K-space (MRI)

independently introduced in 1983 by Ljunggren [Ljunggren S. Journal of Magnetic Resonance 1983; 54:338.] and Twieg [cite journal | author = Twieg D | title = The k-trajectory formulation of the NMR imaging process with applications in analysis and synthesis of imaging methods. | journal = Medical Physics | volume = 10 | issue = 5 | pages = 610–21 | year = 1983 | pmid = 6646065 | doi = 10.1118/1.595331] .

Simply speaking, "k"-space is the "temporary image space" in which data from digitized MR signals are stored during data acquisition. When "k"-space is full (at the end of the scan), the data are mathematically processed to produce a final image. Thus "k"-space holds "raw" data before "reconstruction".

"k"-space is in spatial frequency domain. Thus if we define $k\_mathrm\{FE\}$ and $k\_mathrm\{PE\}$ such that:

and:

where FE refers to "frequency encoding", PE to "phase encoding", $Delta\; t$ is the sampling time (the reciprocal of sampling frequency), $au$ is the duration of "G"_PE, ("gamma bar") is the gyromagnetic ratio, "m" is the sample number in the FE direction and "n" is the sample number in the PE direction (also known as "partition number"), the 2D-Fourier Transform of this encoded signal results in a representation of the spin density distribution in two dimensions. Thus position ("x","y") and spatial frequency ($k\_mathrm\{FE\}$, $k\_mathrm\{PE\}$) constitute a Fourier transform pair.

"k"-space has the same number of rows and columns as the final image. During the scan, "k"-space is filled with raw data one line per TR (Repetition Time).

Although a strict mathematical proof does not exist and counterexamples can be provided, in most cases it is safe to say that data in the middle of "k"-space contain the signal to noise and contrast information for the image, while data around the outside of the image contain all the information about the image resolution. This is the basis for advanced scanning techniques, such as the "keyhole" acquisition, in which a first complete "k"-space is acquired, and subsequent scans are performed by acquiring just the central part of the "k"-space; in this way, different contrast images can be acquired without the need of running full scans.

A nice symmetry property exists in "k"-space, descending from the fact that the object imaged is a contrast-weighted proton density and thus a real quantity, relating the signal at two opposite locations in "k"-space::$S(-k\_mathrm\{FE\},-k\_mathrm\{PE\})\; =\; S*(k\_mathrm\{FE\},k\_mathrm\{PE\})\; ,$

where the star denotes complex conjugation.Thus "k"-space information is somewhat redundant, and an image can be reconstructed using only one half of the "k"-space, either in the PE (Phase Encode) direction saving scan time (such a technique is known as "half Fourier" or "half scan") or in the FE (Frequency Encode) direction, allowing for lower sampling frequencies and/or shorter echo times (such a technique is known as "half echo").

References

Further reading

*McRobbie D., et al. "MRI, From picture to proton." 2003
*Hashemi Ray, et al. "MRI, The Basics" 2ED. 2004.