Sergei Kilin | Belarusian State University (original) (raw)
Papers by Sergei Kilin
Research in Optical Sciences, 2012
ABSTRACT We show that the stationary state of single-qubit laser is a phase-averaged nonlinear co... more ABSTRACT We show that the stationary state of single-qubit laser is a phase-averaged nonlinear coherent state, provide super convergent iterations method for its finding and investigate characteristic quantum properties of the state.
IOCN 2022
This article is an open access article distributed under the terms and conditions of the Creative... more This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY
Journal of Applied Spectroscopy, 2007
Optics letters, Jan 15, 2015
Differential optical detection of a magnetic resonance induced in nitrogen-vacancy (NV) centers i... more Differential optical detection of a magnetic resonance induced in nitrogen-vacancy (NV) centers in diamond is shown to enable a high-spatial-resolution room-temperature magnetic-field gradiometry on a fiber platform. An ultracompact design of this fiber-based solid-state magnetic gradiometer is achieved by integrating an NV-diamond magnetic sensor with a two-fiber opto-microwave interface, which couples NV centers to microwave and optical fields, used to resonantly drive and interrogate the spin of NV centers.
Progress in Optics
ABSTRACT
Physics, Chemistry and Application of Nanostructures, 2005
Technical Digest. 1998 EQEC. European Quantum Electronics Conference (Cat. No.98TH8326)
Coherent transient signals such as echoes, bee induction decay, nutation etc. are known to origin... more Coherent transient signals such as echoes, bee induction decay, nutation etc. are known to originate from coherent sunmation of individual signals from different members of ensemble with inhomogneour distribution of resonant frequencies. Recently, coherent tIBllsients on single molecules have been observed [I]. Physical ream? for these observations i s the jumps of a selected molecule within a distribution of possible resonant transition frequencies which are sampled sequentially during a long time of experiment by applying the exciting pulses repeatedly. Therefore, instead of conventional ensemble averaging in bulktrpe measurements, in the latter case the temporal averaging takes place over many individual transient experiments on B single molecule. We present here a theory to describe the fluorescence detected (FD) coherent transients an single quantum system having long-lived triplet-state. The system i s subjected to the cw laser field to excite the fluorercencc and to the pulsed microwave (MW) field to induce the coherent transient signals f" triplet substates which are monitored as the changes in the fluorescence intensity. Two kinds of objects are considered: (i) A chmophore molecule in low-temperature host organic matrix where the frequency distribution is naturally generated by hyperfine interactions of a photoexcited triplet electron spin with differently configurated proton spins of the molecule. Spectral jumps within the distribution in this case result h m the flip-flops of the proton spins during the molecule slay in B singlet manifold. (ii) A single nitrogen-vacancy (WV) defect center in diamond having triplet ground slate. In the latter case the frequency distribution is inherently absent but can be organized artificially by applying the external magnetic field of strength changing slowly during the time of repeated transient experiments. We have used a Etochastic approach to dexribe the triplet spin pure dephasing resulting boom frequency fluctuations U' induced by host-matrix nuclear spin dynamics [2]. Modeling the fluctuations U' by a sum of h' random telegraph (RT) processes with the same jump rate Y but different variences a. we construct M exaci set of equations for the density matrix of a moleculelcenter averaged over fluctuation U' histories. These equations incorporate the non-Markav effects such as suppression of dephasing by strong MW field. In the case Y >> k; , where k; are inlersydem crossing rates or the ground triplet substater lifetimes, the simple anslytical exgrersionr for the FD transients (Hahn echo, free induction decay, nutation) are obtained and compared with exact calculations within N RT processes model. Available expmimmtal data on FD nulalions and non-exponential Hahn echo at single pentacene molecules in crystalline p-terphenyl are fitted and the model characteristics Y = 30kHz, a = 85kHz (0' = za:) are determined. Analogous information is also presented for the dcpharing of the N-V centers. [ I ] 1. Wrachtrup, C. vonBorczyyskowski, J. Bernard, M. Orrit, R. Brow, Phys. Rev. Len., 71 (1993)3565;1. Chem. Phys., 100(1994)7182. 121 S. Ya. Kilin. A. P. Nirovtsev, P. R. Berman, 1. Wrachtrup. C . van Borczyskowski, Phys. Rev. B, 56 (1997) 24; Phys. Rev. B, submitted. QTuG65
SPIE Proceedings, 1998
ABSTRACT
Proceedings of 5th European Quantum Electronics Conference
2003 European Quantum Electronics Conference. EQEC 2003 (IEEE Cat No.03TH8665), 2003
ABSTRACT
Physical Review Letters, 1996
Suppression of quantum dynamical tunneling is predicted to occur when a laser field drives a tran... more Suppression of quantum dynamical tunneling is predicted to occur when a laser field drives a transition in an isolated, single molecule embedded in a host medium. [S0031-9007(96)00075-0]
Physical Review A, 2011
Entanglement represents an important resource for quantum information processing, but its generat... more Entanglement represents an important resource for quantum information processing, but its generation itself requires physical resources that are limited. We propose a scheme for generating a wide class of entangled qudit-type states of optical field modes at sites separated by noisy medium when only weak optical nonlinearities are available at both sites. The protocol is also based on exploiting a weak probe field, transmitted between the sites and used for generation of quantum correlations between two spatially separated field modes. The idea of probabilistic entanglement enhancement by measurement is discussed, and corresponding scheme for measuring the probe field state with linear optics and photodetectors not resolving photon numbers is proposed. It is shown that the protocol is applicable in the case when decoherence, limited efficiency and dark counts of photodetectors, and uncertainty of nonlinear coupling constants are present.
