Yu. V. Krasnikova
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
Research Interests
Yu. V. Krasnikova has a total of 60 co-authors. Here are the top co-authors by number of shared publications:
- Vasiliy N. Glazkov
P.L. Kapitza Institute for Physical Problems RAS 119334 Moscow Russia
7 shared publications A. Zheludev
Laboratory for Solid State Physics ETH Zurich 8093 Zürich Switzerland
5 shared publications- Kirill Yu. Povarov
Helmholtz-Zentrum Dresden-Rossendorf
3 shared publications V. N. Glazkov
P. L. Kapitza Institute for Physical Problems RAS Kosygina 2 119334 Moscow Russia
3 shared publicationsA Zheludev
Neutron Scattering and Magnetism, Laboratory for Solid State Physics, ETH Zürich, 8006 Zürich, Switzerland
2 shared publicationsA. Ponomaryov
HLD-EMFL) Dresden High Magnetic Field Laboratory ( Helmholtz-Zentrum Dresden -Rossendorf D-01328 Dresden Germany
2 shared publications
Latest Publications
- 6 March 2026
- Published by American Physical Society (APS) in Physical Review B
- Vol. 113 (13)
Experimental observation of short-range magnetic correlations in amorphous Nb 2 O 5 and Ta 2 O 5 thin films
- 6 March 2026
- Published by American Physical Society (APS) in Physical Review B
- Vol. 113 (13)
Experimental observation of short-range magnetic correlations in amorphous Nb 2 O 5 and Ta 2 O 5 thin films
- 9 July 2020
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 125 (2) , 027204
Anisotropy-Induced Soliton Excitation in Magnetized Strong-Rung Spin Ladders
We report low temperature electron spin resonance experimental and theoretical studies of an archetype strong-rung spin ladder material . Unexpected dynamics is detected deep in the Tomonaga-Luttinger spin liquid regime. Close to the point where the system is half-magnetized (and believed to be equivalent to a gapless easy plane chain in zero field) we observed orientation-dependent spin gap and anomalous -factor values. Field theoretical analysis demonstrates that the observed low-energy excitation modes in magnetized are solitonic excitations caused by Dzyaloshinskii-Moriya interaction presence.- 9 July 2020
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 125 (2) , 027204
Anisotropy-Induced Soliton Excitation in Magnetized Strong-Rung Spin Ladders
We report low temperature electron spin resonance experimental and theoretical studies of an archetype strong-rung spin ladder material . Unexpected dynamics is detected deep in the Tomonaga-Luttinger spin liquid regime. Close to the point where the system is half-magnetized (and believed to be equivalent to a gapless easy plane chain in zero field) we observed orientation-dependent spin gap and anomalous -factor values. Field theoretical analysis demonstrates that the observed low-energy excitation modes in magnetized are solitonic excitations caused by Dzyaloshinskii-Moriya interaction presence.- Open Access
Anisotropy-induced soliton excitation in magnetized strong-rung spin ladders
We report low temperature electron spin resonance experimental and theoretical studies of an archetype $S=1/2$ strong-rung spin ladder material (C$_{5}$H$_{12}$N)$_{2}$CuBr$_{4}$. Unexpected dynamics is detected deep in the Tomonaga-Luttinger spin liquid regime. Close to the point where the system is half-magnetized (and believed to be equivalent to a gapless easy plane chain in zero field) we observed orientation-dependent spin gap and anomalous $g$-factor values. Field theoretical analysis demonstrates that the observed low-energy excitation modes in magnetized (C$_{5}$H$_{12}$N)$_{2}$CuBr$_{4}$ are solitonic excitations caused by Dzyaloshinskii-Moriya interaction presence.Open AccessAnisotropy-induced soliton excitation in magnetized strong-rung spin ladders
We report low temperature electron spin resonance experimental and theoretical studies of an archetype $S=1/2$ strong-rung spin ladder material (C$_{5}$H$_{12}$N)$_{2}$CuBr$_{4}$. Unexpected dynamics is detected deep in the Tomonaga-Luttinger spin liquid regime. Close to the point where the system is half-magnetized (and believed to be equivalent to a gapless easy plane chain in zero field) we observed orientation-dependent spin gap and anomalous $g$-factor values. Field theoretical analysis demonstrates that the observed low-energy excitation modes in magnetized (C$_{5}$H$_{12}$N)$_{2}$CuBr$_{4}$ are solitonic excitations caused by Dzyaloshinskii-Moriya interaction presence. - Open Access
Electron spin resonance study of spin relaxation in the strong-leg spin ladder with nonmagnetic dilution
We have studied electron spin resonance (ESR) absorption spectra for the nonmagnetically diluted strong-leg spin ladder magnet ({C}$_{7}$H$_{10}$N)$_{2}$Cu$_{(1-x)}$Zn$_{x}$Br$_{4}$ (abbreviated as DIMPY) down to 450 mK. Formation of the clusters with non-zero net magnetization is confirmed; the cluster-cluster interaction is evidenced by the concentration dependence of ESR absorption. High-temperature spin-relaxation time was found to increase with non-magnetic dilution. The ESR linewidth analysis proves that the Dzyaloshinskii-Moriya (DM) interaction remains the dominant spin-relaxation channel in diluted DIMPY. Experimental data indicate that the dilution results in the weakening of the effective DM interaction, which can be interpreted as total suppression of DM interaction in the close vicinity of impurity atom.
