DOW-UAP-D126, AAWSAP DIRD, Advanced Nuclear Propulsion for Manned Deep Space Missions, March 2010
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This document is a Defense Intelligence Reference Document (DIRD), a technical reference format used by the Defense Intelligence Agency (DIA) to capture baseline knowledge on a specific topic for later analytic use. DIRDs are best understood as reference and synthesis products rather than as original research. It is one of 38 DIRDs produced under the Advanced Aerospace Weapon System Applications Program (AAWSAP) between 2009 and 2011. Because AAWSAP’s scope permitted a broad range of supporting topics, not every DIRD in the series directly concerns aerospace systems or future threat assessment. The following summary reflects the DIRD’s scope and framing at the time of writing and should not be read as implying current validation of the concepts discussed. This DIRD examines advanced nuclear propulsion for crewed deep-space travel and argues that human missions beyond the Moon would require propulsion systems with both very high thrust and very high specific impulse, which the author contends are difficult to achieve with conventional chemical, nuclear-thermal, and nuclear-electric systems. The report focuses on concepts derived from Project Orion, the discontinued General Atomics nuclear pulse propulsion study sponsored first by ARPA and later by the U.S. Air Force between 1958 and 1965, in which a spacecraft would be driven by repeated nuclear explosions. In this case, the DIRD emphasizes small non-fission-triggered fusion explosions using deuterium, magnetic mirrors, and other unconventional ignition concepts intended to avoid the inefficiencies associated with small fission devices. It presents these ideas as a possible pathway to crewed missions across the solar system, while also linking them to broader visions of long-range human expansion into space. The document is exploratory in character and depends on several unproven ignition methods, enabling technologies, and engineering assumptions. Overall, it is a theoretical examination of fusion-based pulse propulsion concepts rather than as a documentary account of a technology nearing practical realization.
[번역 실패: TooManyRequests] UNCLASSIFIED/ /FOR OFFI@IAk WSI: OPtklf Defense Intelligence Reference Document Acquisition Threat Support 11 March 2010 !COD: 1 December 2009 DIA-08-1003-007 Advanced Nuclear Propulsion for Manned Deep Space Missions UNCLASSIFIED/ ,'FOR OFFI@IAk WSE OHkl/ UNCLASSIFIED//F&R 8FFIOIAL l!ISE 8HLY Advanced Nuclear Propulsion for Manned Deep Space Missions Prepared by: Acquisition Support Division (DW0-3) Defense Warning Office Directorate for Analysis Defense Intelligence Agency Author: AAP Person 72 Administrative Note COPYRIGHT WARNING: Further dissemination of the photographs in this publication is not authorized. This product is one in a series of advanced technology reports produced in FY 2009 under the Defense Intelligence Agency, Defense Warning Office's Advanced Aerospace Weapon System Applications (AAWSA). Program. Comments or questions pertaining to l this document should be addressed tolAAP Person 1 AAWSA Program Manager, Defense Intelligence Agency, ATTN: CLAR/DWO-3, Bldg 6000, Washington, DC 20340-5100. ii UNCLASSIFIED//509 OFFICIAL 11&ili Qtll.¥ UNCLASSIFIED/fFOA OFFIEIAk W&liii 8Ptl¥ Contents Preface....................................................................................................................v Introduction ........................................................................................................... 1 Deuterium, Argon Ion Lasers, and Kev Superexplosives ........................................ 1 Magnetic Insulation and Inductive Charging .......................................................... 3 Magnetic Insulation ........................................................................................... 3 Inductive Charging.................................................................................................................................... 4 Deuterium as the Preferred Nuclear Rocket Fuel.................................................... 5 Magnetic Entrapment of the Charged Fusion Products and the Stopping of the Proton Beam in Dense Deuterium .......................................................................... 6 Solution in Between Two Extremes ...................................................................... 10 The Nonfission Ignition of Small Deuterium Nuclear Explosives .......................... 