Physical Review A, 2001
We consider a special kind of correlation measurements in single-atom resonance fluorescence, whi... more We consider a special kind of correlation measurements in single-atom resonance fluorescence, which includes detection of a spectrally filtered photon followed by detection of an unfiltered photon. We relate the stationary normalized intensity correlation function measured in such a scheme to the reduced atomic state following detection of the filtered photon. In the limit of well separated spectral lines of the resonance fluorescence spectrum, we obtain the analytic expression for the reduced atomic state. We show that at resonance excitation, this state is inverted when the filter is tuned in between the central line and any of the sidebands. This effect is interpreted as a result of quantum interference between the complementary atomic radiative transitions giving rise to the detected photon. We propose to observe this effect in measuring the equal-time field correlation function of the filtered and unfiltered photons as a function of the filter resonance frequency.
Physical Review A, 2012
The stationary state of a single-atom (single-qubit) laser is shown to be a phase-averaged nonlin... more The stationary state of a single-atom (single-qubit) laser is shown to be a phase-averaged nonlinear coherent state-an eigenstate of specific deformed annihilation operator. The solution found for the stationary state is unique and valid for all regimes of the single-qubit laser operation. We have found the parametrization of the deformed annihilation operator which provides superconvergence in finding the stationary state by iteration. It is also shown that, contrary to the case of the usual laser with constant Einstein coefficients describing transition probabilities, for the single-atom laser the interaction-induced transition probabilities effectively depend on the field intensity.
Physical Review A, 1993
The effect of amplitude-phase multistability in the Dicke model inside a coherently driven cavity... more The effect of amplitude-phase multistability in the Dicke model inside a coherently driven cavity is discussed for the case of large Rabi frequencies and a small rate of atomic decay, compared with the decay of the cavity mode. The quantum and semiclassical interpretations of the predicted effect are given on the basis of the Tavis-Cummings model and a proposed model of weakly coupled harmonic oscillators. The analytical solution is obtained for a two-atom system. The possibility of observing amplitudephase multistability is also considered.
Physica B: Condensed Matter, 2001
Based on new spectroscopic information retrieved by experiments on individual Nitrogen-Vacancy (N... more Based on new spectroscopic information retrieved by experiments on individual Nitrogen-Vacancy (NV) defect centers in diamond, we introduced the five-level photophysical model of the center and demonstrate its applicability to describe consistently different experiments on single NV centers. The model takes into account the triplet-triplet character of the optical transition 3 A-3 E (637 nm) of the center and the presence of a metastable singlet state 1 A. Supposing optical excitation rates B T from spin substates T ¼ X; Y; Z of the ground 3 A state as well as the fluorescence emission rates A T to these substates to be different (B Z =B X E11; B X ¼ B Y while A Z =A X E18; A X ¼ A Y), we were able to fit consistently the experimental data obtained for green-laser-excited single NV centers at room-temperature: (i) lineshapes of fluorescence-detected magnetic resonance at 2.88 GHz in the ground 3 A state and their changes due to the strains in the diamond crystal, (ii) fluorescence saturation and (iii) photon antibunching/bunching in the fluorescence light emitted by a single NV center.