Open AccessElectron spin resonance study of spin relaxation in the strong-leg spin ladder with nonmagnetic dilution
We have studied electron spin resonance (ESR) absorption spectra for the nonmagnetically diluted strong-leg spin ladder magnet ({C}$_{7}$H$_{10}$N)$_{2}$Cu$_{(1-x)}$Zn$_{x}$Br$_{4}$ (abbreviated as DIMPY) down to 450 mK. Formation of the clusters with non-zero net magnetization is confirmed; the cluster-cluster interaction is evidenced by the concentration dependence of ESR absorption. High-temperature spin-relaxation time was found to increase with non-magnetic dilution. The ESR linewidth analysis proves that the Dzyaloshinskii-Moriya (DM) interaction remains the dominant spin-relaxation channel in diluted DIMPY. Experimental data indicate that the dilution results in the weakening of the effective DM interaction, which can be interpreted as total suppression of DM interaction in the close vicinity of impurity atom.
- 31 October 2019
- Published by American Physical Society (APS) in Physical Review B
- Vol. 100 (14) , 144446
Electron spin resonance study of spin relaxation in the strong-leg spin ladder with nonmagnetic dilution
We have studied electron spin resonance (ESR) absorption spectra for the nonmagnetically diluted strong-leg spin ladder magnet ( (abbreviated as DIMPY) down to 450 mK. Formation of the clusters with nonzero net magnetization is confirmed; the cluster-cluster interaction is evidenced by the concentration dependence of ESR absorption. High-temperature spin-relaxation time was found to increase with nonmagnetic dilution. The ESR linewidth analysis proves that the Dzyaloshinskii-Moriya (DM) interaction remains the dominant spin-relaxation channel in diluted DIMPY. Experimental data indicate that the dilution results in the weakening of the effective DM interaction, which can be interpreted as total suppression of DM interaction in the close vicinity of impurity atom.- 31 October 2019
- Published by American Physical Society (APS) in Physical Review B
- Vol. 100 (14) , 144446
Electron spin resonance study of spin relaxation in the strong-leg spin ladder with nonmagnetic dilution
We have studied electron spin resonance (ESR) absorption spectra for the nonmagnetically diluted strong-leg spin ladder magnet ( (abbreviated as DIMPY) down to 450 mK. Formation of the clusters with nonzero net magnetization is confirmed; the cluster-cluster interaction is evidenced by the concentration dependence of ESR absorption. High-temperature spin-relaxation time was found to increase with nonmagnetic dilution. The ESR linewidth analysis proves that the Dzyaloshinskii-Moriya (DM) interaction remains the dominant spin-relaxation channel in diluted DIMPY. Experimental data indicate that the dilution results in the weakening of the effective DM interaction, which can be interpreted as total suppression of DM interaction in the close vicinity of impurity atom.- Open Access
- 1 March 2018
- Published by IOP Publishing in Journal of Physics: Conference Series
- Vol. 969 (1) , 012113
Low temperature ESR in spin ladder (C7H10N)2Cu(1−x)Zn x Br4
Spin-gap magnet (C7H10N)2Cu(1 − x )Zn x Br4 (DIMPY) is an example of a strong-leg spin ladder. We report here the results of the ESR study of pure and diamagnetically diluted DIMPY. ESR study of the pure system (x=0) revealed that the spin dynamics of DIMPY is affected by uniform Dzyaloshinskii-Moriya (DM) interaction. We observe narrowing of the ESR absorption line in diamagnetically diluted DIMPY pointing to suppression of DM channel of spin relaxation by doping.
- 1 March 2018
- Published by IOP Publishing in Journal of Physics: Conference Series
- Vol. 969 (1) , 012113
Open AccessLow temperature ESR in spin ladder (C7H10N)2Cu(1−x)Zn x Br4
Spin-gap magnet (C7H10N)2Cu(1 − x )Zn x Br4 (DIMPY) is an example of a strong-leg spin ladder. We report here the results of the ESR study of pure and diamagnetically diluted DIMPY. ESR study of the pure system (x=0) revealed that the spin dynamics of DIMPY is affected by uniform Dzyaloshinskii-Moriya (DM) interaction. We observe narrowing of the ESR absorption line in diamagnetically diluted DIMPY pointing to suppression of DM channel of spin relaxation by doping.
