Abstract
1. INTRODUCTION
Locating an emitter and estimating different emitters’ relative positions precisely are key tasks in imaging problems. The question of two-point resolution was first discussed by Rayleigh [1,2]. Rayleigh’s criterion states that two-point sources are resolvable when the maximum of the illuminance produced by one point coincides with the first minimum of the illuminance produced by the other point. This criterion sets the limit of resolving power of optical systems [1]. Many methods have been developed to bypass this limit by converting resolving multi-emitter to locating single emitters. Deterministic super-resolution methods such as stimulated emission depletion microscopy [3], reversible saturable optical fluorescence transitions microscopy [4], and saturated structured illumination microscopy [5] utilize the fluorophores’ nonlinear response to excitation, which leads to individual emitting of emitters. Stochastic super-resolution methods such as stochastic optical reconstruction microscopy [6] and photo-activated localization microscopy [7] utilize the different temporal behavior of light sources, which emit light at separate times and thereby become resolvable in time. Therefore, localization of a single emitter is also an essential and fundamental issue in imaging problems.
Imaging is, as its heart, a multiparameter problem [8]. Targets’ localization and resolution can be viewed as parameter estimation problems. Positions of emitters are treated as parameters encoded in quantum states. The minimal error to estimate these parameters is bounded by the Cramér-Rao lower bound (CRLB). To quantify the precision, researchers utilize Fisher information (FI) associated with CRLB.
Inspired by classical and quantum parameter estimation theory [9–22], Tsang and coworkers [23] reexamined Rayleigh’s criterion. If only intensity is measured in traditional imaging, the CRLB tends to infinite as the separation between two-point sources decreases, which is called the Rayleigh curse. However, when the phase information is also taken into account, two incoherent point sources can be resolved no matter how close the separation is, which has been demonstrated in experiments [24–28]. If the centroid of the two emitters is also an unknown nuisance parameter, the precision to estimate the separation will decrease. Measuring the centroid precisely first can recover the lost precision due to misalignment between the measurement apparatus and the centroid [23,29]. Two-photon interference can be performed to estimate the centroid and separation at the same time [30]. Further developments in this emerging field have addressed the problem in estimating separation and centroid of two unequal brightness sources [31–33], locating more than two emitters [34], and resolving the two emitters in 3D space [35–39], with partial coherence [40–42] and complete coherence [43]. In addition, with the development of the super-resolution microscopy techniques mentioned above, the method to improve precision of locating a single emitter is also important. Efforts along this line include designing optimal point spread functions (PSFs) [44,45] and the quantum-limited longitudinal localization of a single emitter [46].
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In this work, we generalize the quantum-limited super-resolution theory to the localization of a single emitter with symmetric PSF and resolution of two unequal-brightness emitters in 3D space with arbitrary PSF. In the perspective of multiparameter estimation theory, we show that three Cartesian coordinates of a single emitter’s position [Fig. 1(a)] can be estimated in a single measurement scheme. For a two-emitter system, we consider the most general situation with five parameters, including relative intensity, centroids, and separations in transverse and longitudinal directions [see Fig. 1(b)]. We show that only two separations can be measured simultaneously to attain the quantum limit for the most general situation. In some special cases, centroids and separations can be estimated precisely at the same time. Localization and resolution in three dimensions are important in microscopy and astrometry. Our theoretical framework will be useful in these fields.
Figure 1.(a) Schematic of one emitter with position (
Figure 2.Quantum and classical Fisher information of localization in 3D space. For estimation of the transverse coordinates of the emitter, the CFI coincides with the QFI in the position
This paper is organized as follows. In Section 2, we provide a quantum mechanical description of the optical system with one and two emitters; in Section 3, we will review the quantum estimation theory, the main method to quantify the precision of localization and resolution, and introduce the FI and quantum Fisher information (QFI). The specific expressions of QFI of localization and resolution with some discussions will be provided in Section 4, and analysis will be done on the results. Finally, we summarize all the results in Section 5.
