Company presentation Closed Joint Stock Company Superconducting - - PowerPoint PPT Presentation

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Company presentation Closed Joint Stock Company Superconducting - - PowerPoint PPT Presentation

Company presentation Closed Joint Stock Company Superconducting nanotechnology SCONTEL 1 About us SCONTEL was founded in 2004 as a spinoff of the Radio-Physics Research&Education Center (RPhREC) (group leader Prof. Gregory Goltsman )


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Company presentation

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Closed Joint Stock Company

Superconducting nanotechnology SCONTEL

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About us

The commercial activity of company based on the results of the RPhREC’s research in the field of hot-electron phenomena in ultra thin superconducting films and its application to practical superconducting devices.

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SCONTEL was founded in 2004 as a spinoff of the Radio-Physics Research&Education Center (RPhREC) (group leader Prof. Gregory Gol’tsman) at the Department of Physics of Moscow State Pedagogical University.

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Superconducting films

Films from NbN or MoRe are used

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Superconducting Single Photon Detectors Detectors for THz and Middle IR ranges

Products

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Products

5 Cryogenic Insert for a standard liquid helium storage Dewar Liquid Helium Cryostat Closed Cycle Refrigerator (Cryogenic Free)

Superconducting Single Photon Detectors Detectors for THz and Middle IR ranges

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Superconducting Single Photon Detectors

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Sensitive element of SSPD Optical coupling

Standard single-mode optical fibers: Nufern 780-HP, Corning SMF 28, ZBLAN.

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Mechanism of SSPD Photon Detection

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Two-channel Superconducting Single Photon Receiver

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Quantum efficiency and Dark count rate of SSPD receiver

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Advantages and Applications of SSPD

Possible applications:

  • Photonic quantum computing
  • Photon correlation

measurements

  • Quantum cryptography
  • Free space communication
  • LIDAR
  • Time-resolved fluorescence

measurements

  • Picosecond Integrated Circuits

analysis (PICA)

  • Single quantum dot/molecule

fluorescence spectroscopy

  • Registration of extra low IR

photon flux

  • Optical tomography

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Advantages of SSPD:

  • Operation in the visible and

infrared ranges (overlapping unavailable for the APD range);

  • Very low level of dark counts

(below 10 cps)

  • Picosecond time resolution;
  • High quantum efficiency (up to

25%);

  • Operation in a continuous

mode;

  • No afterpulsing;
  • One, two, or multi-channel

systems are available;

  • Standard single-mode fiber

input;

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Comparison with competitors

The type of detector Working temperature, К Quantum efficiency, QE, % Time resolution, t, ps Dark counts, D, Hz Quality parameter, H Dead time, ns Photo Multiplier Tube

200 2 300 2105 3.33102 100

InGaAs photodiode (APD)

200 10 370 91 2.97105 0.1

Frequency up- conversion detectors

300 2 40 2104 2.5104 100

Transition edge sensor (TES)

0.1 50 100 3 1.67106 1

SSPD

2 25 25 10 5107 2

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For λ = 1,55 µm

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Implementation of NbN SSPD: Silicon CMOS IC Device Debug

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Normally operating nMOS transistor emits near IR photons (0.9-1.4um) when current passes through the channel. Time-correlated photon emission detection measures transistor switching time. www.research.ibm.com/topics/serious/c hip/images/

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Long-distance quantum key distribution

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Hiroki Takesue, Sae Woo Nam, Qiang Zhang, et. al., Nature photonics, Vol.1., 343-348, June, 2007.

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Superconducting NbN single-photon detector for detection of individual massive and neutral biological molecules

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Markus Marksteiner, Philipp Haslinger, Michele Sclafani, Hendrik Ulbricht, Markus Arndt, Faculty of Physics, University of Vienna

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Superconducting NbN single-photon detector for detection of individual massive and neutral biological molecules

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A typical individual peak, which we attribute to the detection of neutral molecule hitting the chip. The signal was recorded with a 20x20 m SSPD chip after 20 db amplification. Bias current: 19.5 A.

