Photonics Research, Volume. 5, Issue 4, 329(2017)

Woofertweeter adaptive optical structured illumination microscopy

Qinggele Li1, Marc Reinig1, Daich Kamiyama2,3, Bo Huang2, Xiaodong Tao1, Alex Bardales1, and Joel Kubby1、*
Author Affiliations
  • 1W.M. Keck Center for Adaptive Optical Microscopy, Baskin Engineering, University of California, Santa Cruz, California 95064, USA
  • 2Department of Pharmaceutical Chemistry, University of California, San Francisco, California 94143, USA
  • 3Current address: Department of Cellular Biology, University of Georgia, Athens, Georgia 30602, USA
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    Figures & Tables(7)
    Layout of the woofer–tweeter AOSIM. The DLP with 608×684 pixels (DLP3000 Texas Instruments) is placed at a conjugate plane of the objective lens focal plane. The SHW sensor consists of a lenslet array (f=24 mm) and a CCD camera (Photometrics) and is placed at a conjugate plane of the objective lens aperture plane. Blue line, 488 nm excitation light path (488 nm excitation laser from Spectra-Physics); green line, 515 nm emission path. The focal lengths of the lenses are f1=120 mm, f2=125 mm, f3=120 mm, f4=150 mm, f5=500 mm, f6=750 mm, f7=150 mm, f8=75 mm, f9=100 mm, f10=450 mm, f11=150 mm, f12=50 mm. M, mirror; SF, spatial filter; TL, trial lens (cylinder); F, filter; Di, dichroic mirror; FM, flip mirror.
    Comparison of (a)–(d) widefield and (e)–(h) SIM microscope images with and without wavefront correction. The figure shows the images of nanoparticles (110 nm) after introducing trial lens in between lenses f1 and f2. (a), (e) Without AO correction; (b), (f) woofer-only correction; (c), (d) tweeter-only correction; (d), (h) both woofer and tweeter correction. The scale bar is 5 μm.
    Zernike modes of the wavefront errors with and without woofer–tweeter correction. The inset is the value of the remaining Zernike modes after removing the sixth-order vertical astigmatism. The Zernike order is in Noll single-index order [43].
    Comparison of 0.11 μm beads under AO widefield (black line) and AOSIM (red line), Shown as line plots of the intensity of beads in areas 1 and 2 of Figs. 2(d) and 2(h). (a) Intensity profile of two closely spaced beads. The distance between two well-resolved peaks in AOSIM is 145 nm. (b) The FWHMs of a single bead in widefield and AOSIM are 235 and 140 nm, respectively.
    Images of GFP-labeled aCC/RP2 motoneurons of a Drosophila embryo. (a) Widefield without AO, (b) SIM without AO, (c) widefield with AO, (d) SIM with AO, (e) intensity plots of the line profiles in (a)–(d). The lines are along the dendrites of the aCC. The scale bar is 10 μm.
    Zernike modes of the Drosophila embryo wavefront errors with and without woofer–tweeter correction [43].
    • Table 1. Analysis of Measured Wavefront of Figs. 2(a)2(d)a

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      Table 1. Analysis of Measured Wavefront of Figs. 2(a)2(d)a

       No AOWoofer (W)Tweeter (T)Both W and T
      P-V (waves)8.930.752.310.36
      RMS (waves)2.050.180.460.08
      Strehl ratio0.060.270.080.75
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    Qinggele Li, Marc Reinig, Daich Kamiyama, Bo Huang, Xiaodong Tao, Alex Bardales, Joel Kubby, "Woofertweeter adaptive optical structured illumination microscopy," Photonics Res. 5, 329 (2017)

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    Paper Information

    Category: Microscopy

    Received: Feb. 22, 2017

    Accepted: May. 17, 2017

    Published Online: Oct. 10, 2018

    The Author Email: Joel Kubby (jkubby@soe.ucsc.edu)

    DOI:10.1364/PRJ.5.000329

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