Seminarium Optyczne
2006/2007 | 2007/2008 | 2008/2009 | 2009/2010 | 2010/2011 | 2011/2012 | 2012/2013 | 2013/2014 | 2014/2015 | 2015/2016 | 2016/2017 | 2017/2018 | 2018/2019 | 2019/2020 | 2020/2021 | 2021/2022 | 2022/2023 | 2023/2024 | 2024/2025 | Seminarium na YouTube
2024-11-21 (Czwartek)
Mateusz Bocheński (IFD UW)
Ultracold mixtures of cesium with potassium isotopes
Studies of fundamental physical phenomena with ultracold atoms, from superfluidity, through quantum simulators, to degenerate gases of polar molecules, require exquisite knowledge of collisional properties of atoms used in experiments. Theoretical predictions are usually based on scarce spectroscopic data and even for molecules like KCs, which have been extensively studied in hot vapors, theoretical understanding of ultracold properties of these molecules is rarely satisfactory. This necessitates the development of efficient cooling methods and extensive experimental studies of fine details of interactions between atoms to provide data for theoretical modeling.In the first part of the talk I will introduce our state-of-the-art experimental setup designed to study ultracold mixtures of cesium and potassium. The versatility of the apparatus will be demonstrated by individually cooling 39K, 40K, 41K, and 133Cs atoms as well as their mixtures. I will compare these findings with state of the art results from other research groups and highlight our achievement of the world’s first 39K-40K and 41K-133Cs mixtures. The second part of the talk will focus on Feshbach resonances spectroscopy of 39K-133Cs and 41K-133Cs mixtures. For 39K-133Cs, we provide the first independent verification of the 2017 results obtained by the group of H.-C. Nägerl (University of Innsbruck). The Feshbach spectrum of 41K-133Cs is demonstrated for the first time, showing significant disagreement with theoretical predictions. These results are vital for a deeper understanding of the collisional properties of cesium and potassium mixtures and are a prerequisite for advancing toward the formation of ultracold polar ground state molecules of KCs.
2024-11-14 (Czwartek)
Artur Bednarkiewicz (Institute of Low Temperature and Structure Research, Polish Academy of Sciences)
Photon avalanching in lanthanide doped nanoparticles – the mechanism, applications and challenges
Lanthanide ions doped inorganic nanoparticles (LnNP) are potential candidates and alternative labels to fluorescent molecules and quantum dots. Among the other, they display narrowband absorption and emission lines, multicolour emission, long luminescence lifetimes and are perfectly photostable. In sensitized configuration, they are also capable to efficiently convert NIR excitation to visible range (so called upconversion UC), thus avoiding background fluorescence and enhance signal to background ratio towards super-sensitive biosensing & imaging. They also display non-linearity of luminescence intensity versus pump intensity, which enables imaging beyond diffraction limit with simple, customized confocal setups.Among upconversion processes leading to the anti-Stokes emission, the photon avalanche (PA) became an interesting research topic since 1979, when it was first observed in Pr3+ doped LaCl3 [1]. There are several essential requirements necessary to enable observation of PA in a given system – these include (i) the presence of efficient ESA transition and negligible GSA at the pumping wavelength and (ii) the presence of efficient the cross-relaxation (CR) processes required to populate intermediate excited level. As a consequence, the luminescence intensity of PA increases by several, typically 2-3 orders of magnitude when exciting with power density slightly (e.g. twice) above the PA threshold. Only recently its PA emission was also demonstrated for NaYF4 nanoparticles doped with Tm3+ at the room temperature under 1064 and 1450 nm photoexcitation and 800 nm emission [3].In this lecture, current state-of-the-art on PA emission and the PA emission in nano, micro and bulk LiYF4 crystals will be summarized. Moreover, peculiarities of photon avalanche emission in wider context as the paradigm shift in luminescent nano-bio-labels will be discussed. The wide application potential of PA (e.g. super-resolution imaging [3], biosensing [4], nano-thermometry [5] etc.) makes it extremely interesting to further studies of the PA in various lanthanides and various matrices of various sizes – these applications will be evaluated and future directions & challenges will be emphasized for materialscientists. References: [1] J. S. Chivian, W. E. Case, and D. D. Eden, Appl. Phys. Lett. (1979) 35, 124–125.; [2] M. F. Joubert, Opt. Mater. (Amst). (1999) 11, 181–203.; [3] Ch. Lee et al., Nature (2021), 589, 230-235; A.Bednarkiewicz et al. (2019) Nanoscale Horizons, 4(3), 706-719; [4] A.Bednarkiewicz, E.Chan, K.Prorok, Nanoscale Adv., 2020,2, 4863-4872; [5] M.Szalkowski et
2024-11-07 (Czwartek)
Andrei Nomerotski (Florida International University & Czech Technical University)
Time-stamping photons with sub-nanosecond resolution for quantum-enhanced imaging and telescopy
