ESR and longitudinal response in metals containing localized paramagnetic centers with spin<Emphasis Type="Italic">S</Emphasis>>1/2

The theory describing electron spin resonance (ESR) and the longitudinal magnetization response of coupled spin systems in a metal containing both delocalized conduction electrons (“espins”) and localized paramagnetic centers (“s-spins”) is generalized to the case of arbitrary half-integer spin value,S>1/2, of the s-spins. The consideration is based on the Bloch-Hasegawa equations supplemented by taking into account the coupled evolution of the longitudinal magnetization components and the effect of weak ESR saturation by the microwave field. The ESR transversal susceptibility and longitudinal magnetization response are worked out in terms of normal modes related to the coupled s- and e-spin oscillators taking into account the ESR fine structure (FS) of the s-spins. These modes are characterized by effective (renormalized) frequencies and relaxation rates (decays) which differ from the partial ones. In the specific cases of a well-resolved FS (in the isothermal limit) and of the relaxational collapse of the FS due to strong exchange coupling between the s- and e-spins (in both the isothermal and bottlenecked limits), the analytical expressions are derived which are relevant to the modulation technique of measuring extremely fast spin-lattice relaxation times in metals.     

EPR and longitudinal response signals in spin systems consisting of localized (<Emphasis Type="Italic">s</Emphasis>=1/2) and delocalized spins

The spin system of many new promising materials, such as high-temperature superconductors, fullerenes, fullerides, or manganites with colossal magnetoresistance, consists of localized spins (s-spins of impurity paramagnetic centers) and delocalized spins (e-spins of charge carriers). The two sorts of spins are coupled by exchange interaction, which leads to coupled precession of the corresponding magnetizations. When the materials mentioned above are investigated by EPR methods, the measured longitudinal (T₁) and transverse (T₂) relaxation times provide the most valuable information. However, the presence of inhomogeneous broadening of the EPR of s-spins often makes it difficult to measure T₂, while small values of T₁ do not allow one to measure it by conventional methods. Atsarkin and colleagues [4, 7, 8] proposed a new version of the method for measuring T₁ by longitudinal response signals induced in a longitudinal spin coil (oriented along the constant magnetic field) under low-frequency modulation of the microwave power, which saturates the EPR, even though very weakly. Earlier, the results obtained in experiments on measuring the longitudinal response for samples containing interacting s-and e-spins were interpreted using formulas for an individual sort of spins. In this paper, the magnetization of s-and e-spins that precess under the condition of relaxational coupling is considered, which is characteristic, for example, of fullerides. The complete EPR susceptibility is represented in a form that makes it possible to determine the origin (from s-or e-spins) of two Lorentzians, each of which is characterized by one of the normal decay rates of two coupled oscillators (i.e., of precessing transverse magnetization components). The common EPR line analytically decomposed into those Lorentzians, and special factors take into account the influence of the other sort of spins on the amplitude of the signal generated by the sort under consideration. Similarly to the EPR absorption signals, the expressions for the longitudinal response are decomposed into parts originating from s-and e-spins, and each part is proportional to the form factor of one of the modes (s-or e-like). The qualitative comparison shows good agreement with experimental data in terms of EPR and longitudinal response in a fulleride.     

Dual behavior of excess electrons in rutile TiO2

The behavior of electrons in the conduction band of TiO₂ and other transition‐metal oxides is key to the many applications of these materials. Experiments seem to produce conflicting results: optical and spin‐resonance techniques reveal strongly localized small polarons, while electrical measurements show high mobilities that can only be explained by delocalized free electrons. By means of hybrid functional calculations we resolve this apparent contradiction and show that small polarons can actually coexist with delocalized electrons in the conduction band of TiO₂, the former being energetically only slightly more favorable. We also find that small polarons can form complexes with oxygen vacancies and ionized shallow‐donor impurities, explaining the rich spectrum of Ti³⁺ species observed in electron spin resonance experiments. (© 2013 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)     

Electron spin resonance in Ge0.99Mn0.01 nanowires

Electron spin resonance (ESR) is measured in arrays of Ge_0.99Mn_0.01 nanowires (NWs). We show that the ESR spectrum comprises four lines corresponding to the different magnetic subsystems. Two lines are attributed to spin-wave excitations in the Mn⁺³ ion subsystem. The third component corresponds to the resonance in the Mn⁺² ions. The last component has an asymmetric Dyson form and characterizes the resonance in the mobile paramagnetic centers. We demonstrate that temperature dependences of ESR parameters are correlated in subsystems of the localized magnetic centers (Mn⁺³ and Mn⁺² ions) and delocalized band carriers. It implies the presence of exchange interactions between the localized Mn ions and spin-polarized carriers.     

