Maximum intensity projection
File:Mouse02-spect.gif visualized by a MIP of a mouse]]
File:CT presentation as thin slice, projection and volume rendering.jpgs:
- Average intensity projection
- Maximum intensity projection
- Thin slice (median plane)
- Volume rendering by high and low threshold for radiodensity.]]
In scientific visualization, a maximum intensity projection (MIP) is a method for 3D data that projects in the visualization plane the voxels with maximum intensity that fall in the way of parallel rays traced from the viewpoint to the plane of projection. This implies that two MIP renderings from opposite viewpoints are symmetrical images if they are rendered using orthographic projection.
MIP is used for the detection of lung nodules in lung cancer screening programs which use computed tomography scans. MIP enhances the 3D nature of these nodules, making them stand out from pulmonary bronchi and vasculature. MIP imaging is also used routinely by physicians in interpreting Positron Emission Tomography (PET) or Magnetic Resonance Angiography studies.
Additional techniques
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This technique is computationally fast, but the 2D results do not provide a good sense of depth of the original data. To improve the sense of 3D, animations are usually rendered of several MIP frames in which the viewpoint is slightly changed from one to the other, thus creating the illusion of rotation. This helps the viewer's perception to find the relative 3D positions of the object components. However, since the projection is orthographic the viewer cannot distinguish between left or right, front or back and even if the object is rotating clockwise or anti-clockwise. Use of depth weighting during production of rotating cines of MIP images can avoid the problem of difficulty of distinguishing right from left, and clockwise vs anti-clockwise rotation.
An alternate version of MIP is Local maximum intensity projection. In this technique we don't take the global maximum value, but the first maximum value that is above a certain threshold. Because - in general - we can terminate the ray earlier this technique is faster and also can give better results in some settings as it approximates occlusion.{{Cite journal|title = Local Maximum Intensity Projection (LMIP|url = http://www.image.med.osaka-u.ac.jp/member/yoshi/lmip_index.html|journal = Journal of Computer Assisted Tomography|pages = 912–917|volume = 22|issue = 6|doi = 10.1097/00004728-199811000-00014|first = Yoshinobu|last = Sato|first2 = Nobuyuki|last2 = Shiraga|first3 = Shin|last3 = Nakajima|first4 = Shinichi|last4 = Tamura|first5 = Ron|last5 = Kikinis}} Choice of Local MIP vs Full MIP depends on the display goals and how the MIP is to be used.
History
MIP Display was invented for use in Nuclear Medicine by Jerold Wallis, MD, in 1988 at Washington University in St. Louis, and subsequently published in IEEE Transactions on Medical Imaging.{{cite journal |vauthors=Wallis JW, Miller TR, Lerner CA, Kleerup EC |title=Three-dimensional display in nuclear medicine |journal=IEEE Trans Med Imaging |volume=8 |issue=4 |pages=297–303 |year=1989 |pmid=18230529 |doi=10.1109/42.41482 }} In the setting of Nuclear Medicine, it was originally called MAP (Maximum Activity Projection).{{cite journal |vauthors=Wallis JW, Miller TR |title=Volume rendering in three-dimensional display of SPECT images |journal=J. Nucl. Med. |volume=31 |issue=8 |pages=1421–8 |date=1 August 1990|pmid=2384811 |url=http://jnm.snmjournals.org/cgi/pmidlookup?view=long&pmid=2384811 }}{{cite journal |vauthors=Wallis JW, Miller TR |title=Three-dimensional display in nuclear medicine and radiology |journal=J Nucl Med |volume=32 |issue=3 |pages=534–46 |date=March 1991|pmid=2005466 }}
See also
References
{{Commons category|Maximum intensity projections}}
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{{DEFAULTSORT:Maximum Intensity Projection}}