M. Drechsler’s research while affiliated with French National Centre for Scientific Research and other places

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Publications (53)


Sharpening of metal tips by heat treatment in vacuum
  • Article

February 2001

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15 Reads

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5 Citations

Journal of Physics E Scientific Instruments

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A Piquet

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H Roux

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[...]

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M Drechsler

It is well known that a metal tip blunts if it is heated in vacuum. Sharpening may occur in the case of an evaporation of the tip material. To test this, molybdenum tips were heated in vacuum. A typical result: at 2400K, the tip radius decreases from 8 mu m to 0.3 mu m thus confirming the hypothesis. Measured and calculated final radii agree roughly. The pure material evaporation can be replaced by a surface reaction followed by the evaporation of the reaction products. This is shown on tungsten tips heated (1750K) in the presence of oxygen (0.5 mTorr). The evaporation of tungsten oxides results in a sharpening to a radius to 0.05 mu m. Under special conditions, in connection with the formation of solid drops, radii down to 0.01 mu m are obtained.


Temperature measurement of microcrystals heated by electron bombardment: W tips from 2800K to 3650K

November 2000

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8 Reads

Journal of Physics E Scientific Instruments

For controlled heating of metal microcrystals up to the melting point, the end of the field emitter tips are bombarded by an electron beam (8 keV, 400 mu A, 200 mu m beam diameter). To measure local temperatures on small areas down to 2 mu m diameter a special one-wavelength micropyrometer was built. Using an optical microscope, an image of the glowing tip was projected on to a screen outside the vacuum chamber. The screen has a movable hole behind which a one-wavelength filter and a photomultiplier are placed to measure local radiant intensities. The relative temperatures are obtained from Wien's law, and are absolutely calibrated by a thermocouple spot-welded on the emitter shank. Local relative temperatures and temperature gradients for a tungsten emitter are measured in the range between 2800K and 3650K, with an error and a stability better than 10K. For absolute temperatures the error is 50K when no evaporation occurs.


Vacuum micro-chambers in electron microscopes

December 1990

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9 Reads

Vacuum

In the course of in-situ transmission electron microscope studies, we found and analyzed a phenomenon of self-formation of small evacuated chambers. The chamber wall is partly metal and partly graphite film. The chamber formation is explained as an interface diffusion transport induced by capillarity. The chamber is resistant against atmospheric pressure. Such chambers can be used to study kinetic phenomena by in-situ electron microscopy.


A TIP OSCILLATION PHENOMENON

November 1987

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8 Reads

Le Journal de Physique Colloques

Une étude des cous stables des pointes en microscopie électronique transmission montre l'existence d'une oscillation des pointes avec des amplitudes de ~ 200 Å et des fréquences de ~ 0.3 Hertz (Cu, Au, 900°C). L'oscillation est expliquée par une interaction de deux forces : (1) une force électro-statique causée par l'impact des électrons et annihilée par une décharge d'émission de champ et (2) une force élastique d'une couche graphitique à la surface de la pointe. A detailed study of stable tip necks by in situ transmission electron microscopy shows an existence of tip oscillations with amplitudes in the order of 200 Å and frequencies in the order of 0.3 Hertz (Cu, Au at ~ 900°C). The oscillation is explained by an interaction of two forces : (1) an electrostatic force caused by electron impact and annihilated by a field emission discharge and (2) an elastic force of a graphitized layer on the tip surface.


STABLE NECKS ON METAL TIPS
  • Article
  • Full-text available

November 1987

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30 Reads

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3 Citations

Le Journal de Physique Colloques

On a metal tip (W, Ni, Au, Cu) heated in an electron microscope (SEM) a formation of stable necks is observed. As this does not agree with the theory, experiments are made for clarification. In situ electron microscopy (TEM, STEM, EELS) shows the existence of graphitized surface layers, which surprisingly remain stable up to near the melting point. These layers hinder a complete separation of a solid metal drop from the tip end. On the basis of this result spectacular tip and neck shape changes are explainable as an Ostwald ripening.

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Surface matter transport phenomena studied in situ on crystal tips

October 1987

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2 Reads

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2 Citations

Surface Science Letters

A technique is described to study in situ the matter transport and the morphological evolution on crystals. Used for it is a transmission electron microscope, specimens in form of tips, a heating chamber and video registration. The test system studied is Cu-C. Results found are: (1) techniques to measure in situ the thickness of a layer on a metal surface; (2) an indication that a layer formation begins on surface regions of maximum curvature; and (3) the finding of an oscillating matter transport on tip necks.


Evolution of grain boundaries in very clean metal tips

December 1986

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2 Reads

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2 Citations

Surface Science Letters

Former studies of grain boundaries in metal tips concern static crystallographic problems. In this study we describe temperature increase induced evolutions of grain boundaries in very clean tips (Ni, W, Ta). Results of scanning electron microscope studies are: (1) The initial boundaries migrate to form a system of parallel boundaries. (2) A bamboo-structure boundary migrates towards the tip end but stops at the tip end neck. (3) Measurable boundary grooves are formed. Results of field electron microscope studies are: (1) A migration of the intersection line of the boundary and the surface is directly visible on the screen. (2) Twin boundaries are visible and analysable. (3) The tip end crystal can rotate at the grain boundary until the boundary disappears. It is discussed why such type of experiments are promising for future studies of fundamental recrystallization problems.