Correlations of photons from entangled quantum sources offer advantages and provide additional opportunities such as low light imaging or new sensing approaches. In general, strong spectro-temporal correlations inherent for entangled photons make those sensing techniques much more precise and resource efficient. To take advantage of the correlations one would need efficient single photon imagers with excellent timing resolution. In the presentation I will review the existing detector options focussing on the time-stamping CMOS and SPAD cameras, which have been used recently in a variety of quantum imaging experiments, in particular the Tpx3Cam and LinoSPAD2 cameras, both based on data-driven readouts. As a motivation for fast imaging in astrophysics I will also review the standard techniques of single-photon amplitude (Michelson) interferometry and two-photon (Hanbury Brown & Twiss) intensity interferometry, and then visit recent ideas for how they can be improved in the optical through the use of entanglement distribution. A proposed new technique of two-photon amplitude interferometry requires precise spectral binning and 10 picosecond scale time-stamping of single optical photons with a product of resolutions close to the Heisenberg Uncertainty Principle limit. Another prominent example of multi-dimensional quantum correlations is the parametric down-conversion of x-rays in diamond. In this case all three types of correlations, in momentum, energy and time, can be measured simultaneously. In all cases I will illustrate the concepts with recent results and will discuss future directions for the technology.[1] A. Nomerotski, “Imaging and time stamping of photons with nanosecond resolution in Timepix based optical cameras,” Nuclear Instruments and Methods A: 937, 26 (2019).[2] Y Zhang, D England, A Nomerotski, B Sussman, "High speed imaging of spectral-temporal correlations in Hong-Ou-Mandel interference," Opt. Express 29, 28217 (2021).[3] P Stankus, A Nomerotski, A Slosar, S Vintskevich, “Two-photon amplitude interferometry for precision astrometry”; Open Journal of Astrophysics 5 (2023).[4] T. Milanese et al. "LinoSPAD2: an FPGA-based, hardware-reconfigurable 512×1 single-photon camera system." Optics Express 31.26 (2023): 44295.[5] J.Jirsa et al. "Fast spectrometer with direct measurement of time and frequency for multiple single photons." arXiv:2304.11999 (2023).[6] J.Goodrich et al, “Imaging of X-ray Pairs in a Spontaneous Parametric Down-Conversion Process,” arXiv:2310.13078 (2023).
2024-10-31 (Czwartek)
Jerzy Szuniewicz (IFD UW)
Phase of a single photon: from measuring to shaping
Single photons play a pivotal role in quantum technologies such as metrology, computing, communications, networking, and quantum key distribution (QKD). They have become essential for transmitting quantum states over long distances, thanks to their weak interactions with matter, compatibility with fiber optics, and technical advances in optical telecommunications. Additionally, photons serve as a cornerstone in both theoretical and experimental research in precise measurements and quantum information processing.In this talk, we will explore the phases carried by single photons, beginning with spatial phases and extending to temporal and spectral phases. We will examine current techniques for dynamically modifying the spectral-temporal modes of single photons and investigate methods for measuring these states. Lastly, we will briefly discuss the role of machine learning in optimizing and shaping single-photon modes.
2024-10-24 (Czwartek)
Lars Loetgering (ZEISS Research Microscopy Solutions, Jena)
Advances in ptychography
Ptychography is a label-free phase imaging technique that revolutionized microscopy in spectral domains where high-quality lenses are challenging to come by, including x-rays, extreme ultraviolet, terahertz radiation and electrons. In recent years, related techniques have emerged that utilize ptychography for visible light microscopes, optical diffraction tomography and high throughput whole slide imaging. In my talk, I will give an overview of the several flavors of ptychography and highlight applications from tabletop extreme ultraviolet lensless imaging using high harmonic generation. The goal of this talk is to provide an introduction of what ptychography is and what it is good for.
Dr Lars Loetgering (ZEISS Research Microscopy Solutions, Jena, Germany.)
Advances in ptychography
Ptychography is a label-free phase imaging technique that revolutionized microscopy in spectral domains where high-quality lenses are challenging to come by, including x-rays, extreme ultraviolet, terahertz radiation and electrons. In recent years, related techniques have emerged that utilize ptychography for visible light microscopes, optical diffraction tomography and high throughput whole slide imaging. In my talk, I will give an overview of the several flavors of ptychography and highlight applications from tabletop extreme ultraviolet lensless imaging using high harmonic generation. The goal of this talk is to provide an introduction of what ptychography is and what it is good for.
