Ilya Antonov’s research while affiliated with Royal Holloway University of London and other places

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Publications (13)


FIG 1. Overview of the Bloch Transistor (Top) Cartoon of four BT controls: the gate/bias voltage and the frequency/amplitude of the microwave; (Left) Focused Ion Beam image of the BT. Two identical Al JJs separated by a small island embedded in the circuit with the super-inductors L1+ L2 ∼1 nH, resistors R= 6.3 kΩ and quasiparticle traps QP. The MW is delivered to JJs by the gate electrode with capacitance Cg; (Right) Electric circuit of the BT.
FIG 2. The measured I − V curve without and with the MW: (Left) I − V curve has current blockade below critical voltage V * C = 2.5 µV. The apparent critical current is I * A ∼ 14 nA.(Right) Current quantization under the MW of 6.91 GHz. The horizontal lines indicate the current corresponding to I = 2ef n, n = 0, ±1, ±2. One can tune the BT to different n by varying V b .
FIG 3. Gate control of the BT. (Left) The intensity graph of the differential resistance dV /dI vs normalized induced charge CgVg/Q and Iac/2ef . The peaks of dV /dI are at the centres of the quantized plateaus I dc = 2ef n. They are periodically modulated with the charge e = VgCg induced at the island between the JJs.(Right) Cross section of the intensity graph taken at fixed Iac/2ef corresponding to different n. The curves are shifted by 1.2 kΩ for clarity. There is a phase shift of the gate modulation between different n.
FIG 4. MW control of the BT: (Left) Intensity plot of the differential resistance dV /dI at different bias and Iac. The bright peaks are located at the quantized current plateaus, I dc = 2ef n; (Right) Cross section of dV /dI at I dc = 2ef (green dots). The solid blue line is a fit of the experimental data with the square of Bessel function J 2 n (Iac/2ef ) with n= 1.
Bloch Transistor for Cryogenic Quantum Electronics
  • Preprint
  • File available

January 2025

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14 Reads

Vladimir Antonov

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Ilya Antonov

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Rais Shaikhaidarov

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[...]

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Oleg Astafiev

We report on the development of a Bloch transistor (BT) for the emerging platform of cryogenic quantum electronics. The BT is a fully quantum non-dissipative device facilitating precise delivery of the quantised current to the circuit, I=2efn (where n is an integer, e is the charge of an electron, and f is the microwave frequency). It does not have an analogue in classical electronics, but it is required for quantum ones. The amplitude of the quantized current is adjustable through four controls: the gate or bias voltage and the frequency or amplitude of the microwave. The device features Josephson junctions operating in the regime of Bloch oscillations, an isolating electromagnetic circuit and microwave feeding leads. BT operates at a bias of ∼ 5 μV, and can deliver the quantized currents of up to 10 nA.

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Design and electric circuit of the sample and formation of the Bloch bands in JJ
a The Bloch bands of the JJ in units of the Josephson energy EJ versus normalized flux Φ/Φ0 and charge q/2e (EJ/EC = 4.4). The lowest band shows 2e periodic oscillations in the charge space, with the amplitude corresponding to the phase-slip energy ES. The three lowest Bloch bands are marked by different colours. For current quantization the Bloch oscillations in the lowest band are synchronized with the external MWs; (b) He FIB image of the device and the equivalent electric circuit. A small JJ is embedded into a high impedance environment formed by TiN inductances L1 = 1.15 µH and L2 = 0.34 µH and normal Pd resistors R = 6.3 kΩ.
Stationary I-V curves of the JJ
aI − V curve in wide voltage range has supercurrent-like shape with an apparent supercurrent IC* = 24 nA. bI − V curve in a narrower voltage range reveals a current blockade region with the apparent critical voltage VC* = 2.33 µV. Inset: a differential resistance dV/dI. The center peak is due to the current blockade. The two side maxima indicated by red arrows define the apparent current IC*.
The current quantization at the I − V curves under MW radiation
(a, b) f = 6.495 GHz, and (c, d) f = 10.215 GHz. The dashed lines correspond to the currents Idc = 2 efm, m = 1,2,3,... The amplitude of MW is given as Iac. The red dashed curve in (d) is the theoretical fit made with Eq. (4) (the thermal noise is taken as δIT = 1 nA). The resistance at m = 1 plateau of this curve is 2.2 kΩ.
An intensity plot of dV/dI in coordinates of the normalised dc and ac current taken at 6.495 GHz
The extremes of the dV /dI correspond to the Idc = 2 efm plateaus. They oscillate with MW amplitude Iac.
of measured devices
Experimental VC* versus the JJ area. Three groups of JJs (magenta, green, and brown circles) have different insulating layers with different specific resistances. The solid lines are fitted with Eq. (6). The dashed red line separates devices with and without explicit MW response. The devices demonstrating current quantization are inside the red dashed oval indicated as “Steps”. The characteristic resistance r expressed in units 10⁷ Ω × nm². The resistances for the reference area of 100 × 100 nm² are R0 = 0.9 kΩ (magenta), 1.8 kΩ (green) and 14 kΩ (brown).
Quantized current steps due to the synchronization of microwaves with Bloch oscillations in small Josephson junctions

