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CS-TC03 Scheda tecnica(PDF) 1 Page - Wavelength Electronics, Inc. |
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CS-TC03 Scheda tecnica(HTML) 1 Page - Wavelength Electronics, Inc. |
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1 / 5 page ![]() © 2020 • Sales & Technical Support: (406) 587-4910 • email: sales@teamWavelength.com • web: www.teamWavelength.com Case Study CS-TC03 Rev. A Single-Mode, Narrow Band Photon Source Using SPDC for Hybrid Quantum Systems April, 2020 Page 1 ABSTRACT Generating single-mode, narrow-band photons with high purity and brightness has proven to be difficult. Researchers at the University of Vienna have designed a photon source using Spontaneous Parametric Down-Conversion (SPDC) with a doubly resonant Optical Parametric Oscillator (OPO) utilizing an additional birefringent crystal to tune clusters independent of SPDC phase-matching. Achieving the doubly resonant condition in the OPO that enables a single mode is the challenge when creating a photon source with both single-mode and narrow-bandwidth. This is resolved here, as the resulting photon source has a bandwidth of 10.9 MHz to match the linewidths of atomic transitions. The source also produces single- mode photon pairs at a rate of 47.5 Hz without mode filters reducing loss in the system. This novel design enables research and applications in the quantum realm using hybrid light-matter interactions. HYBRID QUANTUM SYSTEMS Many quantum systems utilize single photons and their spectral properties. Hybrid quantum systems combine single photon-based and matter-based designs to implement two-qubit gates, the foundation for quantum computers and information processing.1 Applications for this type of photon source range from observing quantum phenomena to quantum communication. Spontaneous Parametric Down-Conversion (SPDC) is one hybrid photon-matter based system used to generate single photons at a high purity level. This method also allows some control of the wavelength and bandwidth of the output photons. An Optical Parametric Oscillator (OPO) can be used to generate coherent light.2 The novel use of a birefringent crystal in the OPO combined with SPDC achieves photon selection with minimal losses. METHODS & PROBLEMS To implement two-qubit gates for many quantum applications, hybrid quantum systems need to be created with photon-matter interactions. Several characteristics of the generated photon must be achieved to establish a quality photon source for quantum applications. One challenge is obtaining high-purity single photons. Successful methods include: quantum dots, single nitrogen vacancy center in nanodiamonds, and SPDC.1 The first two methods do not allow for photon heralding. That is, after a photon is down-converted to two lower energy photons, one of the signal or idler photons is detected or measured, ensuring the other will also be detected with accurate knowledge of its state. What is sPDC & OPO? SPDC is, essentially, a "down-conversion" of a single photon instantaneously. Figure 1 shows how SPDC works. Crystal Input Beam γ 1 Signal γ 2 Idler γ 3 One photon (γ 1) enters the nonlinear crystal and is down-converted into two separate photons: signal and idler (γ 2 and γ3). Down-converted means that the two output photons will have lower frequencies (and also energies) than the input photon. Because of the laws of conservation of energy and momentum, the two output photons must have lower energies and momenta than that of the initial photon such that: Eγ 1 = Eγ2 + Eγ3 (1) k 1 = k2 + k3 (2) where E is the energy of the appropriate photon, γ 1,2,3 distinguishes each photon, and k is the momentum of the photon. The frequency of each photon can be related in the same way, as energy is related to frequency by either h or ħ (planck constant or reduced planck constant depending on using frequency or angular frequency). Figure 1. Spontaneous Parametric Down- Conversion Process |
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