Andrii Lazariev’s research while affiliated with Max Planck Institute for Biophysical Chemistry and other places

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Publications (11)


Measuring Environmental Quantum Noise Exhibiting a Nonmonotonic Spectral Shape
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January 2019

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46 Reads

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11 Citations

Physical Review Applied

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A. Lazariev

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I. Avrahami

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N. Bar-Gill

Understanding the physical origin of noise affecting quantum systems is important for nearly every quantum application. Quantum-noise spectroscopy has been used in various quantum systems, such as superconducting qubits, nitrogen-vacancy centers, and trapped ions. Traditional spectroscopy methods are usually efficient in measuring noise spectra with mostly monotonically decaying contributions. However, there are important scenarios in which the noise spectrum is broadband and nonmonotonous, thus posing a challenge to existing noise-spectroscopy schemes. Here we compare several methods for noise spectroscopy: spectral decomposition based on the Carr-Purcell-Meiboom-Gill sequence, the recently presented dynamic sensitivity control (DYSCO) sequence, and a modified DYSCO sequence with a Gaussian envelope (gDYSCO). The performance of the sequences is quantified by analytic and numeric determination of the frequency resolution, bandwidth, and sensitivity, revealing a supremacy of gDYSCO to reconstruct nontrivial features. Using an ensemble of nitrogen-vacancy centers in diamond coupled to a high-density C13-nuclear-spin environment, we experimentally confirm our findings. The combination of the schemes presented offers potential to record high-quality noise spectra as a prerequisite to generate quantum systems unlimited by their spin-bath environment.


Fig. 1 Superadiabtic geometric quantum gate concept. a Anticipated "orange slice" Bloch sphere trajectory (blue) enclosing the solid angle ~ Ω ¼ 2γ (red). b Two-level system and microwave field parameter (detuning Δ(t), Rabi frequency Ω S (t) and phase φ + ϕ S (t)) utilized for the realization of superadiabatic geometric quantum computation
Universal, high-fidelity quantum gates based on superadiabatic, geometric phases on a solid-state spin-qubit at room temperature
  • Article
  • Full-text available

October 2018

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205 Reads

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61 Citations

npj Quantum Information

Quantum logic: Suppressing noise with geometric phases A demonstration of quantum logic gates based on geometric phases could enable quantum computing in noisy experimental conditions. Developing large-scale quantum computation requires the performance of quantum logic gates to be significantly improved. Quantum logic gates are very sensitive to noise but gates that exploit geometric phases are predicted to be resilient against a common source of noise. However, experimentally realising such strategies is not trivial. Using the electron spin of nitrogen-vacancy centers in diamond, Felix Kleißler and colleagues from the Max Planck Institute for Biophysical Chemistry in Göttingen, Germany demonstrate geometric phase-based quantum logic gates under ambient conditions. This implementation shows that such geometric quantum gates in combination with solid-spin qubit systems are a promising platform for realising large-scale quantum computing in noisy environments.

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Figure 2. Superadiabatic geometric gate realization: (a) Simulated and reconstructed Bloch sphere trajectory of the superadiabatic geometric Pauli-Z gate in the driving field frame for a spin initialized into the m s = 0 state. (b) Bloch vector component Ψ x (blue), Ψ y (orange) and Ψ z (green) of the trajectory presented in (a) versus the gate time in multiples of τ. Solid lines represent numerically calculated trajectories and dots indicated measured values. Analogously (c) and (d) follow for the realized Pauli-X gate. (e-g) Measured population of the |0 state for a spin initialized into the orthogonal states (e) |0, (f) 1/ √ 2(|0 − |1) and (g) 1/ √ 2(|0 + i |1) in dependence of γ for superadiabatic rotations around the x (green) and z-axis (blue). Dashed lines represent the expected values. Bloch spheres indicate the initialized state (red arrow). 
Figure 3. Robustness analysis: (a) The randomized benchmarking analysis reveals the decay of the average fidelity in dependence of the number of computational gates l for a set of SAGQG (orange) and a set of dynamic quantum gates (blue). The average probability of error per gate are ε SAGQG g 
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Universal, high-fidelity quantum gates based on superadiabatic, geometric phases on a solid-state spin-qubit at room temperature