Research in Optical Sciences, 2012
ABSTRACT We show that the stationary state of single-qubit laser is a phase-averaged nonlinear co... more ABSTRACT We show that the stationary state of single-qubit laser is a phase-averaged nonlinear coherent state, provide super convergent iterations method for its finding and investigate characteristic quantum properties of the state.
IOCN 2022
This article is an open access article distributed under the terms and conditions of the Creative... more This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY
Journal of Applied Spectroscopy, 2007
Optics letters, Jan 15, 2015
Differential optical detection of a magnetic resonance induced in nitrogen-vacancy (NV) centers i... more Differential optical detection of a magnetic resonance induced in nitrogen-vacancy (NV) centers in diamond is shown to enable a high-spatial-resolution room-temperature magnetic-field gradiometry on a fiber platform. An ultracompact design of this fiber-based solid-state magnetic gradiometer is achieved by integrating an NV-diamond magnetic sensor with a two-fiber opto-microwave interface, which couples NV centers to microwave and optical fields, used to resonantly drive and interrogate the spin of NV centers.
Progress in Optics
ABSTRACT
Physics, Chemistry and Application of Nanostructures, 2005
Technical Digest. 1998 EQEC. European Quantum Electronics Conference (Cat. No.98TH8326)
Coherent transient signals such as echoes, bee induction decay, nutation etc. are known to origin... more Coherent transient signals such as echoes, bee induction decay, nutation etc. are known to originate from coherent sunmation of individual signals from different members of ensemble with inhomogneour distribution of resonant frequencies. Recently, coherent tIBllsients on single molecules have been observed [I]. Physical ream? for these observations i s the jumps of a selected molecule within a distribution of possible resonant transition frequencies which are sampled sequentially during a long time of experiment by applying the exciting pulses repeatedly. Therefore, instead of conventional ensemble averaging in bulktrpe measurements, in the latter case the temporal averaging takes place over many individual transient experiments on B single molecule. We present here a theory to describe the fluorescence detected (FD) coherent transients an single quantum system having long-lived triplet-state. The system i s subjected to the cw laser field to excite the fluorercencc and to the pulsed microwave (MW) field to induce the coherent transient signals f" triplet substates which are monitored as the changes in the fluorescence intensity. Two kinds of objects are considered: (i) A chmophore molecule in low-temperature host organic matrix where the frequency distribution is naturally generated by hyperfine interactions of a photoexcited triplet electron spin with differently configurated proton spins of the molecule. Spectral jumps within the distribution in this case result h m the flip-flops of the proton spins during the molecule slay in B singlet manifold. (ii) A single nitrogen-vacancy (WV) defect center in diamond having triplet ground slate. In the latter case the frequency distribution is inherently absent but can be organized artificially by applying the external magnetic field of strength changing slowly during the time of repeated transient experiments. We have used a Etochastic approach to dexribe the triplet spin pure dephasing resulting boom frequency fluctuations U' induced by host-matrix nuclear spin dynamics [2]. Modeling the fluctuations U' by a sum of h' random telegraph (RT) processes with the same jump rate Y but different variences a. we construct M exaci set of equations for the density matrix of a moleculelcenter averaged over fluctuation U' histories. These equations incorporate the non-Markav effects such as suppression of dephasing by strong MW field. In the case Y >> k; , where k; are inlersydem crossing rates or the ground triplet substater lifetimes, the simple anslytical exgrersionr for the FD transients (Hahn echo, free induction decay, nutation) are obtained and compared with exact calculations within N RT processes model. Available expmimmtal data on FD nulalions and non-exponential Hahn echo at single pentacene molecules in crystalline p-terphenyl are fitted and the model characteristics Y = 30kHz, a = 85kHz (0' = za:) are determined. Analogous information is also presented for the dcpharing of the N-V centers. [ I ] 1. Wrachtrup, C. vonBorczyyskowski, J. Bernard, M. Orrit, R. Brow, Phys. Rev. Len., 71 (1993)3565;1. Chem. Phys., 100(1994)7182. 121 S. Ya. Kilin. A. P. Nirovtsev, P. R. Berman, 1. Wrachtrup. C . van Borczyskowski, Phys. Rev. B, 56 (1997) 24; Phys. Rev. B, submitted. QTuG65
SPIE Proceedings, 1998
ABSTRACT
Proceedings of 5th European Quantum Electronics Conference
2003 European Quantum Electronics Conference. EQEC 2003 (IEEE Cat No.03TH8665), 2003
ABSTRACT
Physical Review Letters, 1996
Suppression of quantum dynamical tunneling is predicted to occur when a laser field drives a tran... more Suppression of quantum dynamical tunneling is predicted to occur when a laser field drives a transition in an isolated, single molecule embedded in a host medium. [S0031-9007(96)00075-0]
Physical Review A, 2011
Entanglement represents an important resource for quantum information processing, but its generat... more Entanglement represents an important resource for quantum information processing, but its generation itself requires physical resources that are limited. We propose a scheme for generating a wide class of entangled qudit-type states of optical field modes at sites separated by noisy medium when only weak optical nonlinearities are available at both sites. The protocol is also based on exploiting a weak probe field, transmitted between the sites and used for generation of quantum correlations between two spatially separated field modes. The idea of probabilistic entanglement enhancement by measurement is discussed, and corresponding scheme for measuring the probe field state with linear optics and photodetectors not resolving photon numbers is proposed. It is shown that the protocol is applicable in the case when decoherence, limited efficiency and dark counts of photodetectors, and uncertainty of nonlinear coupling constants are present.
