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Terahertz emission from a weakly-coupled GaAs/AlGaAs superlattice biased into three different modes of current self-oscillations

AIP advances, 2019-10, Vol.9 (10), p.105220-105220-8

2019

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Statistical features of the response of a superconducting hot-electron bolometer to extremely weak terahertz pulses of picosecond and nanosecond duration

Applied physics letters, 2024-09, Vol.125 (12)

2024

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Ab initio computation of low-temperature phase diagrams exhibiting miscibility gaps

Physical chemistry chemical physics : PCCP, 2006-01, Vol.8 (15), p.1778-1784

2006

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Pulsed terahertz radiation from a double-barrier resonant tunneling diode biased into self-oscillation regime

Journal of applied physics, 2020-12, Vol.128 (22)

2020

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Direct detection of the idler THz radiation generated by spontaneous parametric down-conversion

Optics letters, 2019-03, Vol.44 (5), p.1198-1201

2019

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Ab initio prediction of the low-temperature phase diagrams in the systems CsX–LiX (X = F, Cl, Br, I)

Solid state sciences, 2008-06, Vol.10 (6), p.804-813

2008

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Electric-field domain boundary instability in weakly coupled semiconductor superlattices

Journal of applied physics, 2016-05, Vol.119 (20)

2016

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Characterization of the THz quantum cascade laser using fast superconducting hot electron bolometer

EPJ Web of Conferences, 2018, Vol.195, p.4004

2018

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Ab initio prediction of the low-temperature phase diagrams in the systems KBr-NaBr, KX-RbX, and LiX-RbX (X=Cl,Br)

The Journal of chemical physics, 2007-03, Vol.126 (12), p.124508-124508

2007

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Ab initio prediction of the low-temperature phase diagrams in the systems MBr–MCl (M = Li, Na, K)

Solid state sciences, 2008-04, Vol.10 (4), p.455-460

2008

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The miscibility gap in cadmium, mercury and zinc telluride systems: Theoretical description

Calphad, 2006-06, Vol.30 (2), p.191-195

2006

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A weakly coupled semiconductor superlattice as a potential for a radio frequency modulated terahertz light emitter

Applied physics letters, 2012-03, Vol.100 (13), p.131104-131104-4

2012

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Ab Initio Computation of the Low-Temperature Phase Diagrams of the Alkali Metal Iodide−Bromides: MBrxI1-x (0 ≤ x ≤ 1), Where M = Li, Na, K, Rb, or Cs

The journal of physical chemistry. B, 2007-04, Vol.111 (15), p.3943-3952

2007

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Ab initio computation of the low-temperature phase diagrams of the alkali metal iodide-bromides: MBr(x)I1-x (0 </= x </= 1), Where M = Li, Na, K, Rb, or Cs

The journal of physical chemistry. B, 2007-04, Vol.111 (15), p.3943-3952

2007

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Ab Initio Computation of the Low-Temperature Phase Diagrams of the Alkali Metal Iodide−Bromides: MBr x I 1 - x (0 ≤ x ≤ 1), Where M = Li, Na, K, Rb, or Cs

The journal of physical chemistry. B, 2007-04, Vol.111 (15), p.3943-3952

2007

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Ab initio prediction of the low-temperature phase diagramsin the systems KBr-NaBr, KX-RbX, and LiX-RbX ( X = Cl , Br )

The Journal of chemical physics, 2007-03, Vol.126 (12), p.124508-124508-15

2007

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Ab initio prediction of the low-temperature phase diagrams in the systems MBr-MC1 (M = Li, Na, K): Frontiers in Solid State Chemistry

Solid state sciences, 2008, Vol.10 (4), p.455-460

2008

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Semiconducting superlattice as a solid-state terahertz local oscillator for NbN hot-electron bolometer mixers

Technical physics, 2012-07, Vol.57 (7), p.971-974

2012

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Infrared and terahertz detectors on basis of superconducting nanostructures

2010 20th International Crimean Conference "Microwave & Telecommunication Technology", 2010, p.823-824

2010

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Mutual synchronization of two coupled self-oscillators based on GaAs/AlGaAs superlattices