April 2018

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147 Reads

Geometric phases and holonomies (their non-commuting generalizations) are a promising resource for the realization of high-fidelity quantum operations in noisy devices, due to their intrinsic fault-tolerance against noise and experimental imperfections. Despite their conceptual appeal and proven fault-tolerance, for a long time their practical use in quantum computing was limited to proof of principle demonstrations. Only in 2012 Sj\"oqvist et al. formulated a strategy to generate non-Abelian (i.e. holonomic) quantum gates through non-adiabatic transformation. Successful experimental demonstrations of this concept followed on various physical qubit systems and proved the feasibility of this fast, holonomic quantum gate concept. Despite these successes, the experimental implementation of such non-Abelian quantum gates remains experimentally challenging since in general the emergence of a suitable holonomy requires encoding of the logical qubit within a three (or higher) level system being driven by two (or more) control fields. A very recent proposal by Liang et al. offers an elegant solution generating a non-Abelian, geometric quantum gate on a simple, two-level system driven by one control field. Exploiting the concept of transitionless quantum driving it allows the generation of universal geometric quantum gates through superadiabatic evolution. This concept thus generates fast and robust phase-based quantum gates on the basis of minimal experimental resources. Here, we report on the first such implementation of a set of non-commuting single-qubit superadiabatic geometric quantum gates on the electron spin of the negatively charged nitrogen vacancy center in diamond. The realized quantum gates combine high-fidelity and fast quantum gate performance. This provides a promising and powerful tool for large-scale quantum computing under realistic, noisy experimental conditions.


Quantum noise spectroscopy of non-monotonous spectra

March 2018

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46 Reads

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2 Citations

Understanding the physical origin of noise affecting quantum systems is important for nearly every quantum application. While quantum noise spectroscopy has been employed in various quantum systems, such as superconducting qubits and trapped ions, traditional spectroscopy methods are usually efficient in measuring noise spectra with mostly monotonically decaying contributions. However, there are important scenarios in which the noise spectrum is broadband and non-monotonous, thus posing a challenge to existing noise spectroscopy schemes.Here, we compared several methods for noise spectroscopy: spectral decomposition based on the CPMG sequence, the recently presented DYSCO sequence and a modified DYSCO sequence with a Gaussian envelope (gDYSCO).The performance of the sequences is quantified by analytic and numeric determination of the frequency resolution, bandwidth and sensitivity, revealing a supremacy of gDYSCO to reconstruct non-trivial features.Utilizing an ensemble of nitrogen-vacancy centres in diamond coupled to a high density 13C nuclear spin environment, we experimentally confirm our findings.The combination of the presented schemes offers potential to record high quality noise spectra as a prerequisite to generate quantum systems unlimited by their spin-bath environment.


Dynamical sensitivity control of a single-spin quantum sensor

December 2017

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244 Reads

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10 Citations

The Nitrogen-Vacancy (NV) defect in diamond is a unique quantum system that offers precision sensing of nanoscale physical quantities at room temperature beyond the current state-of-the-art. The benchmark parameters for nanoscale magnetometry applications are sensitivity, spectral resolution, and dynamic range. Under realistic conditions the NV sensors controlled by conventional sensing schemes suffer from limitations of these parameters. Here we experimentally show a new method called dynamical sensitivity control (DYSCO) that boost the benchmark parameters and thus extends the practical applicability of the NV spin for nanoscale sensing. In contrast to conventional dynamical decoupling schemes, where π pulse trains toggle the spin precession abruptly, the DYSCO method allows for a smooth, analog modulation of the quantum probe’s sensitivity. Our method decouples frequency selectivity and spectral resolution unconstrained over the bandwidth (1.85 MHz–392 Hz in our experiments). Using DYSCO we demonstrate high-accuracy NV magnetometry without |2π| ambiguities, an enhancement of the dynamic range by a factor of 4 · 10³, and interrogation times exceeding 2 ms in off-the-shelf diamond. In a broader perspective the DYSCO method provides a handle on the inherent dynamics of quantum systems offering decisive advantages for NV centre based applications notably in quantum information and single molecule NMR/MRI.



