02 2022 档案
摘要:DOI: 10.1103/PhysRevA.105.023718 Eq.(48): \[ \left< \left( n_a-n_b \right) ^2 \right> -\left< \left( n_a-n_b \right) \right> ^2 \\ c\left( |\phi 0\ran
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摘要:DOI: 10.1103/PhysRevLett.111.173601 Eq(17): \[ a_2=\frac{x+ip}{\sqrt{2}} \\ 2\bar{N}+1=2\left< {a_2}^{\dagger}a_2 \right> +1=2\left< \frac{x-ip}{\sqrt
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摘要:State after Beam Splitter Refer to page 9 of [^1] $$ |1\rangle |0\rangle \ \left( \begin{matrix} \cos \frac{\phi}{2}& -\sin \frac{\phi}{2}\ \sin \frac
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摘要:In quantum mechanics, the electric fields are operators as explained by second quantization and Fock states. Each electrical field operator can furthe
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摘要:Norm Norm for vectors \[ \begin{aligned} &\|x\| \geq 0 \\ &\|x\|=0 \text { if and only if } x=0 \\ &\|c x\|=|c|\|x\| \\ &\|x+y\| \leq\|x\|+\|y\| \end{
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摘要:Quoted from StackExchange. Suppose we have two events \((x_1,y_1,z_1,t_1)\) and \((x_2,y_2,z_2,t_2)\). Then we can define \(\Delta s^2 = -(c\Delta t)^
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摘要:DOI: 10.1103/PhysRevA.99.040101 Eq(8): Try to use Lagerange's multipliers method, only find it too complicated: \[ \begin{cases} \sum_{n=1}{\frac{p_nn
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