Patent Number: 
Section: claims

1. A combined magnetic resonance and single photon nuclear imaging system, the system comprising:at least one compound semiconductor detector configured to directly convert incident gamma photons into electron-hole charge carriers;at least one collimator for single photon nuclear imaging an object under study with the at least one compound semiconductor detector;at least one magnet for producing a magnetic field suitable for magnetic resonance imaging, the at least one magnet having a central opening;at least one transceiver for magnetic resonance imaging the object under study with the at least one magnet; anda correction processor,wherein the at least one compound semiconductor detector is configured to single photon nuclear image the object under study under the magnetic field suitable for magnetic resonance imaging,wherein the at least one compound semiconductor detector is configured to single photon nuclear image the object under study at either end of the at least one magnet and outside the central opening of the at least one magnet such that the object under study is single photon nuclear imaged and magnet resonance imaged in a sequential manner,wherein the at least one compound semiconductor detector is adjacent and attached to the outside surface of the at least one magnet,wherein the correction processor is configured to compensate for an effect on the charge carriers traveling within the at least one compound semiconductor detector and under the magnetic field suitable for magnetic resonance imaging,wherein the at least one semiconductor detector comprises a first ring having a plurality of first modules and a second ring having a plurality of second modules, and wherein the first modules of the first ring are aligned to have an angular offset with the second modules of the second ring along an axial direction to view the object under study with twice the angular sampling with one axial motion. 2. The system of claim 1, wherein the at least one compound semiconductor detector comprises a material selected from the group consisting of cadmium telluride (CdTe), mercuric iodide (HgI2), thallium bromide (TlBr), gallium arsenide (GaAs), cadmium zinc telluride (CdZnTe), and cadmium manganese telluride (CdMnTe). 3. The system of claim 1, wherein the at least one compound semiconductor detector is a cadmium zinc telluride (CZT) detector. 4. The system of claim 1, wherein the at least one compound semiconductor detector comprises:at least one compound semiconductor substrate for producing the charge carriers through interaction with the gamma photons; anda plurality of electrodes for collecting the charge carriers. 5. The system of claim 1, wherein the at least one collimator is configured to be positioned between the object under study and the at least one compound semiconductor detector. 6. The system of claim 1, wherein the at least one compound semiconductor detector is a stationary detector. 7. The system of claim 1, wherein the effect on the charge carriers configured to be compensated by the correction processor is a Lorentz-force effect. 8. The system of claim 1, further comprising a signal processor configured to process the charge carriers as a detection signal and comprising a plurality of electronics adapted to amplify, address, and process the detection signal,wherein the signal processor is positioned away from the magnetic field suitable for magnetic resonance imaging to remove an interference effect of the magnetic field suitable for magnetic resonance imaging. 9. A method of combining magnetic resonance and single photon nuclear imaging, the method comprising:injecting a radioactive isotope into an object under study;directly converting gamma photons from the radioactive isotope within the object under study by at least one semiconductor detector into electron-hole charge carriers;single photon nuclear imaging the object under study with at least one collimator positioned between the object under study and the at least one semiconductor detector;producing a magnetic field suitable for magnetic resonance imaging by at least one magnet;magnetic resonance imaging the object under study with at least one transceiver positioned between the object under study and the at least one magnet; andcorrecting for an effect on the charge carriers traveling within the at least one compound semiconductor detector and under the magnetic field suitable for magnetic resonance imagingwherein the object under study is single photon nuclear imaged under the magnetic field suitable for magnetic resonance imaging,wherein the at least one semiconductor detector is at least one compound semiconductor detector,wherein the at least one magnet comprises a central opening,wherein the object under study is single photon nuclear imaged by the at least one semiconductor at either end of the at least one magnet and outside the central opening of the at least one magnet such that the object under study is single photon nuclear imaged and magnet resonance imaged in a sequential manner,wherein the at least one compound semiconductor detector is adjacent and attached to the outside surface of the at least one magnet,wherein the at least one semiconductor detector comprises a first ring having a plurality of first modules and a second ring having a plurality of second modules, and wherein the first modules of the first ring are aligned to have an angular offset with the second modules of the second ring along an axial direction to view the object under study with twice the angular sampling with one axial motion. 