The patent badge is an abbreviated version of the USPTO patent document. The patent badge does contain a link to the full patent document.

The patent badge is an abbreviated version of the USPTO patent document. The patent badge covers the following: Patent number, Date patent was issued, Date patent was filed, Title of the patent, Applicant, Inventor, Assignee, Attorney firm, Primary examiner, Assistant examiner, CPCs, and Abstract. The patent badge does contain a link to the full patent document (in Adobe Acrobat format, aka pdf). To download or print any patent click here.

Date of Patent:
Dec. 08, 2015

Filed:

Feb. 11, 2011
Applicants:

Yair Censor, Haifa, IL;

Scott N. Penfold, North Adelaide, AU;

Reinhard W. Schulte, Grand Terrace, CA (US);

Inventors:

Yair Censor, Haifa, IL;

Scott N. Penfold, North Adelaide, AU;

Reinhard W. Schulte, Grand Terrace, CA (US);

Assignees:

LOMA LINDA UNIVERSITY MEDICAL CENTER, Loma Linda, CA (US);

UNIVERSITY OF HAIFA, Haifa, IL;

UNIVERSITY OF WOLLONGONG, Wollongong, AU;

Attorney:
Primary Examiner:
Int. Cl.
CPC ...
G06G 7/48 (2006.01); G06G 7/56 (2006.01); G01N 33/48 (2006.01); G01N 33/50 (2006.01); G01N 31/00 (2006.01); G01N 23/04 (2006.01); G06F 19/12 (2011.01); G06F 19/24 (2011.01); A61N 5/10 (2006.01); A61B 6/03 (2006.01); A61B 6/00 (2006.01); G06T 11/00 (2006.01);
U.S. Cl.
CPC ...
G01N 23/046 (2013.01); A61B 6/032 (2013.01); A61B 6/4258 (2013.01); A61B 6/5205 (2013.01); A61B 6/583 (2013.01); A61N 5/10 (2013.01); G06F 19/12 (2013.01); G06F 19/24 (2013.01); G06T 11/006 (2013.01); A61N 2005/1087 (2013.01); G01N 2223/419 (2013.01);
Abstract

Disclosed are systems, devices and methodologies relating to proton computed tomography. In some implementations, detection of protons can yield track information before and after an object for each proton so as to allow determination of a likely path of each proton within the object. Further, measurement of energy loss experienced by each proton allows determination that a given likely path results in a given energy loss. A collection of such data allows characterization of the object. Such a characterization can include an image map of relative stopping power of the object. Various reconstruction methodologies for obtaining such an image can include superiorization of a merit function such as total variation. Various forms of total variation superiorization methodology can yield excellent results with reduced computing time. In some implementations, such a methodology can result in high quality proton CT images using relatively low dose of protons.


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