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absolute zero. And it's empty: less than one millionth the density of the highest vacuum that scientists can currently attain. That is how unlike Earth a typical location is. Yet the two are similar in one remarkable way. Take a telescope and gaze even further out than where we've just been, at a "q
299 (11* Cir. 2003); United Stalest. Garrett, 190 F.3d 1220 (11th Cir. 1999); United States' Burgess, 175 F.3d j261 (11th Cir. 1999); United States' Rojas, 145 Fed. Appx. 647 (11* Cir. 2005); United States'. Root, 296 F.3d 1222 (11th Cir. 2002). United Stalest Murrell, 368 F.3d 1283 (116 Cir. 2004), i
absolute zero. And it's empty: less than one millionth the density of the highest vacuum that scientists can currently attain. That is how unlike Earth a typical location is. Yet the two are similar in one remarkable way. Take a telescope and gaze even further out than where we've just been, at a "q
9 (11° Cir. 2003); United States it Garrett, 190 F.3d 1220 (11° Cir. 1999); United States v. Burgess,175 F.3d 1261 (11° Cir. 1999); United States v. Rojas, 145 Fed. Appx. 647 (11° Cir. 2005); United States it Root, 296 F.3d 1222 (11th Cir. 2002). United States it Murrell, 368 F3d 1283 (11th Cir. 2004)
absolute zero. And it's empty: less than one millionth the density of the highest vacuum that scientists can currently attain. That is how unlike Earth a typical location is. Yet the two are similar in one remarkable way. Take a telescope and gaze even further out than where we've just been, at a "q
9); United States' Panfil, supra, 338 I 1299 (116 Cii 2003); United States v. 1999); United &awl Burgess, 175 .3d r61(II.Ci 1999); United States! Rojas, 145 Fed. Appx. 647 (11° Cir. 2005); United States Root, 296 3d 1222 (11° Cir. 200 ). United States! Murrell, 368 II3d 1283 (114 Cir. 2004), is i
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Marc Rich
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Stephen Hawking
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Julie K. Brown
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