- Open Access
- 1 September 2017
- Published by Pleiades Publishing Ltd in Journal of Experimental and Theoretical Physics
- Vol. 125 (3) , 476-479
Experimental study of antiferromagnetic resonance in noncollinear antiferromagnetic Mn3Al2Ge3O12
We have measured antiferromagnetic resonance (AFMR) frequency-field dependences for aluminum–manganese garnet Mn3Al2Ge3O12 at frequencies from 1 to 125 GHz and fields up to 6 T. There are three AFMR modes for all orientations, their zero field gaps are about 40 and 70 GHz. Andreev–Marchenko hydrodynamic theory [7] well describes experimental frequency–field dependences. We have observed hysteresis of resonance absorption as well as history dependence of resonance absorption near gap frequencies below 10 kOe in all three measured field orientations, which are supposedly due to the sample domain structure. Observation of the AFMR signal at the frequencies from 1 to 5 GHz allows to estimate repulsion of nuclear and electron modes of spin precession in the vicinity of spin-reorientation transition at H || [100].
- 1 September 2017
- Published by Pleiades Publishing Ltd in Journal of Experimental and Theoretical Physics
- Vol. 125 (3) , 476-479
Open AccessExperimental study of antiferromagnetic resonance in noncollinear antiferromagnetic Mn3Al2Ge3O12
We have measured antiferromagnetic resonance (AFMR) frequency-field dependences for aluminum–manganese garnet Mn3Al2Ge3O12 at frequencies from 1 to 125 GHz and fields up to 6 T. There are three AFMR modes for all orientations, their zero field gaps are about 40 and 70 GHz. Andreev–Marchenko hydrodynamic theory [7] well describes experimental frequency–field dependences. We have observed hysteresis of resonance absorption as well as history dependence of resonance absorption near gap frequencies below 10 kOe in all three measured field orientations, which are supposedly due to the sample domain structure. Observation of the AFMR signal at the frequencies from 1 to 5 GHz allows to estimate repulsion of nuclear and electron modes of spin precession in the vicinity of spin-reorientation transition at H || [100].
- Open Access
Experimental study of antiferromagnetic resonance in noncollinear antiferromagnet Mn$_{3}$Al$_{2}$Ge$_{3}$O$_{12}$
We have measured antiferromagnetic resonance (AFMR) frequency-field dependences for aluminum-manganese garnet Mn$_{3}$Al$_{2}$Ge$_{3}$O$_{12}$ at frequencies from 1 to 125 GHz and at the fields up to 60 kOe. Three AFMR modes were observed for all orientations, their zero field gaps are about 40 and 70 GHz. Andreev-Marchenko hydrodynamic theory [Sov. Phys. Usp. 130, 39 (1980)] well describes experimental frequency-field dependences. We have observed hysteresis of resonance absorption as well as history dependence of resonance absorption near gap frequencies below 10 kOe in all three measured field orientations, which are supposedly due to the sample domain structure. Observation of the AFMR signal at the frequencies from 1 to 5 GHz allows to estimate repulsion of nuclear and electron modes of spin precession in the vicinity of spin-reorientation transition at H||[100].
Open AccessExperimental study of antiferromagnetic resonance in noncollinear antiferromagnet Mn$_{3}$Al$_{2}$Ge$_{3}$O$_{12}$
We have measured antiferromagnetic resonance (AFMR) frequency-field dependences for aluminum-manganese garnet Mn$_{3}$Al$_{2}$Ge$_{3}$O$_{12}$ at frequencies from 1 to 125 GHz and at the fields up to 60 kOe. Three AFMR modes were observed for all orientations, their zero field gaps are about 40 and 70 GHz. Andreev-Marchenko hydrodynamic theory [Sov. Phys. Usp. 130, 39 (1980)] well describes experimental frequency-field dependences. We have observed hysteresis of resonance absorption as well as history dependence of resonance absorption near gap frequencies below 10 kOe in all three measured field orientations, which are supposedly due to the sample domain structure. Observation of the AFMR signal at the frequencies from 1 to 5 GHz allows to estimate repulsion of nuclear and electron modes of spin precession in the vicinity of spin-reorientation transition at H||[100].
- 27 August 2016
- Published by Springer Nature in Applied Magnetic Resonance
- Vol. 47 (10) , 1069-1080
Numeric Calculation of Antiferromagnetic Resonance Frequencies for the Noncollinear Antiferromagnet
- 27 August 2016
- Published by Springer Nature in Applied Magnetic Resonance
- Vol. 47 (10) , 1069-1080
Numeric Calculation of Antiferromagnetic Resonance Frequencies for the Noncollinear Antiferromagnet