Tomography is imaging by sections or sectioning, through the use of any kind of penetrating wave. The method is used in radiology, archaeology, biology, atmospheric science, geophysics, oceanography, plasma physics, materials science, astrophysics, quantum information, and other areas of science. In most cases the production of these images is based on the mathematical procedure tomographic reconstruction.
- 1 Overview
- 2 Basic principle
- 3 Schematic configuration and motion
- 4 Types of tomography
- 5 See also
- 6 References
- 7 Notes
- 8 External links
Tomography refers to imaging by sections or sectioning, through the use of any kind of penetrating wave or mechanical method. The method is used in radiology, archaeology, biology, atmospheric science, geophysics, oceanography, plasma physics, materials science, astrophysics, quantum information, and other sciences. In most cases it is based on the mathematical procedure called tomographic reconstruction.The word tomography is derived from Ancient Greek τόμος tomos, "slice, section" and γράφω graphō, "to write" (see also Etymology).
In conventional medical X-ray tomography, clinical staff make a sectional image through a body by moving an X-ray source and the film in opposite directions during the exposure. Consequently, structures in the focal plane appear sharper, while structures in other planes appear blurred. By modifying the direction and extent of the movement, operators can select different focal planes which contain the structures of interest. Before the advent of more modern computer-assisted techniques, this technique, developed in the 1930s by the radiologist Alessandro Vallebona, proved useful in reducing the problem of superimposition of structures in projectional (shadow) radiography.
In a 1953 article in the medical journal Chest, B. Pollak of the Fort William Sanatorium described the use of planography, another term for tomography. A chapter in the American Roentgen Ray Society's 1996 book A History of the Radiological Sciences also provides a detailed history of the development of conventional tomography from its inception until being supplanted by computer assisted tomographic techniques starting in the mid to late-1970s.
More modern variations of tomography involve gathering projection data from multiple directions and feeding the data into a tomographic reconstruction software algorithm processed by a computer. Different types of signal acquisition can be used in similar calculation algorithms in order to create a tomographic image. Tomograms are derived using several different physical phenomena listed in the following table:
|Physical phenomenon||Type of tomogram|
|Electrical Capacitance Tomography||ECT|
|electrons||Electron tomography or 3D TEM|
|magnetic particles||magnetic particle imaging|
|fluid flow||hydraulic tomography|
|Mid-infrared||Infrared microtomographic imaging|
The term volume imaging might describe these technologies more accurately than the term tomography. However, in the majority of cases in clinical routine, staff request output from these procedures as 2-D slice images. As more and more clinical decisions come to depend on more advanced volume visualization techniques, the terms tomography/tomogram may go out of fashion.
Many different reconstruction algorithms exist. Most algorithms fall into one of two categories: filtered back projection (FBP) and iterative reconstruction (IR). These procedures give inexact results: they represent a compromise between accuracy and computation time required. FBP demands fewer computational resources, while IR generally produces fewer artifacts (errors in the reconstruction) at a higher computing cost.
Although MRI and ultrasound are transmission methods, they typically do not require movement of the transmitter to acquire data from different directions. In MRI, both projections and higher spatial harmonics are sampled by applying spatially-varying magnetic fields; no moving parts are necessary to generate an image. On the other hand, since ultrasound uses time-of-flight to spatially encode the received signal, it is not strictly a tomographic method and does not require multiple acquisitions at all.
In this section, the basic principle of tomography in the case that especially uses tomography utilizing the parallel beam irradiation optical system will be explained.
Tomography is a technology that uses a tomographic optical system to obtain virtual 'slices' (a tomographic image) of specific cross section of a scanned object, allowing the user to see inside the object without cutting. There are several types of tomographic optical system including the parallel beam irradiation optical system. Parallel beam irradiation optical system may be the easiest and most practical example of a tomographic optical system therefore, in this article, explanation of "How to obtain the Tomographic image" will be based on "the parallel beam irradiation optical system". The resolution in tomography is typically described by the Crowther criterion.
The Fig. 3 is intended to illustrate the mathematical model and to illustrate the principle of tomography.In the Fig.3, absorption coefficient at a cross-sectional coordinate (x, y) of the subject is modeled as μ(x, y). Consideration based on the above assumptions may clarify the following items. Therefore, in this section, the explanation is advanced according to the order as follows:
- (1)Results of measurement, i.e. a series of images obtained by transmitted light are expressed (modeled) as a function p (s,θ) obtained by performing radon transform to μ(x, y), and
- (2)μ(x, y) is restored by performing inverse radon transform to measurement results.
