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Lasers Fabricated by Nanoimprint<br />

Lithography<br />

The team of V. Reboud at the Tyndall National Institute,<br />

Cork, Ireland, report on the fabrication and<br />

characterization of two-dimensional polymer photonic<br />

crystal band-edge lasers operating in the visible<br />

range. The components have been fabricated in<br />

a dye chromophore-loaded polymer matrix by nanoimprint<br />

lithography and high-symmetry bandedge<br />

modes are used to generate laser emission.<br />

Their work demonstrates the potential of nanoimprint<br />

lithography for the fabrication of two-dimensional<br />

planar photonic crystal structures in an active<br />

medium in a one-step process.<br />

» Appl. Phys. Lett. 91, 151101<br />

» doi:10.1063/1.2798250<br />

Optical Coherence Computed<br />

Tomography<br />

L. Li and L.V. Wang from the Washington University<br />

in St Louis, Missouri, USA, propose a device to<br />

bridge the gap between diffuse optical tomography<br />

and optical coherence tomography. Both ballistic<br />

and multiple-scattered photons are measured at<br />

multiple source-detection positions by low-coherence<br />

interferometry providing a temporal resolution<br />

smaller than 100 fs. A light-tissue interaction<br />

model was established using the time-resolved<br />

Monte Carlo method. The optical properties were<br />

then reconstructed by solving the inverse transient<br />

radiative transport problem under the first Born approximation.<br />

Absorbing inclusions of 100 µm diameter<br />

were imaged through a 2.6-mm-thick (~ 30<br />

scattering mean-free-paths) scattering medium.<br />

» Appl. Phys. Lett. 91, 141107<br />

» doi:10.1063/1.2793625<br />

Frequency Response of an AFM:<br />

Magnetic Versus Acoustic Excitation<br />

E.T. Herruzo and R. Garcia from the CSIC, Madrid,<br />

Spain, discuss the dynamics of an amplitude modulation<br />

AFM in different environments such as water<br />

and air, and show that the resonance curves depend<br />

on the excitation method used to drive the<br />

cantilever, either mechanical or magnetic. This dependence<br />

is magnified for small force constants<br />

and quality factors, i.e., below 1 N/m and 10, respectively.<br />

They also show that the equation for the<br />

observable, the cantilever deflection, depends on<br />

the excitation method. Under mechanical excitation,<br />

the deflection involves the base and tip displacements,<br />

while in magnetic excitation, the cantilever<br />

deflection and tip displacement coincide.<br />

» Appl. Phys. Lett. 91, 143113<br />

» doi:10.1063/1.2794426<br />

• G.I.T. Imaging & Microscopy 4/2007<br />

NEwS TICkER<br />

Influence of Sample Conductivity on<br />

Oxidation by the Tip of AFM<br />

V. Cambel and J. Soltys at the Slovak Academy of<br />

Sciences, Bratislava, Slovakia analyzed the role of<br />

the electric field distribution in the nano-oxidation<br />

process realized by the tip of AFM experimentally<br />

and theoretically. Authors show the importance of<br />

the sample conductivity and the water bridge in the<br />

process applied to bulk GaAs and Ga[Al]As heterostructures<br />

in both contact and noncontact AFM<br />

modes and the consequences for the lines witten.<br />

They show that the electric field distribution in the<br />

system tip-sample is controlled by the sample conductivity.<br />

In the case of low-conductive samples,<br />

maximum field is located apart from the tip apex<br />

for both contact and noncontact AFM modes.<br />

» J. Appl. Phys. 102, 074315<br />

» doi:10.1063/1.2794374<br />

High-resolution Microscope for Tipenhanced<br />

Optical Processes in UHV<br />

J. Steidtner and B. Pettinger in Berlin, Germany<br />

present an optical microscope based on tip-enhanced<br />

optical processes that can be used for studies<br />

on adsorbates as well as thin layers and nanostructures.<br />

It provides chemical and topographic<br />