October 2024

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37 Reads

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3 Citations

Synchronization of Bloch oscillations in small Josephson junctions (JJs) under microwave radiation, which leads to current quantization, has been proposed as an effect that is dual to the appearance of Shapiro steps. This current quantization was recently demonstrated in superconducting nanowires in a compact high-impedance environment. Direct observation of current quantization in JJs would confirm the synchronization of Bloch oscillations with microwaves and help with the realisation of the metrological current standard. Here, we place JJs in a high-impedance environment and demonstrate dual Shapiro steps for frequencies up to 24 GHz (I = 7.7 nA). Current quantization exists, however, only in a narrow range of JJ parameters. We carry out a systematic study to explain this by invoking the model of a JJ in the presence of thermal noise. The findings are important for fundamental physics and application in quantum metrology.


Feasibility of the Josephson voltage and current standards on a single chip

October 2024

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6 Reads

The quantum Josephson voltage standard is well established across the metrology community for many years. It relies on the synchronisation of the flux tunneling in the S/I/S Josepson junctions (JJ) with the microwave radiation (MW). The phenomenon is called the Shapiro steps. Together with the Quantum Hall resistance standard, the voltage standard forms the foundation of electrostatic metrology. The current is then defined as the ratio of the voltage and resistance. Realisation of the quantum current standard, would close the electrostatic metrological triangle of voltage-resistance-current. The current quantisation, the inverse Shapiro steps, was recently shown using the superconducting nanowires and small JJ. The effect is a synchronization of the MW with the Cooper pair tunnelling. This paves the way to combine the JJ voltage and current standards on the same chip and demonstrate feasibility of the multi-standard operation. We show the voltage and current quantization on the same chip up to frequency of 10 GHz, corresponding to the amplitudes 0.021 mV and 3.23 nA respectively. The accuracy of the voltage and current quantisation, however, is relatively low, 35 ppk and 100 ppk respectively. We discuss measures to optimise the JJs, circuit and environment to boost the amplitude and accuracy of the standards.


The Bloch bands of the JJ in two regimes: EJ>EC (top) and EJ<EC (bottom). The regime at the top corresponds to the direct Shapiro steps, V=(h/2e)fm, while at the bottom corresponds to the inverse Shapiro steps, I=2efm. The red numbers on the right correspond to the energy levels/bands of the system. The blue dashed lines are charge states with EJ=0.
Focused ion beam photograph of the chip for SS (top) and ISS (bottom). The color leads are V+/− and I+/− for the four-point measurement. The JJs of the SS and ISS have different sizes (insets at the left): 700 × 100 and 80 × 40 nm². The ISS circuit (inset at the right) has Pd resistors R= 6.3 k Ω and TiN superinductances L1+L2 = 1.49  μ H to screen the JJ from the environmental noise. The MW is supplied by the lead through the capacitor Ck≈ 0.1 fF. The main picture and insets have their own scale bars. The measurement circuits for the SS (left) are ISS (right) are shown at the bottom.
I−V curves of the SS and ISS. (a) The SS is in the under-damped regime with IC = 50 nA. (b) The ISS has the current blockade below VC* = 0.65  μ V and apparent critical current IC* = 21 nA. Wide range I−V curve is shown in the inset.
Direct Shapiro steps at 6.695 and 10.095 GHz. The curves are taken at different MW amplitude so that the voltage steps of different orders m are present. The horizontal lines are the guide lines for the expected position of the voltage steps Vm=Φ0fm. The most right curves are taken without the MW.
Inverse Shapiro steps at 6.695 and 10.095 GHz. The curves are taken at different MW amplitudes. The horizontal lines are the guide lines for the expected position of the current steps Im=2efm.
Feasibility of the Josephson voltage and current standards on a single chip

