Abstract:The principles and the basic performance of laser remote sensors are classified and compared. The present state of the art of laser remote sensing techniques and applications for monitoring environmental parameters are reviewed. Future possibilities and requirements of research and development of these techniques are discussed.
“…[2][3][4][5][6][7][8][9][10][11][12] The low-power PA technique has been predominantly utilized in the field of spectroscopy, [11][12][13][14][15][16][17][18] with substantial applications in trace gas detection. 5,[19][20][21][22][23] It exhibited significantly higher sensitivity than most other techniques, [24][25][26][27] with concentration sensitivity in the parts per billion. [3][4][5]25,27 PA spectroscopy is a powerful analytical tool for examining the optical absorption properties of solids as it directly measures the energy absorbed by the material on exposure to light.…”
Section: Introductionmentioning
confidence: 99%
“…5,[19][20][21][22][23] It exhibited significantly higher sensitivity than most other techniques, [24][25][26][27] with concentration sensitivity in the parts per billion. [3][4][5]25,27 PA spectroscopy is a powerful analytical tool for examining the optical absorption properties of solids as it directly measures the energy absorbed by the material on exposure to light. 28 Conventional optical absorption/transmission spectroscopy requires a sample with a specialized surface as the scattering would significantly affect the accuracy of the measurement of optical absorption coefficient.…”
Abstract. An inexpensive noncontact photoacoustic (PA) imaging system using a low-power continuous wave laser and a kilohertz-range microphone has been developed. The system operates in both optical and PA imaging modes and is designed to be compatible with conventional optical microscopes. Aqueous coupling fluids are not required for the detection of the PA signals; air is used as the coupling medium. The main component of the PA system is a custom designed PA imaging sensor that consists of an air-filled sample chamber and a resonator chamber that isolates a standard kilohertz frequency microphone from the input laser. A sample to be examined is placed on the glass substrate inside the chamber. A laser focused to a small spot by a 40× objective onto the substrate enables generation of PA signals from the sample. Raster scanning the laser over the sample with micrometer-sized steps enables high-resolution PA images to be generated. A lateral resolution of 1.37 μm was achieved in this proof of concept study, which can be further improved using a higher numerical aperture objective. The application of the system was investigated on a red blood cell, with a noiseequivalent detection sensitivity of 43,887 hemoglobin molecules (72.88 × 10 −21 mol or 72.88 zeptomol). The minimum pressure detectable limit of the system was 19.1 μPa. This inexpensive, compact noncontact PA sensor is easily integrated with existing commercial optical microscopes, enabling optical and PA imaging of the same sample. Applications include forensic measurements, blood coagulation tests, and monitoring the penetration of drugs into human membrane.
“…[2][3][4][5][6][7][8][9][10][11][12] The low-power PA technique has been predominantly utilized in the field of spectroscopy, [11][12][13][14][15][16][17][18] with substantial applications in trace gas detection. 5,[19][20][21][22][23] It exhibited significantly higher sensitivity than most other techniques, [24][25][26][27] with concentration sensitivity in the parts per billion. [3][4][5]25,27 PA spectroscopy is a powerful analytical tool for examining the optical absorption properties of solids as it directly measures the energy absorbed by the material on exposure to light.…”
Section: Introductionmentioning
confidence: 99%
“…5,[19][20][21][22][23] It exhibited significantly higher sensitivity than most other techniques, [24][25][26][27] with concentration sensitivity in the parts per billion. [3][4][5]25,27 PA spectroscopy is a powerful analytical tool for examining the optical absorption properties of solids as it directly measures the energy absorbed by the material on exposure to light. 28 Conventional optical absorption/transmission spectroscopy requires a sample with a specialized surface as the scattering would significantly affect the accuracy of the measurement of optical absorption coefficient.…”
Abstract. An inexpensive noncontact photoacoustic (PA) imaging system using a low-power continuous wave laser and a kilohertz-range microphone has been developed. The system operates in both optical and PA imaging modes and is designed to be compatible with conventional optical microscopes. Aqueous coupling fluids are not required for the detection of the PA signals; air is used as the coupling medium. The main component of the PA system is a custom designed PA imaging sensor that consists of an air-filled sample chamber and a resonator chamber that isolates a standard kilohertz frequency microphone from the input laser. A sample to be examined is placed on the glass substrate inside the chamber. A laser focused to a small spot by a 40× objective onto the substrate enables generation of PA signals from the sample. Raster scanning the laser over the sample with micrometer-sized steps enables high-resolution PA images to be generated. A lateral resolution of 1.37 μm was achieved in this proof of concept study, which can be further improved using a higher numerical aperture objective. The application of the system was investigated on a red blood cell, with a noiseequivalent detection sensitivity of 43,887 hemoglobin molecules (72.88 × 10 −21 mol or 72.88 zeptomol). The minimum pressure detectable limit of the system was 19.1 μPa. This inexpensive, compact noncontact PA sensor is easily integrated with existing commercial optical microscopes, enabling optical and PA imaging of the same sample. Applications include forensic measurements, blood coagulation tests, and monitoring the penetration of drugs into human membrane.
“…The multi-wavelength DIAL system is, however, capable of high-precision measurement compared to a dual-DIAL and can also simultaneously monitor several target elements (Fukuchi et al 1998). Thus, depending on applications, DIAL uses different probing frequencies (Baumgartner and Byer 1978, Measures 1984, Kobayashi 1987. The initial DIAL measurements were confined to making humidity profiles and then NO 2 detection.…”
The article discusses the development and operational details of Differential Absorption LiDAR (DIAL) for the measurement of methane concentration in the semi-urban environment of Gauhati University. The system comprises two specifically selected wavelengths in 3 μm range: one is an absorbing wavelength (λ on ) and the other is non-absorbed (λ off ) by methane molecules. Pulses of 10 ns for the two wavelengths are transmitted alternately for interleaved sampling of differential absorption. The pulse repetition rate is variable between 1 and 20 Hz. The slope and integrated target approaches are adopted to calculate the methane concentration, and observed figures are compared with globally reported values.
“…Fonte: Rosário (2006). 53 Figura 3.7 Representação esquemática do conjunto fotodetector do MFRSR durante o seu funcionamento (Sayão, 2008 O sensoriamento remoto da atmosfera com a utilização do laser tornou-se um poderoso instrumento no seu estudo e, dada a sua semelhança de operação e princípios físicos com as técnicas de radar, recebeu o nome de LIDAR, acrônimo para Light Detection and Ranging (Kobayashi, 1987, Measures, 1984 (Maiman,1960). No mesmo ano, foi demonstrado o funcionamento do laser de He-Ne, que é o laser na região do visível mais conhecido (Jenkis, 1981).…”
Section: Tabelaunclassified
“…Na aplicação de monitoração de poluentes na atmosfera, os sistemas LIDAR podem fornecer, com uma fonte de laser de comprimento de onda de largura de banda estreita, informação da presença e distribuição de partículas de uns poucos nanômetros a cerca de 100 µm de diâmetro e, se o LIDAR for operado com dois sinais distintos em comprimento de onda, pode-se obter informação da concentração específica do conteúdo de gases na atmosfera, atingindo-se um nível de sensibilidade de até 0,1 ppb, no caso das concentrações moleculares (Kobayashi, 1987).…”
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