2024-10-17 (Czwartek)
Ron Folman (Ben Gurion University of the Negev, Israel)
Can a rock be a wave? From 100 years of de-Broglie's wave-particle duality, to quantum-gravity
It is almost exactly 100 years since De-Broglie made public his outrageous hypothesis regarding Wave-Particle Duality (WPD), where the latter plays a key role in interferometry. In parallel, the Stern-Gerlach (SG) effect, found a century ago, has become a paradigm of quantum mechanics. I will describe the realization of a half- [1-3] and full- [4-5] loop SG interferometer for single atoms [6], and show how WPD, or complementarity, manifests itself. I will then use the acquired understanding to show how this setup may be used to realize an interferometer for macroscopic objects doped with a single spin [5], namely, to show that even rocks may reveal themselves as waves. I emphasize decoherence channels which are unique to macroscopic objects such as those relating to phonons [7,8] and rotation [9]. These must be addressed in such a challenging experiment. The realization of such an experiment could open the door to a new era of fundamental probes, including the realization of previously inaccessible tests of the foundations of quantum theory and the interface of quantum mechanics and gravity, including the probing of exotic theories such as the Diosi-Penrose gravitationally induced collapse. Time permitting, and as an anecdote noting also De-Broglie's less popular assertion, namely, that the standard description of QM is lacking, I will also present our recent work on Bohmian mechanics, which is an extension of De-Broglie's ideas concerning the pilot wave [10].PS I will not talk about quantum technology in this talk, but I invite those interested to talk to me about it, for example, our NV sensor or Yb optical atomic clock projects. Here are two recent quantum technology references [11,12]. More work from our group such as on Dark-Matter can be found on our website: https://tzin.bgu.ac.il/atomchip/[1] Y. Margalit et al., A self-interfering clock as a ""which path"" witness, Science 349, 1205 (2015); [2] Zhifan Zhou et al., Quantum complementarity of clocks in the context of general relativity, Classical and quantum gravity 35, 185003 (2018);[3] Zhifan Zhou et al., An experimental test of the geodesic rule proposition for the non-cyclic geometric phase, Science advances 6, eaay8345 (2020);[4] O. Amit et al., T3 Stern-Gerlach matter-wave interferometer, Phys. Rev. Lett. 123, 083601 (2019);[5] Y. Margalit et al., Realization of a complete Stern-Gerlach interferometer: Towards a test of quantum gravity, Science advances 7, eabg2879 (2021);[6] M. Keil et al., Stern-Gerlach interferometry with the atom chip, Book in honor of Otto Stern, Springer (2021);[7] C. Henkel and R. Folman, Internal decoherence in nano-object interferometry due to phonons, AVS Quantum Sci. 4, 025602 (2022) – invited paper for a special issue in honor of Roger Penrose;[8] C. Henkel and R. Folman, Universal limit on quantum spatial superpositions with massive objects due to phonons, https://arxiv.org/abs/2305.15230 (2023);[9] Y. Japha and R. Folman, Role of rotations in Stern-Gerlach interferometry with massive objects, Phys. Rev. Lett. 130, 113602 (2023)[10] G. Amit et al., Countering a fundamental law of attraction with quantum wave-packet engineering, Phys. Rev. Res. 5, 013150 (2023);[11] Z. Zhou, Geometric phase amplification in a clock interferometer for enhanced metrology, https://arxiv.org/abs/2405.10226 (2024);[12] Y. Halevy et al., Chip-Scale Point-Source Sagnac Interferometer by Phase-Space Squeezing, https://arxiv.org/abs/2405.16972 (2024).
2024-10-10 (Czwartek)
Katarzyna Krajewska (IFT UW)
Strong- versus ultra-strong-field physics
When increasing the intensity of optical pulses we can probe different regimes of laser-matter interactions. Specifically, in the area of strong-field physics we deal with bound electrons that undergo various atomic transformations due to the interaction with the laserfield. The theoretical framework behind is non-relativistic quantum mechanics, based on the time-dependent Schrodinger equation. Going toward higher intensities, we reach the ultra-strong-field regime. Here,we deal with free electrons whose quiver energy in a laser field becomes comparable to their rest mass energy. Thus, we enter the area governed by relativistic quantum mechanics, that is based on the Dirac equation. The physics in those two regimes has to be treated using different theoretical methods and inherently different physical effects should be observed there. But is it always the case? In my talk, I will address this question considering two seemingly different physical processes, representing each of those regimes: ionization and electron-positron pair creation.
2024-10-03 (Czwartek)
Bartosz Krajnik (Politechnika Wrocławska)
Fluorescence Microscopy of Single Nanostructures: From Imaging to Molecular Dynamics
Single-molecule microscopy and spectroscopy are advanced research techniques that enable the real-time tracking and analysis of individual molecules. These methods provide detailed insights into molecular dynamics, interactions, and structures, which cannot be achieved by studying phenomena at the ensemble level. Two techniques in this field, SOFI (Stochastic Optical Fluctuation Imaging) and defocused wide-field fluorescence microscopy, offer unique approaches for high-resolution molecular/nanoparticle analysis. SOFI is based on the statistical analysis of fluorescence signal fluctuations generated by single emitters. This allows for image reconstruction with a resolution beyond the diffraction limit of light, particularly for densely labeled samples. Defocused wide-field fluorescence microscopy involves imaging under deliberately defocused conditions. The emerging single-molecule patterns provide information about the orientation and structure of individual molecules. This technique is particularly suitable for studying rotational dynamics (e.g., molecular motors), allowing for the direct observation of even tens of individual molecules. Both methods are powerful tools in modern molecular research, providing extensive possibilities for analyzing structures and processes at the nanoscale level.