22 Visible and infared stellar parallaxes | 18 |
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222 Age of the Galaxy | 19 |
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224 Stellar evolution | 20 |
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225 Targets of opportunity | 22 |
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232 Astronomy | 24 |
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233 Cosmology | 25 |
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234 Solar system studies | 26 |
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241 Dust | 27 |
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242 Plasma and energetic particle distributions | 28 |
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245 Plasma waves | 29 |
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26 References | 30 |
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Magnifying the nearby stellar systems | 33 |
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33 Keplerian theory of simple hyperbolic flybys | 36 |
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34 The flyby of the Sun performed by the FOCAL spacecraft | 43 |
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35 References | 45 |
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Astrodynamics to exit the solar system at the highest speed | 47 |
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421 Elementary background planar problem | 48 |
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422 Optimization of a single Jupiter flyby | 49 |
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423 Two optimized Jupiter flybys plus one intermediate Sun flyby | 50 |
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43 A chemically powered closeSun flyby? | 51 |
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44 Theory of the Sun Flyby enhanced by a perihelion boost | 52 |
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45 Determining the perihelion boost by knowing the target star the time to get 550 AU and the Sun approach | 53 |
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46 References | 57 |
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SETI and the FOCAL space mission | 58 |
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52 The narrowband assumption SETI | 60 |
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53 A short introduction to the KLT | 63 |
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54 Mathematics of the KLT | 64 |
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advantages of the KLT for the FOCAL space mission | 67 |
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GLSETI gravitational lensing SETI Receiving far ETI signals focused by the gravity of other stars | 71 |
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62 Only two types of SETI searches from the Earth up to 2001 | 72 |
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623 Searches | 73 |
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625 Allsky survey | 74 |
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626 Common requirements | 75 |
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632 Summary | 80 |
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64 Maccones equation relating to 1 magnification of lensing star 2 distance of the ET transmitter and 3 power of the ET transmitter | 81 |
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the Search for ExtraTerrestrial Visitation | 83 |
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66 References | 84 |
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The gravitational lenses of Alpha Centauri A B C and of Barnards Star | 85 |
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72 The Suns gravity+plasma lens as a model for the nearby stars | 86 |
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73 Assumed data about Alpha Centauri A B C and Barnards Star | 90 |
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74 Gravitational lens of the naked Sun | 93 |
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75 Gravitational lens of the naked Alpha Centauri A | 98 |
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76 Gravitational lens of the naked Alpha Centauri B | 101 |
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77 Gravitational Lens of the naked Alpha Centauri C Proxima | 104 |
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78 Gravitational lens of the naked Barnards Star | 107 |
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79 Conclusions | 110 |
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The Coronal Plasma pushing the focus of the gravity+plasma lens far beyond 550AU | 113 |
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82 The refraction of electromagnetic waves in the Sun Coronal Plasma | 115 |
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83 Summary of the Sun pure gravity naked Sun lightbending theory | 116 |
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focal axis intercept for any ray passing at distance b from the Sun | 118 |
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85 Asymptotic z straight light path | 122 |
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closeSun middistance and atinfinity LK and F Corona respectively | 123 |
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87 Focal distance vs height and minimal focal distance for any assigned frequency | 127 |
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88 The two causes of the gravity+plasma lens of the sun | 130 |
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89 Observing frequencies for the closeSun middistance and atinfintity approxiamtions | 131 |
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810 References | 134 |
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NASAs Interstellar Probe ISP20102070 and the Cosmic Microwave Background CMB | 135 |
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2010 to 2055 | 136 |
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93 Looking at the 2728 K Cosmic Microwave Backround through the Suns gravity lens by virtue of NASAs Interstellar Probe ISP | 137 |
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94 The effective minimal focal distance for the gravity+plasma lens looking at the 27K Cosmic Microwave Background is 763 AU which NASAs Int... | 142 |
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95 Improving COBEs angular resolution by nine orders of magnitude by looking at the 27K Cosmic Microwave Background by virtue of NASAs Int... | 145 |
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96 Conclusions | 146 |
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98 References | 147 |
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KLToptimized telecommunications | 148 |
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A simple introduction to the KLT | 151 |
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103 A heuristic derivation of the KL expansion | 152 |
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104 The KLT finds the best basis eigenbasis in Hilbert space spanned by the eigenfunctions of the autocorrelation of Xt | 155 |
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105 Continuous time vs discrete time in the KLT | 157 |
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just a linear transformation in the Hilbert space | 158 |
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The Final Variance theorem | 159 |
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108 BAM Bordered Autocorrelation Method to find the KLT of stationary processes only | 162 |
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109 Developments in 2007 and 2008 | 168 |
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1010 KLT of stationary white noise | 169 |
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1011 KLT of an ET sinusoidal carrier buried white cosmic noise | 170 |
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1012 Analytic proof of the BAMKLT | 172 |
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1013 KLT signaltonoise SNR as a function of the final T eigenvalue index n and alien frequencies v | 174 |
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1014 How to eavesdrop on alien chat | 175 |
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1015 Conclusions | 176 |
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1016 Acknowledgments | 177 |
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KLT of radio signals from relativistic spaceships in uniform and decelerated motion | 180 |
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