13 Delivery of a Gev Proton Beam Onto the Deuterium Fusion Explosive .................. 15 Lifting of Large Payloads Into Earth Orbit ............................................................ 16 Neutron Entrapment in an Autocatalytic Thermonuclear Detonation Wave - a Means to Increase the Specific Impulse and to Solve the Large Radiator Problem18 Testing the Deuterium Microdetonation Concept.................................................. 20 Conclusion............................................................................................................ 25 Appendix: Conjectured Metastable Superexplosives Formed Under High Pressure for Thermonuclear Ignition .................................................................................. 26 Bombardment of a Solid Target With an Intense Relativistic Electron or Ion Beam................................................................................................................ 28 Hypervelocity Impact ....................................................................................... 28 Bombardment of a Solid Target With Beams or By Hypervelocity Impact, Followed By a Convergent Shock Wave ............................................................ 28 References ........................................................................................................... 30 iii UNCLASSIFIED//POil Offl@IAL YSIE 8Ptll/ UNCLASSIFIED//Pelt eFFl@IAL l:ISIE 8HLY Figures Figure 1. Ignition With 107-Ampere GeV Proton Beam ......................................... 11 Figure 2. Pure Deuterium Fusion Explosion Ignited With an Intense Ion Beam ... 14 Figure 3. Screening of the Spacecraft................................................................... 14 Figure 4. Superconducting "Atomic" Spaceship.................................................... 15 Figure 5. Argon Ion Laser Igniter......................................................................... 17 Figure 6. Autocatalytic Thermonuclear Detonation Using a Soft X-ray ................. 18 Figure 7. Ordinary Marx Generator....................................................................... 21 [번역 실패: TooManyRequests] Figure 8. Super Marx Generator ........................................................................... 21 Figure 9. Artist's Conception of a 1.5-km-Long Super Marx Generator ................. 21 Figure 10. Detail View of a Section of the Super Marx Generator ......................... 22 Figure 11. Injection of GeV - 10 MA Proton Beam ................................................ 22 Figure 12. Showing a Few Elements of the Super Marx Generator ....................... 22 Figure 13. The Superconducting Toroidal Capacitor and Its Discharge Onto the Target.................................................................................................. 24 Figure 14. Explosives ........................................................................................... 26 Figure 15. With Increasing Pressure, Electron-Bridges are Formed Between Shells Inside Shells Melting Into Common Shells ................................ 26 Figure 16. p-d, Pressure....................................................................................... 29 Figure 17. Inertial Confinement Fast-Ignition Configuration................................ 30 Tables Table 1. The Charged Fusion Products of a Detonation in Deuterium: Their Energy and Velocity .................................................................................. 5 Table 2. Critical Ignition Currents for Thermonuclear Reactions ............................ 8 iv UNCLASSIFIED//Felt 8Ffl@IAI: l:l&lii &PU.¥ UNCLASSIFIED//FOR OFFl@IAL l::l!H! 8HL'I Advanced Nuclear Propulsion for Manned Deep Space Missions Preface My interest in space flight dates to when I was about 10 years old and received as a birthday gift a popular book about the feasibility of space flight. From it I learned for the first time about Oberth and Goddard and of the possibility of reaching the Moon with a multistage rocket. This occurred at the same time that Hahn and Strassmann announced the discovery of nuclear fission, with the possibility of an atomic bomb by a fission chain reaction. Having been born in Germany in 1929, I received my Ph.D. in physics under Heisenberg in 1955. Inspired by the 15-megaton hydrogen bomb test conducted by the United States in 1952, I have been deeply interested in the nonfission ignition of thermonuclear reactions by inertial confinement since 1954. At the time all fusion research in the United States was still classified, but I had quite independently discovered the basic principles of inertial