Physical Review A, 2001
We consider a special kind of correlation measurements in single-atom resonance fluorescence, whi... more We consider a special kind of correlation measurements in single-atom resonance fluorescence, which includes detection of a spectrally filtered photon followed by detection of an unfiltered photon. We relate the stationary normalized intensity correlation function measured in such a scheme to the reduced atomic state following detection of the filtered photon. In the limit of well separated spectral lines of the resonance fluorescence spectrum, we obtain the analytic expression for the reduced atomic state. We show that at resonance excitation, this state is inverted when the filter is tuned in between the central line and any of the sidebands. This effect is interpreted as a result of quantum interference between the complementary atomic radiative transitions giving rise to the detected photon. We propose to observe this effect in measuring the equal-time field correlation function of the filtered and unfiltered photons as a function of the filter resonance frequency.
Physical Review A, 2012
The stationary state of a single-atom (single-qubit) laser is shown to be a phase-averaged nonlin... more The stationary state of a single-atom (single-qubit) laser is shown to be a phase-averaged nonlinear coherent state-an eigenstate of specific deformed annihilation operator. The solution found for the stationary state is unique and valid for all regimes of the single-qubit laser operation. We have found the parametrization of the deformed annihilation operator which provides superconvergence in finding the stationary state by iteration. It is also shown that, contrary to the case of the usual laser with constant Einstein coefficients describing transition probabilities, for the single-atom laser the interaction-induced transition probabilities effectively depend on the field intensity.
Physical Review A, 1993
The effect of amplitude-phase multistability in the Dicke model inside a coherently driven cavity... more The effect of amplitude-phase multistability in the Dicke model inside a coherently driven cavity is discussed for the case of large Rabi frequencies and a small rate of atomic decay, compared with the decay of the cavity mode. The quantum and semiclassical interpretations of the predicted effect are given on the basis of the Tavis-Cummings model and a proposed model of weakly coupled harmonic oscillators. The analytical solution is obtained for a two-atom system. The possibility of observing amplitudephase multistability is also considered.
Physica B: Condensed Matter, 2001
Based on new spectroscopic information retrieved by experiments on individual Nitrogen-Vacancy (N... more Based on new spectroscopic information retrieved by experiments on individual Nitrogen-Vacancy (NV) defect centers in diamond, we introduced the five-level photophysical model of the center and demonstrate its applicability to describe consistently different experiments on single NV centers. The model takes into account the triplet-triplet character of the optical transition 3 A-3 E (637 nm) of the center and the presence of a metastable singlet state 1 A. Supposing optical excitation rates B T from spin substates T ¼ X; Y; Z of the ground 3 A state as well as the fluorescence emission rates A T to these substates to be different (B Z =B X E11; B X ¼ B Y while A Z =A X E18; A X ¼ A Y), we were able to fit consistently the experimental data obtained for green-laser-excited single NV centers at room-temperature: (i) lineshapes of fluorescence-detected magnetic resonance at 2.88 GHz in the ground 3 A state and their changes due to the strains in the diamond crystal, (ii) fluorescence saturation and (iii) photon antibunching/bunching in the fluorescence light emitted by a single NV center.