September 2024

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22 Reads

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1 Citation

The quantum Josephson voltage standard is well established across the metrology community for many years. It relies on the synchronization of the flux tunneling in the S/I/S Josephson junctions (JJ) with the microwave radiation (MW) of frequency f such that V=Φ0fm, where m = 0, 1, 2, …. The phenomenon is called the Shapiro steps. Together with the quantum Hall resistance standard, the voltage standard forms the foundation of electrostatic metrology. The current is then defined as the ratio of the voltage and resistance. Realization of the quantum current standard would close the electrostatic metrological triangle of voltage–resistance–current. The current quantization I=2efm, the inverse Shapiro steps, was recently shown using the superconducting nanowires and small JJ. The effect is a synchronization of the MW with the Cooper pair tunneling. This paves the way to combine the JJ voltage and current standards on the same chip and demonstrate feasibility of the multi-standard operation. We show the voltage and current quantization on the same chip up to frequency of 10 GHz, corresponding to the amplitudes ∼ 20.67 μV and ∼ 3.2 nA, respectively. The accuracy of the voltage and current quantization, however, is relatively low, 35 and 100 ppk, respectively. We discuss measures to optimize the JJs, circuit, and environment to boost the amplitude and accuracy of the standards.


Fig. 1 (a) FIB image of the device. A small Josephson junction (JJ) is embedded into a high impedance environment. Thin film TiN inductances L 1 and L 2 are made in the form of meanders. (b) The equivalent circuit of the device with the current and voltage measurement probes.
Fig. 2 (a) I−V curve of the JJ. It shows supercurrent-like characteristics with an apparent supercurrent I * C = 24 nA. (b) An I−V curve in a narrower voltage range reveals a current blockade region with the apparent critical voltage V * C = 2.33 µV. Inset: a differential resistance dV /dI. The center peak is due to the current blockade. The two side maxima indicated by red arrows define the apparent current I * C .
Fig. 3 The current quantisation at the I−V curve under the MW radiation at two frequencies, 6.495 GHz and 10.215 GHz. The dashed lines correspond to the currents I dc = 2ef n, n = 1, 2, 3, ... The amplitude of MW is given as Iac. The right bottom curve has the theoretical fit with the thermal noise, δI T = 1 nA [3].
The quantised current steps due to the synchronisation of microwaves with the Bloch oscillations in small Josephson junctions

February 2024

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150 Reads

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1 Citation

Synchronisation of the Bloch oscillations in a small Josephson junction (JJ) under the microwave radiation leading to the current quantisation at a current equal to Cooper-pair charge × frequency × integer has been proposed as the effect dual to the Shapiro steps. Experimental confirmation of this phenomenon was delayed for a long time until last year's breakthrough when the current quantisation was demonstrated in the superconducting nanowires. The compact high impedance environment of the nanowires played a key role in the experiment. Direct observation of the current quantization in the JJs would answer the fundamental question of the Bloch oscillations and open a more feasible road for the metrological application. Here we place JJs in the high impedance environment and demonstrate dual Shapiro steps for frequencies up to 24 GHz (I=7.7 nA). The current quantisation exists, however, only in a narrow range of JJ parameters, the critical current and capacitance. We carry out a systematic study to explain this by invoking the model of the JJ in presence of the thermal noise. The findings are important for the fundamental physics and application to quantum metrology.


