Andrzej Raczynski
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Research Subjects
Andrzej Raczynski has a total of 53 co-authors. Here are the top co-authors by number of shared publications:
- Jarosław Zaremba
Institute of Physics, Faculty of Physics, Astronomy and Informatics, Nicolaus Copernicus University, ul. Grudziadzka 5, 87-100 Torun, Poland
48 shared publications S. Zielińska-Kaniasty
Institute of Mathematics and Physics, University of Technology and Life Sciences, Al. Kaliskiego 7, 85-798 Bydgoszcz, Poland
10 shared publicationsJ. Zaremba
Institute of Physics, Faculty of Physics, Astronomy and Informatics, Nicolaus Copernicus University, Grudziadzka 5, PL-87-100 Toruń, Poland
7 shared publications- Jacek Matulewski
Department of Informatics, Nicolaus Copernicus University, Toruń, Poland and Institute of Advanced Studies, Nicolaus Copernicus University, Toruń, Poland
7 shared publications S. Zielinska-Kaniasty
Univ. of Technology and Life Sciences in Bydgoszcz (Poland)
6 shared publicationsSylwia Zielińska-Raczyńska
Institute of Mathematics and Physics, University of Science and Technology, Aleja Prof. S. Kaliskiego 7, 85-789 Bydgoszcz, Poland
6 shared publications
Latest Publications
- 29 November 2018
- Published by American Physical Society (APS) in Physical Review A
- Vol. 98 (5) , 053444
Photoionization cross sections of the and states of Rb in simultaneous magneto-optical trapping of Rb and HgWe report the measurement of the photoionization cross sections of the and states of in a two-species Hg and Rb magneto-optical trap (MOT) by the cooling laser for Hg. The photoionization cross sections of Rb in the and states at 253.7 nm are determined to be and , respectively. To measure the and state fractions in the MOT we detected the photoionization rate of the state by an additional 401.5 nm laser. The photoionization cross section of Rb in the state at 401.5 nm is determined to be .- 29 November 2018
- Published by American Physical Society (APS) in Physical Review A
- Vol. 98 (5) , 053444
Photoionization cross sections of the and states of Rb in simultaneous magneto-optical trapping of Rb and HgWe report the measurement of the photoionization cross sections of the and states of in a two-species Hg and Rb magneto-optical trap (MOT) by the cooling laser for Hg. The photoionization cross sections of Rb in the and states at 253.7 nm are determined to be and , respectively. To measure the and state fractions in the MOT we detected the photoionization rate of the state by an additional 401.5 nm laser. The photoionization cross section of Rb in the state at 401.5 nm is determined to be .- 27 April 2018
- Published by American Physical Society (APS) in Physical Review A
- Vol. 97 (4) , 043861
Berry phase in controlled light propagation and storage
It is shown that during light storage in an atomic medium in the configuration, with not only the amplitude of the control field but also its phase changing adiabatically, a photon gains a Berry (geometric) phase. In the case of the tripod configuration with two probe fields the Berry phase is replaced by a matrix. The probe fields are shown to be superpositions of two modes, each of them being characterized not only by its own velocity but also by its own Berry phase. If after light storage photons are released backwards, the contributions of the two modes interfere and the distribution of the outgoing photons can be steered by changing the difference between the Berry phases of the modes, due to the choice of the control field at the storage and release stages. In particular, one can turn a single photon of one of the probe fields into a photon of the other field or essentially modify coherent states of the incoming pulses.- 27 April 2018
- Published by American Physical Society (APS) in Physical Review A
- Vol. 97 (4) , 043861
Berry phase in controlled light propagation and storage
It is shown that during light storage in an atomic medium in the configuration, with not only the amplitude of the control field but also its phase changing adiabatically, a photon gains a Berry (geometric) phase. In the case of the tripod configuration with two probe fields the Berry phase is replaced by a matrix. The probe fields are shown to be superpositions of two modes, each of them being characterized not only by its own velocity but also by its own Berry phase. If after light storage photons are released backwards, the contributions of the two modes interfere and the distribution of the outgoing photons can be steered by changing the difference between the Berry phases of the modes, due to the choice of the control field at the storage and release stages. In particular, one can turn a single photon of one of the probe fields into a photon of the other field or essentially modify coherent states of the incoming pulses.- 6 December 2017
- Published by American Physical Society (APS) in Physical Review A
- Vol. 96 (6) , 063809
Three-photon interference with stored light
We present the concept of a realization of three-photon interference based on the procedure of light storage and release. Three probe photons are stored in an atomic medium in the tetrapod configuration. The medium irradiated by three control fields is shown to act as a flexible tritter. By changing the control fields applied at three stages of the photons' release, one can regulate the probabilities of obtaining various numbers of photons at each stage. Some of the signal coincidence probabilities can be made equal to zero, which is a generalization of the Hong-Ou-Mandel effect. The interference is demonstrated to gradually disappear for an increasing degree of the photons' distinguishability.