Citations (18)


... 3-7), namely, ∂T m (r) ∂r = − q 0 r 2 log(r/r 0 ) → 0 as r → r 0 , so as to get a tangible solution near the cone apex. The maximum temperatureT m = T m (r 0 ) ∼ q 0 r 0 occurs near the conical tip (r = r 0 ) and radially decays along the cone axis away from the tip, whereas the maximum heat flux occurs a few radii below the tip (see [60,80,[90][91][92]) as log(r/r 0 ) ∼ 1. Thus, for a conical tip with r 0 ∼ 10 nm and local irradiation power of about 50 μW, the maximum temperature rise at the tip of the cone is approximately 15 • C (gold) and 12 • C (silver). ...

Reference:

Opto-electo- fluidics and tip coax conical surface plasmons.
Temperature distribution along metal tips
  • Citing Article
  • June 1971

Surface Science

... For example, mass shedding of thick Ni=MgO films with h f ¼ 120 nm indicated λ 0 ≈ 5 μm and τ 0 ≈ 1255 min [61]. As discussed in Ref. [40], using physical parameters from the literature [62][63][64][65][66] ...

A measurement of the surface energy anisotropy of nickel by transmission electron microscopy of field emitter crystals
  • Citing Article
  • November 1984

Surface Science Letters

... However, real material systems are often complex, and various, often unrealistic, assumptions have to be made in the material models in order to solve the mathematical equations [9]. Following the classic work of Herring [10], the finite-difference methods have been used to analyse the microstructure evolution, including grain boundary grooving [11,12], the spheroidization of rod-shaped particles of finite length [13], grain boundary cavitation [14], powder sintering [15] and grain-boundary void growth and shrinkage [16][17][18]. The methods based on finite-difference are conceptually simple and relatively fast. ...

Grain boundary grooving under the influence of evaporation (or corrosion)
  • Citing Article
  • January 1979

Surface Science

... Regardless of the study of emission properties, the bombardment of surfaces by low-energy (up to keV units) atoms and ions with the aim of cleaning them, ion etching, etc is a widely used technological method. The information on the state of surfaces, subjected to ion bombardment accumulated up to date (see, for example, [31][32][33][34] and the literature cited there), allows us to conclude that with low-energy bombardment the surface is modified to a depth of tens of atomic layers. Thus, when a tungsten surface is bombarded with helium ions with an average energy of w i ≈ 150 eV and a current of 0.3-0.4 ...

Surface self-diffusion by ion impact
  • Citing Article
  • July 1978

Surface Science

... The thermal motion of the surface atoms dictates many of the physical and chemical properties such as: surface diffusion [86,87]; anharmonicity leading to roughening transitions [88][89][90]; surface reconstructions [91,92]; which all infl uence the extent of compositional inhomogeneities, including defects. The key descriptive parameter of the dynamic motions of atoms on the surface, as well as in the bulk, is the Debye temperature. ...

Une détermination du coefficient d'autodiffusion de surface en présence d'une couche d'adsorption à l'aide de pointes àémission de champ (nickel sur tungsténe)
  • Citing Article
  • September 1976

Surface Science

... Calculated values of surface diffusivity for the np-RMPEA in the current study, as compared to the constituent refractory elements, indicating that the np-RMPEA exhibits slower diffusion kinetics. Surface diffusivity values for the pure metals were plotted using equations found in references[88][89][90]. ...

A measurement of the surface self-diffusion of tantalum
  • Citing Article
  • June 1981

Surface Science

... It is Fig. 6 The radial distribution function at the Pd K-edge (top) and Rh K-edge (bottom) for the 0.5 % Rh-0.5 % Pd/CeO 2 before and during CO treatment at 400°C Fig. 7 The radial distribution function at the Pd K-edge (top) and Rh K-edge (bottom) for the 0.5 % Rh-0.5 % Pd/CeO 2 catalyst during CO treatment at 400°C. The partial pressure of CO was slowly increased with time 2.5 9 10 -3 for Rh [30,31] and 6 9 10 -4 for Pd [32,33]. The corresponding activation energies for diffusions are 17 and 12 kcal mol -1 (or 71 and 50 kJ mol -1 ) for Rh and Pd respectively. ...

Adsorption, diffusion and self-diffusion on tungsten surfaces with adsorbed palladium
  • Citing Article
  • February 1978

Surface Science

... The phenomena of local heating and charge separation has also been observed by surface-enhanced Raman spectroscopy for other surfaces 77 where the local electric field component can lead to ion emission. 78 Thermal diffusion, on the other hand, provides insufficient thermal contribution to the matrix-analyte system. Consequently, since the MALD process occurs only partially, a subsequent decrease in the ion yield is anticipated and in fact observed. ...

Numerical data and experimental proof of the unified theory of electron emission (Christov)
  • Citing Article
  • March 1974

Surface Science

... While being quite successful at removing the contamination layer from the electrochemically etched tungsten tips [38,53], the annealing process has been reported to routinely lead to the blunting of these heated tips [51][52][53][54][55][56]. In our quest for the sharpest tips, this effect is far from desirable and thus deserves some attention in order to be better understood and prevented. ...

Processus simultane d'évaporation libre et de diffusion de surface
  • Citing Article
  • August 1974

Surface Science

... For most of the metals in vacuum or inert atmospheres [29] k is on the order of 0.125-0.25, which yield slopes less than 0.3 (see Table 1 [30][31][32][33][34][35]). Thus, Mullins' small slope solution yielded reasonable results. ...

Grain boundary groove evolutions by surface self-diffusion on a plane and on a wire
  • Citing Article
  • July 1976

Surface Science