10. The method of claim 9, the detecting of the gamma photons comprising:interacting the gamma photons with at least one compound semiconductor substrate of the at least one compound semiconductor detector; andcollecting charge carriers produced by the interaction of the gamma photons with the at least one compound semiconductor substrate. 11. The method of claim 9, wherein the correcting for the effect on the charge carriers comprises correcting for a Lorentz-force effect on the charge carriers traveling within the at least one compound semiconductor detector and under the magnetic field suitable for magnetic resonance imaging. 12. The method of claim 9, further comprising:generating at least one direct detection signal in response to detecting the gamma photons by the at least one compound semiconductor detector;receiving the detection signal by a signal processor comprising a plurality of electronics adapted to amplify, address, and process the detection signal; andremoving an interference effect of the magnetic field suitable for magnetic resonance imaging on the single photon nuclear imaging by positioning the signal processor away from the magnetic field suitable for magnetic resonance imaging. 13. A combined magnetic resonance and single photon nuclear imaging system, the system comprising:at least one compound semiconductor detector configured to directly convert incident gamma photons into electron-hole charge carriers;at least one collimator for single photon nuclear imaging an object under study with the at least one compound semiconductor detector;at least one magnet for producing a magnetic field suitable for magnetic resonance imaging; andat least one transceiver for magnetic resonance imaging the object under study with the at least one magnet,wherein the at least one compound semiconductor detector is configured to single photon nuclear image the object under study under the magnetic field suitable for magnetic resonance imaging,wherein the at least one compound semiconductor detector is adjacent and attached to the outside surface of the at least one magnet,wherein the at least one semiconductor detector comprises a first ring having a plurality of first modules and a second ring having a plurality of second modules, and wherein the first modules of the first ring are aligned to have an angular offset with the second modules of the second ring along an axial direction to view the object under study with twice the angular sampling with one axial motion. 14. The system of claim 13, wherein the at least one compound semiconductor detector comprises a material selected from the group consisting of cadmium telluride (CdTe), mercuric iodide (HgI2), thallium bromide (TlBr), gallium arsenide (GaAs), cadmium zinc telluride (CdZnTe), and cadmium manganese telluride (CdMnTe). 15. The system of claim 13, wherein the at least one compound semiconductor detector is a cadmium zinc telluride (CZT) detector. 16. The system of claim 13, wherein the at least one compound semiconductor detector comprises:at least one compound semiconductor substrate for producing the charge carriers through interaction with the gamma photons; anda plurality of electrodes for collecting the charge carriers. 17. The system of claim 13, wherein the at least one collimator is configured to be positioned between the object under study and the at least one compound semiconductor detector. 18. The system of claim 13, wherein the at least one compound semiconductor detector is a stationary detector. 19. A method of combining magnetic resonance and single photon nuclear imaging an object under study injected with a radioactive isotope, the method comprising:directly converting gamma photons from the radioactive isotope within the object under study by at least one compound semiconductor detector into electron-hole charge carriers;single photon nuclear imaging the object under study with at least one collimator positioned between the object under study and the at least one compound semiconductor detector;producing a magnetic field suitable for magnetic resonance imaging by at least one magnet; andmagnetic resonance imaging the object under study with at least one transceiver positioned between the object under study and the at least one magnet,wherein the object under study is single photon nuclear imaged under the magnetic field suitable for magnetic resonance imaging,wherein the at least one compound semiconductor detector is adjacent and attached to the outside surface of the at least one magnet,wherein the at least one semiconductor detector comprises a first ring having a plurality of first modules and a second ring having a plurality of second modules, and wherein the first modules of the first ring are aligned to have an angular offset with the second modules of the second ring along an axial direction to view the object under study with twice the angular sampling with one axial motion.