Classical Fully Homomorphic Encryption for Quantum Circuits: Difference between revisions

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####Server generates following superposition sampled over random distribution D for the TCF function pairs (<math>f_0=</math>AltHE.Enc<math>_{pk}(),f_1</math>) based on the condition <math>f_0\oplus_H f_1=\hat{c}</math></br><math>\sum_{\mu\in\{0,1\},r} \sqrt{D(\mu,r)}|\mu,r\rangle</math>
####Server generates following superposition sampled over random distribution D for the TCF function pairs (<math>f_0=</math>AltHE.Enc<math>_{pk}(),f_1</math>) based on the condition <math>f_0\oplus_H f_1=\hat{c}</math></br><math>\sum_{\mu\in\{0,1\},r} \sqrt{D(\mu,r)}|\mu,r\rangle</math>
#### Servers then entangles the two superposition states on quantum input and random distribution D with a third register for function output as follows:</br><math>\sum_{a,b,\mu\in\{0,1\},r}\alpha_{ab}\sqrt{D(\mu,r)}|a,b\rangle|\mu,r\rangle|f_a(r)\rangle</math>
#### Servers then entangles the two superposition states on quantum input and random distribution D with a third register for function output as follows:</br><math>\sum_{a,b,\mu\in\{0,1\},r}\alpha_{ab}\sqrt{D(\mu,r)}|a,b\rangle|\mu,r\rangle|f_a(r)\rangle</math>
####Server measures the last register to get a secret text <math>y = </math>AltHE.Enc<math>_{pk}(\mu_0,r_0)</math>, where <math>\mu_0\oplus\mu_1=s</math>.
####Server measures the last register to get a secret text <math>y = AltHE.Enc_{pk}(\mu_0,r_0)</math>, where <math>\mu_0\oplus\mu_1=s</math>.
####Server performs Hadamard on second register and measures it to get a string d such that first register of input quantum state is reduced to: the following ideal state:</br><math>(Z^{d\cdot ((\mu_0,r_0)\oplus (\mu_1,r_1))}\otimes X^{\mu_0})\textrm{CNOT}_{1,2}^s|\psi\rangle</math> </br>where <math>\text{AltHE.Enc}_{pk}(\mu_0;r_0) = \text{AltHE.Enc}_{pk}(\mu_1;r_1) \oplus_H \hat{c}</math> and <math>\oplus_H</math> is the homomorphic XOR operation.
####Server performs Hadamard on second register and measures it to get a string d such that first register of input quantum state is reduced to: the following ideal state:</br><math>(Z^{d\cdot ((\mu_0,r_0)\oplus (\mu_1,r_1))}\otimes X^{\mu_0})\textrm{CNOT}_{1,2}^s|\psi\rangle</math> </br>where <math>\text{AltHE.Enc}_{pk}(\mu_0;r_0) = \text{AltHE.Enc}_{pk}(\mu_1;r_1) \oplus_H \hat{c}</math> and <math>\oplus_H</math> is the homomorphic XOR operation.
####The server uses <math>pk_{i+1}</math> to compute HE.Enc<math>_{pk_{i+1}}(c_{x,z,pk_i})</math> and HE.Enc<math>_{pk_{i+1}}(\hat{c},y,d)</math>.  
####The server uses <math>pk_{i+1}</math> to compute HE.Enc<math>_{pk_{i+1}}(c_{x,z,pk_i})</math> and HE.Enc<math>_{pk_{i+1}}(\hat{c},y,d)</math>.  
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