Geometry of CQPS device: (a) Schematic of the λ/2 resonator capacitively coupled to the transmission line and CQPS qubit with coloured TiN (dark) and Au (yellow); (b) The energy diagram of the qubit at different magnetic flux. The degeneracy is lifted at half flux quantum because of the phase slip energy. (c) The micrograph of the CQPS qubits capacitively coupled via fingers ( Cq−r ) to the TiN resonator. The fingers have a 3 µm overlap with the qubit loop. The CQPS qubit is grounded through the line running to the bottom ground plane; (d) a focused-ion beam micrograph of the constriction in the qubit loop, across which the phase slip occurs (shown in green).
Characterisation of qubits: (a) Two-tone spectroscopy in a narrow range of the external magnetic field. The phase of transmission arg(t) through the resonator at f2=3.14 GHz is monitored while a probe frequency ω p and external field B ext are independently swept. Strong phase variations occur on qubit resonance δω=ωp−ωq≡0 , which maps out the multiple qubit spectra. The horizontal lines are the resonator modes; (b) line fits to the experimentally measured energy spectrum from the analytical solution of the Hamiltonian (1).
Avoided crossings of qubit 12 on the m = 3 resonator mode with cross sections in frequency (blue arrow) and magnetic flux (red arrow): (a) measured transmission spectrum around the f3=5.12GHz resonance. The dashed orange line is the simulated qubit-resonator anticrossing from just the Jaynes–Cummings Hamiltonian; (b) simulated transmission spectrum with using the full master equation formalism of (3); (c), (d) cross section comparing measured and simulated transmission spectra.
Capacitive Coupling of Coherent Quantum Phase Slip Qubits to a Resonator

November 2023

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103 Reads

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4 Citations

xD;We demonstrate capacitive coupling of coherent quantum phase slip (CQPS) flux qubits to a resonator patterned on a highly disordered TiN film. We are able to detect and characterise CQPS flux qubits with linewidths down to ∆ω = 12 ± 1 MHz on several resonator modes, and show that, unlike inductive coupling, here the coupling strength does not depend on the qubit’s energy. Since the qubit is galvanically decoupled from the resonator, our approach provides flexibility in material, design and fabrication choices for CQPS-based devices. Our results are two-fold: We report CQPS in TiN and demonstrate, to our knowledge for the first time, capacitive coupling of a CQPS flux qubit.


Quantized current steps due to the a.c. coherent quantum phase-slip effect

August 2022

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4 Reads

The AC Josephson effect predicted in 1962 and observed experimentally in 1963 as quantised voltage steps (the Shapiro steps) from photon assisted tunnelling of Cooper pairs is among the most fundamental phenomena of quantum mechanics and is vital for metrological quantum voltage standards. The physically dual effect, the AC coherent quantum phase slip (CQPS), photon assisted tunnelling of magnetic fluxes through a superconducting nanowire, is envisaged to reveal itself as quantised current steps. The basic physical significance of the AC CQPS is also complemented by practical importance in future current standards; a missing element for closing the Quantum Metrology Triangle. In 2012, the CQPS was demonstrated as superposition of magnetic flux quanta in superconducting nanowires. However the direct sharp current steps in superconductors; the only unavailable basic effect of superconductivity to date, was unattainable due to lack of appropriate materials and challenges in circuit engineering. Here we report the direct observation of the dual Shapiro steps in a superconducting nanowire. The sharp steps are clear up to 26 GHz frequency with current values 8.3 nA and limited by the present setup bandwidth. The current steps have been theoretically predicted in small Josephson junctions (JJs) 30 years ago. However, broadening unavoidable in JJs prevents their direct experimental observation. We solve this problem by placing a thin NbN nanowire in an inductive environment.


