Zero-order suppression for two-photon holographic excitation.

Wavefront shaping with liquid-crystal spatial light modulators (LC-SLMs) is frequently hindered by a remaining fraction of undiffracted light, the so-called "zero-order." This contribution is all the more detrimental in configurations for which the LC-SLM is Fourier conjugated to a sample by a lens, because in these cases this undiffracted light produces a diffraction-limited spot at the image focal plane. In this Letter we propose to minimize two-photon (2P) excitation of the sample, resulting from this unmodulated light, by introducing optical aberrations to the excitation beam. Aberrations are subsequently compensated by the LC-SLM, but only for the modulated part of the beam, and not for the zero-order component. In order to experimentally demonstrate the method, we use astigmatism as the optical aberration, by simply adding one or two cylindrical lenses in the optical path of the beam. A 10⁴ decrease in zero-order-induced 2P fluorescence intensity is demonstrated. Combining this approach with temporal focusing is shown to decrease zero-order fluorescence by a factor of 4·10⁶.

[1]  Valentina Emiliani,et al.  Patterned two-photon illumination by spatiotemporal shaping of ultrashort pulses. , 2008, Optics express.

[2]  S. Popoff,et al.  Measuring the transmission matrix in optics: an approach to the study and control of light propagation in disordered media. , 2009, Physical review letters.

[3]  Valentina Emiliani,et al.  Three-dimensional holographic photostimulation of the dendritic arbor , 2011, Journal of neural engineering.

[4]  Alexander Jesacher,et al.  Parallel direct laser writing in three dimensions with spatially dependent aberration correction. , 2010, Optics express.

[5]  Marcos Dantus,et al.  Quantitative investigation of the multiphoton intrapulse interference phase scan method for simultaneous phase measurement and compensation of femtosecond laser pulses , 2006 .

[6]  Pál Ormos,et al.  Two-photon polymerization with optimized spatial light modulator , 2011 .

[7]  Ivo M Vellekoop,et al.  Digital optical phase conjugation of fluorescence in turbid tissue. , 2012, Applied physics letters.

[8]  Valentina Emiliani,et al.  Holographic Photolysis for Multiple Cell Stimulation in Mouse Hippocampal Slices , 2010, PloS one.

[9]  Valentina Emiliani,et al.  Two-photon excitation in scattering media by spatiotemporally shaped beams and their application in optogenetic stimulation. , 2013, Biomedical optics express.

[10]  G. Spalding,et al.  Computer-generated holographic optical tweezer arrays , 2000, cond-mat/0008414.

[11]  Y. Silberberg,et al.  Scanningless depth-resolved microscopy. , 2005, Optics express.

[12]  Tony Wilson,et al.  Image-based adaptive optics for two-photon microscopy. , 2009, Optics letters.

[13]  Christoph Lutz,et al.  Holographic photolysis of caged neurotransmitters , 2008, Nature Methods.

[14]  Vincent Ricardo Daria,et al.  Holographic projection of arbitrary light patterns with a suppressed zero-order beam. , 2007, Applied optics.

[15]  R. Gerchberg A practical algorithm for the determination of phase from image and diffraction plane pictures , 1972 .

[16]  N Farah,et al.  Design and characteristics of holographic neural photo-stimulation systems , 2009, Journal of neural engineering.

[17]  Valentina Emiliani,et al.  LCoS nematic SLM characterization and modeling for diffraction efficiency optimization, zero and ghost orders suppression. , 2012, Optics express.

[18]  Yael Roichman,et al.  Optimized holographic optical traps. , 2005, Optics express.