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55 "metadata" : {},
66 "source" : [
7- " # Simulating Gate Noise"
7+ " # Simulating Gate Noise\n " ,
8+ " $$\n " ,
9+ " \\ newcommand{ket}[1]{\\ left|{#1}\\ right\\ rangle}\n " ,
10+ " \\ newcommand{bra}[1]{\\ left\\ langle {#1}\\ right|}\n " ,
11+ " \\ newcommand{tr}{\\ mathrm{Tr}}\n " ,
12+ " $$"
813 ]
914 },
1015 {
1318 "source" : [
1419 " ## Pure states vs. mixed states\n " ,
1520 " \n " ,
16- " \n " ,
1721 " Errors in quantum computing can introduce classical uncertainty in what the underlying state is.\n " ,
1822 " When this happens we sometimes need to consider not only wavefunctions but also probabilistic sums of\n " ,
1923 " wavefunctions when we are uncertain as to which one we have. For example, if we think that an X gate\n " ,
555559 {
556560 "data" : {
557561 "text/plain" : [
558- " <matplotlib.legend.Legend at 0x1320abdd8 >"
562+ " <matplotlib.legend.Legend at 0x1384f5160 >"
559563 ]
560564 },
561565 "execution_count" : 12 ,
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