informations with a resolution of a few nanometers<br />

and can be employed in ultrahigh vacuum as well<br />

as gas phase. The central idea is to mount, within<br />

an UHV system, an optical platform with all necessary<br />

optical elements to a rigid frame that also carries<br />

the scanning tunneling microscope unit and to<br />

integrate a high numerical aperture parabolic mirror<br />

between the scanning probe microscope head<br />

and the sample. Authors present the first results of<br />

Raman measurements using the device and the experimentally<br />

determined requirements of the parabolic<br />

mirror in terms of alignment accuracy.<br />

» Rev. Sci. Instrum. 78, 103104<br />

» doi:10.1063/1.2794227<br />

An UHV Fast-scanning and Variable<br />

Temperature STM for Large Scale<br />

Imaging<br />

B. Diaconescu and co-workers from the University<br />

of New Hampshire, USA describe the design and<br />

performance of a fast-scanning, variable temperature<br />

scanning tunneling microscope (STM) operating<br />

from 80 to 700 K in ultrahigh vacuum (UHV),<br />

which routinely achieves large scale atomically resolved<br />

imaging of compact metallic surfaces. The<br />

vertical resolution of the instrument was found to<br />

be about 2 pm at room temperature. The total<br />

scanning area is about 8 × 8 µm 2 . The sample tem-<br />

perature can be adjusted by a few tens of degrees<br />

while scanning over the same sample area.<br />

» Rev. Sci. Instrum. 78, 103701<br />

» doi:10.1063/1.2789655<br />

Suppression of Spurious Vibration of<br />

Cantilever in AFM<br />

T. Tsuji and colleagues from Tohoku University, Japan,<br />

developed a simple but effective method for<br />

suppressing spurious response (SR) to improve the<br />

precision of dynamic AFM using cantilever vibration<br />

spectra. The dominant origin of SR was identified<br />

to be the bending vibration of the cantilever<br />

substrate, but while a rigid cover pressing the<br />

whole surface of the substrate suppressed SR, the<br />

utility was insufficient. Then, a method of enhancing<br />

the bending rigidity of the substrate by gluing a<br />

rigid plate (clamping plate, CP) to the substrate<br />

was developed. The CP method will particularly<br />

contribute to improving dynamic-mode AFM, in<br />

which resonance spectra with a low quality factor<br />

are used, such as noncontact mode AFM in liquid or<br />

contact resonance mode AFM.<br />

» Rev. Sci. Instrum. 78, 103703<br />

» doi:10.1063/1.2793498<br />

High Resolution Gamma Ray<br />

Tomography Scanner<br />

U. Hampel and co-workers at Forschungszentrum<br />

Dresden-Rossendorf e.V., Dresden, Germany, report<br />

on the development of a high resolution gamma<br />

ray tomography scanner that is operated with a Cs-<br />

137 isotopic source at 662 keV gamma photon energy<br />

and achieves a spatial image resolution of 0.2<br />

line pairs/mm at 10 % modulation transfer function<br />

for noncollimated detectors. It is primarily intended<br />

for the scientific study of flow regimes and phase<br />

fraction distributions in fuel element assemblies,<br />

chemical reactors, pipelines, and hydrodynamic machines,<br />

but it is applicable to nondestructive testing<br />

of larger radiologically dense objects. They also<br />

built a computed tomography scanner gantry for<br />

measurements at fixed vessels or plant components.<br />

» Rev. Sci. Instrum. 78, 103704<br />

» doi:10.1063/1.2795648<br />

Correction of Axial Geometrical Distortion<br />

in Microscopic <strong>Images</strong><br />

H.J. Van Elburg and colleagues from the University<br />

of Antwerp, Belgium, discuss the extraction of<br />

quantitative data from microscopic volume images<br />

when imperfectly matched immersion and mounting<br />

media result in axial geometrical distortion. Linear<br />

correction of the axial distortion using the

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