- 6 December 2017
- Published by American Physical Society (APS) in Physical Review A
- Vol. 96 (6) , 063809
Three-photon interference with stored light
We present the concept of a realization of three-photon interference based on the procedure of light storage and release. Three probe photons are stored in an atomic medium in the tetrapod configuration. The medium irradiated by three control fields is shown to act as a flexible tritter. By changing the control fields applied at three stages of the photons' release, one can regulate the probabilities of obtaining various numbers of photons at each stage. Some of the signal coincidence probabilities can be made equal to zero, which is a generalization of the Hong-Ou-Mandel effect. The interference is demonstrated to gradually disappear for an increasing degree of the photons' distinguishability.
- 28 March 2017
- Published by American Physical Society (APS) in Physical Review A
- Vol. 95 (3) , 033836
Double two-photon coalescence in a controlled propagation
The propagation, storage, and release of two quantized light fields in an optically dressed atomic medium in the tripod configuration are studied. Using the formalism of spinor dark-state polaritons, the probabilities are obtained of finding outgoing photons of two possible localizations and two possible types, i.e., having different frequencies or polarizations. An additional interaction at the storage stage is applied which modifies the atomic coherences due to the stored photons; this results in a modification of the states of the outgoing photons. The conditions are examined for the photons' spatial and type coalescence typical of the Hong-Ou-Mandel effect, i.e., a zero probability of finding the outgoing photons having not only different localizations but also types. These results can possibly be observed in rubidium vapors.
- 28 March 2017
- Published by American Physical Society (APS) in Physical Review A
- Vol. 95 (3) , 033836
Double two-photon coalescence in a controlled propagation
The propagation, storage, and release of two quantized light fields in an optically dressed atomic medium in the tripod configuration are studied. Using the formalism of spinor dark-state polaritons, the probabilities are obtained of finding outgoing photons of two possible localizations and two possible types, i.e., having different frequencies or polarizations. An additional interaction at the storage stage is applied which modifies the atomic coherences due to the stored photons; this results in a modification of the states of the outgoing photons. The conditions are examined for the photons' spatial and type coalescence typical of the Hong-Ou-Mandel effect, i.e., a zero probability of finding the outgoing photons having not only different localizations but also types. These results can possibly be observed in rubidium vapors.
- 24 June 2016
- Published by Optica Publishing Group in Journal of the Optical Society of America B
- Vol. 33 (7) , 1529-1537
Laser pulse propagation in a medium optically dressed by a phase-modulated field
Pulse propagation is studied in an atomic medium in the configuration with the control field having a periodically varying phase (chirp). Numerical calculations of a probe-pulse shape have been performed and the results are compared with those for an approximate model neglecting absorption and nonadiabatic effects. It is shown that transparency occurs for probe pulses having a sufficiently narrow envelope and an appropriately suited chirp. For other chirped probe pulses the evolution of their spectra along a sample is studied. Using a projection method, one can divide a pulse into two components: one for which the medium is transparent and the remaining one for which it is opaque.- 24 June 2016
- Published by Optica Publishing Group in Journal of the Optical Society of America B
- Vol. 33 (7) , 1529-1537
Laser pulse propagation in a medium optically dressed by a phase-modulated field
Pulse propagation is studied in an atomic medium in the configuration with the control field having a periodically varying phase (chirp). Numerical calculations of a probe-pulse shape have been performed and the results are compared with those for an approximate model neglecting absorption and nonadiabatic effects. It is shown that transparency occurs for probe pulses having a sufficiently narrow envelope and an appropriately suited chirp. For other chirped probe pulses the evolution of their spectra along a sample is studied. Using a projection method, one can divide a pulse into two components: one for which the medium is transparent and the remaining one for which it is opaque.- Open Access
Pulse propagation in a medium optically dressed by a phase-modulated field
Pulse propagation is studied in an EIT medium with the control field having a periodically varying phase (chirp). Based both on numerical calculations and on an approximate approach neglecting absorption and nonadiabatic effects, it is shown that transparency occurs for probe pulses having a sufficiently narrow envelope and an appropriately suited chirp. For other chirped pulses the evolution of their spectra along a sample is studied. Using a projection method one can divide a pulse into a part for which the medium is transparent and a rest for which it is opaque.
Open AccessPulse propagation in a medium optically dressed by a phase-modulated field
Pulse propagation is studied in an EIT medium with the control field having a periodically varying phase (chirp). Based both on numerical calculations and on an approximate approach neglecting absorption and nonadiabatic effects, it is shown that transparency occurs for probe pulses having a sufficiently narrow envelope and an appropriately suited chirp. For other chirped pulses the evolution of their spectra along a sample is studied. Using a projection method one can divide a pulse into a part for which the medium is transparent and a rest for which it is opaque.
