Image formation in cellular X-ray microscopy

https://doi.org/10.1016/j.jsb.2012.01.006Get rights and content

Abstract

Soft X-ray Tomographic (TomoX) microscopy has become a reality in the last years. The resolution range of this technique nicely fits between confocal and electron microscopies and will play a key role in the elucidation of the organization between the molecular and the organelle levels. In fact, it offers the possibility of imaging three-dimensional structures of hydrated biological specimens near their native state without chemical pre-treatment. Ideally, TomoX reconstructs the specimen absorption coefficients from projections of this specimen, but, unfortunately, X-ray micrographs are only an approximation to projections of the specimen, resulting in inaccuracies if a tomographic reconstruction is performed without explicitly incorporating these approximations. In an attempt to mitigate some of these inaccuracies, we develop in this work an image formation model within the approximation of assuming incoherent illumination.

Introduction

Structural biology aims at the visualization of microscopic biological structures with the ultimate goal of understanding the molecular mechanisms taking place in the healthy as well as in the pathological cell. In the last decade a new microscopy technique has emerged, a technique able to visualize whole cells in cryo conditions with a resolution between 50 and 15 nm. This is the field of Cellular Soft X-ray Tomography (TomoX) (Schneider, 1998). Many studies so far have presented 3D reconstructions generated by X-ray microscopy (Weiss et al., 2000a, Thieme et al., 2003, Larabell and Le Gros, 2004, Le Gros et al., 2005, Gu et al., 2007, Parkinson et al., 2008, Uchida et al., 2009, Carrascosa et al., 2009, Hanssen et al., 2011). In most cases, the data have been processed using software developed for electron microscopy (EM) data (as can be SPIDER (Frank et al., 1996) or IMOD (Kremer et al., 1996)) without considering the particularities of the new microscope. Obviously, this is a suboptimum situation, and still better results would be obtained should an accurate TomoX image formation model were embedded within the 3D reconstruction process. The main purpose of this article is to start investigating this issue, presenting a first development in which we describe the image formation process within the simplification of assuming incoherent illumination. However, and still within its approximation, this modeling work opens the door to the design of new 3D reconstruction algorithms that explicitly incorporate the image model within the reconstruction algorithm.

Clearly, image processing for TomoX data should be rather different from the EM case, since TomoX images have larger contrast and are less noisy than EM ones. Moreover, the data collection geometry (usually single-tilt axis) helps to reduce the space of possible solutions. Unfortunately, TomoX images are, in general, a poorer approximation to ideal projection images than EM ones. Therefore, in this field the image processing challenge is not the one of fighting the poor signal-to-noise ratio as in EM, but that of the characterization of the microscope PSF and its appropriate incorporation into 3D reconstruction methods. As in any other microscopy, the objective in the X-ray microscope acts as a low-pass spatial frequency filter. Therefore, the PSF of the zone plate objective has to be taken into account. Weiss et al. (2000b) presented PSF calculations for realistic X-ray objectives assuming that the whole specimen is in focus.

Section snippets

Theoretical background

In this section we discuss the physical principles in which X-ray microscopy is based. First, the interaction of X-ray and matter is introduced and then the image formation process for an ideal microscope is presented for the incoherent case.

The practical situation in TomoX

So far we have assumed that the PSF of an X-ray microscope is properly approximated by the PSF of a perfect system computed at the focal point. In this subsection we discuss how similar is the PSF of a perfect system to the one made by a Fresnel zone plate. We also explore how the PSF changes for points far away from (i) the object plane that is in focus or (ii) the optical axis.

The answer to the first question is given by Mendoza-Yero et al. (2010) using numeric computation. In this work

Experiments

In order to visualize the importance of the depth of focus in TomoX, several experiments have been made. The first set of experiments uses a phantom made from simple geometrical structures (fringes) which is fully described in Fig. 3. These experiments were designed to find the resolution limits induced by the limited depth of focus. A simple phantom was selected since reconstruction artifacts are more clearly identifiable in these structures. For the second set of experiments we used a more

Discussion

In this work we have followed a systematic approach to the study of the image formation process in a cellular X-ray microscope at the task of visualizing objects of several microns and within the approximation of incoherent illumination. This study is to be considered an initial contribution to the field, that should be followed by more realistic illumination models, including partially coherent illumination, as well as the modification of reconstruction algorithms so that they incorporate at

Acknowledgments

This work was funded by the Spanish Ministerio de Ciencia e Innovación (CSD2006-0023, BFU2009-09331, BIO2010-16566, ACI2009-1022, ACI2010-1088) and NSF grant 1114901. We give special thanks to Stephan Heim, Ph.D. student at Bessy Synchrotron, for his contributions to the Preprocessing section. C.O. Sorzano is a recipient of a Ramón y Cajal fellowship financed by the European Social Fund and the Ministerio de Educación y Ciencia. Joaquin Oton is supported by a Juan de la Cierva Research

References (33)

  • C.O.S. Sorzano et al.

    The effect of overabundant projection directions on 3D reconstruction algorithms

    J. Struct. Biol.

    (2001)
  • C.O.S. Sorzano et al.

    XMIPP: a new generation of an open-source image processing package for electron microscopy

    J. Struct. Biol.

    (2004)
  • J. Thieme et al.

    X-ray tomography of a microhabitat of bacteria and other soil colloids with sub-100 nm resolution

    Micron

    (2003)
  • D. Attwood

    Soft X-Rays and Extreme Ultraviolet Radiation: Principles and Applications

    (2007)
  • M. Bertilson et al.

    Numerical model for tomographic image formation in transmission X-ray microscopy

    Optics Express

    (2011)
  • Dey, N., Boucher, A., Thonnat, M., 2002. Image formation model of a 3D translucent object observed in light microscopy....
  • Cited by (0)

    View full text