Sandia Corporation

National Technology & Engineering Solutions of Sandia, LLC

Daniel B S Soh

Ryan Camacho

Scott E Bisson

Mohan Sarovar

Anthony L Lentine

Christopher Todd DeRose

Paul Davids

David Aaron Farley

Constantin Brif

Sean Moore

Described herein are various technologies pertaining to detecting tampering of a seal based upon quantum optical communication via a communications channel comprising the seal. A plurality of pulses of light encoded with random data are transmitted on the communications channel, whereupon they are received and their data values measured. The measured data values of the pulses are then compared to the known transmitted data to determine a correlation statistic between the transmitted and received data values. Tampering with the seal can be detected based upon identifying that the correlation statistic has dropped below a threshold non-tampered level of correlation between transmitted and received values.

Secure fiber optic seals enabled by quantum optical communication concepts

The various technologies presented herein relate to extracting a portion of each pulse in a series of pulses reflected from a target to facilitate determination of a Doppler-shifted frequency for each pulse and, subsequently, a vibration frequency for the series of pulses. Each pulse can have a square-wave configuration, whereby each pulse can be time-gated to facilitate discarding the leading edge and the trailing edge (and associated non-linear effects) of each pulse and accordingly, capture of the central portion of the pulse from which the Doppler-shifted frequency, and ultimately, the vibration frequency of the target can be determined. Determination of the vibration velocity facilitates identification of the target being in a state of motion. The plurality of pulses can be formed from a laser beam (e.g., a continuous wave), the laser beam having a narrow bandwidth.

Narrow bandwidth detection of vibration signature using fiber lasers

Various technologies for performing continuous-variable (CV) and discrete-variable (DV) quantum key distribution (QKD) with integrated electro-optical circuits are described herein. An integrated DV-QKD system uses Mach-Zehnder modulators to modulate a polarization of photons at a transmitter and select a photon polarization measurement basis at a receiver. An integrated CV-QKD system uses wavelength division multiplexing to send and receive amplitude-modulated and phase-modulated optical signals with a local oscillator signal while maintaining phase coherence between the modulated signals and the local oscillator signal.

Transceivers and receivers for quantum key distribution and methods pertaining thereto

Various technologies for continuous-variable quantum key distribution without transmitting a transmitter's local oscillator are described herein. A receiver on an optical transmission channel uses an oscillator signal generated by a light source at the receiver's location to perform interferometric detection on received signals. An optical reference pulse is sent by the transmitter on the transmission channel and the receiver computes a phase offset of the transmission based on quadrature measurements of the reference pulse. The receiver can then compensate for the phase offset between the transmitter's reference and the receiver's reference when measuring quadratures of received data pulses.

Self-referenced continuous-variable quantum key distribution

Various technologies pertaining to an on-chip entangled photon source are described herein. A light source is used to pump two resonator cavities that are resonant at two different respective wavelengths and two different respective polarizations. The resonator cavities are coupled to a four-wave mixing cavity that receives the light at the two wavelengths and outputs polarization-entangled photons.

On-chip entangled photon source

The various technologies presented herein relate to utilizing photons at respective idler and signal frequencies to facilitate generation of photons at a pump frequency. A strong pump field can be applied at the &#x3c9;and the &#x3c9;frequencies, with the generated idler and signal pulses being utilized to generate a photon pair at the &#x3c9;frequency. Further, the idler pump power can be increased relative to the signal pump power such that the pump power P&#x3e;pump power P. Such reversed operation (e.g., &#x3c9;+&#x3c9;&#x2192;&#x3c9;+&#x3c9;) can minimize and/or negate Raman scattering effects. By complying with an energy conservation requirement, the &#x3c9;and &#x3c9;photons interacting with the material through the four-wave mixing process facilitates the entanglement of the &#x3c9;and &#x3c9;photons. The &#x3c9;and &#x3c9;photons can be respectively formed in different length waveguides with a delay utilized to facilitate common timing between the &#x3c9;and &#x3c9;photons.

High-yield entangled single photon source

Embodiments relate to an all fiber passively Q-switched laser. The laser includes a large core doped gain fiber having a first end. The large core doped gain fiber has a first core diameter. The laser includes a doped single mode fiber (saturable absorber) having a second core diameter that is smaller than the first core diameter. The laser includes a mode transformer positioned between a second end of the large core doped gain fiber and a first end of the single mode fiber. The mode transformer has a core diameter that transitions from the first core diameter to the second core diameter and filters out light modes not supported by the doped single mode fiber. The laser includes a laser cavity formed between a first reflector positioned adjacent the large core doped gain fiber and a second reflector positioned adjacent the doped single mode fiber.

Growing community of inventors

Pleasanton, CA, United States of America

Daniel B S Soh