Freeman Posted December 20, 2005 Share Posted December 20, 2005 My head is spinning from Penrose's treatment of twistors. Isn't it essentially a special sort of spinor? [math]Z^{/alpha} = (\omega^{A}, \pi_{A'})[/math] where Z is a twistor. Also, why is the linear and angular momentum used? Can't I use, say, something else that satisfies: [math] \omega^{A} = i r^{AA'}\pi_{A'}[/math]; [math]\frac{\omega^{A}}{\pi_{A'}} = ir^{AA'}[/math] or am I on the wrong track totally? Link to comment Share on other sites More sharing options...
□h=-16πT Posted January 10, 2006 Share Posted January 10, 2006 Are you reading this from his "Road to Reality" or the second volume of his and Rindler's book on spinors/twistors? Link to comment Share on other sites More sharing options...
Freeman Posted January 15, 2006 Author Share Posted January 15, 2006 I first came upon them in Three Roads to Quantum Gravity by Lee Smolin, then I dug them up in the internet. I have read his book Road to Reality and from his description, it's just a more complex spinor. Rather than working with two axes, one works with four? Is that it? Or am I way off? Link to comment Share on other sites More sharing options...
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