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- pile-up_effect
- {{tag> TCSPC pile-up dead_time}} ~~TOC~~ ====== Pile-Up Effect ====== The Pile-Up effect describes the e... gh photon count rates due to the dead time of the TCSPC devices. Most single photon counting detectors and [[TCSPC]] electronics have a [[dead time]]. After registe... for the next photon to detect. The dead time for TCSPC devices used for the measurement of fluorescence
- dead_time
- ====== Dead Time ====== In TCSPC the term dead time refers to the time the TCSPC system needs armed again after detecting an event. During the dead time the TCSPC system is blind. If for example two photons are detected with the dead time of the TCSPC device the second photon will be lost. This leads
- differential_count_rate
- val when a detected signal is really present. In TCSPC, decay curves are measured at count rates that ar... textbooks, it is required by basic principles of TCSPC in order to avoid various counting losses.(E.g. t... bility density function//. The detected signal in TCSPC has a very inhomogeneous time distribution. Note
- pre-histogrammed_image
- |TCSPCChannels||||''int32'' |number of TCSPC channels per pixel | |TimeRe... ||||''float32'' |time resolution of the TCSPC histograms in ns | |The following block... HistogramData [x,y,t]'' |''int32''| counts of the TCSPC channel t of pixel (x,y) | | | | end of bloc
- tttr
- mode is to record every individual photon of a [[TCSPC]] experiment. Both the arrival time as well as the TCSPC timing information (i.e. the time from the preced... ode]] files is possible with all recent PicoQuant TCSPC devices ([[Products:TimeHarp 260]], [[Products:Pi
- poisson_distribution
- sson distribution is of interest especially for [[TCSPC]]: The expected number of photons in any TCSPC channel is given by the 'real' decay (including convoluti
- tcspc
- ====== TCSPC ====== TCSPC stands for **T**ime **C**orrelated **S**ingle **P**hoton **C**ounting: A stream of photons
- bifl
- ents of a complete burst are accumulated into a [[TCSPC]] histogram which is used for lifetime analysis m
- fwhm
- ss of a peak, for example, of the [[IRF]] in an [[TCSPC]] measurement or the focal width(s) in a [[FLIM]]
- least_squares
- uncertainty of each individual data point. For [[TCSPC]] data $w^{}_i$ is defined as $$w_i=\sqrt{D_i^{e
- mcs
- binned ensemble of photons can be used to form [[TCSPC]] histograms, which in turn can be used for lifet
- residuals
- uncertainty of each individual data point. For [[TCSPC]] data $w^{}_i$ is defined as $$w_i=\sqrt{D_i^{