Figure 2 | Results of dynamical sensitivity and dynamic range enhancement. a) Experimental results  
Figure 3 | High-resolution magnetic sensing in the frequency domain. a) Frequency domain sensing of an 8 kHz phase-synchronized signal using DYSCO and conventional sensing by multi-pulse scheme. b) Free  
Figure 4 | High-resolution noise spectrum of 13 C nuclear spin bath in diamond free from harmonics.  
Dynamical sensitivity control of a single-spin quantum sensor

December 2015

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146 Reads

The Nitrogen-Vacancy (NV) defect in diamond is a unique quantum system that offers precision sensing of nanoscale physical quantities beyond the current state-of-the-art. Here we present a method to controllably encode the interactions in the population of the spin states, thereby introducing a way to control the sensitivity of a single spin as a continuum in contrast to free-evolution based methods. By adopting this feature we demonstrate high-accuracy NV magnetometry without 2pi ambiguities, enhance the dynamic range by a factor of 4*10^3 achieve interaction times exceeding 2 ms in off-the-shelf diamond. We perform nuclear spin-noise spectroscopy in the frequency domain by dynamically controlling the NV spin's sensitivity piecewise and in a smooth manner thereby precluding harmonic artefacts and undesired interactions. On a broader perspective dynamical sensitivity control provides an elegant handle on the inherent dynamics of quantum systems, while offering decisive advantages for NV centre applications notably in quantum controls and single molecule NMR/MRI.


Figure 1 | Dynamical sensitivity control (DYSCO). a) Schematic representation of a DYSCO 4 ⋅ í µí¼‹-pulse unit. Simulations and experimentally traced spin vector trajectory for one 4 ⋅ í µí¼‹-pulse unit represented on the Bloch sphere spanned by|0⟩ and |−⟩. The green trajectory in simulations depicts spin evolution when sequentially driven by 4 ⋅ í µí¼‹-pulse and í µí°µ RF = 0. The coloured trajectories in the Simulations and Experiment are shown for í µí°µ RF ≠ 0. Individual í µí¼‹-pulses are shown in red, blue, magenta and cyan dots and traces. b) Schematic of the DYSCO method and the expected changes in the final state population í µí±ƒ 0 for different values of the í µí°µ RF field amplitude shown in comparison to the Hahn-echo sensing method (note the last í µí¼‹/2 pulse used in NV-metrology based on free-precession/interferometry is not included here for vividly contrasting the sensing mechanism of DYSCO). c) Explicit calculation of the level occupancy í µí±ƒ 0 and its dependence on the í µí°µ RF field and the phase angle í µí¼‘ of the driving pulses at the end of the pulse sequence for N=1 (the í µí°µ RF field is given in units of Ω -) d) Experimental results showing the dependence of state population í µí±ƒ 0 as a function of í µí°µ RF and í µí¼‘ for í µí± = 20.  
Figure 2 | Results of dynamical sensitivity and dynamic range enhancement. a) Experimental results  
Figure 3 | High-resolution magnetic sensing in the frequency domain. a) Frequency domain sensing of an 8 kHz phase-synchronized signal using DYSCO and conventional sensing by multi-pulse scheme. b) Free  
Figure 4 | High-resolution noise spectrum of 13 C nuclear spin bath in diamond free from harmonics.  
Dynamical sensitivity control of a single-spin quantum sensor

December 2015

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181 Reads

The Nitrogen-Vacancy (NV) defect in diamond is a unique quantum system that offers precision sensing of nanoscale physical quantities beyond the current state-of-the-art. Here we present a method to controllably encode the interactions in the population of the spin states, thereby introducing a way to control the sensitivity of a single spin as a continuum in contrast to free-evolution based methods. By adopting this feature we demonstrate high-accuracy NV magnetometry without 2pi ambiguities, enhance the dynamic range by a factor of 4*10^3 achieve interaction times exceeding 2 ms in off-the-shelf diamond. We perform nuclear spin-noise spectroscopy in the frequency domain by dynamically controlling the NV spin's sensitivity piecewise and in a smooth manner thereby precluding harmonic artefacts and undesired interactions. On a broader perspective dynamical sensitivity control provides an elegant handle on the inherent dynamics of quantum systems, while offering decisive advantages for NV centre applications notably in quantum controls and single molecule NMR/MRI.