Magnetic susceptibility, heat capacity, and optical conductivity of LiPc and LiPcI

The magnetic susceptibility, using dc and electron spin resonance (ESR) methods, the specific heat, and the infrared properties of the one-dimensional molecular semiconductors lithium phthalocyanine (LiPc) and the iodinated compound LiPcI have been investigated for temperatures K. LiPc has a half-filled conduction band and is expected to be an organic metal. However, due to the strong Coulomb repulsion the system is a one-dimensional Mott-Hubbard insulator with a Hubbard gap of 0.75 eV as inferred from optical measurements. The localized electrons along the molecular stacks behave like a S = 1/2 antiferromagnetic spin chain. The spin susceptibility, as determined by ESR experiments, and the magnetic contribution to the heat capacity show a Bonner-Fisher type of behavior with an exchange constant K. LiPcI is an intrinsic narrow-gap semiconductor with an optical gap of 0.43 eV. In ESR experiments it is silent, indicating that all the unpaired electrons have been removed from the macrocycle via doping with iodine. Received: 16 June 1998 / Accepted: 14 July 1998     

Low-Temperature Phase Transition Detected by ESR in ����-(BEDT-TTF)2IBr2 Single Crystals

Hysteresis of the electron spin resonance (ESR) spectra of localized charge carriers has been observed in ????-(BEDT-TTF)₂IBr₂ single crystals in the temperature range of 15?C30?K. The first-order phase transition has been detected by ESR components. Two lines observed in the ESR spectrum correspond to low-temperature and high-temperature phases.     

Evolution of the 4f electron localization from YbRh2Si2 to YbRh2Pb studied by electron spin resonance

We report on electron spin resonance (ESR) experiments on the Heusler alloy YbRh₂Pb and compare its spin dynamics with that of several other Yb-based intermetallics. A detailed analysis of the derived ESR parameters indicates the extremely weak hybridization, more localized distribution of the 4f states, and a smaller RKKY interaction in YbRh₂Pb. These findings reveal the important interplay between hybridization effects, chemical substitution, and crystalline electric field interactions that determines the ground state properties of strongly correlated electron systems.     

Electron and nuclear spin dynamics in antiferromagnetic molecular rings

We study theoretically the spin dynamics of antiferromagnetic molecular rings, such as the ferric wheel Fe10. For a single nuclear or impurity spin coupled to one of the electron spins of the ring, we calculate nuclear and electronic spin correlation functions and show that nuclear magnetic resonance (NMR) and electron spin resonance (ESR) techniques can be used to detect coherent tunneling of the Néel vector in these rings. The location of the NMR/ESR resonances gives the tunnel splitting and its linewidth an upper bound on the decoherence rate of the electron spin dynamics. We illustrate the experimental feasibility of our proposal with estimates for Fe10 molecules.     

ESR study of the ferrimagnetic spinel selenide CuCr2Se4

Ferrimagnetic spinel selenide CuCr₂Se₄ has been investigated by the electron spin resonance (ESR) spectroscopy. Experimental results reveal that ESR signals originate from the localized d-shell electrons of Cr³⁺ ions. In addition, the ESR linewidth ΔH _PP increases linearly with decreasing temperature. It is suggested that the spin-orbit coupling may be one of the contributions to the broadening of ΔH _PP . Our ESR results support the model of the ferrimagnetic hybridization between localized 3d ³ electrons of Cr³⁺ with delocalized holes of Se 4p band.     

Rates of rotational diffusion and Heisenberg spin exchange as obtained from CW ESR and ESR tomographic experiments on model systems and human skin

The purpose of the present paper is to describe possibilities and limitations for the determination of the rates of rotational diffusion and Heisenberg spin exchange, obtained from continuous-wave electron spin resonance (cw ESR) and ESR tomographic experiments. Model systems including nitroxides as paramagnetic reporter molecules have been examined in order to verify data, which have been obtained from cw ESR and ESR tomography. This has been done with particular emphasis on checking the influence of concentration, temperature, and viscosity on the spectral-spatial properties. These findings have been applied to the evaluation of penetration and permeation studies on human skin. The extracted full spectral information from ESR tomography allows the determination of the above mentioned dynamic parameters for model systems of definite geometry and for samples of human skin. It has been found that the signal-to-noise ratio is critical for all discussed applications.     

ESR Investigations on Polyethylene–Fluorine Functionalized Single Wall Carbon Nanotubes Composites

Electron spin resonance investigations on nanocomposites obtained by dispersing fluorinated single walled carbon nanotubes within polyethylene are reported. Three resonance lines assigned to uncoupled electronic spins confined within magnetic impurities, amorphous carbon, and single wall carbon nanotubes have been observed. The temperature dependence of these lines is analyzed in detail and used to assign each component of the as-recorded ESR spectrum to a precise component of the nanocomposite. Magnetic impurities are originating from catalysts residues (in our case, Fe impurities). Surprisingly, the narrowest line is due to paramagnetic defects (amorphous carbon) while the broad line originates from electrons delocalized over conducting nanotubes. The broadening of this line reflects a bottleneck in the relaxation mechanism, triggered by the interaction of the uncoupled electrons localized on carbon nanotubes with the magnetic impurities.     

