1,992 research outputs found

    Magnetism of mixed quaternary Heusler alloys: (Ni,T)2_{2}MnSn (T=Cu,Pd) as a case study

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    The electronic properties, exchange interactions, finite-temperature magnetism, and transport properties of random quaternary Heusler Ni2_{2}MnSn alloys doped with Cu- and Pd-atoms are studied theoretically by means of {\it ab initio} calculations over the entire range of dopant concentrations. While the magnetic moments are only weakly dependent on the alloy composition, the Curie temperatures exhibit strongly non-linear behavior with respect to Cu-doping in contrast with an almost linear concentration dependence in the case of Pd-doping. The present parameter-free theory agrees qualitatively and also reasonably well quantitatively with the available experimental results. An analysis of exchange interactions is provided for a deeper understanding of the problem. The dopant atoms perturb electronic structure close to the Fermi energy only weakly and the residual resistivity thus obeys a simple Nordheim rule. The dominating contribution to the temperature-dependent resistivity is due to thermodynamical fluctuations originating from the spin-disorder, which, according to our calculations, can be described successfully via the disordered local moments model. Results based on this model agree fairly well with the measured values of spin-disorder induced resistivity.Comment: 13 pages, 13 figure

    Magnetism of 3d transition metal atoms on W(001): submonolayer films

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    We have investigated random submonolayer films of 3d transition metals on W(001). The tight-binding linear muffin-tin orbital method combined with the coherent potential approximation was employed to calculate the electronic structure of the films. We have estimated local magnetic moments and the stability of different magnetic structures, namely the ferromagnetic order, the disordered local moments and the non-magnetic state, by comparing the total energies of the corresponding systems. It has been found that the magnetic moments of V and Cr decrease and eventually disappear with decreasing coverage. On the other hand, Fe retains approximately the same magnetic moment throughout the whole concentration range from a single impurity to the monolayer coverage. Mn is an intermediate case between Cr and Fe since it is non-magnetic at very low coverages and ferromagnetic otherwise.Comment: 5 pages, 3 figures in 6 files; presented at ICN&T 2006, Basel, Switzerlan

    Π­Ρ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ ΠΈΠΎΠ½ΠΈΠ·Π°Ρ†ΠΈΠΈ Π² горячСй плоской дискообразной полости

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    Hot cavity ion sources of different kinds are widely used in nuclear and mass spectroscopy, especially in on-line isotope separation devices attracting attention of scientists and engineers looking for high ionization efficiency, robustness and beam purity. In the paper a new type of hot ionizer cavity is proposed: namely cavity having the shape of a flat disc, which may be especially suitable for short-lived nuclides to be ionized. A numerical model of the ion source is presented in the paper. The particle tracking code takes into account ionization at hot surfaces and enables modeling of both flat disc cavity and standard elongated cavity ionizers. The code enables calculation of total ionization efficiency and is suitable for stable and long-lived nuclides. Influence of the flat disc cavity geometry (thickness and radius) and its temperature on total ionization efficiency was considered – it was shown that the efficiency increases with cavity radius due to the growing number of particle-wall collisions. This effect may be important in the case of the hard-to-ionize nuclides. The optimal ionizer geometry is characterized by 90 % efficiency, even for substances with rather low ionization coefficient (of order 0.05). The role played by the size of the extraction opening is explained – it is demonstrated that the ionization efficiency increases due to the opening radius reduction. It is also proven that extraction voltage of 1–2 kV is sufficient to maintain optimal ionizer efficiency

    Rhythmic Leptin Is Required for Weight Gain from Circadian Desynchronized Feeding in the Mouse

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    The neuroendocrine and metabolic effects of leptin have been extensively researched since the discovery, and the later identification, of the leptin gene mutated within the ob/ob mouse. Leptin is required for optimal health in a number of physiological systems (e.g. fertility, bone density, body weight regulation). Despite the extensive leptin literature and many observations of leptin’s cyclical pattern over the 24-hour day, few studies have specifically examined how the circadian rhythm of leptin may be essential to leptin signaling and health. Here we present data indicating that a rhythmic leptin profile (e.g. 1 peak every 24 hours) leads to excessive weight gain during desynchronized feeding whereas non-rhythmic leptin provided in a continuous manner does not lead to excessive body weight gain under similar feeding conditions. This study suggests that feeding time can interact with leptin’s endogenous rhythm to influence metabolic signals, specifically leading to excessive body weight gains during β€˜wrongly’ timed feeding

    Circadian Disruption and Metabolic Disease: Findings from Animal Models

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    Social opportunities and work demands have caused humans to become increasingly active during the late evening hours, leading to a shift from the predominantly diurnal lifestyle of our ancestors to a more nocturnal one. This voluntarily decision to stay awake long into the evening hours leads to circadian disruption at the system, tissue, and cellular levels. These derangements are in turn associated with clinical impairments in metabolic processes and physiology. The use of animal models for circadian disruption provides an important opportunity to determine mechanisms by which disorganization in the circadian system can lead to metabolic dysfunction in response to genetic, environmental, and behavioral perturbations. Here we review recent key animal studies involving circadian disruption and discuss the possible translational implications of these studies for human health and particularly for the development of metabolic disease

