Publications by authors named "Khakimov R"

Article Synopsis
  • The study investigates how a bottom TiO interfacial layer affects the ferroelectric properties of TiN/HfZrO/TiN capacitors, showing that adding this layer increases the polar orthorhombic phase in the HfZrO film.
  • The thickness of the TiO layer significantly influences the crystalline structure of HfZrO, leading to a stabilization of the monoclinic phase at greater TiO thicknesses.
  • While the TiO layer enhances retention performance by reducing oxygen vacancies and imprint effects, there are limitations in endurance due to phase transitions in the TiO layer when the effective electric field is increased.
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  • HfZrO (HZO) ferroelectrics show great potential for nonvolatile memory but face reliability challenges including wake-up, fatigue, and retention loss.
  • A comparison of HZO-based stacks with TiN and Ru electrodes indicates that both exhibit significant wake-up and retention losses, with Ru implementation worsening fatigue due to the generation of oxygen vacancies.
  • The study reveals that reliability issues in HZO capacitors depend heavily on the electrode type, suggesting that simply replacing electrodes for improved properties may not address underlying problems.
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  • Resistive switching (RS) device performance is influenced by the material properties of both the insulator and the bottom electrode (BE), particularly the surface roughness of the BE, which in this case is a Ru film on a TiN layer.
  • The study demonstrates that increasing the thickness of the Ru films through radical-enhanced atomic layer deposition (REALD) leads to a significant rise in surface roughness and results in changes to various RS parameters such as switching voltage and resistance states.
  • A simplified model links the roughness of the Ru surface to the RS characteristics by simulating field distribution and indicating that the roughness enhances local fields, leading to specific conducting filament formation, which was confirmed using conductive atomic force microscopy.
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This work demonstrates by in vacuo X-ray photoelectron spectroscopy and grazing-incidence X-ray diffraction that Ru(EtCp) and O radical-enhanced atomic layer deposition, where EtCp means the ethylcyclopentadienyl group, provides the growth of either RuO or Ru thin films depending on the deposition temperature (T), while different mechanisms are responsible for the growth of RuO and Ru. The thin films deposited at temperatures ranging from 200 to 260 °C consisted of polycrystalline rutile RuO phase revealing, according to atomic force microscopy and the four-point probe method, a low roughness (∼1.7 nm at 15 nm film thickness) and a resistivity of ≈83 µΩ cm.

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Ghost imaging is a quantum optics technique that uses correlations between two beams to reconstruct an image from photons that do not interact with the object being imaged. While pairwise (second-order) correlations are usually used to create the ghost image, higher-order correlations can be utilized to improve the performance. In this Letter, we demonstrate higher-order atomic ghost imaging, using entangled ultracold metastable helium atoms from an s-wave collision halo.

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In quantum many-body theory, all physical observables are described in terms of correlation functions between particle creation or annihilation operators. Measurement of such correlation functions can therefore be regarded as an operational solution to the quantum many-body problem. Here, we demonstrate this paradigm by measuring multiparticle momentum correlations up to third order between ultracold helium atoms in an s-wave scattering halo of colliding Bose-Einstein condensates, using a quantum many-body momentum microscope.

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We have developed and characterised a stable, narrow linewidth external-cavity laser (ECL) tunable over 100 nm around 1080 nm, using a single-angled-facet gain chip. We propose the ECL as a low-cost, high-performance alternative to fibre and diode lasers in this wavelength range and demonstrate its capability through the spectroscopy of metastable helium. Within the coarse tuning range, the wavelength can be continuously tuned over 30 pm (7.

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Ghost imaging is a counter-intuitive phenomenon-first realized in quantum optics-that enables the image of a two-dimensional object (mask) to be reconstructed using the spatio-temporal properties of a beam of particles with which it never interacts. Typically, two beams of correlated photons are used: one passes through the mask to a single-pixel (bucket) detector while the spatial profile of the other is measured by a high-resolution (multi-pixel) detector. The second beam never interacts with the mask.

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We present the first measurement for helium atoms of the tune-out wavelength at which the atomic polarizability vanishes. We utilize a novel, highly sensitive technique for precisely measuring the effect of variations in the trapping potential of confined metastable (2^{3}S_{1}) helium atoms illuminated by a perturbing laser light field. The measured tune-out wavelength of 413.

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An important aspect of the rapidly growing field of quantum atom optics is exploring the behavior of ultracold atoms at a deeper level than the mean field approximation, where the quantum properties of individual atoms becomes important. Major recent advances have been achieved with the creation and detection of reliable single-atom sources, which is a crucial tool for testing fundamental quantum processes. Here, we create a source comprised of a single ultracold metastable helium atom, which enables novel free-space quantum atom optics experiments to be performed with single massive particles with large de Broglie wavelengths.

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We present an approach for numerically solving the multimode generalized nonlinear Schrödinger equation (MM-GNLSE). We propose to transform the MM-GNLSE to a system of first-order ordinary differential equations (ODEs) that can then be solved using readily available ODE solvers, thus making modeling of pulse propagation in multimode fibers easier. The solver is verified for the simplest multimode case in which only the two orthogonal polarization states in a non-birefringent microstructured optical fiber are involved.

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