Interaction of two magnetic resonance modes in the polar phase of superfluid <Superscript>3</Superscript>He

We report results of low frequency nuclear magnetic resonance (NMR) experiments in the superfluid polar phase of ³He, which is stabilized by a new type of “nematic” aerogel—nafen. We have found that an interaction between transverse and longitudinal NMR modes may essentially influence the spin dynamics. Theoretical formulas for NMR resonant frequencies are derived and applied for interpretation of the experimental results.     

Room temperature electrical detection of spin coherence in C60

An experimental demonstration of electrical detection of coherent spin motion of weakly coupled, localized electron spins in thin fullerene C60 films at room temperature is presented. Pulsed electrically detected magnetic resonance experiments on vertical photocurrents through Al/C(60)/ZnO samples showed that an electron spin Rabi oscillation is reflected by transient current changes. The nature of possible microscopic mechanisms responsible for this spin to charge conversion as well as its implications for the readout of endohedral fullerene (N@C(60)) spin qubits are discussed.     

Shot noise in a quantum dot coupled to non-magnetic leads: effects of Coulomb interaction

We study electron transport through a quantum dot, connected to non-magnetic leads, in a magnetic field. A super-Poissonian electron noise due to the effects of both interacting localized states and dynamic channel blockade is found when the Coulomb blockade is partially lifted. This is sharp contrast to the sub-Poissonian shot noise found in the previous studies for a large bias voltage, where the Coulomb blockade is completely lifted. Moreover, we show that the super-Poissonian shot noise can be suppressed by applying an electron spin resonance (ESR) driving field. For a sufficiently strong ESR driving field strength, the super-Poissonian shot noise will change to be sub-Poissonian.     

ESR study of the undoped heavy-fermion compound YbRh2Si2

The electron spin resonance (ESR) of the heavy-fermion metal YbRh₂Si₂ has been studied. The angular variation and the temperature dependence of the ESR line width have been measured in YbRh₂Si₂ single crystals in the temperature range of 4–25 K. The characteristic spin-fluctuation temperatureT ^* ～ 17 K estimated from these studies coincides very well with other experimental data. A well-behaved ESR signal due to local Yb³⁺ moments strongly supports the localized moment scenario for heavy-fermion quantum critical points.     

Electrically detected electron spin resonance in a high-mobility silicon quantum well

The resistivity change due to electron spin resonance (ESR) absorption is investigated in a high-mobility two-dimensional electron system formed in a Si/SiGe heterostructure. Results for a specific Landau level configuration demonstrate that the primary cause of the ESR signal is a reduction of the spin polarization, not the effect of electron heating. The longitudinal spin relaxation time T1 is obtained to be of the order of 1 ms in an in-plane magnetic field of 3.55 T. The suppression of the effect of the Rashba fields due to high-frequency spin precession explains the very long T1.     

Electron spin resonance determination of proton locations in a hydride

The low temperature electron spin resonance (ESR) spectrum of dilute Er in ScH_x powder contains distinct signals which are due to the presence of octahedral as well as tetrahedral protons in the vicinity of the Er ions. The occupation probability for the octahedral protons versus the bulk hydrogen-to-metal ratio is determined from the ESR signal intensities and compared with a lattice-gas calculation.     

Spin waves on the surface of the nonferromagnetic nanotube in magnetic field

Propagating in the nonferromagnetic electron gas on the cylindrical nanotube's surface spin waves in longitudinal magnetic field are considered. The spectrum of electrons in the Hartree-Fock approximation was applied. The dynamic spin susceptibility of a degenerate electron gas was derived using the random phase approximation. The spectra of intra-subband and inter-subband magnons were calculated in quasiclassical and quantum limits. The quantity of spin waves spectrum branches depends on the amount of filled subbands. In case the filled subband numbers are large, the wave's frequencies undergo oscillations of de Haas-van Alphen and Aharonov-Bohm types with the electron density and the magnetic induction changes.     

矩形辐射器压电多频超声换能器的研究

研究了一种具有多个共振频率的矩形辐射器夹心式超声换能器,换能器由圆柱形后盖板、压电陶瓷晶堆及矩形六面体辐射器前盖板组合而成。利用表观弹性法和一维近似理论给出了多频换能器横向及纵向理论共振频率方程。对一种特殊情况下的此类换能器进行了有限元及实验分析,给出了各自的频率输入导纳曲线。对理论和实验结果进行分析后表明,此类矩形辐射器夹心式超声换能器可以在不同的振动模态上工作,具有多个共振频率.     

Low temperature electron spin resonance of the Kondo ion in a heavy fermion metal: YbRh2Si2

We report an electron spin resonance (ESR) study on single crystals of the heavy fermion metal YbRh2Si2 which shows pronounced non-Fermi liquid behavior related to a close antiferromagnetic quantum critical point. It is shown that the observed ESR spectra can be ascribed to a bulk Yb3+ resonance. This is the first observation of ESR of the Kondo ion itself in a dense Kondo lattice system. The ESR signal occurs below the Kondo temperature (T(K)) which thus indicates the existence of large unscreened Yb3+ moments below T(K). We observe the spin dynamics as well as the static magnetic properties of the Yb3+ spins to be consistent with the results of nuclear magnetic resonance and magnetic susceptibility.