Short-Lived PET Radioisotope Production in a Small Plasma Focus Device
High-energy deuterons from a small plasma focus device (1.7 kJ) have been used for short-lived radioisotope production. For the 12 C(d, n) 13 N reaction, 40 kBq of 13 N was obtained by bombarding a graphite target at a 1-Hz shot repetition rate for 30 s. This could be increased to 10 MBq at a 16-Hz...
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| Veröffentlicht in: | IEEE transactions on plasma science 2010-12, Vol.38 (12), p.3393-3397 |
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| container_title | IEEE transactions on plasma science |
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| creator | Roshan, M V Springham, S V Rawat, R S Lee, P |
| description | High-energy deuterons from a small plasma focus device (1.7 kJ) have been used for short-lived radioisotope production. For the 12 C(d, n) 13 N reaction, 40 kBq of 13 N was obtained by bombarding a graphite target at a 1-Hz shot repetition rate for 30 s. This could be increased to 10 MBq at a 16-Hz repetition rate. Plasma focus devices operating with higher bank energies should produce substantially higher isotope yields. |
| doi_str_mv | 10.1109/TPS.2010.2083699 |
| format | Article |
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For the 12 C(d, n) 13 N reaction, 40 kBq of 13 N was obtained by bombarding a graphite target at a 1-Hz shot repetition rate for 30 s. This could be increased to 10 MBq at a 16-Hz repetition rate. Plasma focus devices operating with higher bank energies should produce substantially higher isotope yields.</description><identifier>ISSN: 0093-3813</identifier><identifier>EISSN: 1939-9375</identifier><identifier>DOI: 10.1109/TPS.2010.2083699</identifier><identifier>CODEN: ITPSBD</identifier><language>eng</language><publisher>New York, NY: IEEE</publisher><subject>Banks ; Devices ; Discharges ; Electrons ; Exact sciences and technology ; Gamma-ray spectroscopy ; Graphite ; Ion beams ; Isotopes ; medical isotopes ; Other confinement methods ; Physics ; Physics of gases, plasmas and electric discharges ; Physics of plasmas and electric discharges ; Plasma focus ; Plasma physics ; Plasmas ; Positron emission tomography ; positron emission tomography (PET) ; Radioactive materials ; Radioisotopes ; Repetition ; Scintillation counters ; scintillation detectors ; Shot ; Z-pinches, plasma focus and other pinch devices</subject><ispartof>IEEE transactions on plasma science, 2010-12, Vol.38 (12), p.3393-3397</ispartof><rights>2015 INIST-CNRS</rights><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. 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For the 12 C(d, n) 13 N reaction, 40 kBq of 13 N was obtained by bombarding a graphite target at a 1-Hz shot repetition rate for 30 s. This could be increased to 10 MBq at a 16-Hz repetition rate. Plasma focus devices operating with higher bank energies should produce substantially higher isotope yields.</description><subject>Banks</subject><subject>Devices</subject><subject>Discharges</subject><subject>Electrons</subject><subject>Exact sciences and technology</subject><subject>Gamma-ray spectroscopy</subject><subject>Graphite</subject><subject>Ion beams</subject><subject>Isotopes</subject><subject>medical isotopes</subject><subject>Other confinement methods</subject><subject>Physics</subject><subject>Physics of gases, plasmas and electric discharges</subject><subject>Physics of plasmas and electric discharges</subject><subject>Plasma focus</subject><subject>Plasma physics</subject><subject>Plasmas</subject><subject>Positron emission tomography</subject><subject>positron emission tomography (PET)</subject><subject>Radioactive materials</subject><subject>Radioisotopes</subject><subject>Repetition</subject><subject>Scintillation counters</subject><subject>scintillation detectors</subject><subject>Shot</subject><subject>Z-pinches, plasma focus and other pinch devices</subject><issn>0093-3813</issn><issn>1939-9375</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2010</creationdate><recordtype>article</recordtype><sourceid>RIE</sourceid><recordid>eNpdkE1LAzEQhoMoWD_ugpcgiKetk8ymuzlKbVUoWGw9hzSbxZTtpia7Bf-9kZYePA0v87zD8BByw2DIGMjH5Xwx5JAShxJHUp6QAZMoM4mFOCUDAIkZlgzPyUWMawCWC-ADMl18-dBlM7ezFZ1PlvRDV8676Du_tXQefNWbzvmWupZqutjopqHzRseNplNv-kif7c4Ze0XOat1Ee32Yl-RzOlmOX7PZ-8vb-GmWGRS8y5jgKyikkFqCAdRSlgKrCgvJV5zrymrQKxylXI1MjobXuGI1FAVnHGQh8ZI87O9ug__ubezUxkVjm0a31vdRlbnMiwJ5mci7f-Ta96FNz6mScyFA5HmCYA-Z4GMMtlbb4DY6_CgG6k-rSlrVn1Z10Joq94e7Ohrd1EG3xsVjj2Mp8lRM3O2ec9ba41qMoBQM8BdQIX1b</recordid><startdate>20101201</startdate><enddate>20101201</enddate><creator>Roshan, M V</creator><creator>Springham, S V</creator><creator>Rawat, R S</creator><creator>Lee, P</creator><general>IEEE</general><general>Institute of Electrical and Electronics Engineers</general><general>The Institute of Electrical and Electronics Engineers, Inc. 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For the 12 C(d, n) 13 N reaction, 40 kBq of 13 N was obtained by bombarding a graphite target at a 1-Hz shot repetition rate for 30 s. This could be increased to 10 MBq at a 16-Hz repetition rate. Plasma focus devices operating with higher bank energies should produce substantially higher isotope yields.</abstract><cop>New York, NY</cop><pub>IEEE</pub><doi>10.1109/TPS.2010.2083699</doi><tpages>5</tpages></addata></record> |
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| issn | 0093-3813 1939-9375 |
| language | eng |
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| source | IEEE Electronic Library (IEL) |
| subjects | Banks Devices Discharges Electrons Exact sciences and technology Gamma-ray spectroscopy Graphite Ion beams Isotopes medical isotopes Other confinement methods Physics Physics of gases, plasmas and electric discharges Physics of plasmas and electric discharges Plasma focus Plasma physics Plasmas Positron emission tomography positron emission tomography (PET) Radioactive materials Radioisotopes Repetition Scintillation counters scintillation detectors Shot Z-pinches, plasma focus and other pinch devices |
| title | Short-Lived PET Radioisotope Production in a Small Plasma Focus Device |
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