11 research outputs found
Magnetic field dependence of the neutron spin resonance in CeB6
In zero magnetic field, the famous neutron spin resonance in the f-electron
superconductor CeCoIn5 is similar to the recently discovered exciton peak in
the non-superconducting CeB6. Magnetic field splits the resonance in CeCoIn5
into two components, indicating that it is a doublet. Here we employ inelastic
neutron scattering (INS) to scrutinize the field dependence of spin
fluctuations in CeB6. The exciton shows a markedly different behavior without
any field splitting. Instead, we observe a second field-induced magnon whose
energy increases with field. At the ferromagnetic zone center, however, we find
only a single mode with a non-monotonic field dependence. At low fields, it is
initially suppressed to zero together with the antiferromagnetic order
parameter, but then reappears at higher fields inside the hidden-order phase,
following the energy of an electron spin resonance (ESR). This is a unique
example of a ferromagnetic resonance in a heavy-fermion metal seen by both ESR
and INS consistently over a broad range of magnetic fields.Comment: 7 pages, 6 figures including one animation, accepted to Phys. Rev.
ΠΠΠΠΠΠΠΠΠΠ― ΠΠΠΠΠΠΠΠΠ― Π‘ΠΠ‘Π’ΠΠΠ ΠΠΠ ΠΠΠΠΠ Π‘Π ΠΠ§ΠΠΠ Π ΠΠΠΠΠΠΠ ΠΠΠΠΠΠΠ ΠΠΠΠΠ’ΠΠ¦ΠΠ ΠΠ ΠΠΠΠΠΠΠ Π ΠΠΠ‘Π’Π ΠΠΠΠΠ¬ΠΠ«Π ΠΠΠΠΠΠΠ‘Π’ΠΠΠ―Π. ΠΠΠ Π‘ΠΠΠΠ’ΠΠΠ« ΠΠΠΠΠΠ§ΠΠ‘ΠΠΠΠ ΠΠ ΠΠΠΠΠΠΠΠ― ΠΠΠΠΠΠΠΠ«Π₯ ΠΠΠΠ’ΠΠΠΠ
It has been well established that opioid peptides (OPs) affect various hormonal systems. Opioids exhibit stress-limiting and gastro-protective effects in stressed animals, acting via ΞΌ- and Ξ΄-opioid receptors (OR). Peripheral ΞΌ-OR stimulation by endogenous