Skip to main content

Thank you for visiting You are using a browser version with limited support for CSS. To obtain the best experience, we recommend you use a more up to date browser (or turn off compatibility mode in Internet Explorer). In the meantime, to ensure continued support, we are displaying the site without styles and JavaScript.

Nonlinear Imaging using Object-Dependent Illumination


Nonlinear imaging systems can surpass the limits of linear optics, but nearly all rely on physical media and atomic/molecular response to work. These materials are constrained by their physical properties, such as frequency selectivity, environmental sensitivity, time behavior, and fixed nonlinear response. Here, we show that electro-optic spatial light modulators (SLMs) can take the place of traditional nonlinear media, provided that there is a feedback between the shape of the object and the pattern on the modulator. This feedback creates a designer illumination that generalizes the field of adaptive optics to include object-dependent patterns. Unlike physical media, the SLM response can provide a wide range of mathematical functions, operate over broad bandwidths at high speeds, and work equally well at high power and single-photon levels. We demonstrate the method experimentally for both coherent and incoherent light.


Feedback is a natural way to engineer nonlinearity, as it creates a functional relationship between input and output. Commonly used in control systems, feedback can act to amplify1, filter2, and process signals3. Historically, there have been two main applications, with two distinct approaches and methodologies: logical operations, with a focus on small degrees of freedom and stable processing, e.g.4 and dynamical systems, with an emphasis on large degrees of freedom and instability, e.g. pattern formation5. Here, we combine and extend these approaches to improve information transfer in nonlinear imaging systems.

The experimental design is shown in Fig. 1a. The method consists of two basic steps. First, a standard image is obtained using uniform illumination. Second, the measured pattern is fed into a spatial light modulator (SLM) and used to re-illuminate the object. The resulting feedback loop between the (digital) image of the object and the (digital) pattern of illumination effectively creates a nonlinearity that can be controlled electro-optically. Unlike nonlinearities that are determined – and limited – by physical media, such as crystals and polymers, SLMs are robust to the environment, respond well to wide ranges of intensity, bandwidth, and coherence, and can generate nearly any mathematical form. This nonlinear tunability (on a pixel-by-pixel basis), both by itself and for optimization on different figures of merit (such as contrast, resolution, edge detection, etc.), distinguishes our approach from earlier attempts at feedback6.

Figure 1

Principle of nonlinear digital imaging. (a) Experimental setup. A collimated laser beam is first sent onto a reflective SLM. The surface of the SLM is imaged onto the object via a 4-f lens relay. A CCD camera collects the light transmitted through the sample at a defocused distance ∆z = 4.5 cm. (b) Pseudo-code for the image retrieval algorithm (see Methods for details). (ce) Experimental intensity measured at (c) the focal plane, (d) the defocused plane with uniform illumination, and (e) the defocused plane with nonlinear (designer) illumination.

Our feedback generalizes two well-known pathways in computational imaging: adaptive optics and structured illumination. In the former, aberrations along an optical path are “pre-compensated” by first measuring and then correcting for the distortions, e.g. using deformable mirror arrays. This has enabled a revolution in remote sensing and ground-based astronomy, e.g. for imaging through a varying atmosphere, and is used routinely in ophthalmology for optical examination of the retina. It is also experiencing resurgence in imaging through turbid media, such as paint and fog7,8, in which scatterers randomize the information from object to image. However, the adaptation is independent of the object, used instead for correcting the path along the rest of the optical system.

In structured illumination, a patterned light source adds information at the input of the system, allowing more information about the object to be extracted (deconvolved) at the output. Examples include Zernike masks for phase observation9, periodic masks for improved resolution10,11 and depth sectioning12, Bessel13 and Airy14 beams for extended depth of focus, and random masks, which enable single-pixel cameras15 and coherence engineering16,17. As in adaptive optics, though, all these techniques use illumination patterns that are independent of the sample.