    Π­Ρ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ ΠΈΠΎΠ½ΠΈΠ·Π°Ρ†ΠΈΠΈ Π² горячСй плоской дискообразной полости

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    Hot cavity ion sources of different kinds are widely used in nuclear and mass spectroscopy, especially in on-line isotope separation devices attracting attention of scientists and engineers looking for high ionization efficiency, robustness and beam purity. In the paper a new type of hot ionizer cavity is proposed: namely cavity having the shape of a flat disc, which may be especially suitable for short-lived nuclides to be ionized.A numerical model of the ion source is presented in the paper. The particle tracking code takes into account ionization at hot surfaces and enables modeling of both flat disc cavity and standard elongated cavity ionizers. The code enables calculation of total ionization efficiency and is suitable for stable and long-lived nuclides.Influence of the flat disc cavity geometry (thickness and radius) and its temperature on total ionization efficiency was considered – it was shown that the efficiency increases with cavity radius due to the growing number of particle-wall collisions. This effect may be important in the case of the hard-to-ionize nuclides.The optimal ionizer geometry is characterized by 90 % efficiency, even for substances with rather low ionization coefficient (of order 0.05). The role played by the size of the extraction opening is explained – it is demonstrated that the ionization efficiency increases due to the opening radius reduction. It is also proven that extraction voltage of 1–2 kV is sufficient to maintain optimal ionizer efficiency.Β Β Π˜ΠΎΠ½ΠΈΠ·Π°Ρ‚ΠΎΡ€Ρ‹ с горячСй ΠΏΠΎΠ»ΠΎΡΡ‚ΡŒΡŽ Ρ€Π°Π·Π»ΠΈΡ‡Π½ΠΎΠ³ΠΎ Ρ‚ΠΈΠΏΠ° находят ΡˆΠΈΡ€ΠΎΠΊΠΎΠ΅ ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ Π² Π°Ρ‚ΠΎΠΌΠ½ΠΎΠΉ ΠΈ массспСктроскопии, Π² частности, Π² устройствах для раздСлСния ΠΈΠ·ΠΎΡ‚ΠΎΠΏΠΎΠ² Π² Ρ€Π΅ΠΆΠΈΠΌΠ΅ ΠΎΠ½Π»Π°ΠΉΠ½, ΠΏΡ€Π΅Π΄ΡΡ‚Π°Π²Π»ΡΡŽΡ‚ большой интСрСс для ΡƒΡ‡Ρ‘Π½Ρ‹Ρ… ΠΈ ΠΈΠ½ΠΆΠ΅Π½Π΅Ρ€ΠΎΠ² вслСдствиС высокой эффСктивности ΠΈΠΎΠ½ΠΈΠ·Π°Ρ†ΠΈΠΈ, надёТности ΠΈ чистоты Π»ΡƒΡ‡Π°. Π’ Ρ€Π°Π±ΠΎΡ‚Π΅ ΠΏΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½ Π½ΠΎΠ²Ρ‹ΠΉ Ρ‚ΠΈΠΏ горячСй ΠΈΠΎΠ½ΠΈΠ·Π°Ρ†ΠΈΠΎΠ½Π½ΠΎΠΉ полости, Π° ΠΈΠΌΠ΅Π½Π½ΠΎ полости Π² Ρ„ΠΎΡ€ΠΌΠ΅ плоского диска, особСнно эффСктивной для ΠΈΠΎΠ½ΠΈΠ·Π°Ρ†ΠΈΠΈ ΠΊΠΎΡ€ΠΎΡ‚ΠΊΠΎΠΆΠΈΠ²ΡƒΡ‰ΠΈΡ… Π½ΡƒΠΊΠ»ΠΈΠ΄ΠΎΠ². ΠŸΡ€Π΅Π΄ΡΡ‚Π°Π²Π»Π΅Π½Π° числСнная модСль ΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ источника. МодСль отслСТивания частиц ΡƒΡ‡ΠΈΡ‚Ρ‹Π²Π°Π΅Ρ‚ ΠΈΠΎΠ½ΠΈΠ·Π°Ρ†ΠΈΡŽ Π½Π° горячих повСрхностях ΠΈ позволяСт ΠΌΠΎΠ΄Π΅Π»ΠΈΡ€ΠΎΠ²Π°Ρ‚ΡŒ ΠΊΠ°ΠΊ ΠΏΠΎΠ»ΠΎΡΡ‚ΡŒ плоского диска, Ρ‚Π°ΠΊ ΠΈ стандартныС ΠΈΠΎΠ½ΠΈΠ·Π°Ρ‚ΠΎΡ€Ρ‹ с ΡƒΠ΄Π»ΠΈΠ½Ρ‘Π½Π½ΠΎΠΉ ΠΏΠΎΠ»ΠΎΡΡ‚ΡŒΡŽ. МодСль позволяСт Π²Ρ‹ΠΏΠΎΠ»Π½ΡΡ‚ΡŒ расчёт ΠΎΠ±Ρ‰Π΅ΠΉ эффСктивности ΠΈΠΎΠ½ΠΈΠ·Π°Ρ†ΠΈΠΈ ΠΈ ΠΏΡ€ΠΈΠΌΠ΅Π½ΠΈΠΌΠ° ΠΊ ΡΡ‚Π°Π±ΠΈΠ»ΡŒΠ½Ρ‹ΠΌ ΠΈ Π΄ΠΎΠ»Π³ΠΎΠΆΠΈΠ²ΡƒΡ‰ΠΈΠΌ Π½ΡƒΠΊΠ»ΠΈΠ΄Π°ΠΌ.