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Vocabulary practice flashcards covering photodetectors, thermal detectors, spectral lineshape analysis, and noise handling techniques.
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Detector Responsivity
The ratio of the electrical output voltage (V) to the incident radiant power (W).
Detector Sensitivity (Q(λ))
The slope of the electrical response curve of a detector plotted as a function of incident radiant power (Φ) at a specific wavelength, defined mathematically as Q(λ)=dΦdS.
Spectral Response
A plot showing detector electrical sensitivity (Q(λ)) as a function of wavelength (λ).
Candela (cd)
The SI unit of luminous intensity, defined as the luminous intensity in a given direction of a source emitting monochromatic radiation of frequency 540×1012Hz with a radiant intensity of 6831Wsr−1.
Noise Equivalent Power (NEP)
A detector performance metric defined as NEP=RvVn, where Vn is the rms detector noise voltage in VHz1/2 and Rv is the voltage responsivity in VW−1.
Specific Detectivity (D∗)
A detector performance parameter independent of detector element area (AD), calculated as D∗=NEP(AD)1/2 with units of cmHz1/2W−1.
Photovoltaic Cell
A passive photon detector operating in the visible region where radiant energy generates current at the interface of a semiconductor and a metal (e.g., Fe/Se/Ag) without external electricity.
Phototube
A photon detector in which incident radiation causes photoemission of electrons from a photosensitive cathode surface, which are collected by an anode to produce electric current.
Photomultiplier Tube (PMT)
A sensitive UV-vis photon detector consisting of a photocathode, anode, and a series of biased dynodes that produce an electron multiplication cascade yielding a 106 to 107 amplification factor.
Silicon Photodiode
A photon detector based on a reverse-biased p-n or p-i-n junction formed on a silicon chip; radiation creates electron-hole pairs in the depletion layer, producing a current proportional to radiant power.
Photoconductivity Detector
An IR detector constructed from semiconductors (e.g., PbS, PbSe, InSb, HgCdTe) that acts as a light-dependent resistor whose electrical resistance decreases upon absorbing photons.
Pneumatic Cell (Golay Cell)
An IR thermal detector in which radiation heats gas in an enclosed chamber, causing pressure changes that alter the capacitance of a thin flexible membrane.
Thermocouple Detector
An IR thermal detector consisting of a thin junction between two dissimilar metals (such as Bi-Sb) that generates a temperature-dependent electrical potential.
Bolometer
A thermal detector operating as a resistance thermometer made from intrinsic semiconducting materials (such as Ge or Si) that measures temperature-dependent resistance changes ΔR(T).
Pyroelectric Detector
An IR thermal detector constructed from single crystals of pyroelectric insulator material (such as triglycine sulfate, TGS) that exhibits temperature-dependent surface charge polarization.
Photodiode Array (PDA)
A multichannel detector comprising an integrated circuit array of silicon photodiodes (typically 256, 512, 1024, or 2048 junctions) capable of recording an entire spectrum simultaneously.
Charge-Coupled Device (CCD)
A multichannel charge-transfer detector where incident photons generate charges on MOS capacitors that are stored in potential wells and read out serially in a destructive mode.
Charge-Injection Device (CID)
A multichannel charge-transfer detector where generated positive charge is collected beneath negatively biased capacitor plates and read out serially in a non-destructive mode.
Homogeneous Line Broadening
Line broadening processes (such as natural and collisional broadening) that affect all individual atoms or molecules in an ensemble identically.
Inhomogeneous Line Broadening
Line broadening processes (such as Doppler broadening) that affect different atoms or molecules in an ensemble unequally.
Natural Line Broadening
Homogeneous line broadening dictated by the Heisenberg Uncertainty Principle (ΔE≥τℏ), where the finite excited state lifetime (τ) results in a Lorentzian energy distribution.
Collisional Broadening
Homogeneous line broadening caused by atomic/molecular collisions that distort electron energy levels and shorten excited state lifetimes through quenching, producing a Lorentzian line shape.
Doppler Broadening
Inhomogeneous line broadening caused by the thermal motion of particles relative to the detector (following a Boltzmann distribution of speeds), resulting in a Gaussian energy distribution.
Instrumental Broadening
Practical line broadening caused by spectrometer imperfections such as optical beamspread, slit width, aperture diffraction, and finite detector resolution, typically dominating fundamental broadening by a factor of at least 1000.
Voigt Profile
A realistic spectral band profile generated by the mathematical convolution integral of Gaussian and Lorentzian profiles.
Pseudo-Voigt Function
A simplified linear combination sum function of Lorentzian L(x) and Gaussian G(x) profiles weighted by a parameter η, given by pV(x)=η⋅L(x)+(1−η)⋅G(x).
Difference Amplifier
An analog circuit stage with two inputs that amplifies the difference between sample and reference signals, suppressing common-mode electrical noise.
Modulation
The process of encoding a low-frequency or DC analytical signal onto a high-frequency carrier wave to shift the signal away from low-frequency 1/f noise.
Demodulation
The process of extracting the original low-frequency analytical signal from a modulated carrier wave using rectification and low-pass filtering.
Ensemble Averaging
A digital noise reduction method that co-adds n repeated scans to improve the Signal-to-Noise Ratio by a factor of n, relying on the random cancellation of uncorrelated noise.
Boxcar Averaging
A digital smoothing filter that divides spectral data into equal, non-overlapping windows of width j=2n+1 points and replaces the points in each window with their centroid average.
Moving Average Filter
A linear digital smoothing technique in which a window of width j=2n+1 points slides sequentially across the dataset one point at a time to calculate local averages.
Savitzky-Golay Smoothing
A digital filtering procedure that performs a local polynomial least-squares fit across 2n+1 points using pre-calculated set weighting coefficients, smoothing noise while preserving peak shapes.
Chemical Noise
Uncontrollable noise inherent to the chemical system or sample, such as thermal fluctuations, humidity shifts, or chemical equilibrium changes.
Fundamental Noise
Noise types (such as thermal noise and shot noise) arising from the physical nature of light and matter that cannot be completely eliminated from measurements.
Non-Fundamental Noise
Noise arising from external, environmental, or instrumental sources (such as power line hum or flicker noise) that can theoretically be eliminated.
Noise Power Spectrum (NPS)
A plot showing mean-square noise per unit frequency interval (V2Hz−1) as a function of frequency (Hz).
Flicker Noise (1/f Noise)
A non-fundamental, frequency-dependent random noise characterized by significant amplitudes at low frequencies, manifesting as slow signal or baseline drift.
White Noise
Random noise whose power spectral density is constant across all frequencies in the frequency spectrum.
Interference Noise
Non-fundamental, non-random noise occurring at specific, discrete frequencies due to electromagnetic coupling with external sources (e.g., 60Hz power line hum).
Thermal Noise (Johnson-Nyquist Noise)
A fundamental white noise caused by thermal agitation of electrons in resistive circuit components, which drops to zero at 0K.
Shot Noise
A fundamental white noise caused by random statistical fluctuations in the arrival of discrete, quantized particles (photons or electrons) across junctions or energy barriers.
Limit of Detection (LOD)
The lowest analyte concentration or signal level that can be reliably distinguished from baseline noise, conventionally defined where the Signal-to-Noise Ratio is 3 (SNR=3).