The primary reason for sample independence is that the object is typically unknown and a universal form of illumination is desired. This results in a general, shift-invariant transfer function that is suitable for arbitrary objects but is optimized for none of them. The introduction of feature-based illumination, through feedback, will improve information transfer and all metrics of image quality.


In our geometry, the feedback between source and detector closes the loop in computational imaging. While the functional relationship between the SLM and the object is essentially arbitrary, we consider here the simplest case of an intensity-dependent phase modulation: ϕSLM = γIα, where γ is the strength of the modulation and α is its order. This makes the system a physical implementation of the conventional split-step method in beam propagation codes, with one step for diffraction and one step for nonlinear effect, and allows a straightforward comparison with more conventional nonlinearities, e.g. the Kerr response for which α = 1. We emphasize, though, that much more complex responses are possible, including the ability to impose separate amplitude and phase modulations using a second SLM. More details about the digital nonlinear response are given in the Supplementary Information.

Nonlinear phase reconstruction

While the method can be applied to any type of image (provided there is a signal to bootstrap), phase reconstruction is particularly important. Phase contains most of the information in the signal, is crucial for a variety of important applications, and responds particularly well to nonlinearity18. Consequently, we experimentally demonstrate the method by nonlinearly improving the imaging of a phase object (Fig. 1c).

We use a modified version of the Gerchberg-Saxton (GS) method19 to retrieve the phase, taking advantage of the fact that phase matching from the nonlinear illumination-object feedback provides a strict constraint on the behavior of the algorithm20. As the shape of the object is not known a priori, we first record a defocused intensity (IU = |AU|2) that is obtained using uniform illumination (Fig. 1d). The amplitude distribution, |AU|, is then fed into a SLM as a phase modulation ϕSLM|AU|, enabling a second intensity measurement (ID = |AD|2) with designer illumination (Fig. 1e). As in previous examples of nonlinear imaging18,21, we use a self-defocusing nonlinearity; this enables sufficient wave mixing to enhance imaging while suppressing the fast instabilities common to self-focusing systems.

From the two images IU and ID, the nonlinear phase retrieval algorithm proceeds in a manner similar to GS reconstruction. First, a field with amplitude AU and initial uniform phase ϕ = 0 is numerically back-propagated from the (out-of-focus) camera plane to the sample plane (in focus). The phase modulation ϕSLM is then added to the phase of the field in order to simulate the action of the SLM, and the new field is forward-propagated to the camera plane. This simulated amplitude is then replaced by the amplitude of the actual measurement (AD), and the field is backward-propagated to the sample plane again. After subtraction of the phase modulation ϕSLM from the phase of the field at the sample plane, the new field is once again forward-propagated to the camera plane, followed by replacement of the numerical amplitude by the measured amplitude AU. The process is repeated until convergence. A pseudocode for this algorithm is shown in Fig. 1b.

As a phase object, we used a sample consisting of a glass plate with the three characters “DIC” etched on it. The in-focus image of the sample is shown in Fig. 1c. As the object is thin and transparent, no intensity modulation appear on the image in focus apart from scattering from the character edges. In Fig. 1d,e, we show the measured diffraction intensity distributions in the detector plane (out-of-focus) with uniform and designer (feedback) illumination, respectively. In general, more diffraction fringes are visible in the latter image, since the illumination has the shape of the object itself. The second pass of illumination effectively doubles the diffraction pattern, giving at least a two-fold increase in phase sensitivity to the object. Larger multiplication is of course possible21, especially with cascaded interactions22, with potentially exponential improvement upon repeated iteration.

