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Physical Review A

Influence of conformational changes in complex molecules on photon statistics of single molecule fluorescence

Игорь Сергеевич Осадько, V. V. Fedyanin

Published Jun 28, 2011• 13 citations
Publisher

Abstract

A single complex molecule with conformational changes (conformations 0 and 2) is considered. When such a molecule is irradiated by cw-laser light it can randomly change the intensity or polarization of its fluorescence due to jumps from one conformation to another. In fact, the molecule manifests itself either like the 0-type or the 2-type emitter. An expression for the matrix ${s}_{\ensuremath{\alpha}\ensuremath{\beta}}(t)$ called the start-stop correlator (waiting time distribution) in which $\ensuremath{\alpha}=0,2$ and $\ensuremath{\beta}=0,2$ is derived. An expression for the matrix ${p}_{\ensuremath{\alpha}\ensuremath{\beta}}(t)$ called the full correlator is derived as well. It determines the density of the probability of finding an event of $\ensuremath{\alpha}$ type and an event of $\ensuremath{\beta}$ type separated by time interval $t$. A relation between matrices ${s}_{\ensuremath{\alpha}\ensuremath{\beta}}(t)$ and ${p}_{\ensuremath{\alpha}\ensuremath{\beta}}(t)$ is found. A mathematical expression for the distribution ${w}_{N}(T)$ of events measured in time interval $T$ is derived. It is expressed solely via the matrix ${s}_{\ensuremath{\alpha}\ensuremath{\beta}}(t)$. Numerical calculations of the event distribution function for various rates of intra- and interconformational jumps are carried out with the help of the formula for ${w}_{N}(T)$ and by the Monte Carlo method. Both methods of the calculation yield identical distributions. Fluctuating fluorescence intensity $I$($t$) for a bin time of 5 ms is calculated for slow and fast interconformational jumps. A relation is found between the autocorrelation function ${g}^{(2)}(t)$ of fluorescence measurable in experiments and the matrix ${p}_{\ensuremath{\alpha}\ensuremath{\beta}}(t)$ calculated theoretically.