confinement, the Guderley convergent shock wave, and the Rayleigh imploding shell solutions. In 1956 I presented my findings at a meeting organized by Von Weizsacker at the Max Planck Institute in Goettingen. The abstracts of this meeting reside today in the University of Stuttgart library. In 1958 I had delivered a paper at the 2nd United Nations Conference on the Peaceful Use of Atomic Energy on Nerva-type nuclear rocket reactors. The paper turned out to be of some importance as I was invited by the U.S. government to come to the United States under "Operation Paperclip." In San Diego I met Ted Taylor and Freeman Dyson, who were working on the famous "Orion" nuclear bomb propulsion concept. This concept is generally credited to Stanislaw Ulam, but I know from conversations I had with Heisenberg that a similar idea had been presented to Heisenberg by Wernher von Braun in Berlin in or around 1942. Because of my idea to use the Guderley convergent shock wave solution for thermonuclear ignition, Ted Taylor and Freeman Dyson were interested in my joining their group. But because at that time this work was classified and I was not yet a U.S. citizen, this was not possible. In 1967 I saw a new possibility for the nonfission ignition of thermonuclear microexplosions by intense relativistic electron and ion beams, driven by a high-voltage Marx generator. This ignition concept could be used not only to control the release of energy by nuclear fusion, but also to propel a spacecraft, replacing the pusher plate of the Orion concept with a magnetic mirror, reflecting the plasma-fireball of the thermonuclear microexplosion (Reference 1, 2). This idea was adopted by the British Interplanetary Society in its 1978 Project Daedalus starship study, replacing a neutron-rich deuterium-tritium (OT) thermonuclear explosive with a neutron-poor deuterium-helium3 (DHe3) explosive (Reference 3). Unlike the OT reaction, in which 80 percent of the [번역 실패: TooManyRequests] released energy goes into neutrons, most of the energy in the D-He3 reaction goes into alpha particles, which can be deflected by a magnetic mirror. But V UNCLASSIFIED/,'FOR OFFI&I.t.k Wliliii QfslL¥ UNCLASSIFIED//PO" OPPICIJ!tt l:191! OHL'f because He3 is not abundantly available everywhere, it was proposed to "mine" it from Jupiter's atmosphere. Studies have been conducted on spacecraft propulsion with the matter antimatter annihilation reaction, however, it is an enormous technical challenge to produce antimatter in appreciable quantities. The idea of using nano-gram amounts of antimatter for the ignition of fission-fusion microexplosions appears to have credible potential, but even there the production and storage of nano-gram quantities of antimatter pose serious technical problems (Reference 4). We have little reason to expect that new fundamental laws of physics that could lead to a breakthrough in propulsion still await discovery. Very much as America was discovered only once, it is quite possible that all the fundamental laws of physics relevant to propulsion have been discovered, challenging our imagination to find out if they are sufficient to invent propulsion systems that ultimately might bring us to Earthlike planets of nearby solar systems. I conclude this preface with an imaginary talk by Ted Taylor to Freeman Dyson as recorded by the latter's son, George Dyson, in his book Project Orion - The True Story of the Atomic Spaceship (Reference 5), followed by a dream of Ted Taylor's. "Freeman's hope for the Orion had rested on the fact that there seems to be no law of nature forbidding the construction of fission-free bombs," and on the belief that "improvements in the design of the nuclear devices (by reducing the fraction of total yield due to fission) might achieve reduction factors of 102 to 103• This belief in small, fission-free bombs has largely evaporated." "One exception is Ted (Taylor). He remains convinced that small, clean bombs could propel Orion - but he still fears more than ever that such devices would be irresistible as weapons, until we outgrow the habit of war. There are lots of different routes to that final result of a very clean bomb." "Could you make a one-kiloton explosion in which the fission yield was zero, which is bad news on the proliferation front, but could turn Orion into something quite clean?" "Freeman thinks Ted is wrong - and Ted hopes Freeman is right." I for my part think Freeman is wrong. Many years later, shortly before his death, Ted Taylor reported: "I had a dream last night, about a new form of nuclear weapon, and I am really scared of it." He reported