-shot variations in intensity
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We used a flash-lamp-pumped, frequency-quadrupled Nd:YAG laser having a non-Gaussian spatial profile, and significant shot-to-shot variations in intensity.
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56
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0000704494
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An ink jet aerosol generator
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Bottiger JR, Deluca PJ, Stuebing EW, VanReenen DR. An ink jet aerosol generator. J Aerosol Sci 1998;29(suppl 1), s965-966.
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(1998)
J Aerosol Sci
, vol.29
, Issue.1 SUPPL.
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Bottiger, J.R.1
Deluca, P.J.2
Stuebing, E.W.3
VanReenen, D.R.4
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57
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0041391147
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The Q-switched UV laser is either the 266-nm, fourth harmonic of a Nd:YAG laser [30- or 70-ns pulse duration (Spectra Physics models X-30 or Y-70)]. or the 351 -nm, third-harmonic of a Nd: YLF laser [120-ns pulse duration (Quantronix)]. The Q-switched laser fires within about 3 μs of the trigger pulse, during which time the particle travels (about 10 m/s) less than 40 μm. This vertical displacement is compensated for by a small vertical displacement of the focal volume of the two diode-laser beams from the UV laser beam (which is focused to the focal point of the reflecting objective)
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The Q-switched UV laser is either the 266-nm, fourth harmonic of a Nd:YAG laser [30- or 70-ns pulse duration (Spectra Physics models X-30 or Y-70)]. or the 351 -nm, third-harmonic of a Nd: YLF laser [120-ns pulse duration (Quantronix)]. The Q-switched laser fires within about 3 μs of the trigger pulse, during which time the particle travels (about 10 m/s) less than 40 μm. This vertical displacement is compensated for by a small vertical displacement of the focal volume of the two diode-laser beams from the UV laser beam (which is focused to the focal point of the reflecting objective).
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58
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0042894177
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The ICCD camera (Princeton Instruments) is placed at the exit port of the spectrograph (Acton model SP-150 with 300 groove/mm grating blazed at 500 nm, numerical aperture 0.125, input slit width 1 mm). The ICCD detector's image intensifier acts as a fast shutter, opening when the targeted particle is illuminated by the UV laser. A long-pass filter is placed in front of the spectrograph to block elastically scattered light and to pass the fluorescence
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The ICCD camera (Princeton Instruments) is placed at the exit port of the spectrograph (Acton model SP-150 with 300 groove/mm grating blazed at 500 nm, numerical aperture 0.125, input slit width 1 mm). The ICCD detector's image intensifier acts as a fast shutter, opening when the targeted particle is illuminated by the UV laser. A long-pass filter is placed in front of the spectrograph to block elastically scattered light and to pass the fluorescence.
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59
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85088001808
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3
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3.
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60
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85088002802
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3, geometric mean diameter ≈0.18 μm, and log-normal standard deviation ≈0.4. Thus we would expect the ≈ 100 particles to occupy a spherical sample volume with 10-μm radius
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3, geometric mean diameter ≈0.18 μm, and log-normal standard deviation ≈0.4. Thus we would expect the ≈ 100 particles to occupy a spherical sample volume with 10-μm radius.
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61
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0001050948
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Determination of particle-size distribution and concentration of cigarette smoke by a light-scattering method
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Okada T, Matsunuma K. Determination of particle-size distribution and concentration of cigarette smoke by a light-scattering method. J Colloid Interface Sci 1974;48:461-469.
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(1974)
J Colloid Interface Sci
, vol.48
, pp. 461-469
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Okada, T.1
Matsunuma, K.2
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62
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0000114408
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Spectrally resolved absolute fluorescence cross sections for bacillus spores
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Faris GW, Copeland RA, Mortelmens K, Bronk BV. Spectrally resolved absolute fluorescence cross sections for bacillus spores. Appl Opt 1997;36:958-967.
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(1997)
Appl Opt
, vol.36
, pp. 958-967
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Faris, G.W.1
Copeland, R.A.2
Mortelmens, K.3
Bronk, B.V.4
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63
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Gelbachs and Birnbaum (Ref. 64) used the 488-nm line of an argonion laser to excite fluorescence from atmospheric aerosols. They spectrally dispersed the fluorescence into four large bands, but were unable to obtain detailed spectra or single particle spectra. They noted that if "one type of aerosol predominates, such as cigarette smoke or pollen, a low resolution spectrum," may be adequate. They also suggested that such an instrument may be useful for detecting and identifying aerosol emissions (e.g., fly ash (Ref. 65)) from stacks
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Gelbachs and Birnbaum (Ref. 64) used the 488-nm line of an argonion laser to excite fluorescence from atmospheric aerosols. They spectrally dispersed the fluorescence into four large bands, but were unable to obtain detailed spectra or single particle spectra. They noted that if "one type of aerosol predominates, such as cigarette smoke or pollen, a low resolution spectrum," may be adequate. They also suggested that such an instrument may be useful for detecting and identifying aerosol emissions (e.g., fly ash (Ref. 65)) from stacks.
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64
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0015670244
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Fluorescence of a atmospheric aerosols and lidar implications
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Gelbwachs J, and Birnbaum M. Fluorescence of a atmospheric aerosols and lidar implications. Appl Opt 1973;12:2442-2447.
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(1973)
Appl Opt
, vol.12
, pp. 2442-2447
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Gelbwachs, J.1
Birnbaum, M.2
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65
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0042894178
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Laser-excited fluorescence techniques in air pollution monitoring
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Wehry EL, editor. New York: Plenum; Chapter 5
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Birnbaum M. Laser-excited fluorescence techniques in air pollution monitoring. In: Wehry EL, editor. Modern Fluorescence Spectroscopy, Vol. 1. New York: Plenum; 1976. Chapter 5.
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(1976)
Modern Fluorescence Spectroscopy
, vol.1
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Birnbaum, M.1
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