(1)The Results of measurement p(s,θ) of parallel beam irradiation optical system
Considers the mathematical model such that the absorption coefficient of the object at each (x,y) are represented by μ(x,y) and one supposes that "the transmission beam penetrates without diffraction, diffusion, or reflection although it is absorbed by the object and its attenuation is assumed to occur in accordance with the Beer-Lambert law. In this matter, what we want to know” is μ(x,y) and what we can measure will be following p(s,θ).
When the attenuation is conformed to Beer-Lambert law, the relation between and is as following (eq.1) and therefore, the absorbance () along the light beam path (l(t)) is as following (eq.2). Here the is intensity of light beam before transmission is intensity of after transmission.
- (eq. 1)
- (eq. 2)
Here, a direction from the light source toward the screen is defined as t direction and that perpendicular to t direction and parallel with the screen is defined as s direction. (Both t-s and x-y coordinate systems are set up such that they are reflected each other without mirror-reflective transformation.)
By using a parallel beam irradiation optical system, one can experimentally obtain the series of fluoroscopic images (a one-dimensional images” pθ(s) of specific cross section of a scanned object) for each θ. Here, θ represents angle between the object and the transmission light beam. In the Fig.3, X-Y plane rotates counter clockwise [Notes 1] around the point of origin in the plane in such a way “to keep mutual positional relationship between the light source (2) and screen (7) passing through the trajectory (5).” Rotation angle of this case is same as above-mentioned θ.
The beam having an angle θ,to will be the collection of lays, represented by of following (eq. 3).
- (eq. 3)
The pθ(s) is defined by following (eq. 4). That is equal to the line integral of μ(x,y) along of (eq. 3) as the same manner of (eq.2). That means that, of following (eq. 5) is a resultant of Radon transformation of μ(x,y).
- (eq. 4)
One can define following function of two variables (eq. 5). In this article, following p(s, θ) is called to be "the collection of fluoroscopic images".
- p (s, θ)=pθ(s) (eq. 5)
(2)μ(x, y) is restored by performing inverse radon transform to measurement results
“What we want to know (μ(x,y))” can be reconstructed from “What we measured ( p(s,θ))” by using inverse radon transformation . In the above-mentioned descriptions, “What we measured” is p(s,θ) . On the other hand, “What we want to know ” is μ(x,y). So, the next will be "How to reconstruct μ(x,y) from p(s,θ)".
Schematic configuration and motion
In this section, the schematic configuration and motion of the parallel beam irradiation optical system configured to obtain the p(s,θ) of above-mentioned (eq. 5) will be explained. In this section, how to obtain the p(s,θ) of (eq.5) by utilizing parallel beam irradiation optical system will also be explained. Configuration and motions of parallel beam irradiation optical system, referring the Fig. 3.
Numbers (1)–(7) shown in the Fig. 3 (see the numbers within the parentheses) respectively indicate: (1) = an object; (2) = the parallel beam light source; (3) = the screen; (4) = transmission beam; (5) = the datum circle (a datum feature); (6) = the origin (a datum feature); and (7) = a fluoroscopic image (a one-dimensional image; p (s, θ)).
Two datum coordinate systems xy and ts are imagined in order to explain the positional relations and movements of features (0)–(7) in the figure. The xy and ts coordinate systems share the origin (6) and they are positioned on the same plane. That is, the xy plane and the ts plane are the same plane. Henceforth, this virtual plane will be called “the datum plane”. In addition, a virtual circle centered at the abovementioned origin (6) is set on the datum plane (it will be called “the datum circle” henceforth). This datum circle (6) will be represents the orbit of the parallel beam irradiation optical system. Naturally, the origin (6), the datum circle (5), and the datum coordinate systems are virtual features which are imagined for mathematical purposes.
The μ(x,y) is absorption coefficient of the object (3) at each (x,y), p(s,θ) (7)is the collection of fluoroscopic images.
Motion of parallel beam irradiation optical system
The parallel beam irradiation optical system is the key component of a CT scanner. It consists of a parallel beam X-ray source (2) and the screen (3). They are positioned so that they face each other in parallel with the origin (6) in between, both being in contact with the datum circle (6).
These two features ((2) and (3)) can rotate counterclockwise [Notes 1] around the origin (6) together with the ts coordinate system while maintaining the relative positional relations between themselves and with the ts coordinate system (so, these two features ((2) and (3)) are always opposed each other). The ts plane is positioned so that the direction from a collimated X-ray source (2) to the screen (3) matches the positive direction of the t-axis while the s-axis parallels these two features. Henceforth, the angle between the x- and the s-axes will be indicated as θ. That is, parallel beam irradiation optical system where the angle between the object and the transmission beam equals θ. This datum circle (6) will be represents the orbit of the parallel beam irradiation optical system.
