Super-resolution quantum interference measurement system based on parity detection strategy and super-resolution quantum interference measurement method thereof
A quantum interference and measurement system technology, which is applied in the direction of measuring devices, instruments, and optical devices, can solve the problem of low resolution of interferometers, achieve the effect of improving detection resolution, improving resolution, and realizing performance advantages
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specific Embodiment approach 1
[0023] Specific implementation mode one: combine figure 1 Illustrate this embodiment mode, a kind of super-resolution quantum interferometry system based on odd-even detection strategy, it is characterized in that it comprises: synchronous signal device (1), pulsed laser (2), odd-even detector (9), interferometer (10) ;
[0024] The parity detector (9) includes a photon number resolution counter (7) and a control and signal processing system (8);
[0025] The synchronous annunciator (1) generates two beams of synchronous signals, one beam of synchronous signals is transmitted to the pulsed laser (2), and the pulsed laser (2) is driven to generate pulsed lasers, and the pulsed lasers are passed through the interferometer (10) to generate two beams of pulsed lasers, and one of them is selected Any beam of pulsed laser light is transmitted to the photon number resolution counter (7), and the photon number resolution counter (7) detects the pulsed laser light; the detection resu...
specific Embodiment approach 2
[0028] Specific implementation mode two: combination figure 2 Describe this embodiment, the difference between this embodiment and specific embodiment one is that: the interferometer (10) includes a first non-polarizing beamsplitter prism (3), a first total reflection mirror (4), a second total reflection mirror ( 5) and the second non-polarizing beam splitter prism (6);
[0029] The synchronous annunciator (1) generates two beams of synchronous signals, one beam of synchronous signals is transmitted to the pulsed laser (2), and the pulsed laser (2) is driven to generate pulsed laser, and the pulsed laser is divided into two beams by the first non-polarizing beam splitter (3), One beam is reflected by the first total reflection mirror (4) and reaches the second non-polarization beam splitter (6), and the other beam is reflected by the second total reflection mirror (5) and reaches the second non-polarization beam splitter (6), and the two beams reach the second non-polarizati...
specific Embodiment approach 3
[0033]Embodiment 3: This embodiment differs from Embodiment 1 or Embodiment 2 in that: the interferometer is a Mach-Zehnder interferometer (MZI).
[0034] Other steps and parameters are the same as those in Embodiment 1 or Embodiment 2.
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