Time-bin QKD: Difference between revisions
No edit summary |
|||
| (3 intermediate revisions by the same user not shown) | |||
| Line 6: | Line 6: | ||
== Theoretical Background == | == Theoretical Background == | ||
== List of Equipment == | == List of Equipment == | ||
== Experiment Setup == | {| class="wikitable" | ||
|- | |||
! Equipment !! Manufacturers !! Quantities | |||
|- | |||
| Function Generator AFG1022 || Tektronix, Inc || 1 | |||
|- | |||
| Oscilloscope HDO6104 || Teledyne LeCroy || 1 | |||
|- | |||
| NIM FAN-OUT Module || S-Fifteen Instruments || 1 | |||
|- | |||
| NIM Anti-coincidence Module || S-Fifteen Instruments || 2 | |||
|- | |||
| NIM cables || || multiples | |||
|- | |||
| BNC cables || || multiples | |||
|} | |||
== Experiment Setup == | |||
=== 1. Producing a short pulse === | |||
The shortest pulse that can be generated by the function generator is about 40 nanoseconds, which is too long for our purpose. To create a shorter pulse, we performed pulse shortening using delayed Anti-Coincidence Logic. | |||
A short electrical pulse was first generated using function generator with high level as 0V and low level as -1.0V, following NIM (Nuclear Instrumentation Module) Standard. | |||
The input pulse was first passed through a fanout module to produce two identical copies, B and B'. A relative time delay, <math>\Delta t</math>, was introduced between the two signals before they were sent to the signal and veto inputs of the anti-coincidence module. The anti-coincidence module produces an output only when B is present while the delayed signal B' is absent. This operation can be represented as | |||
<math> V_{out} = B \land \overline{B'}</math>. | |||
When the leading edge of B arrives, the output becomes high. After a delay <math>\Delta t</math>, the leading edge of B' reaches the veto input and suppresses the output. Consequently, the original pulse is converted into a much shorter pulse whose width is approximately determined by the relative delay: | |||
<math>T_{\mathrm{pulse}}\approx \Delta t</math>. | |||
Thus, by controlling the delay between the two copies of the input signal, the output pulse width can be adjusted independently of the width of the original pulse. The short pulse is generated at the rising edge of the input signal. | |||
== Result and Discussion == | == Result and Discussion == | ||
== Conclusion == | == Conclusion == | ||
Latest revision as of 20:00, 6 October 2026
Team Members: Wang Ziyan, Wu Jinbin
Summary
The project is to implement time-bin QKD on the encoding and decoding ends.
Theoretical Background
List of Equipment
| Equipment | Manufacturers | Quantities |
|---|---|---|
| Function Generator AFG1022 | Tektronix, Inc | 1 |
| Oscilloscope HDO6104 | Teledyne LeCroy | 1 |
| NIM FAN-OUT Module | S-Fifteen Instruments | 1 |
| NIM Anti-coincidence Module | S-Fifteen Instruments | 2 |
| NIM cables | multiples | |
| BNC cables | multiples |
Experiment Setup
1. Producing a short pulse
The shortest pulse that can be generated by the function generator is about 40 nanoseconds, which is too long for our purpose. To create a shorter pulse, we performed pulse shortening using delayed Anti-Coincidence Logic.
A short electrical pulse was first generated using function generator with high level as 0V and low level as -1.0V, following NIM (Nuclear Instrumentation Module) Standard.
The input pulse was first passed through a fanout module to produce two identical copies, B and B'. A relative time delay, , was introduced between the two signals before they were sent to the signal and veto inputs of the anti-coincidence module. The anti-coincidence module produces an output only when B is present while the delayed signal B' is absent. This operation can be represented as
.
When the leading edge of B arrives, the output becomes high. After a delay , the leading edge of B' reaches the veto input and suppresses the output. Consequently, the original pulse is converted into a much shorter pulse whose width is approximately determined by the relative delay:
.
Thus, by controlling the delay between the two copies of the input signal, the output pulse width can be adjusted independently of the width of the original pulse. The short pulse is generated at the rising edge of the input signal.