Configurable platform
US-2024366089-A1 · Nov 7, 2024 · US
US9445722B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9445722-B2 |
| Application number | US-201313792502-A |
| Country | US |
| Kind code | B2 |
| Filing date | Mar 11, 2013 |
| Priority date | Mar 12, 2012 |
| Publication date | Sep 20, 2016 |
| Grant date | Sep 20, 2016 |
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A method is disclosed for performing a combined magnetic resonance/positron emission tomography scan of an examination object in an MR/PET system. An embodiment of the method entails acquiring first magnetic resonance data using a first readout gradient field. The first readout gradient field is chosen such that, at a location of the field of view of the magnetic resonance system, a distortion caused by a nonlinearity of the first readout gradient field and a distortion caused by a B 0 field inhomogeneity substantially cancel each other out. First magnetic resonance images for planning the combined magnetic resonance/positron emission tomography session and determining an attenuation correction map for a positron emission tomography scan are determined on the basis of the first magnetic resonance data. Positron emission data and second magnetic resonance data are acquired using a second readout gradient field.
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What is claimed is: 1. A method for performing a combined magnetic resonance/positron emission tomography scan of an examination object in a magnetic resonance/positron emission tomography (MR/PET) system, the method comprising: acquiring first magnetic resonance data using a first readout gradient field such that, at a location of a field of view of a magnetic resonance system of the MR/PET system, a distortion caused by a nonlinearity of the first readout gradient field and a distortion caused by a B 0 field inhomogeneity reduce the effect of each other; generating first magnetic resonance images on the basis of the first magnetic resonance data; determining an attenuation correction map for a positron emission tomography scan on the basis of the first magnetic resonance images; acquiring positron emission data based on the first magnetic resonance images and second magnetic resonance data based on the first magnetic resonance images, the acquiring acquires the second magnetic resonance data using a second readout gradient field; and correcting the positron emission data using the attenuation correction map. 2. The method of claim 1 , wherein the second readout gradient field is independent of the first readout gradient field. 3. The method of claim 1 , wherein the first magnetic resonance data are acquired at a first resolution and the second magnetic resonance data are acquired at a second resolution, the second resolution being relatively higher than the first resolution. 4. The method of claim 1 , wherein the acquisition of the first magnetic resonance data includes a continuous moving of the examination object through the MR/PET system. 5. The method of claim 1 , wherein the location, at which the distortion caused by the nonlinearity of the first readout gradient field and the distortion caused by the B 0 field inhomogeneity reduce the effect of each other, includes a location in a peripheral region of the field of view. 6. The method of claim 5 , wherein the MR/PET system includes a tunnel-shaped bore for receiving the examination object, the peripheral region of the field of view including an inner casing area along an inner surface of the tunnel-shaped bore. 7. The method of claim 6 , wherein the inner casing area has an inner casing thickness of approximately 5 cm. 8. The method of claim 1 , wherein the first magnetic resonance data are acquired in a transverse plane in relation to the examination object. 9. The method of claim 1 , wherein the acquiring the first magnetic resonance data comprises: determining the first readout gradient field such that, at the location of the field of view, the distortion caused by the nonlinearity of the first readout gradient field and the distortion caused by the B 0 field inhomogeneity reduce the effect of each other, determining a further readout gradient field such that at a further location of the field of view, that is different from the location, a distortion caused by a nonlinearity of the further readout gradient field and the distortion caused by the B 0 field inhomogeneity reduce the effect of each other, and performing a multi-echo sequence, wherein following a 180° pulse, magnetic resonance data of a first spin echo are acquired using the first readout gradient field and following a further 180° pulse, further magnetic resonance data of a second spin echo are acquired using the further readout gradient field, wherein the first magnetic resonance images are determined on the basis of the magnetic resonance data of the first spin echo and the further magnetic resonance data. 10. The method of claim 1 , wherein the acquiring the first magnetic resonance data comprises: determining the first readout gradient field such that, at the location of the field of view, the distortion caused by the nonlinearity of the first readout gradient field and the distortion caused by the B 0 field inhomogeneity reduce the effect of each other, the location of the field of view being a first location, determining a further readout gradient field in such a way that, at a second location of the field of view that is different from the first location, a distortion caused by a nonlinearity of the further readout gradient field and the distortion caused by the B 0 field inhomogeneity reduce the effect of each other, and performing a mixed spin echo/gradient echo sequence, wherein following a 180° pulse of the spin echo sequence, magnetic resonance data of a first spin echo are acquired using the first readout gradient field and subsequently further magnetic resonance data are acquired using the further readout gradient field, wherein the first magnetic resonance images are determined on the basis of the magnetic resonance data of the first spin echo and the further magnetic resonance data. 11. A non-transitory computer-readable medium configured to cause a control device to perform the method of claim 1 when executed by the control device, the control device being part of the MR/PET system.
involving electronic [EMR] or nuclear [NMR] magnetic resonance, e.g. magnetic resonance imaging · CPC title
combining images from an ionising-radiation diagnostic technique and a non-ionising radiation diagnostic technique, e.g. X-ray and ultrasound · CPC title
adapted for acquisition of images from more than one imaging mode, e.g. combining MRI and optical tomography · CPC title
related to combined acquisition of different diagnostic modalities · CPC title
caused by a distortion of a gradient magnetic field, e.g. non-linearity of a gradient magnetic field (G01R33/56509, G01R33/56518, G01R33/56536 take precedence) · CPC title
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