We compare our nonlinear algorithm with a variation of the GS algorithm for linear propagation, for the same defocused distance. The conventional algorithm relies on one in-focus and one out-of-focus intensity measurement using uniform illumination. Simulation results are shown in Fig. 2a,b. In real imaging cases, the target is unknown and the reconstructed phase error cannot be accessed; in the simulation test case, the ground truth is chosen a priori, and we can quantitatively measure the reconstructed phase error

$${\rm{ER}}=\frac{{\sum }_{r{\epsilon }S}|f(r)-g(r)|}{{\sum }_{r{\epsilon }S}|g(r)|}\,$$

where f(r), g(r), and S are the reconstructed image, the ground truth, and the image space, respectively.

Figure 2

Comparison between linear and nonlinear reconstructions. (a,b) Simulation of phase reconstruction with (a) the linear algorithm and (b) the nonlinear algorithm. (c,d) Experimental phase reconstruction with (c) the linear algorithm and (d) the nonlinear algorithm using partially coherent light (corresponding to a speckle spatial frequency of 2.5 × 104 rad/m).

As expected, the nonlinear reconstruction (Fig. 2b) is about 2x better than the linear reconstruction (Fig. 2a) in term of the phase error (ER 0.8 vs. 1.5). The experimental counterparts, shown in Fig. 2c,d, confirm the result that the nonlinear algorithm provides much better reconstruction than the linear algorithm. For quantitative comparison, we define contrast and resolution as:

$$R={({\nabla }_{x}I)}_{x\in DICE}^{-1}$$

where \(\bar{I}\) represents the mean value of the intensity, the subscript “DIC” denotes the region of the DIC characters, “BKG” denotes the rest of the image, and “DICE” denotes the edge domain of the DIC region. (For a consistent measure of resolution based on a single image, we take the highest resolvable spatial frequency, given by the inverse of the normalized image gradient averaged over all the character edges.) By these metrics, the nonlinear algorithm yields a 260% improvement in contrast (1.50 vs. 0.58) and a 15% improvement in resolution (14.8 vs 17.1 microns) over linear reconstruction.

Another advantage of the digital system, and the corresponding algorithm, is the ability to work for different degrees of spatial coherence. We demonstrate this experimentally by making the illumination beam partially spatially coherent by passing it through a rotating diffuser23. The performance of linear and nonlinear modulation, in terms of contrast and resolution, are shown in Fig. 3j,k, respectively. In all cases, the figures of merit for linear propagation get worse monotonically as the degree of coherence is decreased (consistent with a progressive decrease in visibility of diffraction fringes24). In the nonlinear case, both contrast and resolution are improved simultaneously beyond their linear limits. [This win-win situation, normally an engineering trade-off in linear systems25, is a general feature of nonlinear imaging systems21.] For designer illumination, the contrast actually improves with decreasing coherence, up to an optimal value, while the system resolution is relatively constant above and below this value. The former is a stochastic resonance effect26, peaking when the smallest significant feature of the object (the stroke width of the DIC characters, ~167 μm) matches the spatial correlation length of the illumination (characterized by the speckle spatial frequency 3.75 × 104 rad/m). The latter results from improved visibility due to mean-field (DC) scattering21.

Figure 3

Experimental results as a function of nonlinear strength and power. (ai) Show the phase variance (a,d,g), contrast (b,e,h) and resolution (c,f,i) of the nonlinear reconstructions. (a–c) Show the nonlinear reconstructions for coherent illumination while (df) and (g–i) are reconstructions for partially coherent illumination with speckle spatial frequency 2.3 × 104 rad/m and 4.9 × 104 rad/m, respectively. (j,k) Comparison of linear (blue) and nonlinear (red) reconstructions for (j) contrast and (k) resolution. Full coherence is given by zero spatial frequency, and the nonlinearity is fixed at modulation power = 0.5 and modulation strength = 1.5π. The dashed line corresponds to the spatial frequency (3.75 × 104 rad/m), at which the illumination speckle size becomes comparable to the DIC character stroke width. When the spatial frequency exceeds this value, the image quality becomes worse as the statistics washes out the diffraction fringes.