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Fast Receivers for THz and Middle IR ranges

  • Receiver System based on the Superconducting Hot

Electron Bolometer (SHEB) technology

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Superconducting Hot Electron Bolometer

Any radiation impinging on the absorptive element raises its temperature what destruct superconductive state of film and leads to voltage’s change.

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System’s operating characteristics

Typical frequency dependence of the noise equivalent power (NEP) for the three types of receiver systems.

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Technical specifications of the THz receivers

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Type

1 1a 2 2a 3 3a

Frequency range, THz

0.1-6 1-40 20-100

Noise equivalent power (NEP), W×Hz-1/2

5-7×10-14 3-5×10-13 1-2×10-11 6-8×10-11 1-2×10-12 4-5×10-12

Response time, ns

1 0.05 1 0.05 1 0.05

Dynamic range, µW

0.1 50 2

Bandwidth of amplifier, MHz

0.01-200 1-3500 0.01-200 1-3500 0.01-200 1-3500

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Advantages and Applications of THz receivers

Possible applications:

  • Radio astronomy observations

(including space-based)

  • Terahertz spectroscopy
  • Near-field microscopy
  • All-weather navigation systems
  • Atmospheric Remote Sensing
  • Fusion Diagnostics
  • Electron cyclotron emission and

interferometry

  • Terahertz imaging for security
  • Laser radiation detection
  • Materials Characterization
  • Network Analyses

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Advantages:

  • Response time down to 50 ps
  • Ultra high sensitivity (noise

equivalent power (NEP) down to 10-14 W·Hz-1/2)

  • Operation frequency range

from 0.1 THz to 70 THz

  • Registration of short pulses

(from nano- to picoseconds THz pulses)

  • Different beam geometry

(beam pattern F/3 to F/∞ (collimated beam))

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Comparison with others

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Semiconductors THz receivers SCONTEL HEB Neceivers

Detector type

HgCdTe InSb Ge:Ga Si NbN MoRe

Operation temperature

77 K 4 K 4 K 4 K 4 K 4 K

Wavelength range

4÷20 m

bandwidth ~30%

0.6÷5 mm 60÷120 m 15÷2000 m 3÷1000 m 3÷1000 m

Response time

~1 s ~ 1 s ~ 10 s ~ 200 s ~ 50 ps ~ 1 ns

NEP, W/Hz0.5

~10-12 ~10-12 ~10-12 ~10-13 <3∙10-13 <5∙10-14

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HEB mixer application in ground- based radio astronomy

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10-meter the Heinrich Hertz Telescope (HHT) on Mt. Graham (Arizona, USA).

http://www.cfa.harvard.edu/srlab/rxlabHEB.html http://www.cfa.harvard.edu/srlab/secure/rxlabTerahertzScience.html First fully-resolved ground-based detection of a terahertz spectral line from an astronomical source (CO 9-8 in Orion BN/KL) was obtained with the HEB receiver (January 2000). The first ground- based heterodyne detection in the terahertz band.

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Heterodyne astronomy projects with wide-bandwidth HEB mixers

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Millimetron

12-m diameter space telescope Heterodyne receivers in 1- 6 THz range

SOFIA

2.7-m diameter stratospheric telescope Heterodyne receivers in the ranges 1.6-1.9 THz, 2.4-2.7 THz, 4.7 THz

The GBW of the HEB receiver installed at the HERSHEL telescope does not exceed 4 GHz. Future heterodyne missions will require a GBW of 8 GHz. PDHEBs already have a GBW of 6.5 GHz and potentially can have a GBW of up to 12 GHz.

HERSCHEL

3.5-m diameter space telescope Bands 6 and 7 of the HIFI: 1.41 THz – 1.91 THz

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Security systems

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THz imagine of hidden in the shoes ceramic knife and explosive. Thermovisors of THz range able to distinguish

  • bjects on distance about 20-30m hidden under

clothes: plastic and metallic weapon, explosion materials, drugs, etc. Fast identification of chemical components is possible in THz range even in close package (for example box on mail post).

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SCONTEL

Full-support service (installation, operation training, technical support) Easy to integrate with LabView and other standard environment Optimization of receiver system characteristics to the customer needs One, two, or multi- channel systems are available Local or remote control

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Our customers

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Europe Asia North America

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Thank you for your attention

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