Figure 1: Schematics of the molecular scale spatial encoding using magnetic field gradients.: (a) Schematic representation of a biomolecule in the vicinity of an NV-center; ωL in the inset signifies the Larmor peak position in the spectrum. (b) Gradient encoding of the molecule’s proton density; a spectrum is presented in direction of the gradient vector. (c,d) Schematic representation of different magnetic field gradients induced by an approached magnetic tip; insets: their influence on the spectrum.
Figure 2: Simulations of projection-reconstruction method using a molecular phantom β-cyclodextrin.: (a) 3D visualization of hydrogen atoms in β-cyclodextrin molecule in a space filling representation. (b) Simulated spin noise spectra for two different gradient orientations. (c) Encoded signal matrix (some slices are omitted for visual clarity). (d) Reconstructed three dimensional image of a β-cyclodextrin molecule.
A nitrogen-vacancy spin based molecular structure microscope using multiplexed projection reconstruction

May 2015

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63 Reads

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17 Citations

Methods and techniques to measure and image beyond the state-of-the-art have always been influential in propelling basic science and technology. Because current technologies are venturing into nanoscopic and molecular-scale fabrication, atomic-scale measurement techniques are inevitable. One such emerging sensing method uses the spins associated with nitrogen-vacancy (NV) defects in diamond. The uniqueness of this NV sensor is its atomic size and ability to perform precision sensing under ambient conditions conveniently using light and microwaves (MW). These advantages have unique applications in nanoscale sensing and imaging of magnetic fields from nuclear spins in single biomolecules. During the last few years, several encouraging results have emerged towards the realization of an NV spin-based molecular structure microscope. Here, we present a projection-reconstruction method that retrieves the three-dimensional structure of a single molecule from the nuclear spin noise signatures. We validate this method using numerical simulations and reconstruct the structure of a molecular phantom \b{eta}-cyclodextrin, revealing the characteristic toroidal shape.


Figure 1: NV centre geometry and level structure. (a) Illustration of the unit cell of diamond including an NV colour centre. Spin projections ms=0,±1 are defined with respect to the NV symmetry axis. (b) Energy levels of the triplet (left) and singlet states (right) of the NV centre and the applied excitation (EXC) and microwave (MW) fields and the detected fluorescence (FLUO). (c) Three-level V-scheme of the NV ground state triplet employed for the realization of the single-qubit holonomic quantum gate.
Figure 2: Concept for the realization of an NV-based holonomic single-qubit gate. (a) Schematic representation of the total Hilbert space and a projected Hilbert space therein defined through a projective map π: ↦ by means of the local U(2) fibre bundle. Driving the system on a suitable loop (red curve) on this U(2) fibre bundle of nontrivial topology gives rise to a holonomy. Here, this holonomy is employed for the generation of a relative phase for quantum computation applications. (b) Experimental sequence for the quantum process tomography (QPT): First the NV state is initialized by a green laser pulse (EXC) to state |0›. In the following first part of the QPT microwave pulses (MW) tuned to ω+ and ω− prepare the spin into one of the nine QPT states |ψj›. After application of the holonomic quantum gate (HQG), the second part of the QPT project the NV state onto one of the nine measurement bases |ψj› by means of microwave pulses (MW). State selective detection concludes the sequence composed of simultaneous application of a green laser pulse (EXC) and signal and reference windows detection (DET). Due to the different numbers and types of pulses necessary for the 81 preparation and readout combinations of the QPT, the durations of the QPT blocks 1 and 2 vary for each QPT measurement.
Figure 3: Representations of the experimentally accomplished quantum processes. (a) Process matrix of the identity operation, (b) the Pauli-X, (c) the Pauli-Y, (d) the Pauli-Z and (e) the Hadamard gate (coloured bars: experimental data and and error bars, transparent boxes: ideal quantum gates).
Room temperature high-fidelity holonomic single-qubit gate on a solid-state spin

September 2014

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1,977 Reads

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260 Citations

At its most fundamental level, circuit-based quantum computation relies on the application of controlled phase shift operations on quantum registers. While these operations are generally compromised by noise and imperfections, quantum gates based on geometric phase shifts can provide intrinsically fault-tolerant quantum computing. Here we demonstrate the high-fidelity realization of a recently proposed fast (non-adiabatic) and universal (non-Abelian) holonomic single-qubit gate, using an individual solid-state spin qubit under ambient conditions. This fault-tolerant quantum gate provides an elegant means for achieving the fidelity threshold indispensable for implementing quantum error correction protocols. Since we employ a spin qubit associated with a nitrogen-vacancy colour centre in diamond, this system is based on integrable and scalable hardware exhibiting strong analogy to current silicon technology. This quantum gate realization is a promising step towards viable, fault-tolerant quantum computing under ambient conditions.