Theoretically, the improvements in image quality are unlimited11,21. In practice, there are many factors that hinder the performance. These include the usual trade-off between pixel size and dynamic range in the camera and SLM27, pixel-mapping and tone-mapping mismatches between devices, amplitude corruption in the phase modulation, and genuine issues of noise. There are also frame-rate limitations if multiple iterations are desired, and issues of convergence and computational complexity as a function of basis, method of phase retrieval28, type of nonlinearity, and desired spatial detail (e.g. different class of response for individual SLM pixels).

The best approach to retrieving (estimating) the phase object is to maximize the information in the encoded illumination. This is given by the most widespread sampling in phase space, which for the experimental setup here corresponds to the most diverse distribution of phase on the modulator (Fig. 4). Using variance as a measure, we find that \({\sigma }_{SLM}^{2}=E[{(X-\mu )}^{2}]=A{\alpha }^{2}\exp (-B{\alpha }^{C})\), where X represents the pixel value on the SLM, μ = E[X] is the mean value of all the pixels, and α is the modulation power. This stretched-exponential form suggests a nontrivial (i.e. non-diffusive) optical flow as the object modes are mixed by the modulator26,29,30,31. As shown in Fig. 3a–i, the optimal system response ranges from a strict proportionality to amplitude \(({\varphi }_{SLM}=\gamma \sqrt{{I}_{U}})\) for the coherent case to a more conventional Kerr nonlinearity \(({\varphi }_{SLM}=\gamma {I}_{U})\) for the incoherent case.

Figure 4

Diversity of phase modulation. (ae) Modulation ϕSLM = γIα for coherent light (strength γ = 2π). The largest phase/information diversity (for better sampling) occurs when α = 0.5. (f) Shows the relation between diversity/variance and modulation power. Lower and upper curves represent modulation strengths γ = 2π and 4π, while solid, dashed, and dotted lines denote coherent and partially coherent illumination with speckle spatial frequency 2.3 × 104 rad/m (Incoherent_1) and 4.9 × 104 rad/m (Incoherent_2). Blue: experiment; red: theoretical fits for stretched exponential \({\sigma }_{SLM}^{2}=A{\alpha }^{2}\exp (-B{\alpha }^{C})\), with A = 33 and 132 for the lower and upper curves, B = {4.9, 4.1, 3.7}, and C = {0.8, 0.7, 0.6} for the coherent and incoherent cases.

These optimum transfer functions can be understood by considering the extremes of nonlinear response. For very weak response, there is little difference between linear and nonlinear output, and therefore little gain in information. Stronger responses give more significant differences, evidenced by more pronounced intensity fringes as modes interfere, until high-intensity regions start dominating the image. Above this point, the growth of hot spots leads to a modulation that is not indicative of the object as a whole (an effect exacerbated by noise, e.g. through modulation instability). From an information perspective, the structured feedback acts as a nonlinear matched filter32, with an amplitude-dependent response appropriate for the optical transfer function of coherent light and an intensity-dependent response appropriate for the modulation transfer function of incoherent light33. More details of this response are given in the Supplemental Information.

The quality of the reconstructed image using the nonlinear algorithm is comparable to what we obtained in a previous work using a nonlinear photorefractive crystal18. In that system, the intensity pattern of the object induced an index change in the crystal, creating a self-reinforcing diffraction grating during light propagation. Here, the object-dependent pattern on the spatial light modulator creates a similar grating (computer-generated hologram) in the plane of the SLM, which acts more like an iterative map. In both cases, the nonlinear feedback means that the grating structure is automatically phase-matched with the object, guaranteeing an optimized diffraction pattern. For the computational part, the interplay between intensity and phase gives an extra constraint on the algorithm, resulting in improved phase sensitivity, selectivity, and convergence.

