Instrumental Analysis: Photodetectors, Lineshape Analysis, and Noise Handling

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Vocabulary practice flashcards covering photodetectors, thermal detectors, spectral lineshape analysis, and noise handling techniques.

Last updated 8:55 PM on 9/25/26
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43 Terms

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Detector Responsivity

The ratio of the electrical output voltage (VV) to the incident radiant power (WW).

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Detector Sensitivity (Q(λ)Q(\lambda))

The slope of the electrical response curve of a detector plotted as a function of incident radiant power (Φ\Phi) at a specific wavelength, defined mathematically as Q(λ)=dSdΦQ(\lambda) = \frac{dS}{d\Phi}.

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Spectral Response

A plot showing detector electrical sensitivity (Q(λ)Q(\lambda)) as a function of wavelength (λ\lambda).

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Candela (cdcd)

The SI unit of luminous intensity, defined as the luminous intensity in a given direction of a source emitting monochromatic radiation of frequency 540×1012 Hz540 \times 10^{12}\,\text{Hz} with a radiant intensity of 1683 W sr−1\frac{1}{683}\,\text{W\,sr}^{-1}.

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Noise Equivalent Power (NEPNEP)

A detector performance metric defined as NEP=VnRvNEP = \frac{V_n}{R_v}, where VnV_n is the rms detector noise voltage in V Hz1/2\text{V\,Hz}^{1/2} and RvR_v is the voltage responsivity in V W−1\text{V\,W}^{-1}.

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Specific Detectivity (D∗D^*)

A detector performance parameter independent of detector element area (ADA_D), calculated as D∗=(AD)1/2NEPD^* = \frac{(A_D)^{1/2}}{NEP} with units of cm Hz1/2 W−1\text{cm\,Hz}^{1/2}\,\text{W}^{-1}.

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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\text{Fe/Se/Ag}) without external electricity.

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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.

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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 10610^6 to 10710^7 amplification factor.

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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.

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Photoconductivity Detector

An IR detector constructed from semiconductors (e.g., PbS\text{PbS}, PbSe\text{PbSe}, InSb\text{InSb}, HgCdTe\text{HgCdTe}) that acts as a light-dependent resistor whose electrical resistance decreases upon absorbing photons.

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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.

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Thermocouple Detector

An IR thermal detector consisting of a thin junction between two dissimilar metals (such as Bi-Sb\text{Bi-Sb}) that generates a temperature-dependent electrical potential.

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Bolometer

A thermal detector operating as a resistance thermometer made from intrinsic semiconducting materials (such as Ge\text{Ge} or Si\text{Si}) that measures temperature-dependent resistance changes ΔR(T)\Delta R(T).

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Pyroelectric Detector

An IR thermal detector constructed from single crystals of pyroelectric insulator material (such as triglycine sulfate, TGS\text{TGS}) that exhibits temperature-dependent surface charge polarization.

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Photodiode Array (PDA)

A multichannel detector comprising an integrated circuit array of silicon photodiodes (typically 256256, 512512, 10241024, or 20482048 junctions) capable of recording an entire spectrum simultaneously.

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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.

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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.

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Homogeneous Line Broadening

Line broadening processes (such as natural and collisional broadening) that affect all individual atoms or molecules in an ensemble identically.

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Inhomogeneous Line Broadening

Line broadening processes (such as Doppler broadening) that affect different atoms or molecules in an ensemble unequally.

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Natural Line Broadening

Homogeneous line broadening dictated by the Heisenberg Uncertainty Principle (ΔE≥ℏτ\Delta E \ge \frac{\hbar}{\tau}), where the finite excited state lifetime (τ\tau) results in a Lorentzian energy distribution.

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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.

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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.

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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 10001000.

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Voigt Profile

A realistic spectral band profile generated by the mathematical convolution integral of Gaussian and Lorentzian profiles.

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Pseudo-Voigt Function

A simplified linear combination sum function of Lorentzian L(x)L(x) and Gaussian G(x)G(x) profiles weighted by a parameter η\eta, given by pV(x)=η⋅L(x)+(1−η)⋅G(x)pV(x) = \eta \cdot L(x) + (1 - \eta) \cdot G(x).

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Difference Amplifier

An analog circuit stage with two inputs that amplifies the difference between sample and reference signals, suppressing common-mode electrical noise.

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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/f1/f noise.

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Demodulation

The process of extracting the original low-frequency analytical signal from a modulated carrier wave using rectification and low-pass filtering.

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Ensemble Averaging

A digital noise reduction method that co-adds nn repeated scans to improve the Signal-to-Noise Ratio by a factor of n\sqrt{n}, relying on the random cancellation of uncorrelated noise.

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Boxcar Averaging

A digital smoothing filter that divides spectral data into equal, non-overlapping windows of width j=2n+1j = 2n + 1 points and replaces the points in each window with their centroid average.

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Moving Average Filter

A linear digital smoothing technique in which a window of width j=2n+1j = 2n + 1 points slides sequentially across the dataset one point at a time to calculate local averages.

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Savitzky-Golay Smoothing

A digital filtering procedure that performs a local polynomial least-squares fit across 2n+12n + 1 points using pre-calculated set weighting coefficients, smoothing noise while preserving peak shapes.

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Chemical Noise

Uncontrollable noise inherent to the chemical system or sample, such as thermal fluctuations, humidity shifts, or chemical equilibrium changes.

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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.

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Non-Fundamental Noise

Noise arising from external, environmental, or instrumental sources (such as power line hum or flicker noise) that can theoretically be eliminated.

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Noise Power Spectrum (NPS)

A plot showing mean-square noise per unit frequency interval (V2 Hz−1\text{V}^2\,\text{Hz}^{-1}) as a function of frequency (Hz\text{Hz}).

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Flicker Noise (1/f1/f Noise)

A non-fundamental, frequency-dependent random noise characterized by significant amplitudes at low frequencies, manifesting as slow signal or baseline drift.

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White Noise

Random noise whose power spectral density is constant across all frequencies in the frequency spectrum.

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Interference Noise

Non-fundamental, non-random noise occurring at specific, discrete frequencies due to electromagnetic coupling with external sources (e.g., 60 Hz60\,\text{Hz} power line hum).

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Thermal Noise (Johnson-Nyquist Noise)

A fundamental white noise caused by thermal agitation of electrons in resistive circuit components, which drops to zero at 0 K0\,\text{K}.

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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.

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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\text{SNR} = 3).