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Kspace (MRI)Template:DISPLAYTITLE:kspace (MRI) Additional recommended knowledgekspace is a formalism widely used in magnetic resonance imaging independently introduced in 1983 by Ljunggren^{[1]} and Twieg^{[2]}. Simply speaking, kspace is the temporary image space in which data from digitized MR signals are stored during data acquisition. When kspace is full (at the end of the scan), the data are mathematically processed to produce a final image. Thus kspace holds raw data before reconstruction. kspace is in spatial frequency domain. Thus if we define k_{FE} and k_{PE} such that and where FE refers to frequency encoding, PE to phase encoding, Δt is the sampling time (the reciprocal of sampling frequency), τ 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 2DFourier 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_{FE}, k_{PE}) constitute a Fourier transform pair. kspace has the same number of rows and columns as the final image. During the scan, kspace is filled with raw data one line per TR. 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 kspace 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 kspace is acquired, and subsequent scans are performed by acquiring just the central part of the kspace; in this way, different contrast images can be acquired without the need of running full scans. A nice symmetry property exist in the kspace, descending from the fact that the object imaged is a contrastweighted proton density and thus a real quantity, relating the signal at two opposite locations in kspace: where the star denotes complex conjugation. Thus kspace information is somewhat redundant, and an image can be reconstructed using only one half of the kspace, either in the PE direction saving scan time (such a technique is known as half Fourier or half scan) or in the FE direction, allowing for lower sampling frequencies and/or shorter echo times (such a technique is known as half echo). References
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This article is licensed under the GNU Free Documentation License. It uses material from the Wikipedia article "Kspace_(MRI)". A list of authors is available in Wikipedia. 