2. QUANTUM DESCRIPTION OF LOCALIZATION AND RESOLUTION
We assume that the emitters are point-like sources and the electromagnetic wave emitted by the emitters is quasimonochromatic and paraxial, with (, ) denoting the image-plane coordinates, denoting the distance from the emitters to the image plane. The quasimonochromatic paraxial wave obeys the paraxial Helmholtz equation
For two incoherent point sources, without the loss of generality, we only consider the displacement in the and directions. The quantum state is
3. QUANTUM ESTIMATION THEORY
Localization and resolution can be treated as the estimation of the coordinates of emitters. In this section, we review the quantum and classical estimation theory for further analysis. The quantum states in localization and resolution problems are dependent on the parameters to be estimated. Let the parameters be , and we use to substitute the parameters in Eqs. (2) and (3) for convenience. A quantum measurement described by a positive operator-valued measure (POVM) with the outcome is performed on the image plane to estimate , so that the probability distribution of the outcome is . The estimators are , which are the functions of measurement results. The precision of the estimates is quantified by the covariance matrix or mean square error
For unbiased estimators, the covariance matrix is lower bounded by the Cramér-Rao bound
Here, we give an example of FIm that the measurement method is the intensity detection, projecting the quantum state into the eigenstates of the spatial coordinates. The elements of this POVM are , and the FIm
To obtain the ultimate precision, it is necessary to obtain the bound, which only depends on the quantum states rather than the measurement systems:
4. RESULTS
Our main results contain two parts. First, we show the QFIm of locating an emitter with symmetric wave functions satisfying the paraxial Helmholtz equation in 3D space. Second, we give the QFIm of two incoherent point sources in which the parameters to be estimated include relative intensity, centroids, and separations in both transverse and longitudinal directions.
A. Quantum Localization in 3D Space
In general, we assume that the wave function is symmetric in the transverse direction with respect to its center:
We take the Gaussian beam as an example, which is the most common beam in practical experiments. The pure state without displacement in Eq. (2) is
The result of QFIm is Ratio between the QFI of Gaussian Beam and That of LG Beam with Respect to the Azimuthal Mode Index Here, we select 1 3 5 7 2 4 6 8 3 5 7 9 4 6 8 10
B. Quantum Limited Resolution in Three Dimensions
Now we consider two incoherent point sources with the quantum state in Eq. (3). Different from single emitters, the quantum state is a mixed state, which implies that Eq. (15) cannot be used here. We need a new method to calculate the QFIm. According to the definition of SLD in Eq. (11), we find the quantum state and its derivatives, which is associated with SLDs supported in the subspace spanned by , , , , , and . Thus, similar to Ref. [38], our analysis relies on the expansion of the quantum state in the nonorthogonal but normalized basis:
We take the Gaussian beam in Eq. (21) as an example. We obtain , , , , , and . The condition in Eq. (30) is satisfied if . Here, the value of is shown in Fig. 3 with and wavelength . In Fig. 3(a), the relative intensity is a constant ; in the other three pictures, relative intensity is also a parameter to be estimated. From these results, we find is close to zero in some regions, especially when the separations in two directions are nearly zero.
Figure 3.Contour plot of
When the separations in the and directions are infinitesimal (far less than the wavelength), the QFIm and weak commutativity condition matrix of the Gaussian beam become
5. CONCLUSION AND DISCUSSION
In summary, we give the general model and fundamental limitation for the localization of a single emitter and resolution of two emitters in 3D space. For one emitter, although the parameters in three directions are compatible with each other, the intensity detection cannot extract the maximal information of 3D positions simultaneously. Optimal measurement methods remain to be explored.
For two emitters, there are five parameters, including the relative intensity, separations, and centroids in the transverse and longitudinal directions of two emitters. We have obtained the quantum-limited resolution via the QFIm. In the most general case that one does not have any prior information of these parameters, only separations in the longitudinal and transverse directions can be estimated simultaneously to achieve the quantum-limited precision. More parameters can achieve the quantum-limited precision under special conditions, e.g., Eq. (30). The Gaussian beam example shows that, if and only if separation in longitudinal direction is zero, one can estimate separation, centroid in longitudinal direction, and the relative intensity with the quantum-limited precision. The example also shows that, when the separations in two directions are much smaller than the wavelength, all of the elements in the QFIm are constants, which indicates that separations and centroids in the longitudinal and transverse directions can be estimated precisely with a single measurement scheme. Spatial-mode demultiplexing [24–26,53,54] or a mode sorter [35] can be useful here.
We should note that our results are suitable not only for Gaussian beams but also for arbitrary symmetric wave functions satisfying paraxial Helmholtz equations. Our results give a fundamental bound of quantum limit in localization and resolution in 3D space and will stimulate the development of new imaging methods.
APPENDIX A: SPECIFIC FORMULATIONS OF THE DERIVATIVE OF QUANTUM STATE
In this appendix, we give the derivation of QFIm and a weak commutativity condition matrix. From Eqs.?(
Next, QFIm and a weak commutativity condition matrix can be derived from Eqs.?(
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