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Noise-equivalent power NEP

Detectivity. Detector sensitivity (1,2) is expressed in terms of the minimum detectable signal power or noise equivalent power (NEP) given in units of watts or W. The reciprocal function when normalized for detector area, M, and noise bandwidth, is defined as detectivity, D, in units of /W. Thus,... [Pg.422]

EP. The noise components may be combined with the responsivity to give the noise equivalent power (NEP) equation ... [Pg.427]

The SNR of the detected signal is defined as the ratio of the signal change (produced as a result of the intensity modulation in the measurement cell) to the noise equivalent power (NEP) of the detection system for a given average received light intensity. In order to derive a figure for the NEP, various assumptions about the optical receiver must first be made. [Pg.470]

Noise correlation function, 22 113 Noise equivalent power (NEP), 19 133 Noise spectral density, 19 134-135 Nomarski, Georges, 16 480 Nomarski-modified Wollaston prism, 16 481... [Pg.629]

The fundamental performance parameter of any detector is its noise equivalent power (NEP). This is simply the input irradiance power necessary to achieve a detector output just equal to the noise. This NEP is dependent on a number of detector and signal variables such as modulation frequency and wavelength (the input signal is defined as sine wave modulated monochromatic light), and detector area, bandwidth and temperature. [Pg.118]

There are a variety of FPA detectors available that are sensitive in the NIR spectral region. The optimal choice of detectors depends on several factors desired wavelength range, whether the application will be laboratory based or part of a process environment, the sensitivity needed to adequately differentiate sample spectra and price. The figure of merit most often used to describe detector performance is specific detectivity or D, which is the inverse of noise equivalent power (NEP), normalized for detector area and unit bandwidth. NEP is defined as the radiant power that produces a signal-to-dark-current noise ratio of unity. [Pg.28]

It is evidently insufficient to consider only the response of a detector when analysing its usefulness for a particular application. It is generally necessary to analyse both intrinsic and extrinsic noise signals and compare them with the response. The result of this comparison can be expressed in many different ways. One of the most useful is the noise-equivalent power nep which is the power of an rms signal input (in watts) required to give a response equal to the total rms noise voltage AVN. Then ... [Pg.225]

The noise level can be expressed in terms of the power incident on the detector necessary to give a signal equivalent to the noise. If the noise voltage is A EN then the noise equivalent power (NEP) is defined by... [Pg.417]

The responsivity (E) or specific detectivity (D ) and the noise equivalent power NEP (Wn), are often used to measure the sensitivity of a detector. The responsivity depends on the wavelength of the radiation and the temperature of the detector. The NEP, also called minimum detectable power, is the quotient of detector noise (N) divided by voltage responsivity (E). The D is the reciprocal of NEP, thus W = NIE and D = 1/Wn- A more sensitive detector has a smaller NEP and larger D, which results in less noise and a faster response time. [Pg.3409]

The noise equivalent power (NEP) of an infrared detector is a measure of the noise generated by the detector and is given by ... [Pg.10]

Figure 3. Broadband spectrum of a conventional 2000 Globar IR source (short dashed line), and the spectrum of the NSLS synchrotron source (solid line) limited by an experimental throughput of 4.4><1 O 4 mm2sr. This is the etendue for a 1 pm by 1 pm sample measured with an infrared microscope. The measured, background limited Noise Equivalent Power (NEP) of a Mercury Cadmium Telluride (MCT) (long dashed line) detector is shown. This detector is operated at liquid nitrogen temperatures. Figure 3. Broadband spectrum of a conventional 2000 Globar IR source (short dashed line), and the spectrum of the NSLS synchrotron source (solid line) limited by an experimental throughput of 4.4><1 O 4 mm2sr. This is the etendue for a 1 pm by 1 pm sample measured with an infrared microscope. The measured, background limited Noise Equivalent Power (NEP) of a Mercury Cadmium Telluride (MCT) (long dashed line) detector is shown. This detector is operated at liquid nitrogen temperatures.
The noise equivalent power (NEP) and specific detectivity (D ) are figures of merit that express the sensitivity of infrared detectors. The NEP is the root-mean-square (rms) power in a sinusoidally modulated radiation signal incident on the detector that gives a response equal to the rms dark noise in a 1-Hz... [Pg.235]

At the Detector Noise Moduie, the Noise Equivalent Power (NEP) associated to the detectors and the 1 // noise are calculated. In parallel, with the physical properties of the system defined, the Background Power Module calculates the background power noise due to the instmment and the Cosmic Microwave Background (CMB), Cosmic Infrared Background (CIB) and Zodiacal Light. [Pg.75]

These calculations allow us to have an idea of the background power level at the detectors. However, to include these contributions to the simulator the Noise Equivalent Power (NEP) is calculated following Lamarre s derivations (Lamarre... [Pg.90]

The Detector Noise Module calculates the Noise Equivalent Power (NEP) and the 1 // noise of the selected detection system. This module is flexible and different types of detectors will require the computation of different parameters. The detector selected for further development is the Lumped Element Kinetic inductance Detector (Doyle et al. 2008), LeKID, as it presents the most promising solution high sensitivity spectro-spatial interferometry. For the current version of the simulator, a single pixel and single mode detector is assumed for simplicity and computational reasons. [Pg.91]

This signal should be larger than the noise equivalent power NEP (this is the input power of the detector which gives the same detector output as the noise). [Pg.3]

The minimum still detectable concentration Ni of absorbing molecules is determined by the noise-equivalent power NEP, the radiation input power Pq, the absorption cross section ct, of the absorbing transition and the length L of the absorption... [Pg.3]

Noise equivalent power, NEP That optical power which produces a detector output current equal to the total noise current. A detector with input power, NEP, produces an output signal-to-noise ratio of unity. [Pg.212]

Noise equivalent power (NEP) The amount of light equivalent to the noise level of the device. Responsivity (R) The ratio of the output current to the input optical power, amperes per watt. [Pg.979]

The Raman cross-section is proportional to v and to a. The molecular cross-section of Raman spectroscopy is some ten orders of magnitude smaller than that of IR spectroscopy. However, for a typical classical detector of Raman spectra, the photomultiplier (PMT), the number of photons to produce the noise equivalent power (NEP), which is the light flux necessary to produce a signal of the same magnitude as the noise, is up to ten orders of magnitude smaller than those of detectors employed... [Pg.53]

Noise equivalent power NEP The incident radiation power generating in the detector an output signal equal to the detector internal noise corresponds to the minimum detectable flux. Measured in W/Hz NEP = - ... [Pg.3]


See other pages where Noise-equivalent power NEP is mentioned: [Pg.193]    [Pg.293]    [Pg.165]    [Pg.84]    [Pg.193]    [Pg.165]    [Pg.341]    [Pg.117]    [Pg.636]    [Pg.107]    [Pg.100]    [Pg.327]    [Pg.2517]    [Pg.123]    [Pg.965]    [Pg.470]    [Pg.345]    [Pg.194]    [Pg.1543]   
See also in sourсe #XX -- [ Pg.225 ]




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