On the other hand, the object (1) will be scanned by CT scanner is fixed to xy coordination system. Hence, object (1) will not be moved while the parallel beam irradiation optical system are rotated around the object (1). The object (1) must be smaller than datum circle.
Obtaining transmission image ‘s’
During the above-mentioned motion (that is pivoting around the object(1)) of parallel beam irradiation optical system, the collimated X-ray source (2) emits transmission beam (4) which are effectively “parallel rays” in a geometrical optical sense. The traveling direction of each ray of the transmission beam (4) is parallel to the t-axis. The transmission beam (4), emitted by the X-ray source (2), penetrates the object and reaches the screen (3) after attenuation due to absorption by the object.
Optical transmission can be presumed to occur ideally. That is, transmission beam penetrates without diffraction, diffusion, or reflection although it is absorbed by the object and its attenuation is assumed to occur in accordance with the Beer-Lambert law.
Consequently, a fluoroscopic image (7) is recorded on the screen as a one-dimensional image (one image is recorded for every θ corresponding to all s values). When the angle between the object and transmission beam is θ and if the intensity of transmission beam (4) having reached each "s" point on the screen is expressed as p (s, θ), it expresses a fluoroscopic image (7) corresponding to each θ.
Types of tomography
Discrete tomography and Geometric tomography, on the other hand, are research areas that deal with the reconstruction of objects that are discrete (such as crystals) or homogeneous. They are concerned with reconstruction methods, and as such they are not restricted to any of the particular (experimental) tomography methods listed above.
Synchrotron X-ray tomographic microscopy
The construction of third-generation synchrotron sources combined with the tremendous improvement of detector technology, data storage and processing capabilities since the 1990s has led to a boost of high-end synchrotron tomography in materials research with a wide range of different applications, e.g. the visualization and quantitative analysis of differently absorbing phases, microporosities, cracks, precipitates or grains in a specimen. Synchrotron radiation is created by accelerating free particles in high vacuum. By the laws of electrodynamics this acceleration leads to the emission of electromagnetic radiation (Jackson, 1975). Linear particle acceleration is one possibility, but apart from the very high electric fields one would need it is more practical to hold the charged particles on a closed trajectory in order to obtain a source of continuous radiation. Magnetic fields are used to force the particles onto the desired orbit and prevent them from flying in a straight line. The radial acceleration associated with the change of direction then generates radiation.
Media related to Tomography at Wikimedia Commons
- Chemical imaging
- Discrete tomography
- Geometric tomography
- Geophysical imaging
- Industrial CT scanning
- Medical imaging
- MRI compared with CT
- Network tomography
- Nonogram, a type of puzzle based on a discrete model of tomography
- Radon transform
- Tomographic reconstruction
- Multiscale Tomography
- Tomography at the US National Library of Medicine Medical Subject Headings (MeSH)
- Pollak, B. (December 1953). "Experiences with Planography". Chest. American College of Chest Physicians. 24 (6): 663–669. doi:10.1378/chest.24.6.663. ISSN 0012-3692. Retrieved July 10, 2011.
- Littleton, J.T. "Conventional Tomography". A History of the Radiological Sciences (PDF). American Roentgen Ray Society. Retrieved 29 November 2014.
- Herman, G. T., Fundamentals of computerized tomography: Image reconstruction from projection, 2nd edition, Springer, 2009
- Martin; et al. (2013). "3D spectral imaging with synchrotron Fourier transform infrared spectro-microtomography". Nature Methods. 10: 861–864. doi:10.1038/nmeth.2596.
- Ralf Habel, Michael Kudenov, Michael Wimmer: Practical Spectral Photography
- Mojtaba Ahadi; et al. "Three dimensions localization of tumors in confocal microwave imaging for breast cancer detection". Microwave and Optical Technology Letters,Volume 57, Issue 12, pages 2917–2929, December 2015 . DOI: 10.1002/mop.29470
- Donoghue; et al. (Aug 10, 2006). "Synchrotron X-ray tomographic microscopy of fossil embryos (letter)". Nature. 442 (7103): 680–683. Bibcode:2006Natur.442..680D. doi:10.1038/nature04890. PMID 16900198.
- Banhart, John, ed. Advanced Tomographic Methods in Materials Research and Engineering. Monographs on the Physics and Chemistry of Materials. Oxford ; New York: Oxford University Press, 2008.
- In this article, the following discussion is developed based on anticlockwise motion. But, whether the direction of the rotation is anti-clockwise or a clockwise is not an essential problem. Even if the rotational direction is assumed to be in an opposite direction, no specific impact is caused on essential level except for some minor deformation of formula including reversing a part of positive or negative signs.