that when he woke up, he wrote down his dream, and it appeared scientifically sound and feasible. What was it? We never will know with certainty, but I have a guess: it is the possibility of chemical superexplosives (explained in the appendix) powerful enough to ignite a thermonuclear bomb. vi UNCLASSIFIED//POil orr1e1s1tt tl!H! OHL¥ UNCLASSIFIED/;'FOR OFFl&I.t.k Wlilii QNL¥ Introduction As Hermann Oberth proved for chemical rockets in his 1923 book The Rocket into Planetary Space (Reference 6), this paper will try to prove for thermonuclear rockets the following: • At the present state of science and technology one can build spaceships driven by deuterium thermonuclear reactions, able to reach the outer limits of the solar system. • Such spaceships permit the manned exploration of the entire solar system and beyond, with the ultimate potential to reach nearby solar systems. • The cost in research and development to build such spaceships will be high but still well within what is economically feasible. • Using the same physical principles as for deuterium fusion rockets will also lead to the realization of clean nuclear energy, justifying the expenditures for these large projects. Deuterium can be used as the rocket fuel of choice in addition to any inert material that is suitable as a propellant. This propellant material is available on most planetary bodies and particularly on the comets of the Oort cloud. The main idea is that by gradual radial expansion from the Sun by building bridges over the Oort clouds, which presumably surround all suns, Earthlike planets in neighboring solar systems can eventually be reached. The first and most important step toward this goal is to reach the focus of the Einstein gravitational lens at 550 AU (astronomical units). At this location, one can use the Sun [번역 실패: TooManyRequests] as the lens of a super telescope, an idea first proposed by Claudio Maccone in 1993. Present knowledge is that there are planets in nearby solar systems that are likely Earthlike planets. It is only with this gigantic telescope that one can determine if life on these planets is possible. But because of the complexity of this task, a manned mission to the Einstein gravitational lens focus is likely to be needed, possible only with advanced nuclear rocket propulsion. Deuterium, Argon Ion Lasers, and KeV Superexplosives The goal is a spacecrah that can be refueled while landing on a planetary body, which can be a planet, an asteroid, or a comet. With heavy water available on many planetary bodies but in particular on comets, this suggests the use of deuterium (D) as the thermonuclear rocket fuel. Ignition of deuterium though, is more difficult than ignition of the deuterium-tritium (DT) reaction or of the deuterium-helium3 (DHe3) reaction. The DT reaction is the easiest to ignite, but 80 percent of the energy goes into neutrons, which cannot be deflected by a magnetic mirror. In the DHe3 reaction all the energy goes into charged fusion products, but in a mixture of D with He3 there are still some neutron-producing deuterium-deuterium (DD) reactions. More important is the fact that, unlike deuterium, He3 is largely unavailable. There is some indication of He3 on the surface of Moon. In the Daedalus starship study by the British Interplanetary 1 UNCLASSIFIED//FOR 8FFl@IAL t:191!! 8HL t UNCLASSIFIED//FOR err1e1J1tt U.!I! l>NLI Society, it was proposed to "mine" He3 from the atmosphere of Jup
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UNCLASSIFIED/ /FOR OFFI@IAk WSI: OPtklf Defense Intelligence Reference Document Acquisition Threat Support 11 March 2010 !COD: 1 December 2009 DIA-08-1003-007 Advanced Nuclear Propulsion for Manned Deep Space Missions UNCLASSIFIED/ ,'FOR OFFI@IAk WSE OHkl/ UNCLASSIFIED//F&R 8FFIOIAL l!ISE 8HLY Advanced Nuclear Propulsion for Manned Deep Space Missions Prepared by: Acquisition Support Division (DW0-3) Defense Warning Office Directorate for Analysis Defense Intelligence Agency Author: AAP Person 72 Administrative Note COPYRIGHT WARNING: Further dissemination of the photographs in this publication is not authorized. This product is one in a series of advanced technology reports produced in FY 2009 under the Defense Intelligence Agency, Defense Warning Office's Advanced Aerospace Weapon System Applications (AAWSA). Program. Comments or questions pertaining to l this document should be addressed tolAAP Person 1 AAWSA Program Manager, Defense Intelligence Agency, ATTN: CLAR/DWO-3, Bldg 6000, Washington, DC 20340-5100. ii UNCLASSIFIED//509 OFFICIAL 11&ili Qtll.