Time-bin QKD: Difference between revisions

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2. A NIM FAN-OUT Module was used to split the short pulse into two identical NIM pulses, with the rise time (10% to 90%) decreased to about 780ps.
2. A NIM FAN-OUT Module was used to split the short pulse into two identical NIM pulses, with the rise time (10% to 90%) decreased to about 780ps.


3. The two identical NIM pulse were sent to the signal and veto inputs of an NIM Anti-coincidence Module respectively, producing an output pulse with a width of about 1ns. The rise time of the pulse is about xxxps.
3. The two identical NIM pulse were sent to the signal and veto inputs of an NIM Anti-coincidence Module respectively, producing an output pulse with a width of about 2ns. The rise time of the pulse is about 780ps.


== Result and Discussion ==  
== Result and Discussion ==  


== Conclusion ==
== Conclusion ==

Revision as of 11:59, 19 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, Δt, 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

Vout=B∧B′‾.

When the leading edge of B arrives, the output becomes high. After a delay Δt, 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:

Tpulse≈Δt.

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.

Experiment Record

2026-10-5

1. Prof. Kurtsiefer explained the principles of experiments and the experimental apparatuses.

2. We learned how to use Oscilloscope HDO6104.

2026-10-6

1. We used the Function Generator AFG1022 to generate a short pulse that followed NIM Standard and had a width of about 40ns. The rise time (10% to 90%) of the pulse is approximately 2ns.

2. A NIM FAN-OUT Module was used to split the short pulse into two identical NIM pulses, with the rise time (10% to 90%) decreased to about 780ps.

3. The two identical NIM pulse were sent to the signal and veto inputs of an NIM Anti-coincidence Module respectively, producing an output pulse with a width of about 2ns. The rise time of the pulse is about 780ps.

Result and Discussion

Conclusion