GHZ-state-based joint remote M-bit W state preparation method
A remote preparation and bit technology, applied in the field of quantum communication, can solve problems such as difficult implementation, multi-bit W states have not been widely studied, and a large number of quantum channel resources.
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Embodiment 1
[0060] Such as figure 1 , provides a method for joint remote preparation of M-bit W states based on GHZ states. The form of any four-bit W states to be prepared is:
[0061]
[0062] The specific steps for the joint remote preparation of the four-bit W state include:
[0063] Step 1: The sender Alice first preprocesses the quantum communication channel according to the amplitude information of the W state to realize amplitude modulation.
[0064] A quantum communication channel and a classical communication channel are established between the sender Alice and another sender Bob and the receiver Charlie. Among them, two senders Alice, another sender Bob and a receiver Charlie share two GHZ quantum entangled states:
[0065]
[0066] Among them, the parameter α 1 ,α 2 ,β 1 ,β 2 is a real number, b 0 = α 1 alpha 2 ,b 1 = α 1 beta 1 ,b 2 = α 2 beta 1 ,b 3 = α 2 beta 2 To meet the conditions Particle A 1 ,A 2 Belonging to the sender Alice, Particle B 1 ...
Embodiment 2
[0101] Such as figure 2 As shown, a method for joint remote preparation of a five-bit W state based on the GHZ state is provided. The form of any five-bit W state to be prepared is:
[0102]
[0103] The specific steps for the joint remote preparation of the five-bit W state include:
[0104] Step 1: The sender Alice first preprocesses the quantum communication channel according to the amplitude information of the W state to realize amplitude modulation.
[0105] A quantum communication channel and a classical communication channel are established between the sender Alice and another sender Bob and the receiver Charlie. Among them, two senders Alice, another sender Bob, and a receiver Charlie share three GHZ quantum entangled states:
[0106]
[0107] Among them, the parameter α 1 ,α 2 ,α 3 ,β 1 ,β 2 ,β 3 is a real number, b 0 = α 1 alpha 2 alpha 3 ,b 1 = α 1 beta 2 alpha 3 ,b 2 = β 1 alpha 2 alpha 3 ,b 3 = β 1 beta 2 alpha 3 ,b 4 = α 1 alpha ...
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