DOI
10.1103/physreva.83.063841

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A single complex molecule with conformational changes (conformations 0 and 2) is considered. When such a molecule is irradiated by cw-laser light it can randomly change the intensity or polarization of its fluorescence due to jumps from one conformation to another. In fact, the molecule manifests itself either like the 0-type or the 2-type emitter. An expression for the matrix s\ensuremathα\ensuremathβ(t){s}_{\ensuremath{\alpha}\ensuremath{\beta}}(t)s\ensuremathα\ensuremathβ​(t) called the start-stop correlator (waiting time distribution) in which \ensuremathα=0,2\ensuremath{\alpha}=0,2\ensuremathα=0,2 and \ensuremathβ=0,2\ensuremath{\beta}=0,2\ensuremathβ=0,2 is derived. An expression for the matrix p\ensuremathα\ensuremathβ(t){p}_{\ensuremath{\alpha}\ensuremath{\beta}}(t)p\ensuremathα\ensuremathβ​(t) called the full correlator is derived as well. It determines the density of the probability of finding an event of \ensuremathα\ensuremath{\alpha}\ensuremathα type and an event of \ensuremathβ\ensuremath{\beta}\ensuremathβ type separated by time interval ttt. A relation between matrices s\ensuremathα\ensuremathβ(t){s}_{\ensuremath{\alpha}\ensuremath{\beta}}(t)s\ensuremathα\ensuremathβ​(t) and p\ensuremathα\ensuremathβ(t){p}_{\ensuremath{\alpha}\ensuremath{\beta}}(t)p\ensuremathα\ensuremathβ​(t) is found. A mathematical expression for the distribution wN(T){w}_{N}(T)wN​(T) of events measured in time interval TTT is derived. It is expressed solely via the matrix s\ensuremathα\ensuremathβ(t){s}_{\ensuremath{\alpha}\ensuremath{\beta}}(t)s\ensuremathα\ensuremathβ​(t). Numerical calculations of the event distribution function for various rates of intra- and interconformational jumps are carried out with the help of the formula for wN(T){w}_{N}(T)wN​(T) and by the Monte Carlo method. Both methods of the calculation yield identical distributions. Fluctuating fluorescence intensity III(ttt) for a bin time of 5 ms is calculated for slow and fast interconformational jumps. A relation is found between the autocorrelation function g(2)(t){g}^{(2)}(t)g(2)(t) of fluorescence measurable in experiments and the matrix p\ensuremathα\ensuremathβ(t){p}_{\ensuremath{\alpha}\ensuremath{\beta}}(t)p\ensuremathα\ensuremathβ​(t) calculated theoretically.
Fluorescence from an ensemble of noninteracting molecules excited by continuous laser radiation is considered as a glow of M individual molecules. The expression that governs the autocorrelation function (ACF) of fluorescence from M molecules is derived based on the theoretical expression that governs the ACF of fluorescence from a single-molecule. Fluctuations of blinking fluorescence and its statistical properties are analyzed using a computer simulation. The results of statistical analysis of the computer experiment are in good agreement with the derived formula that governs the ACF of fluorescence from several molecules.
The method previously used by the author for the measurement and calculation of the distribution function w N(T)of fluorescence photons from a single two-level atom that is continuously excited by laser light and has a unity fluorescence quantum yield is generalized to the case of a single molecule whose fluorescence quantum yield is smaller than unity and to the case of a three-level molecule whose fluorescence is blinking. The functions w N(T) calculated for these two cases demonstrate a sub-Poissonian distribution of fluorescence photons.
The stream of photons emitted by a single quantum system such as a molecule or a nanocrystal is often statistically characterized by the distribution of delays between consecutive photons, or by the autocorrelation function of the intensity, or by the distributions of on- and off-times. We derive and discuss general relations between their Laplace transforms, addressing the influence of detection yield and background. Our analytical treatment applies to any distribution of delays and to random telegraph signals, including nonexponential distributions. We examine the special case of systems switching between two states characterized by different distributions of delays, where the switching can obey various statistics. We show that the second-order autocorrelation function keeps track of long-time fluctuations which are obviously lost in averaging the distributions of delays. We apply our formalism to random telegraphs, in particular to those with power-law distributions of on- and/or of off-times, which are encountered in the blinking of single semiconductor nanocrystals.
The use of techniques for analyzing the fluorescence photon statistics of a single molecule for modeling single-emitter dynamics is demonstrated. The photon distribution function measured in the fluorescence of a single tetra-tert-butylterrylene molecule embedded in polyisobutylene is used to devise a theoretical model for single emitters with complicated fluorescence photon statistics. Our analysis was carried out with the theoretical approach developed by Osad'ko and co-workers [J. Chem. Phys. 130, 064904 (2009); J. Phys. Chem. C 114, 10349 (2010)] for photon distribution functions. Although the experimental data were obtained at cryogenic temperature where narrow zero-phonon lines are present, the method is based on a purely statistical approach and does not require spectrally resolved data. It can also be applied to the analysis of broad fluorescence bands as measured at room temperature. Therefore, the method has prospects for revealing the quantum dynamics of single biological objects and other single quantum emitters in ambient conditions.
The statistics of spontaneous photon emission times in single atom resonance fluorescence are investigated through the radiative cascade of the dressed atom. The delay function which gives the distribution of the delays between two successive emissions is calculated for a coherent as well as an incoherent laser excitation. For a two-level atom, various signals that reflect the fluorescence intensity (average value, photon counting, fluctuation spectrum, etc.) are reviewed by this method. For a three-level atom, this approach is applied to the analysis of the recently observed phenomenon of intermittent fluorescence and quantum jumps.>
The three-level dye molecule single quantum system interacting with a cw laser field is investigated.The dynamic process of a single-molecule emitted photon is described by rate equations with absorbing boundary condition.It is demonstrated that the dynamics of the single-molecule processes and the statistics of time-resolved photon detection can be conveniently described in terms of renewal stochastic processes.The approach of calculating the correlation function by calculating the delay function that is an important physics quantity reflecting single quantum system dynamic process is given,and explicit expressions of correlation functions for two-levels and two-states systems are derived.This approach can be used for calculate dynamics parameter of molecular transition based on the fluorescence intensity correlation function.