ABSTRACT
Spin-polarized scanning tunneling microscopy has produced a great amount of images presenting magnetic contrast between different magnetic domains with an unsurpassed spatial resolution but getting values like the surface polarization has proven to be a difficult task. We will discuss in detail how to extract this information for the case of manganese layers grown on Fe(001) whiskers. Mn layers adopt a body-centered-tetragonal (bct) structure when they are grown on the Fe(001) surface at room temperature. The Mn layers show an antiferromagnetic coupling between the layers. Comparing our spin-polarized scanning tunneling spectra measured with Fe-coated W tips with spin-resolved band structure calculations, we are able to find the value of the sample surface polarization. Also discussed is a method to change the tip magnetization. Finally, the magnetic structure around a screw dislocation on the surface is reviewed.
Subject(s)
Iron/chemistry , Magnetics , Manganese/chemistry , Microscopy, Scanning Tunneling , Models, Theoretical , Tungsten/chemistryABSTRACT
We report the observation of a magnetic contrast of up to 20% in the scanning tunneling spectroscopy dI/dV maps obtained with Fe-coated tips on Mn(001) layers grown on an Fe(001) whisker at 370 K. These nanometer resolution microscopy results show that the layers couple antiferromagnetically. By normalizing the dI/dV curves by tunneling probability functions, we found a spin-dependent peak on the body-centered-tetragonal (bct) Mn(001) surface at +0.8 V, whose high spin polarization gives rise to the dI/dV map contrast. Band structure calculations allow one to identify the +0.8 V peak as due to two spin-polarized d(z(2)) surface states.
ABSTRACT
Scanning tunneling microscopy studies on the growth of Au on Fe(001) are reported. A surface alloy is observed for submonolayer deposition ( <0.5 monolayer) at temperatures higher than 370 K. This surface-confined alloy demixes when it is covered with Au and in combination with imperfect layer-by-layer growth a rough interface consisting of Au islands in and Fe islands on the original Fe(001) substrate is created. A real-space high resolution study of this buried interface is possible because of the large difference in interlayer spacing between bcc Fe(001) and fcc Au(001).
ABSTRACT
The first scanning tunneling spectroscopy measurements on V(001) are reported. A strong surface state is detected which is very sensitive to the presence of segregated carbon impurities. The surface state energy shifts from 0.03 eV below the Fermi level at clean areas towards higher energies (up to approximately 0.2 eV) at contaminated areas. Because of the negative dispersion of this state, the upward shift cannot be described in a simple confinement picture. Rather, the surface state energy is governed by vanadium surface s- d interactions which are altered by carbon coverage.
ABSTRACT
Detection of the ventilatory threshold during an incremental load exercise test by eye can be difficult. Although various alternative methods employing information other than the ventilation can be used to assist in determining the ventilatory threshold, they rely on underlying assumptions about the physiological basis for the ventilatory threshold. The method presented here (CUSUM) uses only the ventilation data, and therefore avoids such assumptions. Twelve subjects performed a total of 47 incremental exercise tests to exhaustion. Determinations of the ventilatory thresholds made by eye from the ventilation data (mean of three independent observers) were used as a standard for comparison with determinations using the modified V-slope method and the CUSUM method. A mean (SD) difference of 0.6 (2.84) ml.min-1.kg-1 was found between the standard ventilatory thresholds and those determined using the modified V-slope method. A similar comparison between the standard ventilatory thresholds and those determined using the CUSUM method yielded a difference of -0.11 (2.35) ml.min-1.kg-1. It was concluded that the CUSUM method was a useful aid for the detection of the ventilatory threshold using the ventilation data alone.