and exogenous opioids increases cardiac tolerance to pathological consequences of stress. Enhancement of prostacyclin synthesis, decrease of thromboxane production as well as suppression of lipid peroxidation can be directly responsible for cardioprotective effects of OPs in stressed animals. Adaptive responses are accompanied by increased OP levels in blood and tissues. Reduction of ventricular arrhythmias induced by repeated short-term immobilization stress is mediated via ΞΌ-OR stimulation by endogenous opioids, while Ξ΄-OR account for an antiarrhythmic effect of adaptation to chronic intermittent hypobaric hypoxia. The mechanism of infarct size-limiting effect of continuous normobaric hypoxia involves both ΞΌ- and Ξ΄-OR stimulation. Peptide OR agonists can be considered in future clinical practice for treatment of withdrawal syndrome, stress-related cardiac disease or myocardial injury caused by ischemia-reperfusion insult.Β Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ ΠΎΠΏΠΈΠΎΠΈΠ΄Π½ΡΠ΅ ΠΏΠ΅ΠΏΡΠΈΠ΄Ρ (ΠΠ) Π²Π»ΠΈΡΡΡ Π½Π° ΡΠ°Π·Π»ΠΈΡΠ½ΡΠ΅ Π³ΠΎΡΠΌΠΎΠ½Π°Π»ΡΠ½ΡΠ΅ ΡΠΈΡΡΠ΅ΠΌΡ. ΠΠΏΠΈΠΎΠΈΠ΄Ρ ΠΎΠΊΠ°Π·ΡΠ²Π°ΡΡ ΡΡΡΠ΅ΡΡ-Π»ΠΈΠΌΠΈΡΠΈΡΡΡΡΠΈΠΉ ΠΈ Π³Π°ΡΡΡΠΎΠΏΡΠΎΡΠ΅ΠΊΡΠΎΡΠ½ΡΠΉ ΡΡΡΠ΅ΠΊΡ Π½Π° ΡΡΡΠ΅ΡΡΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΠΎΡΠΎΠ±Π΅ΠΉ, Π΄Π΅ΠΉΡΡΠ²ΡΡ Π½Π° ΞΌ- ΠΈ Ξ΄-ΠΎΠΏΠΈΠΎΠΈΠ΄Π½ΡΠ΅ ΡΠ΅ΡΠ΅ΠΏΡΠΎΡΡ (ΠΠ ). Π‘ΡΠΈΠΌΡΠ»ΡΡΠΈΡ ΠΏΠ΅ΡΠΈΡΠ΅ΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΞΌ-ΠΠ ΡΠ½Π΄ΠΎ- ΠΈ ΡΠΊΠ·ΠΎΠ³Π΅Π½Π½ΡΠΌΠΈ ΠΎΠΏΠΈΠΎΠΈΠ΄Π°ΠΌΠΈ ΡΠΏΠΎΡΠΎΠ±ΡΡΠ²ΡΠ΅Ρ ΠΏΠΎΠ²ΡΡΠ΅Π½ΠΈΡ ΡΠΎΠ»Π΅ΡΠ°Π½ΡΠ½ΠΎΡΡΠΈ ΡΠ΅ΡΠ΄ΡΠ° ΠΊ ΠΏΠ°ΡΠΎΠ³Π΅Π½Π½ΠΎΠΌΡ Π΄Π΅ΠΉΡΡΠ²ΠΈΡ ΡΡΡΠ΅ΡΡΠ°. Π£ΡΠΈΠ»Π΅Π½ΠΈΠ΅ ΡΠΈΠ½ΡΠ΅Π·Π° ΠΏΡΠΎΡΡΠ°ΡΠΈΠΊΠ»ΠΈΠ½Π°, ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΠ΅ ΠΏΡΠΎΠ΄ΡΠΊΡΠΈΠΈ ΡΡΠΎΠΌΠ±ΠΎΠΊΡΠ°Π½Π°, Π° ΡΠ°ΠΊΠΆΠ΅ ΠΏΠΎΠ΄Π°Π²Π»Π΅Π½ΠΈΠ΅ ΠΏΡΠΎΡΠ΅ΡΡΠΎΠ² ΠΏΠ΅ΡΠΎΠΊΡΠΈΠ΄Π½ΠΎΠ³ΠΎ ΠΎΠΊΠΈΡΠ»Π΅Π½ΠΈΡ Π»ΠΈΠΏΠΈΠ΄ΠΎΠ² (ΠΠΠ) ΠΌΠΎΠ³ΡΡ ΠΈΠΌΠ΅ΡΡ ΠΏΡΡΠΌΠΎΠ΅ ΠΎΡΠ½ΠΎΡΠ΅Π½ΠΈΠ΅ ΠΊ ΠΊΠ°ΡΠ΄ΠΈΠΎΠΏΡΠΎΡΠ΅ΠΊΡΠΎΡΠ½ΠΎΠΌΡ ΡΡΡΠ΅ΠΊΡΡ ΠΠ Ρ ΡΡΡΠ΅ΡΡΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΠΆΠΈΠ²ΠΎΡΠ½ΡΡ
. ΠΠ΄Π°ΠΏΡΠ°ΡΠΈΡ ΡΠΎΠΏΡΠΎΠ²ΠΎΠΆΠ΄Π°Π΅ΡΡΡ ΡΠ²Π΅Π»ΠΈΡΠ΅Π½ΠΈΠ΅ΠΌ ΡΠΎΠ΄Π΅ΡΠΆΠ°Π½ΠΈΡ ΠΠ Π² ΠΊΡΠΎΠ²ΠΈ ΠΈ ΡΠΊΠ°Π½ΡΡ
ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½ΡΡ
ΠΆΠΈΠ²ΠΎΡΠ½ΡΡ
. Π‘Π½ΠΈΠΆΠ΅Π½ΠΈΠ΅ ΡΠ°ΡΡΠΎΡΡ Π²ΠΎΠ·Π½ΠΈΠΊΠ½ΠΎΠ²Π΅Π½ΠΈΡ ΠΆΠ΅Π»ΡΠ΄ΠΎΡΠΊΠΎΠ²ΡΡ
Π°ΡΠΈΡΠΌΠΈΠΉ, ΠΈΠ½Π΄ΡΡΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠ΅ ΠΏΠΎΠ²ΡΠΎΡΠ½ΡΠΌΠΈ ΠΈΠΌΠΌΠΎΠ±ΠΈΠ»ΠΈΠ·Π°ΡΠΈΡΠΌΠΈ, ΠΎΠΏΠΎΡΡΠ΅Π΄ΡΠ΅ΡΡΡ ΡΠ΅ΡΠ΅Π· ΡΡΠΈΠΌΡΠ»ΡΡΠΈΡ ΞΌ-ΠΠ ΡΠ½Π΄ΠΎΠ³Π΅Π½Π½ΡΠΌΠΈ ΠΎΠΏΠΈΠΎΠΈΠ΄Π°ΠΌΠΈ, Π² ΡΠΎ Π²ΡΠ΅ΠΌΡ ΠΊΠ°ΠΊ Ξ΄-ΠΠ ΠΎΡΠ²Π΅ΡΡΡΠ²Π΅Π½Π½Ρ Π·Π° Π°Π½ΡΠΈΠ°ΡΠΈΡΠΌΠΈΡΠ΅ΡΠΊΠΈΠΉ ΡΡΡΠ΅ΠΊΡ Π°Π΄Π°ΠΏΡΠ°ΡΠΈΠΈ ΠΊ ΠΏΠ΅ΡΠΈΠΎΠ΄ΠΈΡΠ΅ΡΠΊΠΎΠΉ Π³ΠΈΠΏΠΎΠ±Π°ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ Π³ΠΈΠΏΠΎΠΊΡΠΈΠΈ. ΠΠ½ΡΠ°ΡΠΊΡ-Π»ΠΈΠΌΠΈΡΠΈΡΡΡΡΠΈΠΉ ΡΡΡΠ΅ΠΊΡ Π°Π΄Π°ΠΏΡΠ°ΡΠΈΠΈ ΠΊ Π½Π΅ΠΏΡΠ΅ΡΡΠ²Π½ΠΎΠΉ Π½ΠΎΡΠΌΠΎΠ±Π°ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ Π³ΠΈΠΏΠΎΠΊΡΠΈΠΈ Π·Π°Π²ΠΈΡΠΈΡ ΠΎΡ Π°ΠΊΡΠΈΠ²Π°ΡΠΈΠΈ ΞΌ- ΠΈ Ξ΄-ΠΠ . ΠΠ΅ΠΏΡΠΈΠ΄Π½ΡΠ΅ Π°Π³ΠΎΠ½ΠΈΡΡΡ ΠΠ Π² Π±ΡΠ΄ΡΡΠ΅ΠΌ ΠΌΠΎΠ³ΡΡ Π½Π°ΠΉΡΠΈ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ Π² ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΏΡΠ°ΠΊΡΠΈΠΊΠ΅ Π² Π»Π΅ΡΠ΅Π½ΠΈΠΈ Π°Π±ΡΡΠΈΠ½Π΅Π½ΡΠ½ΠΎΠ³ΠΎ ΡΠΈΠ½Π΄ΡΠΎΠΌΠ°, ΡΡΡΠ΅ΡΡ-ΠΈΠ½Π΄ΡΡΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π½ΠΈΠΉ ΡΠ΅ΡΠ΄ΡΠ° ΠΈΠ»ΠΈ ΠΏΠΎΠ²ΡΠ΅ΠΆΠ΄Π΅Π½ΠΈΠΉ ΠΌΠΈΠΎΠΊΠ°ΡΠ΄Π°, Π²ΡΠ·Π²Π°Π½Π½ΡΡ
ΠΈΡΠ΅ΠΌΠΈΠ΅ΠΉ ΠΈ ΡΠ΅ΠΏΠ΅ΡΡΡΠ·ΠΈΠ΅ΠΉ.
