How to use the dispersion in the $\chi^{(3)}$ tensor for broadband generation of polarization-entangled photons
Polarization-entangled photon pairs are a widely used resource in quantum optics and technologies, and are often produced using a nonlinear process. Most sources based on spontaneous parametric downconversion have relatively narrow optical bandwidth because the pump, signal and idler frequencies mus...
Gespeichert in:
Hauptverfasser: | , , , |
---|---|
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext bestellen |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
Zusammenfassung: | Polarization-entangled photon pairs are a widely used resource in quantum
optics and technologies, and are often produced using a nonlinear process. Most
sources based on spontaneous parametric downconversion have relatively narrow
optical bandwidth because the pump, signal and idler frequencies must satisfy a
phase-matching condition. Extending the bandwidth, for example to achieve
spectral multiplexing, requires changing some experimental parameters such as
temperature, crystal angle, poling period, etc. Here, we demonstrate broadband
(tens of THz for each photon) generation of polarization-entangled photon pairs
by spontaneous four-wave mixing in a diamond crystal, with a simple colinear
geometry requiring no further optical engineering. Our approach leverages the
quantum interference between electronic and vibrational contributions to the
$\chi^{(3)}$ tensor. Entanglement is characterized in a single realization of a
Bell test over the entire bandwidth using fiber dispersion spectroscopy and
fast single-photon detectors. The results agree with the biphoton wavefunction
predicted from the knowledge of the $\chi^{(3)}$ and Raman tensors and
demonstrate the general applicability of our approach to other crystalline
materials. |
---|---|
DOI: | 10.48550/arxiv.2408.11477 |