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January 31, 2021 13:40
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{ | |
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"### Spinors for Symmetric matrix , 2D for starters" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": 5, | |
"id": "decreased-world", | |
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"[(2.0^e1), (6.0^e2)]" | |
] | |
}, | |
"execution_count": 5, | |
"metadata": {}, | |
"output_type": "execute_result" | |
} | |
], | |
"source": [ | |
"\n", | |
"from pylab import * \n", | |
"from clifford import Cl\n", | |
"\n", | |
"l,b = Cl(sig=[-1,1,1],firstIdx=0)\n", | |
"locals().update(b)\n", | |
"\n", | |
"up = lambda x: x + abs(x)*e0\n", | |
"dn = lambda X: (X^e0)/e0\n", | |
" \n", | |
"x = l.randomV()(e12)\n", | |
"assert(dn(up(x))==x)\n", | |
"\n", | |
"d = 2 # size of smallest eigenval\n", | |
"r = 3 # ratio of eigenval 1 to eigenval2\n", | |
"\n", | |
"\n", | |
"B = up(e1)^up(e2) # plane of rotation, squeeze map between e1,e2\n", | |
"D = sqrt(d)*sqrt(sqrt(r))*e**(log(sqrt(r))/2*B) # the spinor\n", | |
"\n", | |
"Y = [dn(D*up(x)*~D) for x in [e1,e2]]\n", | |
"Y" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": 6, | |
"id": "going-approach", | |
"metadata": {}, | |
"outputs": [ | |
{ | |
"data": { | |
"text/plain": [ | |
"array([[2., 0.],\n", | |
" [0., 6.]])" | |
] | |
}, | |
"execution_count": 6, | |
"metadata": {}, | |
"output_type": "execute_result" | |
} | |
], | |
"source": [ | |
"# Convert to a matrix \n", | |
"X = e12.basis()\n", | |
"y = array([float(x|y) for x in X for y in Y]).reshape(2,2)\n", | |
"y" | |
] | |
}, | |
{ | |
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"execution_count": null, | |
"id": "prepared-living", | |
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"outputs": [], | |
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} | |
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"version": "3.7.3" | |
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