Principles of the microwave-induced transport in dual circuits
a, JJ transport. b, CQPS transport. In a and bI–V characteristics without microwaves (blue curve) and with microwaves (red curve) are shown schematically. Insets show energy diagrams for the microwave-assisted transport between reservoirs separated by tunnel barriers (an insulator and a nanowire) biased by Q0Vd.c. in JJ and Φ0Id.c. in CQPS. c,d, Effective electrical circuits for the transport measurements for JJ (c) and for CQPS (d). Tunnelling of Cooper pairs in the JJ is replaced by tunnelling of vortices through a CQPS nanowire. A capacitance C and a resistor R parallel to the JJ are replaced by an inductance L and an admittance Y in series to the CQPS junction.
Device and transport
a, The device layout. The superconducting 100 nm wide wire with a constriction of approximately 20 × 50 nm² geometrical size (zoomed out) is embedded into the circuit with four compact series meandering inductances made of the NbN films with kinetic inductances L′≈1.7\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${L}^{{\prime} }\approx 1.7$$\end{document} μH, L″ ≈ 0.5 μH. Inductances are connected to series Pd resistances (R′=11.5\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${R}^{{\prime} }=11.5$$\end{document} kΩ) and Pd contact pads. The circuit is connected to current, I⁺/I⁻, and voltage, V⁺/V⁻, leads. The microwaves are delivered through an on-chip coplanar line, coupled to the circuit via capacitances Cκ. An inset shows a CQPS junction: a small nanowire constriction. b, I–V characteristics in a wide voltage range demonstrate high re-trapping (Ir) and excess (Iexc) currents. c, An I–V characteristic of the central part. A clear blockade is found with the re-trapping voltage Vc*=2.3\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${V}_{{\rm{c}}}^{* }=2.3$$\end{document} μV.
Inverse Shapiro steps in four-probe I–V measurements
Horizontal lines show the expected position of plateaus at nQ0f. a, fI = 14.924 GHz. b, fI = 14.924 GHz with an a.c. current 2.6 times higher than in a. c, fII = 19.845 GHz. d, fIII = 25.963 GHz.
Oscillations of dV/dI peaks
a, dV/dI characteristics in a two-dimensional plot experimentally measured at 14.924 GHz. b, Simulations, accounting for the heating effect from Pd resistors. c, Cross-sections at positions n of the quantized steps. Solid lines are simulations. Each plot is offset by n × 1.5 kΩ in the y axis. d, dV/dI for n = ±1 peak position difference calculated as Ĩ1=(I1max−I−1max)/2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${\widetilde{I}}_{1}=({I}_{1}^{\max }-{I}_{-1}^{\max })/2$$\end{document} from various samples with different Vc*\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${V}_{c}^{* }$$\end{document} (specified in the plot legend). The typical accuracy for each point is 2 × 10⁻³ defined by fitting the peak position. An inset shows q/Q0 − 1 with q=Ĩ1/f\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$q={\widetilde{I}}_{1}/f$$\end{document}. The red dotted line is I = Q0f.
Quantized current steps due to the a.c. coherent quantum phase-slip effect

August 2022

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254 Reads

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71 Citations

Nature

The a.c. Josephson effect predicted in 19621 and observed experimentally in 19632 as quantized ‘voltage steps’ (the Shapiro steps) from photon-assisted tunnelling of Cooper pairs is among the most fundamental phenomena of quantum mechanics and is vital for metrological quantum voltage standards. The physically dual effect, the a.c. coherent quantum phase slip (CQPS), photon-assisted tunnelling of magnetic fluxes through a superconducting nanowire, is envisaged to reveal itself as quantized ‘current steps’3,4. The basic physical significance of the a.c. CQPS is also complemented by practical importance in future current standards, a missing element for closing the quantum metrology triangle5,6. In 2012, the CQPS was demonstrated as superposition of magnetic flux quanta in superconducting nanowires 7. However, the direct flat current steps in superconductors, the only unavailable basic effect of superconductivity to date, was unattainable due to lack of appropriate materials and challenges in circuit engineering. Here we report the direct observation of the dual Shapiro steps in a superconducting nanowire. The sharp steps are clear up to 26 GHz frequency with current values 8.3 nA and limited by the present set-up bandwidth. The current steps were theoretically predicted in small Josephson junctions 30 years ago5. However, unavoidable broadening in Josephson junctions prevents their direct experimental observation8,9. We solve this problem by placing a thin NbN nanowire in an inductive environment. Direct observation of the physical dual a.c. Josephson effect, a series of quantized current steps in a superconducting nanowire, is reported and may offer a way to establish new metrological standards for currents.