While electro-optic devices have their limitations, they are far more versatile than the physical media traditionally used for nonlinear optics. Of particular significance is the ability to create nonlinearities that are distinct from those of physical media by leveraging independent control of amplitude and phase modulation. This freedom opens new applications for functional forms that have remained purely in the mathematical domain. The ability to adjust parameters dynamically also holds much promise for improving the efficiency and performance of adaptive optics and compressed sensing/imaging. Finally, digital methods have the potential to revolutionize imaging at extremely low light levels, such as fluorescence microscopy and quantum imaging, as SLMs are inherently non-destructive and can operate at the single photon level.


A 532 nm Coherent Verdi laser was used as a light source, and a phase-only spatial light modulator (SLM, Holoeye PLUTO, with a resolution of 1920 × 1080 pixels, 8-micron pixel size, and 8-bit depth) was placed in the illumination path before a phase object, modulating the illumination light as a function of the diffracted pattern of the sample. As a direct image does not reveal the object, we defocused the CCD camera (with a resolution of 1280 × 1024 pixels, 6.7-micron pixel size, and 16-bit depth) a distance Δz = 4.5 cm from the image plane and recorded the subsequent diffraction pattern. To produce partially incoherent light, the experimental setup was modified by inserting a rotating diffuser in the illumination path, and the degree of spatial incoherence was quantified by measuring the spatial frequency of the speckles, i.e. 2π over the correlation length of speckles at the detection plane.

To align the SLM and the CCD camera for feedback, it is essential to find the transformation matrix between the two devices. A 100 × 100 square mask was created on the SLM and moved in x and y direction with an interval of 200 pixels; we then found 25 point-by-point correspondences between the SLM and the camera by measuring the centroids of the mask on the SLM and the corresponding pattern on the camera. A 3 × 3 transformation matrix between the two devices was thus calculated.

From the uniform- and designer-illuminated images IU and ID, the nonlinear phase retrieval algorithm proceeds as follows:

  1. (1)

    An object field urec with amplitude AU and initial uniform phase 𝜙 = 0 is numerically back-propagated from the (out-of-focus) camera plane to the (in-focus) sample plane.

  2. (2)

    A phase modulation 𝜙SLM is added to the phase of urec to simulate the action of the SLM.

  3. (3)

    The new field is forward-propagated to the camera plane, yielding a field u′D with amplitude A′D.

  4. (4)

    The simulated amplitude A′D is replaced by the amplitude of the actual measurement AD.

  5. (5)

    The field is back-propagated again to the sample plane, yielding a new field urec.

  6. (6)

    The phase modulation 𝜙SLM is subtracted from the phase of urec.

  7. (7)

    The field is forward-propagated, yielding an estimate of the un-modulated image amplitude A′U.

  8. (8)

    A new field is generated by replacing A′U with the actual measurement AU. At this point, the algorithm restarts from step 1.

This algorithm effectively interpolates between the infinitesimal displacement of transport-of-intensity algorithms34 and the infinite (far-field) displacement of the Gerchberg-Saxton algorithm19. That is, it works for any distance of defocus, subject to the limits of Fresnel diffraction (which can be modified by changing the propagator). The method also works for arbitrary degrees of spatial coherence, as in this case the algorithm converges on an overall envelope phase35.


  1. 1.

    Black, H. S. Stabilized feedback amplifiers. Bell Syst Tech J 13, 1–18 (1934).

    Article  Google Scholar 

  2. 2.

    Kalman, R. E. & Bucy, R. S. New results in linear filtering and prediction theory. Transactions of ASME, Series D, Journal of Basic Engineering 83, 95–108 (1961).

    MathSciNet  Article  Google Scholar 

  3. 3.

    Widrow, B. & Stearns, S. D. Adaptive signal processing. (Prentice-Hall, 1985).

  4. 4.

    Athale, R. A. & Lee, S. H. Development of an Optical Parallel Logic Device and a Half-Adder Circuit for Digital Optical-Processing. Opt Eng 18, 513–517, (1979).

    ADS  Article  Google Scholar 

  5. 5.