- 26 May 2015
- Published by Optica Publishing Group in Journal of the Optical Society of America B
- Vol. 32 (6) , 1229
Pulse propagation in a medium optically dressed by three fields forming a triangular loop configuration
A probe pulse propagation is examined in a medium irradiated by three control fields which constitute a triangular loop system being, in general, out of resonance. As a consequence, the probe field interacts with the medium dressed in a time-dependent way. Coupled equations for the Floquet components of the probe field are written and solved by diagonalizing the coupling matrix. Examples of numerical solutions are presented and discussed.
- 26 May 2015
- Published by Optica Publishing Group in Journal of the Optical Society of America B
- Vol. 32 (6) , 1229
Pulse propagation in a medium optically dressed by three fields forming a triangular loop configuration
A probe pulse propagation is examined in a medium irradiated by three control fields which constitute a triangular loop system being, in general, out of resonance. As a consequence, the probe field interacts with the medium dressed in a time-dependent way. Coupled equations for the Floquet components of the probe field are written and solved by diagonalizing the coupling matrix. Examples of numerical solutions are presented and discussed.
- 6 November 2014
- Published by Optica Publishing Group in Journal of the Optical Society of America B
- Vol. 31 (12) , 2965
Spectra of pulses propagating in atomic media in the closed double ? configuration
Simultaneous propagation of two probe pulses in a medium of four-level atoms irradiated by three control fields is studied. The double Λ configuration has been closed by a fifth field, coupling the lower levels. It is shown that the propagation can be described in terms of four modes characterized by particular effective susceptibilities, which have absorption or gain peaks and transparency windows. For incoming one-peak pulses, multipeak spectra are built during the propagation including a few components of well-defined frequencies. They evolve along the sample with some of their spectral components being transmitted, absorbed, or amplified.
- 6 November 2014
- Published by Optica Publishing Group in Journal of the Optical Society of America B
- Vol. 31 (12) , 2965
Spectra of pulses propagating in atomic media in the closed double ? configuration
Simultaneous propagation of two probe pulses in a medium of four-level atoms irradiated by three control fields is studied. The double Λ configuration has been closed by a fifth field, coupling the lower levels. It is shown that the propagation can be described in terms of four modes characterized by particular effective susceptibilities, which have absorption or gain peaks and transparency windows. For incoming one-peak pulses, multipeak spectra are built during the propagation including a few components of well-defined frequencies. They evolve along the sample with some of their spectral components being transmitted, absorbed, or amplified.
- 10 May 2013
- Published by Optica Publishing Group in Journal of the Optical Society of America B
- Vol. 30 (6) , 1517
Pulse propagation in atomic media in the triangular configuration
Weak probe-pulse propagation is studied in a three-level atomic system irradiated by a strong control laser field and a strong microwave field in the closed-loop triangular (Δ) configuration. In addition to the direct absorption channel, a second channel is activated in which a probe photon’s absorption is replaced by its emission accompanied by an absorption of two control and two microwave photons. The pulse can be considered a superposition of two components, each of which experiences a separated effective susceptibility, exhibiting its absorption/gain windows. The evolution of the pulse spectrum in space and the pulse evolution in space–time are discussed. In particular it is shown that the number and positions of the spectrum peaks change and the pulse exhibits beats. In addition to the propagating field, a stationary light generated by the sample is also discussed.
- 10 May 2013
- Published by Optica Publishing Group in Journal of the Optical Society of America B
- Vol. 30 (6) , 1517
Pulse propagation in atomic media in the triangular configuration
Weak probe-pulse propagation is studied in a three-level atomic system irradiated by a strong control laser field and a strong microwave field in the closed-loop triangular (Δ) configuration. In addition to the direct absorption channel, a second channel is activated in which a probe photon’s absorption is replaced by its emission accompanied by an absorption of two control and two microwave photons. The pulse can be considered a superposition of two components, each of which experiences a separated effective susceptibility, exhibiting its absorption/gain windows. The evolution of the pulse spectrum in space and the pulse evolution in space–time are discussed. In particular it is shown that the number and positions of the spectrum peaks change and the pulse exhibits beats. In addition to the propagating field, a stationary light generated by the sample is also discussed.
- 1 May 2012
- Published by Elsevier in Optics Communications
- Vol. 285 (9) , 2392-2396
Light storage in a tripod medium as a basis for logical operations
- 1 May 2012
- Published by Elsevier in Optics Communications
- Vol. 285 (9) , 2392-2396
Light storage in a tripod medium as a basis for logical operations