Cryogenic spectral imaging system. An array of terahertz detectors is coupled to the cold finger of the compact cryocooler (8). Radiation of THz sources (1) transmitted/reflected by the LiNbO3\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$_{3}$$\end{document} crystal (2) is collected by the Teflon lens (3) at the entrance to the vacuum chamber (4) (shown in disassembled form) and passed by the 3 mm diameter plexiglass waveguide (6) to the Si lens integrated to a standard 20 pin package (top of (7)). The array of detectors is glued back to back to the Si lens. The attenuation of the optical system is 35dB. The electronics box (5) enables access to any of the 14 detectors in the array. The vacuum chamber is evacuated down to 10-5\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$10^{-5}$$\end{document} mTorr enabling for the cold finger to cool down the array to 70 K in 40 minutes from the room temperature. The system demonstrated continuous stable operation for more than a month
a) The source-drain current (black) and the photocurrent (red) vs gate voltage. The photocurrent has a maximum close to the pinch-off of the channel where the source drain current tends to zero (Vsd\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$V_{sd}$$\end{document}=15 μ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mu$$\end{document}V is applied between the source and drain); insert: optical image of two detectors of the array, b) photocurrent of the typical detector normalised to the source power (the maximum of the emitted power, ∼\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\sim$$\end{document} 1 mW at ν\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\nu$$\end{document}=189 GHz, is taken as 1); insert: SEM image of central part of the detector. Two negatively biased metal gates define conductive channel in 2DEG of GaAs/AlGaAs heterostructure mesa stripe. The 2DEG is below the surface of the heterostructrure, at the depth of 90 nm. The mesa stripe itself is a focal point of the bow tie antenna. The photocurrent is taken in the transmitted mode. The experimental data are taken with the detector cooled down to T=70 K
Reflection spectrum of LiNbO3\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$_{3}$$\end{document}. Detector is kept at T∼\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\sim$$\end{document} 70 K. There is a strong absorption at ν\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\nu$$\end{document}=174 GHz. The absorption dip is fitted with the Lorenzian (red solid line). The FWHM of the resonance absorption is 16 GHz
(a) Maximum photocurrent at different temperatures. The amplitude is suppressed by two orders of magnitude at higher temperatures. (b) Temperature dependance of the photo-induced δVsd\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\delta {V}_{sd}$$\end{document}. It has a sharp drop between 0.5 K and 2 K. Then the decrease of δVsd\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\delta {V}_{sd}$$\end{document} is flattened out. Solid line is an approximation with the exponential decay function
The source-drain current (black) and the absolute value of photocurrent (red) under illumination of two close frequencies, 180 GHz (solid curves) and 186 GHz (dotted lines). The source-drain current close to pinch-off changes sign from positive to negative when illuminated by radiation of 180 GHz. Under the radiation of 186 GHz, there is a positive contribution to the source-drain current. Power supplied by the source at two frequencies is different by the factor of 25: it is 1 mW at 180 GHZ and 40 μ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mu$$\end{document}W at 186 GHz
Compact Remote Spectral Terahertz Imager

July 2022

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115 Reads

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1 Citation

Journal of Infrared, Millimeter and Terahertz Waves

We report on development of an array of spectral sensitive detectors cooled down to 70 K by the compact cryocooler. The spectral sensitive operation of the detectors, explored between 0.16 THz and 0.22 THz, is due to the resonant excitation of the plasma waves in the two-dimensional electron gas of GaAs/AlGaAs heterostructure. A typical responsivity of the detectors is 0.01 A/W at 70 K while it increases by two orders of magnitude when the detector array is cooled down to 0.5 K. The photo-response has surprisingly a narrow peak of spectral sensitivity, \sim ∼ 2–5%, which are highly likely due to the dimensional resonances of the plasma waves. As a demonstration of the spectral sensitive operation we detect a spectral feature of LiNbO 3_{3} 3 crystal at 0.174 THz.


Detection of black body radiation using a compact terahertz imager

December 2020

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159 Reads

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2 Citations

We detect terahertz radiation emitted by a black-body object at room temperature. The probe consists of semiconductor detectors coupled to the cold finger of a compact cryo-cooler. The detectors are narrow conductive channels in two-dimensional electron gas which is sensitive to variations of photon flux through the mechanism of excitation and rectification of plasma waves. The excitation has a resonance nature, with an unexpectedly narrow FWHM, below 10%. The key element of the concept is a compact cryo-platform, which enables to use of highly sensitive cryo-detectors, while keeping the system compact, ∼ 34 cm side, and mobile. We discriminate the temperature variation of the black-body object as small as 1.0 K at a distance of 1 m. There is room for further optimisation of the detectors and optical system to boost the temperature resolution down to 0.5 K and the operation distance to 5 m, which are needed for practical applications.