    Hausler, G., Seckmeyer, G. & Weiss, T. Chaos and Cooperation in Nonlinear Pictorial Feedback-Systems .1. Experiments. Applied Optics 25, 4656–4663 (1986).

    ADS  CAS  Article  Google Scholar 

  6. 6.

    Akins, R. P., Athale, R. A. & Lee, S. H. Feedback in Analog and Digital Optical-Image Processing - a Review. Optical Engineering 19, 347–358 (1980).

    ADS  Article  Google Scholar 

  7. 7.

    Vellekoop, I. M. & Mosk, A. P. Focusing coherent light through opaque strongly scattering media. Optics Letters 32, 2309–2311 (2007).

    ADS  CAS  Article  Google Scholar 

  8. 8.

    Bertolotti, J. et al. Non-invasive imaging through opaque scattering layers. Nature 491, 232–234 (2012).

    ADS  CAS  Article  Google Scholar 

  9. 9.

    Zernike, F. Phase contrast, a new method for the microsopic observation of transparent objects. Physica 9, 686–698 (1942).

    ADS  Article  Google Scholar 

  10. 10.

    Gustafsson, M. G. L. Surpassing the lateral resolution limit by a factor of two using structured illumination microscopy. Journal of Microscopy-Oxford 198, 82–87 (2000).

    CAS  Article  Google Scholar 

  11. 11.

    Gustafsson, M. G. L. Nonlinear structured-illumination microscopy: Wide-field fluorescence imaging with theoretically unlimited resolution. Proceedings of the National Academy of Sciences of the United States of America 102, 13081–13086 (2005).

    ADS  CAS  Article  Google Scholar 

  12. 12.

    Mertz, J. Optical sectioning microscopy with planar or structured illumination. Nat Methods 8, 811–819 (2011).

    CAS  Article  Google Scholar 

  13. 13.

    Planchon, T. A. et al. Rapid three-dimensional isotropic imaging of living cells using Bessel beam plane illumination. Nat Methods 8, 417–U468 (2011).

    CAS  Article  Google Scholar 

  14. 14.

    Dowski, E. R. & Cathey, W. T. Extended Depth of Field through Wave-Front Coding. Applied Optics 34, 1859–1866 (1995).

    ADS  Article  Google Scholar 

  15. 15.

    Duarte, M. F. et al. Single-pixel imaging via compressive sampling. IEEE Signal Processing Magazine 25, 83–91 (2008).

    ADS  Article  Google Scholar 

  16. 16.

    Waller, L., Situ, G. & Fleischer, J. W. Phase-space measurement and coherence synthesis of optical beams. Nature Photonics 6, 474–479 (2012).

    ADS  CAS  Article  Google Scholar 

  17. 17.

    Baleine, E. & Dogariu, A. Variable coherence scattering microscopy. Physical Review Letters 95 (2005).

  18. 18.

    Lu, C. H., Barsi, C., Williams, M. O., Kutz, J. N. & Fleischer, J. W. Phase retrieval using nonlinear diversity. Appl Optics 52, D92–D96 (2013).

    Article  Google Scholar 

  19. 19.

    Gerchberg, R. W. & Saxton, W. O. Practical Algorithm for Determination of Phase from Image and Diffraction Plane Pictures. Optik 35, 237-& (1972).

    Google Scholar 

  20. 20.

    Lu, J. T., Lu, C. H. & Fleischer, J. W. Enhanced phase retrieval using nonlinear dynamics. Optics Express 24, 25091–25102 (2016).

    ADS  Article  Google Scholar 

  21. 21.

    Barsi, C. & Fleischer, J. W. Nonlinear Abbe theory. Nature Photonics 7, 639–643 (2013).

    ADS  CAS  Article  Google Scholar 

  22. 22.

    Jia, S., Wan, W. J. & Fleischer, J. W. Forward four-wave mixing with defocusing nonlinearity. Optics Letters 32, 1668–1670 (2007).