Superconducting properties and pseudogap from preformed Cooper pairs in the triclinic (CaFePtAs)PtAs
Using a combination of muon-spin relaxation (SR), inelastic neutron
scattering (INS) and nuclear magnetic resonance (NMR), we investigated the
novel iron-based superconductor with a triclinic crystal structure
(CaFePtAs)PtAs (T = 13 K), containing
platinum-arsenide intermediary layers. The temperature dependence of the
superfluid density obtained from the SR relaxation-rate measurements
indicates the presence of two superconducting gaps,
. According to our INS measurements,
commensurate spin fluctuations are centered at the (, 0) wave vector, like
in most other iron arsenides. Their intensity remains unchanged across
T, indicating the absence of a spin resonance typical for many
Fe-based superconductors. Instead, we observed a peak in the spin-excitation
spectrum around 7 meV at the same wave vector, which
persists above T and is characterized by the ratio
6.2, which is significantly
higher than typical values for the magnetic resonant modes in iron pnictides
(~4.3). The temperature dependence of magnetic intensity at 7 meV revealed an
anomaly around T* = 45 K related to the disappearance of this new mode. A
suppression of the spin-lattice relaxation rate, , observed by NMR
immediately below T* without any notable subsequent anomaly at T,
indicates that T* could mark the onset of a pseudogap in
(CaFePtAs)PtAs, which is likely associated with the
emergence of preformed Cooper pairs
Recommended from our members
Magnon spectrum of the helimagnetic insulator Cu2OSeO3
Complex low-temperature-ordered states in chiral magnets are typically governed by a competition between multiple magnetic interactions. The chiral-lattice multiferroic Cu2OSeO3 became the first insulating helimagnetic material in which a long-range order of topologically stable spin vortices known as skyrmions was established. Here we employ state-of-the-art inelastic neutron scattering to comprehend the full three-dimensional spin-excitation spectrum of Cu2OSeO3 over a broad range of energies. Distinct types of high- and low-energy dispersive magnon modes separated by an extensive energy gap are observed in excellent agreement with the previously suggested microscopic theory based on a model of entangled Cu4 tetrahedra. The comparison of our neutron spectroscopy data with model spin-dynamical calculations based on these theoretical proposals enables an accurate quantitative verification of the fundamental magnetic interactions in Cu2OSeO3 that are essential for understanding its abundant low-temperature magnetically ordered phases
Destruction of long range magnetic order in an external magnetic field and the associated spin dynamics in Cu2GaBO5 and Cu2AlBO5 ludwigites
The quantum spin systems Cu2M BO5 M Al,Ga with the ludwigite crystal structure consist of a structurally ordered Cu2 sublattice in the form of three leg ladders, interpenetrated by a structurally disordered sublattice with a statistically random site occupation by magnetic Cu2 and nonmagnetic Ga3 or Al3 ions. A microscopic analysis based on density functional theory calculations for Cu2GaBO5 reveals a frustrated quasi two dimensional spin model featuring five inequivalent antiferromagnetic exchanges. A broad low temperature 11B nuclear magnetic resonance points to a considerable spin disorder in the system. In zero magnetic field, antiferromagnetic order sets in below TN approximation 4.1 K and 2.4 K for the Ga and Al compounds, respectively. From neutron diffraction, we find that the magnetic propagation vector in Cu2GaBO5 is commensurate and lies on the Brillouin zone boundary in the H0L plane, qm 0.45, 0, 0.7 , corresponding to a complex noncollinear long range ordered structure with a large magnetic unit cell. Muon spin relaxation is monotonic, consisting of a fast static component typical for complex noncollinear spin systems and a slow dynamic component originating from the relaxation on low energy spin fluctuations. Gapless spin dynamics in the form of a diffuse quasielastic peak is also evidenced by inelastic neutron scattering. Most remarkably, application of a magnetic field above 1 T destroys the static long range order, which is manifested in the gradual broadening of the magnetic Bragg peaks. We argue that such a crossover from a magnetically long range ordered state to a spin glass regime may result from orphan spins on the structurally disordered magnetic sublattice, which are polarized in magnetic field and thus act as a tuning knob for field controlled magnetic disorde
Magnon spectrum of the helimagnetic insulator Cu<sub>2</sub>OSeO<sub>3</sub>
Complex low-temperature-ordered states in chiral magnets are typically governed by a competition between multiple magnetic interactions. The chiral-lattice multiferroic Cu2OSeO3 became the first insulating helimagnetic material in which a long-range order of topologically stable spin vortices known as skyrmions was established. Here we employ state-of-the-art inelastic neutron scattering to comprehend the full three-dimensional spin-excitation spectrum of Cu2OSeO3 over a broad range of energies. Distinct types of high-and low-energy dispersive magnon modes separated by an extensive energy gap are observed in excellent agreement with the previously suggested microscopic theory based on a model of entangled Cu-4 tetrahedra. The comparison of our neutron spectroscopy data with model spin-dynamical calculations based on these theoretical proposals enables an accurate quantitative verification of the fundamental magnetic interactions in Cu2OSeO3 that are essential for understanding its abundant low-temperature magnetically ordered phases