Volume 14, Issue 13, Pages (July 2004)

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Volume 14, Issue 13, Pages 1181-1186 (July 2004) Positioning and Elongation of the Fission Yeast Spindle by Microtubule-Based Pushing  Iva M Tolić-Nørrelykke, Leonardo Sacconi, Geneviève Thon, Francesco S Pavone  Current Biology  Volume 14, Issue 13, Pages 1181-1186 (July 2004) DOI: 10.1016/j.cub.2004.06.029

Figure 1 Astral Microtubules Push on the Spindle Poles (A) Time-lapse images of mitosis in an intact S. pombe cell with GFP-tagged tubulin. Each image is a maximum-intensity projection of a set of optical sections acquired at a 0.5 μm z interval. Numbers refer to time in minutes. Scale bar, 2 μm. (B) Superposition of three pairs of images from the sequence in (A). In each pair the first image is shown in red, and the second one in green. Numbers refer to time as in (A). Rotation of the spindle is clearly visible (arrows). The spindle pole body (SPB) moved away from the contact site of the astral microtubule and the cell cortex (A-C contact site; dotted line marks the cell edge). (C) The spindle was laser dissected in its midzone (blue arrow), which induced bending of the spindle. Note a large rotation (white arrow) of the lower part of the spindle away from the A-C contact site. (D) Two astral microtubules extended in opposite directions from the upper SPB. One of them was laser dissected (blue arrow) and subsequently disappeared, whereas the other one remained intact. The upper SPB moved away from the A-C contact site (white arrow). (E) Control for laser-dissection experiments. The cytoplasm was irradiated close to the upper SPB (blue arrow), which did not induce a significant change in spindle position. (F) Histogram of the spindle rotation angle. Positive angles imply astral pushing, whereas negative angles imply pulling. Green indicates events observed in intact cells, yellow in cells with severed spindle, and red in cells with severed astral microtubules. One measurement from an intact spindle (α = +18°) and two from severed spindles (α = +24° and +33°) are not shown. Current Biology 2004 14, 1181-1186DOI: (10.1016/j.cub.2004.06.029)

Figure 2 Poles of Severed Spindles Move Centrally In each group of images the spindle before the midzone dissection (blue arrows) is shown in the first image, followed by two images taken 2–6 min later. Four types of spindle conformations after dissection: (A), collapse; (B), bend; (C), cross; and (D), slide. Current Biology 2004 14, 1181-1186DOI: (10.1016/j.cub.2004.06.029)

Figure 3 Broken Spindles Can Recover (A) Chosen frames from a time-lapse sequence showing breakage and recovery of the spindle in the Slide-configuration. (B) Distance between SPBs versus time for the cell from (A). After laser dissection (blue arrow), the spindle breaks and the distance between the SPBs decreases slightly. The spindle recovers and subsequently grows at a speed of 0.25 μm/min. (C) Chosen frames from a time-lapse sequence showing breakage and recovery of the spindle in the cross configuration. A postanaphase array is visible in the last image. (D) Image of the DNA (blue) superimposed on the image of the cell from (C). Although the spindle had been broken, the division finished successfully: the septum is formed and each daughter cell contains one nucleus. Current Biology 2004 14, 1181-1186DOI: (10.1016/j.cub.2004.06.029)

Figure 4 A Model for Spindle Positioning and Elongation in S. pombe The spindle consists of arrays of antiparallel microtubules (MT, only two are shown) growing from the spindle pole bodies (SPB). Kinesin-like proteins (Klp) crosslink the spindle microtubules and elongate the spindle by moving toward the microtubule plus ends (red arrows). Astral microtubules extend from the SPBs and position the spindle by pushing against the edges of the cell (white arrows). Current Biology 2004 14, 1181-1186DOI: (10.1016/j.cub.2004.06.029)