    ADS  Article  Google Scholar 

  23. 23.

    Martienssen, W. & Spiller, E. Coherence + Fluctuations in Light Beams. American Journal of Physics 32, 919 (1964).

    ADS  Article  Google Scholar 

  24. 24.

    Goodman, J. W. Statistical optics. (Wiley, 1985).

  25. 25.

    Murphy, D. B., Davidson, M. W. & ebrary Inc. xiii, 538 p. (Wiley-Blackwell, Hoboken, N.J., 2012).

  26. 26.

    Dylov, D. V. & Fleischer, J. W. Nonlinear self-filtering of noisy images via dynamical stochastic resonance. Nature Photonics 4, 323–327 (2010).

    CAS  Article  Google Scholar 

  27. 27.

    Pegard, N. C. & Fleischer, J. W. Optimizing holographic data storage using a fractional Fourier transform. Optics Letters 36, 2551–2553 (2011).

    ADS  Article  Google Scholar 

  28. 28.

    Fienup, J. R. Phase Retrieval Algorithms - a Comparison. Appl Optics 21, 2758–2769 (1982).

    ADS  CAS  Article  Google Scholar 

  29. 29.

    Wan, W., Jia, S. & Fleischer, J. W. Dispersive superfluid-like shock waves in nonlinear optics. Nature Physics 3, 46–51, (2007).

    ADS  CAS  Article  Google Scholar 

  30. 30.

    Laherrere, J. & Sornette, D. Stretched exponential distributions in nature and economy: “fat tails” with characteristic scales. European Physical Journal B 2, 525–539 (1998).

    ADS  CAS  Article  Google Scholar 

  31. 31.

    Anteneodo, C. & Plastino, A. R. Maximum entropy approach to stretched exponential probability distributions. Journal of Physics a-Mathematical and General 32, 1089–1097 (1999).

    ADS  MathSciNet  Article  Google Scholar 

  32. 32.

    Dylov, D. V., Waller, L. & Fleischer, J. W. Nonlinear restoration of diffused images via seeded instability. IEEE Journal of Quantum Electronics 18, 916–925 (2012).

    CAS  Article  Google Scholar 

  33. 33.

    Goodman, J. W. Introduction to Fourier optics. 3rd edn, (Roberts & Co. Publishers, 2005).

  34. 34.

    Teague, M. R. Deterministic Phase Retrieval - a Green-Function Solution. Journal of the Optical Society of America 73, 1434–1441 (1983).

    ADS  Article  Google Scholar 

  35. 35.

    Sun, C., Dylov, D. V. & Fleischer, J. W. Nonlinear focusing and defocusing of partially-coherent spatial beams. Optics Letters 34, 3003–3005 (2009).

    ADS  Article  Google Scholar 

Download references


This work was funded by AFOSR Grants FA9550-14-1-0177 and FA9550-12-1-0054.

Author information




J.L. and A.S.G. performed the experiments and simulations. All authors analyzed the data and contributed to the preparation of the manuscript.

Corresponding author

Correspondence to Jason W. Fleischer.

Ethics declarations

Competing Interests

The authors declare no competing interests.

Additional information

Publisher’s note: Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.

Supplementary information

Rights and permissions

Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit

Reprints and Permissions

About this article

Verify currency and authenticity via CrossMark

Cite this article

Lu, JT., Goy, A.S. & Fleischer, J.W. Nonlinear Imaging using Object-Dependent Illumination. Sci Rep 9, 725 (2019).

Download citation

Further reading


By submitting a comment you agree to abide by our Terms and Community Guidelines. If you find something abusive or that does not comply with our terms or guidelines please flag it as inappropriate.


Quick links

Nature Briefing

Sign up for the Nature Briefing newsletter — what matters in science, free to your inbox daily.

Get the most important science stories of the day, free in your inbox. Sign up for Nature Briefing