РассмотрСно влияниС Π³Π΅ΠΎΠΌΠ΅Ρ‚Ρ€ΠΈΠΈ полости плоского диска (Ρ‚ΠΎΠ»Ρ‰ΠΈΠ½Π° ΠΈ радиус) ΠΈ Π΅Π³ΠΎ Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρ‹ Π½Π° ΠΎΠ±Ρ‰ΡƒΡŽ ΡΡ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ ΠΈΠΎΠ½ΠΈΠ·Π°Ρ†ΠΈΠΈ – ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΎ, Ρ‡Ρ‚ΠΎ ΡΡ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ увСличиваСтся с радиусом полости ΠΈΠ·-Π·Π° растущСго числа столкновСний частиц со стСнками. Π”Π°Π½Π½Ρ‹ΠΉ эффСкт ΠΌΠΎΠΆΠ΅Ρ‚ ΠΎΠΊΠ°Π·Π°Ρ‚ΡŒΡΡ Π²Π°ΠΆΠ΅Π½ для Ρ‚Ρ€ΡƒΠ΄Π½ΠΎΠΈΠΎΠ½ΠΈΠ·ΠΈΡ€ΡƒΠ΅ΠΌΡ‹Ρ… Π½ΡƒΠΊΠ»ΠΈΠ΄ΠΎΠ².ΠžΠΏΡ‚ΠΈΠΌΠ°Π»ΡŒΠ½Π°Ρ гСомСтрия ΠΈΠΎΠ½ΠΈΠ·Π°Ρ‚ΠΎΡ€Π° характСризуСтся ΡΡ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒΡŽ 90 % Π΄Π°ΠΆΠ΅ для Ρ‚Ρ€ΡƒΠ΄Π½ΠΎΠΈΠΎΠ½ΠΈΠ·ΠΈΡ€ΡƒΠ΅ΠΌΡ‹Ρ… вСщСств с коэффициСнтом ΠΈΠΎΠ½ΠΈΠ·Π°Ρ†ΠΈΠΈ порядка 0,05. ΠžΠ±ΡŠΡΡΠ½ΡΠ΅Ρ‚ΡΡ Ρ€ΠΎΠ»ΡŒ, ΠΊΠΎΡ‚ΠΎΡ€ΡƒΡŽ ΠΈΠ³Ρ€Π°Π΅Ρ‚ Ρ€Π°Π·ΠΌΠ΅Ρ€ экстракционного отвСрстия – ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΎ, Ρ‡Ρ‚ΠΎ ΡΡ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ ΠΈΠΎΠ½ΠΈΠ·Π°Ρ†ΠΈΠΈ увСличиваСтся ΠΈΠ·-Π·Π° ΡƒΠΌΠ΅Π½ΡŒΡˆΠ΅Π½ΠΈΡ радиуса отвСрстия. Π’Π°ΠΊΠΆΠ΅ Π΄ΠΎΠΊΠ°Π·Π°Π½ΠΎ, Ρ‡Ρ‚ΠΎ Π²Ρ‹Ρ…ΠΎΠ΄Π½ΠΎΠ΅ напряТСниС 1–2 ΠΊΠ’ достаточно для поддСрТания ΠΎΠΏΡ‚ΠΈΠΌΠ°Π»ΡŒΠ½ΠΎΠΉ эффСктивности

    Advantages of nonclassical pointer states in postselected weak measurements

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    We investigate, within the weak measurement theory, the advantages of non-classical pointer states over semi-classical ones for coherent, squeezed vacuum, and Schr\"{o}inger cat states. These states are utilized as pointer state for the system operator A^\hat{A} with property A^2=I^\hat{A}^{2}=\hat{I}, where I^\hat{I} represents the identity operator. We calculate the ratio between the signal-to-noise ratio (SNR) of non-postselected and postselected weak measurements. The latter is used to find the quantum Fisher information for the above pointer states. The average shifts for those pointer states with arbitrary interaction strength are investigated in detail. One key result is that we find the postselected weak measurement scheme for non-classical pointer states to be superior to semi-classical ones. This can improve the precision of measurement process.Comment: 8 pages, 5 figure
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