Citations (8)


... The further study of the CQPS effect led to the demonstration of the current quantization I = 2ef n (n = 0, 1, 2, · · · is integer, e is electron charge) when a microwave of frequency f is applied to small Josephson junction adequately isolated from the environment [8][9][10]. This effect is dual to the conventional Shapiro voltage steps and is consequently called the Inverse Shapiro Steps (ISS). ...

Reference:

Bloch Transistor for Cryogenic Quantum Electronics
Quantized current steps due to the synchronization of microwaves with Bloch oscillations in small Josephson junctions

... The BT can be used as the absolute quantum current standard in metrology. We recently reported on developing the metrological chip that contains the voltage and current standards [17]. The BT can be naturally accommodated on this chip. ...

Feasibility of the Josephson voltage and current standards on a single chip

... During the review of our manuscript we became aware of a preprint by Antonov et al. 42 , demonstrating dual Shapiro steps in Al/AlO x / Al Josephson junctions. However, we note that our result seem to contradict the observation of Antonov et al. that dual Shapiro steps are only observed in samples with a Coulomb blockade smaller than 5 μV. ...

The quantised current steps due to the synchronisation of microwaves with the Bloch oscillations in small Josephson junctions

... To verify the self-consistency and uniqueness of the reconstructed GS we use the Hilbert-Schmitt distance to quantify errors arising from spurious harmonics added to the correct model Hamiltonian. Finally, drawing from recent work [21] we propose longitudinal coupling using the Aharonov-Casher effect [22] recently exploited in quantum phase slip devices [23,24] and flux qubit systems [25][26][27][28] where frequencies can be significantly tuned by use of Josephson junctions with reduced tunnelling rate [29,30]. ...

Capacitive Coupling of Coherent Quantum Phase Slip Qubits to a Resonator

... However, achieving currents above 100 pA using GaAs and Si-based tunablebarrier SECS accurate to within a relative uncertainty better than 10 −7 remains a very challenging goal because of increasing error rates at high frequencies (~1 GHz) 15,16 . Very recently, as a consequence of the phase-charge quantum mechanical duality in Josephson junctions (JJ), dual Shapiro steps have been evidenced in superconducting nanowires and small JJ placed in high impedance environments under microwave radiation [17][18][19] . Here, the enhanced phase variance allows photon-assisted tunneling of fluxons ϕ 0 = h/2e (h is the Planck constant) and a synchronized transfer of Cooper pairs. ...

Quantized current steps due to the a.c. coherent quantum phase-slip effect

Nature

... THz imaging is also applied in clinical applications such as endoscopy (examining the inside of a hollow organ) and otoscopy (examining the inside of ears) [Son et al. 2019]. Whereas its main limitation is the high cost of the THz source and detector [Afsah-Hejri et al. 2020], and the detectable blackbody radiation emitted by many materials at room temperature as noise [Hegedüs et al. 2020]. Furthermore, at the end of the electromagnetic radiation spectrum, there are microwave and radio wave imaging techniques with long wavelengths between 100,000 km and 1 mm (or frequency between 3 Hz and 300 GHz). ...

Detection of black body radiation using a compact terahertz imager

... In particular, in the field of quantum computing, the most efficient control of qubit states has been demonstrated for solid-state qubits. In the context of this work, we would like to highlight promising implementations of quantum bits (qubits) which are based on the general features of the energy spectrum of the doublewell potential [7][8][9][10][11][12][13][14][15][16]. In various flux qubits and double quantum dots, tunneling splitting of the ground state allows the formation of a qubit basis. ...

Superconducting ‘twin’ qubit

... Lately, there has been significant interest in attaining robust light-matter interaction within a cavity-free setup, specifically through waveguides, for applications in quantum information processing [1][2][3][4][5]. Waveguide quantum electrodynamics (QED) involves a scenario where a series of atoms are interconnected to a shared optical channel characterized by a continuum of electromagnetic modes spanning a broad bandwidth [6,7]. ...

Mixing of coherent waves in a single three-level artificial atom
  • Citing Article
  • October 2018

Physical Review A