Citations (7)


... Noise spectroscopy elucidates the fundamental noise sources in spin systems, which is essential to develop spin qubits with long coherence times for quantum information processing [1], communication [2], and sensing [3]. But noise spectroscopy typically relies on microwave spin control to extract the noise spectrum [4][5][6][7][8][9], which becomes infeasible when high-frequency noise components are stronger than the available microwave power. Here, we demonstrate an alternative all-optical approach to perform noise spectroscopy. ...

Reference:

All-optical noise spectroscopy of a solid-state spin
Measuring Environmental Quantum Noise Exhibiting a Nonmonotonic Spectral Shape
  • Citing Article
  • January 2019

Physical Review Applied

... On the practical side, several recent investigations have shown the most important role of the geometric phase in the advancement of quantum information science. Indeed, it is a valuable feature for generating quantum logic gates that are critical to quantum computation [42][43][44]. Furthermore, the conditional phase gate has been experimentally demonstrated for nuclear magnetic resonance [45] and trapped ions [46]. ...

Universal, high-fidelity quantum gates based on superadiabatic, geometric phases on a solid-state spin-qubit at room temperature

npj Quantum Information

... Although the idea is rather simple and appealing, using such a spectrometer to obtain quantitative data on the spatiotemporal spectrum of the noise field requires more caution than when a single qubit is used to reconstruct the spectrum of temporal fluctuations of the local noise affecting it (note that the latter task, while routinely performed in recent years, is not entirely trivial either, especially in case of temporal spectra having peaks at finite frequencies [48,56]). Large part of the paper has been devoted to detailed explanation of methods allowing for reliable extraction of "spectroscopic" information (spectroscopic formulas defined in Sec. ...

Quantum noise spectroscopy of non-monotonous spectra
  • Citing Article
  • March 2018

... They also, however, experience decoherence due to this same environment, which limits their sensitivity in practice. Techniques to suppress decoherence, without equally suppressing the signal, are therefore of central importance in quantum sensing [2][3][4][5][6][7][8][9]. Quantum error correction (QEC) is currently emerging as an important technique to this end, and has attracted substantial theoretical and experimental interest of late [10][11][12][13][14][15][16][17][18][19][20][21][22][23][24][25][26][27]. ...

Dynamical sensitivity control of a single-spin quantum sensor

... Due to the nanometre dimensions of molecular systems, a pathway for achieving single protein imaging can be found in sensors that are atomic in scale. Recently, the nitrogen vacancy (NV) centre in diamond [20,21] has shown a great promise as a biocompatible, nanoscopic qubit-probe for room temperature magnetometry [22][23][24][25] and, in particular, high resolution nuclear magnetic resonance (NMR) spectroscopy [26][27][28][29][30][31][32][33][34][35][36][37][38][39][40]. However, imaging the atomic makeup of single molecular structures requires low temperatures, as a means of arresting atomic motion and capturing desired instances of protein conformation states. ...

A nitrogen-vacancy spin based molecular structure microscope using multiplexed projection reconstruction

... To this end, fidelity estimation for entangled states is a promising candidate. Fidelity quantifies the quality of quantum states [9][10][11] and can be estimated with separable quantum measurements and classical post-processing. Fidelity estimation protocols for several types of states are designed in [12][13][14], a fidelity estimation protocol for general pure states using only Pauli observables is proposed in [15], and a low-complexity fidelity estimation protocol for mixed states is proposed in [16]. ...

Room temperature high-fidelity holonomic single-qubit gate on a solid-state spin

... To establish NV-centers as an alternative label for superresolution microscopy, in this contribution, first, we investigate the distribution of NV-centers in a diamond substrate using Raman spectroscopy in photoluminescence (PL) mode for the existence of NV centers in the substrate and for comparing the spectral resolution as proposed by Balasubramanian et al. [8]. Then, we imaged a random feature on the substrate surface with the NV-centers in STED and confocal mode with the aid of the STED microscopy system. ...

Nitrogen-Vacancy color center in diamond - emerging nanoscale applications in bioimaging and biosensing
  • Citing Article
  • May 2014

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