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Project Mission
To conduct quantum information related research to:
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Provide solutions for advanced quantum information science and technology to enhance US industrial competitiveness.
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Develop and exploit new calibration and metrology techniques to achieve standardization in the area of quantum information and communication.
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Provide an infrastructure for quantum communication metrology, testing, calibration, and technology development.
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R&D 100 Award (2007)


IET Finalist Award (2007)


DoC Silver (2008) and Bronze (2005) Medals

ITL Outstanding Authorship (2007)

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Most Resent Publications
Lijun Ma, S Nam, Hai Xu, B Baek, Tiejun Chang, O Slattery, A Mink and Xiao Tang, " 1310 nm differential-phase-shift QKD system using superconducting single-photon detectors ". New Journal of Physics, Vol. 11, April 2009.

Alan Mink, Joshua C Bienfang, Robert Carpenter, Lijun Ma, Barry Hershman, Alessandro Restelli and Xiao Tang, " Programmable instrumentation and gigahertz signaling for single-photon quantum communication systems ". New Journal of Physics, Vol. 11, April 2009.

Lijun Ma, Alan Mink and Xiao Tang, "High Speed Quantum Key Distribution over Optical Fiber Network System ", Journal of Research of the National Institute of Standards and Technology, Vol. 114, Number 3, Page 149, May- June 2009.

A. Mink, S. Frankel, and R. Perlner, " Quantum Key Distribution (QKD) and Commodity Security Protocols: Introduction and Integration ", International Journal of network security and its applications, Vol. 1, No. 2, July 2009.

Lijun Ma, Oliver Slattery, Tiejun Chang and Xiao Tang, " Non-degenerated sequential time-bin entanglement generation using periodically poled KTP waveguide ", Optics Express, Vol. 17 Issue 18, pp.15799-15807 (2009).

Lijun Ma, Oliver Slattery and Xiao Tang, " Experimental study of high sensitivity infrared spectrometer with waveguide-based up-conversion detector ", Optics Express Vol. 17, Issue 16, pp. 14395–14404 (2009).

Xiao Tang, Lijun Ma, Oliver Slattery, “Single photon detection and spectral measurement in near infrared region using up-conversion technology” invited talk, presented at LPHYS09, Barcelona, Spain, July 13-17, 2009.

Lijun Ma, Oliver Slattery, Tiejun Chang and Xiao Tang, “Sequential time-bin entanglement generation using periodically poled KTP waveguide”, CLEO/ IQEC (Optical Society of America, Washington, DC, 2009), JWA85.

Xiao Tang, Lijun Ma, Oliver Slattery, “Single photon detection and spectral measurement in near infrared region using up-conversion technology” invited talk, presented at LPHYS09, Barcelona, Spain, July 13-17, 2009.

Burm Baek, Lijun Ma, Alan Mink, Xiao Tang and Sae Woo Nam, " Detector performance in long-distance quantum key distribution using superconducting nanowire single-photon detectors ", Proc. SPIE, Vol. 7320, 73200D (2009).

Oliver Slattery, Alan Mink, and Xiao Tang, " Low noise up-conversion single photon detector and its applications in quantum information systems ", Proc. of SPIE Vol. 7465, 74650W, 2009.

Oliver Slattery, Lijun Ma and Xiao Tang, " Optimization of photon pair generation in dual-element PPKTP waveguide ", Proc. of SPIE Vol. 7465, 74650K, 2009.

Oliver Slattery, Lijun Ma and Xiao Tang, “High-Speed Coincidence Photon Pair Generation by Dual-Element PPKTP Waveguide over GHz repetition rate”, submitted to Frontier in Optics 2009 (the 93rd annual meeting of Optical Society of American, San Jose, October, 2009). WERB review approved.

All Publications.

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Low noise frequency up-conversion SPD demonstrated

ITL announces new frequency up-conversion technique:
For fiber-based QKD over transmission distances longer than 10 km, the wavelength of the quantum signal must be in the low-loss band of telecommunications fiber, usually around 1310 nm or 1550 nm. The available single-photon detectors that are directly sensitive to these wavelengths are InGaAs avalanche photodiodes (APDs) and superconducting single-photon detectors. Due to strong after-pulsing effects, InGaAs APDs are usually operated in a gated mode, typically limiting the clock rate of the system to several MHz. As a result, the key rate is also limited. Superconducting single-photon detectors can operate in the free-running mode and their only limitation to the sifted-key rate is the dead time, usually below 10 ns. Moreover, the time response of superconducting single-photon detectors can be less than 100 ps. However superconducting single-photon detectors are not generally available and need to be operated at low temperatures (typically 4 K). In contrast, silicon-based APDs (Si-APDs) are readily available and easy to operate. Their dead time is approximately 50 ns and their timing resolution is 300 ps or less [10, 11]. Unfortunately, while the peak detection efficiency of Si-APD can be as high as 70% around 650 nm their detection efficiency decreases rapidly at wavelengths longer than 1000 nm.

To resolve this complication, we have applied sum frequency generation to up-convert the transmitted photons from the low-loss fiber wavelengths to wavelengths where they can be efficiently detected by Si-APDs. Using periodically poled LiNbO3 (PPLN) the internal sum frequency conversion can be achieved with nearly 100% efficiency. The overall detection efficiency is 20%. Such an up-conversion single-photon detector is used in our 1310-nm QKD system and good performance is achieved.

Outline of the NIST frequency Up-Conversion module

The figure shows the configuration of the up-conversion detector. An amplified 1557-nm optical pulse train is used to pump two quantum channels. An optical filter, FLT0, is used to suppress noise from the pump. After proper polarization alignment, the pump signals are combined with the 1306-nm quantum signal and sent into periodically-polling LiNbO3 waveguide (PPLN). Through the sum-frequency generation process inside PPLN the quantum signal is up-converted to 710 nm. The output of PPLN is then efficiently detected by Si-APD once its noise is filtered off by the filters FLT1/2.

When compared with other up-conversion detectors, ours has the advantage of low dark count rate. Most of the dark counts are induced by the strong pump via Raman-Stokes effects. When we set the signal wavelength shorter than the pump wavelength, the Raman-Stokes effects are greatly reduced. Moreover, we modulate the pump to a pulse train that is synchronous to the quantum signal. By this, the dark count rate is further reduced.

H. Xu, L. Ma and X. Tang. "Low noise PPLN-based single photon detector" Proceedings of SPIE, Vol.6780, pp. 6780OU.

H. Xu, L. Ma, A. Mink, B. Hershman and X. Tang. "1310-nm quantum key distribution system with up-conversion pump wavelength at 1550 nm". Optics Express, Vol. 15, Issue 12, pp. 7247-7260.

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