Tomography and Subtomogram Averaging

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1 Tomography and Subtomogram Averaging John Briggs EM course 2017

2 What do we need to get a 3D structure? Sample preparation methods A transmission electron microscope Different views of our object of interest Computational approaches for producing a 3D reconstruction from 2D projections Methods for validation and interpretation of the 3D structure

3 What do we need to get a 3D structure? Sample preparation methods A transmission electron microscope Different views of our object of interest Computational approaches for producing a 3D reconstruction from 2D projections Methods for validation and interpretation of the 3D structure

4 We need different views of our object

5 Tomography? In single-particle methods we obtain different views of our object of interest by imaging many different copies that are oriented differently relative to the electron beam. In tomography we obtain different views by physically rotating the sample in the microscope

6 Movie from the Baumeister lab, Max-Planck Institute for Biochemistry

7 Tilt series and tomogram Tilt-series Tomogram

8 Why do tomography? Because our sample is a unique structure (bits of cells, tissues, viruses etc.) Because our sample is within a complex environment

9 Topics to be covered Sample preparation methods Data collection and microscope requirements Alignment and reconstruction Subtomogram averaging

10 Sample preparation Sample must have structure preserved Sample must be thin Sample must be stable in vacuum

11 Cellular sample preparation methods Chemical fixation Cryo-fixation (high pressure freezing or plunge freezing) Dehydratation Freezing in LN 2 with Cryoprotectant Freezesubstitution / fixation Resin embedding LT-Embedding FIB milling Sectioning Cryo-sectioning Sectioning Immunolabelling Staining (UA,LC) Cryo-sectioning TEM TEM RT-TEM Cryo-TEM

12 Cryo-sectioning The end (CEMOVIS) High-pressure freezer Cryo-microtome

13 Cryo-sectioning The end (CEMOVIS) Nucleus Multivesicular structures Mitochondria ER Lipid droplet Artefacts due to cutting Petr Chlanda

14 Sample preparation - FIBSEM Rigort and Plitzko 2015

15 Sample preparation - FIBSEM Mahamid et al, Science 2015

16 Data collection Set new tilt angle Track correct for shifts Focus Exposure Baumeister et al. Trends in Cell Biology 1999

17 Microscope requirements (for cryo-electron tomography of thicker samples) High-voltage (ideally 300kV) Energy filter Very stable and well-calibrated microscope stage Appropriate software

18 Tilt series and tomogram Tilt-series Tomogram

19 Forward and back projection 3D object -> 2D projections 2D projections -> 3D reconstruction

20 The data is incomplete: the missing wedge 2D projections -> 3D reconstruction Missing information

21 The missing wedge leads to smearing in z

22 Missing information due to discrete sampling thicker for thinner objects Crowther Criterion r = pd/n r: Resolution limit N: Number of projections D: Object thickness

23 Data collection Set new tilt angle Track correct for shifts Focus What questions should we ask before data collection? Exposure

24 Data collection What total dose? Resolution vs signal-to-noise What tilt range? Completeness of information vs dose and speed What angular increment? Resolution vs dose and speed What order to collect the images? Speed, reliability, optimal dose, sample distortion What magnification? Resolution and DQE vs field of view What defocus? High-frequency information vs low frequency information

25 Alignment and Reconstruction Once we have collected the data how do we reconstruct a tomogram?

26 Alignment and Reconstruction We need to know how the projections relate to each other: the angles and shifts between the projections. We have defined the angles in the microscope by tilting around a defined axis by defined increments. Alignment is necessary to deal with the shifts in the image. (at larger fields of view, other distortions may become important)

27 Alignment and Reconstruction - Reconstruction by weighted back projection

28 Back-projection

29 Back-projection 1/r

30 Back-projection

31 Software Data Collection: SerialEM, FEI Tomo, Leginon Tomogram reconstruction: IMOD, TOM, protomo, PyTOM

32 Subtomogram averaging

33 Subtomogram averaging Mahamid et al, Science 2015

34 Subtomogram averaging use new reference for alignment iterate until reference is stable subtomograms (randomly oriented) aligned to reference subtomograms (aligned) tomogram averaged subtomograms (new reference)

35 Subtomogram averaging process Data CTF correction Assign initial Euler angles (priors) Align tilt-series Align subtomograms (3D) Reconstruct tomogram Classify subtomograms Average subtomograms Extract subtomograms Post-processing Structure

36 Software for subtomogram averaging Dynamo (Castano-Diez, Basel) PEET (Heumann and Mastronarde, Boulder) PyTOM (Foerster, Utrecht) RELION (Bharat and Scheres, LMB) Maximum cross-correlation or Maximum likelihood

37 Subtomogram averaging Why not just do single particle reconstruction? (if you can, then do it!) Subtomogram averaging allows structures to be determined when other objects in the path of the electron beam would otherwise prevent alignment. (and has potential for application in single-particle type projects)

38 Subtomogram averaging Can generate two kinds of information Structure Position and context

39 Subtomogram averaging - challenges Sample flexibility and heterogeneity Higher apparent sample thickness (especially at tilt) Two alignment and reconstruction steps Sample movement/change during data collection Higher total electron dose Smaller datasets (due to more time-consuming data collection and processing) Difficult in determination and correction of CTF

40 Subtomogram averaging - challenges In which order should we collect the images?

41 Continuous tilt scheme

42 Bidirectional tilt scheme

43 Dose-symmetric tilt scheme

44 Tilt schemes Continuous Bidirectional from 0 Dose-symmetric Hagen et al. JSB 2017

45 Tilt schemes signal transfer Continuous Bidirectional from 0 Bidirectional from -21 Bidirectional from -21 deleting second branch Dose-symmetric Note the difference is greater if you also consider increased sample movement at tilt Hagen et al. JSB 2017

46 Dose-dependent sample changes Hagen et al. JSB 2017

47 Subtomogram averaging - challenges CTF Correction

48 Defocus gradients in the sample Turonova. et al 2D CTF correction considers only the gradient due to tilt, 3D CTF also considers the gradient through the thick sample

49 Defocus gradients in the sample

50 Defocus gradients in the sample Turonova. et al

51 Subtomogram averaging - challenges Sample flexibility and heterogeneity Higher apparent sample thickness (especially at tilt) Separate alignment and reconstruction steps Sample movement/change during data collection Higher total electron dose Smaller datasets (due to more time-consuming data collection and processing) Difficult in determination and correction of CTF

52 It is possible to obtain <4Å resolution C E344 R286 R299 [H11] H8 E291 Q287 Schur et al. Science 2016

53 Subtomogram averaging Structure in situ Cellular context Structure for Discovery Potential SP applications Mahamid et al, Science 2015 Mattei et al. Science 2016

54 Wan, W. and Briggs, J.A.G., Cryo-electron tomography and subtomogram averaging (2016) Methods in Enzymology, 579, and articles by many authors cited therein

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