Technical physics, 2011-06, Vol.56 (6), p.826-830

2011

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Ab initio prediction of low-temperature parts of the phase diagram for the M Sb- M ′ Sb ( M , M ′ = Al , Ga, or In) and AlSb-GaSb-InSb systems

Physical review. B, Condensed matter and materials physics, 2010-10, Vol.82 (14), Article 144102

2010

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Low-noise wide-band hot-electron bolometer mixer based on an NbN film

Radiophysics and quantum electronics, 2009-08, Vol.52 (8), p.576-582

2009

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The miscibility gap in cadmium, mercury and zinc telluride systems : Theoretical description

Calphad, 2006, Vol.30 (2), p.191-195

2006

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Ab Initio Computation of the Low-Temperature Phase Diagrams of the Alkali Metal Iodide−Bromides: MBr x I1 - x (0 ≤ x ≤ 1), Where M = Li, Na, K, Rb, or Cs

The journal of physical chemistry. B, 2007-04, Vol.111 (15), p.3943-3952

2007

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tability of Tetragonal ZrO sub 2 toward External Influences

Inorganic materials, 2002-10, Vol.38 (10), p.1012-1014

2002

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Terahertz emission from a weakly-coupled GaAs/AlGaAs superlattice biased into three different modes of current self-oscillations

Statistical features of the response of a superconducting hot-electron bolometer to extremely weak terahertz pulses of picosecond and nanosecond duration

Ab initio computation of low-temperature phase diagrams exhibiting miscibility gaps

Pulsed terahertz radiation from a double-barrier resonant tunneling diode biased into self-oscillation regime

Direct detection of the idler THz radiation generated by spontaneous parametric down-conversion

Ab initio prediction of the low-temperature phase diagrams in the systems CsX–LiX (X = F, Cl, Br, I)

Electric-field domain boundary instability in weakly coupled semiconductor superlattices

Characterization of the THz quantum cascade laser using fast superconducting hot electron bolometer

Ab initio prediction of the low-temperature phase diagrams in the systems KBr-NaBr, KX-RbX, and LiX-RbX (X=Cl,Br)

Ab initio prediction of the low-temperature phase diagrams in the systems MBr–MCl (M = Li, Na, K)

The miscibility gap in cadmium, mercury and zinc telluride systems: Theoretical description

A weakly coupled semiconductor superlattice as a potential for a radio frequency modulated terahertz light emitter

Ab Initio Computation of the Low-Temperature Phase Diagrams of the Alkali Metal Iodide−Bromides: MBrxI1-x (0 ≤ x ≤ 1), Where M = Li, Na, K, Rb, or Cs

Ab initio computation of the low-temperature phase diagrams of the alkali metal iodide-bromides: MBr(x)I1-x (0 </= x </= 1), Where M = Li, Na, K, Rb, or Cs

Ab Initio Computation of the Low-Temperature Phase Diagrams of the Alkali Metal Iodide−Bromides: MBr x I 1 - x (0 ≤ x ≤ 1), Where M = Li, Na, K, Rb, or Cs

Ab initio prediction of the low-temperature phase diagramsin the systems KBr-NaBr, KX-RbX, and LiX-RbX ( X = Cl , Br )

Ab initio prediction of the low-temperature phase diagrams in the systems MBr-MC1 (M = Li, Na, K): Frontiers in Solid State Chemistry

Semiconducting superlattice as a solid-state terahertz local oscillator for NbN hot-electron bolometer mixers

Infrared and terahertz detectors on basis of superconducting nanostructures

Mutual synchronization of two coupled self-oscillators based on GaAs/AlGaAs superlattices

Ab initio prediction of low-temperature parts of the phase diagram for the M Sb- M ′ Sb ( M , M ′ = Al , Ga, or In) and AlSb-GaSb-InSb systems

Low-noise wide-band hot-electron bolometer mixer based on an NbN film

The miscibility gap in cadmium, mercury and zinc telluride systems : Theoretical description

Ab Initio Computation of the Low-Temperature Phase Diagrams of the Alkali Metal Iodide−Bromides: MBr x I1 - x (0 ≤ x ≤ 1), Where M = Li, Na, K, Rb, or Cs

tability of Tetragonal ZrO sub 2 toward External Influences

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