¥ UNCLASSIFIED/fFOA OFFIEIAk W&liii 8Ptl¥ Contents Preface....................................................................................................................v Introduction ........................................................................................................... 1 Deuterium, Argon Ion Lasers, and Kev Superexplosives ........................................ 1 Magnetic Insulation and Inductive Charging .......................................................... 3 Magnetic Insulation ........................................................................................... 3 Inductive Charging.................................................................................................................................... 4 Deuterium as the Preferred Nuclear Rocket Fuel.................................................... 5 Magnetic Entrapment of the Charged Fusion Products and the Stopping of the Proton Beam in Dense Deuterium .......................................................................... 6 Solution in Between Two Extremes ...................................................................... 10 The Nonfission Ignition of Small Deuterium Nuclear Explosives .......................... 13 Delivery of a Gev Proton Beam Onto the Deuterium Fusion Explosive .................. 15 Lifting of Large Payloads Into Earth Orbit ............................................................ 16 Neutron Entrapment in an Autocatalytic Thermonuclear Detonation Wave - a Means to Increase the Specific Impulse and to Solve the Large Radiator Problem18 Testing the Deuterium Microdetonation Concept.................................................. 20 Conclusion............................................................................................................ 25 Appendix: Conjectured Metastable Superexplosives Formed Under High Pressure for Thermonuclear Ignition .................................................................................. 26 Bombardment of a Solid Target With an Intense Relativistic Electron or Ion Beam................................................................................................................ 28 Hypervelocity Impact ....................................................................................... 28 Bombardment of a Solid Target With Beams or By Hypervelocity Impact, Followed By a Convergent Shock Wave ............................................................ 28 References ........................................................................................................... 30 iii UNCLASSIFIED//POil Offl@IAL YSIE 8Ptll/ UNCLASSIFIED//Pelt eFFl@IAL l:ISIE 8HLY Figures Figure 1. Ignition With 107-Ampere GeV Proton Beam ......................................... 11 Figure 2. Pure Deuterium Fusion Explosion Ignited With an Intense Ion Beam ... 14 Figure 3. Screening of the Spacecraft................................................................... 14 Figure 4. Superconducting "Atomic" Spaceship.................................................... 15 Figure 5. Argon Ion Laser Igniter......................................................................... 17 Figure 6. Autocatalytic Thermonuclear Detonation Using a Soft X-ray ................. 18 Figure 7. Ordinary Marx Generator....................................................................... 21 Figure 8. Super Marx Generator ........................................................................... 21 Figure 9. Artist's Conception of a 1.5-km-Long Super Marx Generator ................. 21 Figure 10. Detail View of a Section of the Super Marx Generator ......................... 22 Figure 11. Injection of GeV - 10 MA Proton Beam ................................................ 22 Figure 12. Showing a Few Elements of the Super Marx Generator ....................... 22 Figure 13. The Superconducting Toroidal Capacitor and Its Discharge Onto the Target.................................................................................................. 24 Figure 14. Explosives ........................................................................................... 26 Figure 15. With Increasing Pressure, Electron-Bridges are Formed Between Shells Inside Shells Melting Into Common Shells ................................ 26 Figure 16. p-d, Pressure....................................................................................... 29 Figure 17. Inertial Confinement Fast-Ignition Configuration................................ 30 Tables Table 1. The Charged Fusion Products of a Detonation in Deuterium: Their Energy and Velocity .................................................................................. 