---
title: "预告单光子：少掉的符合，要除以什么"
description: "触发后的探测记录，怎样区分单光子源与衰减光束？"
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page_type: "story"
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  en: "https://sandboxphysics.com/stories/quantum-evidence/heralded-photon-anticorrelation-gates/"
last_modified: "2026-10-18"
---

[量子物理：读懂证据](https://sandboxphysics.com/zh/stories/quantum-evidence/)

诺奖 A · 证据与操控

# 预告单光子：少掉的符合，要除以什么

Sandbox Physics · 2026-10-18

触发后的探测记录，怎样区分单光子源与衰减光束？

## 一次点击打开试次

Grangier、Roger 与 Aspect 在 1986 年实验中使用原子辐射级联。第一个光子的探测打开短时间门，分束器后的两个探测器在门内接收第二个光子。因此，光源提供的不只有光，还有计时预告。

同一采集过程要保留四种计数：打开的门、两个输出分别点击的次数，以及同一门内的联合点击。若两个探测器几乎收不到光，联合计数很小本身说明不了多少；单路计数和门数提供比较尺度。

证据阅读：P. Grangier, G. Roger and A. Aspect (1986), Experimental Evidence for a Photon Anticorrelation Effect on a Beam Splitter, EPL 1, 173–179 — institutional copy

## 先声明经典比较

用下式的下标标记门数、两个单路计数和联合计数。在弱响应的半经典模型中，两路探测概率分别正比于同一个非负的门内积分强度，效率稳定，给定强度后的探测相互独立。强度的方差不能为负。

这使归一化反关联参数的经典下界为一；理想单光子输入则没有联合探测。比较依赖探测与采样约定：分子分母之间不能悄悄更换时间门、背景、饱和或电子串扰的处理方式。

$$
\alpha=\frac{N_{\mathrm{gate}}N_{AB}}{N_A N_B}\geq 1\quad\text{(classical, linear response)}
$$

证据阅读：P. Grangier, G. Roger and A. Aspect (1986), Experimental Evidence for a Photon Anticorrelation Effect on a Beam Splitter, EPL 1, 173–179 — institutional copy Institut d’Optique, Lab work in photonics, Single-Photon Interferences: Grangier–Roger–Aspect, pp. 71–95

## 重建一张小计数表

设一次虚拟采集有一万个门，输出 A 点击一千次，输出 B 点击八百次，联合点击八次，参数便为十分之一。相容的事件表是：八次双路、992 次仅 A、792 次仅 B，以及 8,208 次空门。

这张表避免把联合点击又算成额外试次，也让问题可复核：改变符合窗口，会改变哪些点击算作同一次事件。算例只是算术，不声称统计显著性；真实置信区间要处理联合计数及共享分母。

证据阅读：P. Grangier, G. Roger and A. Aspect (1986), Experimental Evidence for a Photon Anticorrelation Effect on a Beam Splitter, EPL 1, 173–179 — institutional copy

## 损失与背景改变不同的事

在线性响应近似内，两路各自独立的损失会从比值中抵消，但低效率仍可使大部分时间门为空。即使联合概率理想地为零，也无法区分每次预告都有一个光子，还是大量真空与至多一个光子的理想混合。

暗计数、不相关发射和多次级联会增加符合；探测器死时间或共用电子学也可能人为压低联合记录。因此，评价光源还要同时检查预告后的成功概率与背景，并让原始计数和修正计数可辨认。

证据阅读：P. Grangier, G. Roger and A. Aspect (1986), Experimental Evidence for a Photon Anticorrelation Effect on a Beam Splitter, EPL 1, 173–179 — institutional copy Institut d’Optique, Lab work in photonics, Single-Photon Interferences: Grangier–Roger–Aspect, pp. 71–95

## 衰减不会自动筛出数态

另取一个自己的泊松算例：每个指定脉冲平均含十分之一个光子。约百分之九点五的脉冲非空，而这些非空脉冲中仍约有百分之四点九含两个或更多光子。降低亮度主要增加空脉冲，并不保证有光时恰好一个。

理想模型中的衰减保留泊松统计。预告有用，是因为它改变了所检验的条件系综，但预告本身仍需测量条件记录。只说两种光源都很弱，会遮住触发实验所要辨别的差别。

证据阅读：Institut d’Optique, Lab work in photonics, Single-Photon Interferences: Grangier–Roger–Aspect, pp. 71–95

## 干涉提出另一个问题

历史实验还把同一光源送入干涉仪。条纹检验带有相位的不同可能性，输出反关联则检验联合探测统计。衰减的经典场也能产生清晰条纹，因此可见度不能代替触发计数比较。

所链接的量子擦除和双光子干涉 Lab，在各自声明的光源模型中展示相关的条件记录；它们没有采集级联光源，也没有测量这里的预告参数。应按顺序理解：先表征输入统计，再辨认不同可能性，最后解释所选符合记录。

证据阅读：P. Grangier, G. Roger and A. Aspect (1986), Experimental Evidence for a Photon Anticorrelation Effect on a Beam Splitter, EPL 1, 173–179 — institutional copy Institut d’Optique, Lab work in photonics, Single-Photon Interferences: Grangier–Roger–Aspect, pp. 71–95

## 接着操作模型

以下为已有教学 Lab；其模拟记录与上文历史观测分别对待。

- [在另一实验中比较两个输入光子](https://sandboxphysics.com/zh/labs/hong-ou-mandel/)
- [检查条件干涉记录](https://sandboxphysics.com/zh/labs/quantum-eraser/)

## 来源与阅读说明

本文核读机构镜像中的 Grangier、Roger 与 Aspect 1986 年七页论文，重点为触发计数定义与经典界限；另以 Institut d’Optique 实验讲义比较现代装置。下列计数均为虚拟算例，没有重新拟合历史记录。

1. [P. Grangier, G. Roger and A. Aspect (1986), Experimental Evidence for a Photon Anticorrelation Effect on a Beam Splitter, EPL 1, 173–179 — institutional copy](https://www.cpt.univ-mrs.fr/~verga/pdfs/Grangier-1986.pdf)
2. [Institut d’Optique, Lab work in photonics, Single-Photon Interferences: Grangier–Roger–Aspect, pp. 71–95](https://lense.institutoptique.fr/ressources/Annee3/TP_Photonique/S9-2526-PolyPhQ.EN.pdf)

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