5 Table 2. Critical Ignition Currents for Thermonuclear Reactions ............................ 8 iv UNCLASSIFIED//Felt 8Ffl@IAI: l:l&lii &PU.¥ UNCLASSIFIED//FOR OFFl@IAL l::l!H! 8HL'I Advanced Nuclear Propulsion for Manned Deep Space Missions Preface My interest in space flight dates to when I was about 10 years old and received as a birthday gift a popular book about the feasibility of space flight. From it I learned for the first time about Oberth and Goddard and of the possibility of reaching the Moon with a multistage rocket. This occurred at the same time that Hahn and Strassmann announced the discovery of nuclear fission, with the possibility of an atomic bomb by a fission chain reaction. Having been born in Germany in 1929, I received my Ph.D. in physics under Heisenberg in 1955. Inspired by the 15-megaton hydrogen bomb test conducted by the United States in 1952, I have been deeply interested in the nonfission ignition of thermonuclear reactions by inertial confinement since 1954. At the time all fusion research in the United States was still classified, but I had quite independently discovered the basic principles of inertial confinement, the Guderley convergent shock wave, and the Rayleigh imploding shell solutions. In 1956 I presented my findings at a meeting organized by Von Weizsacker at the Max Planck Institute in Goettingen. The abstracts of this meeting reside today in the University of Stuttgart library. In 1958 I had delivered a paper at the 2nd United Nations Conference on the Peaceful Use of Atomic Energy on Nerva-type nuclear rocket reactors. The paper turned out to be of some importance as I was invited by the U.S. government to come to the United States under "Operation Paperclip." In San Diego I met Ted Taylor and Freeman Dyson, who were working on the famous "Orion" nuclear bomb propulsion concept. This concept is generally credited to Stanislaw Ulam, but I know from conversations I had with Heisenberg that a similar idea had been presented to Heisenberg by Wernher von Braun in Berlin in or around 1942. Because of my idea to use the Guderley convergent shock wave solution for thermonuclear ignition, Ted Taylor and Freeman Dyson were interested in my joining their group. But because at that time this work was classified and I was not yet a U.S. citizen, this was not possible. In 1967 I saw a new possibility for the nonfission ignition of thermonuclear microexplosions by intense relativistic electron and ion beams, driven by a high-voltage Marx generator. This ignition concept could be used not only to control the release of energy by nuclear fusion, but also to propel a spacecraft, replacing the pusher plate of the Orion concept with a magnetic mirror, reflecting the plasma-fireball of the thermonuclear microexplosion (Reference 1, 2). This idea was adopted by the British Interplanetary Society in its 1978 Project Daedalus starship study, replacing a neutron-rich deuterium-tritium (OT) thermonuclear explosive with a neutron-poor deuterium-helium3 (DHe3) explosive (Reference 3). Unlike the OT reaction, in which 80 percent of the released energy goes into neutrons, most of the energy in the D-He3 reaction goes into alpha particles, which can be deflected by a magnetic mirror. But V UNCLASSIFIED/,'FOR OFFI&I.t.k Wliliii QfslL¥ UNCLASSIFIED//PO" OPPICIJ!tt l:191! OHL'f because He3 is not abundantly available everywhere, it was proposed to "mine" it from Jupiter's atmosphere. Studies have been conducted on spacecraft propulsion with the matter antimatter annihilation reaction, however, it is an enormous technical challenge to produce antimatter in appreciable quantities. The idea of using nano-gram amounts of antimatter for the ignition of fission-fusion microexplosions appears to have credible potential, but even there the production and storage of nano-gram quantities of antimatter pose serious technical problems (Reference 4). We have little reason to expect that new fundamental laws of physics that could lead to a breakthrough in propulsion still await discovery. Very much as America was discovered only once, it is quite possible that all the fundamental laws of physics relevant to propulsion have been discovered, challenging our imagination to find out if they are sufficient to invent propulsion systems that ultimately might bring us to Earthlike planets of nearby solar systems. I conclude this preface with an imaginary talk by Ted Taylor to Freeman Dyson as recorded by the latter's son, George Dyson, in his book Project Orion - The True Story of the Atomic Spaceship (Reference 5), followed by a dream of Ted Taylor's. "Freeman's hope for the Orion had rested on the fact that there seems to be no law of nature forbidding the construction of fission-free bombs," and on the belief that "improvements in the design of the nuclear devices (by reducing the fraction of total yield due to fission) might achieve reduction factors of 102 to 103• This belief in small, fission-free bombs has largely evaporated." "One exception is Ted (Taylor). He remains convinced that small, clean bombs could propel Orion - but he still fears more than ever that such devices would be irresistible as weapons, until we outgrow the habit of war. There are lots of different routes to that final result of a very clean bomb." "Could you make a one-kiloton explosion in which the fission yield was zero, which is bad news on the proliferation front, but could turn Orion into something quite clean?" "Freeman thinks Ted is wrong - and Ted hopes Freeman is right." I for my part think Freeman is wrong. Many years later, shortly before his death, Ted Taylor reported: "I had a dream last night, about a new form of nuclear weapon, and I am really scared of it." He reported that when he woke up, he wrote down his dream, and it appeared scientifically sound and feasible. What was it? We never will know with certainty, but I have a guess: it is the possibility of chemical superexplosives (explained in the appendix) powerful enough to ignite a thermonuclear bomb. vi UNCLASSIFIED//POil orr1e1s1tt tl!H! OHL¥ UNCLASSIFIED/;'FOR OFFl&I.t.k Wlilii QNL¥ Introduction As Hermann Oberth proved for chemical rockets in his 1923 book The Rocket into Planetary Space (Reference 6), this paper will try to prove for thermonuclear rockets the following: • At the present state of science and technology one can build spaceships driven by deuterium thermonuclear reactions, able to reach the outer limits of the solar system. • Such spaceships permit the manned exploration of the entire solar system and beyond, with the ultimate potential to reach nearby solar systems. • The cost in research and development to build such spaceships will be high but still well within what is economically feasible. • Using the same physical principles as for deuterium fusion rockets will also lead to the realization of clean nuclear energy, justifying the expenditures for these large projects. Deuterium can be used as the rocket fuel of choice in addition to any inert material that is suitable as a propellant. This propellant material is available on most planetary bodies and particularly on the comets of the Oort cloud. The main idea is that by gradual radial expansion from the Sun by building bridges over the Oort clouds, which presumably surround all suns, Earthlike planets in neighboring solar systems can eventually be reached. The first and most important step toward this goal is to reach the focus of the Einstein gravitational lens at 550 AU (astronomical units). At this location, one can use the Sun as the lens of a super telescope, an idea first proposed by Claudio Maccone in 1993. Present knowledge is that there are planets in nearby solar systems that are likely Earthlike planets. It is only with this gigantic telescope that one can determine if life on these planets is possible. But because of the complexity of this task, a manned mission to the Einstein gravitational lens focus is likely to be needed, possible only with advanced nuclear rocket propulsion. Deuterium, Argon Ion Lasers, and KeV Superexplosives The goal is a spacecrah that can be refueled while landing on a planetary body, which can be a planet, an asteroid, or a comet. With heavy water available on many planetary bodies but in particular on comets, this suggests the use of deuterium (D) as the thermonuclear rocket fuel. Ignition of deuterium though, is more difficult than ignition of the deuterium-tritium (DT) reaction or of the deuterium-helium3 (DHe3) reaction. The DT reaction is the easiest to ignite, but 80 percent of the energy goes into neutrons, which cannot be deflected by a magnetic mirror. In the DHe3 reaction all the energy goes into charged fusion products, but in a mixture of D with He3 there are still some neutron-producing deuterium-deuterium (DD) reactions. More important is the fact that, unlike deuterium, He3 is largely unavailable. There is some indication of He3 on the surface of Moon. In the Daedalus starship study by the British Interplanetary 1 UNCLASSIFIED//FOR 8FFl@IAL t:191!! 8HL t UNCLASSIFIED//FOR err1e1J1tt U.!I! l>NLI Society, it was proposed to "mine" He3 from the atmosphere of Jup