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Manipulation pushing

In this paper, we address the manipulation of the Csq on the Si(OOl) surface. The manipulation has been achieved at room temperature with STM [5-7]. Different regimes of manipulation (pushing and pulling) have been identified [6] depending on the tip height. [Pg.499]

Scanning probes can also be used to manipulate atoms and molecules individually, placing the tip in contact with the subject atom and pushing or pulling (atoms stick to the tip by virtue of the van der Waals force). [Pg.812]

The motion of droplets in solution was used to manipulate micro-partides on surfaces. The didiloromethane droplet pushed aside hydrophilic glass beads of about... [Pg.288]

Indoles, which are especially electron-rich and thus unsuitable for ordinary Diels-Alder reactions, have performed successfully in the cation-radical reaction as dienophiles (Scheme 44)107 and as dienes (Scheme 45)126. Interestingly, the site of annulation (across the C—C or the C—N bond) in vinylindole cation radicals (functioning as dienes for eneamine dienophiles) may be manipulated by varying the substituent on the enamine and thereby altering its push-pull nature (Scheme 45). [Pg.1322]

Fig. 65. (left) Vacancies on a silver surface can be manipulated by using an STM tip to move a neighbouring molecule into the gap. Here Bohringer et al. (University of Lausanne) show how the six vacancies in (a) can be repositioned into a rectangular cluster (d). (right) The beads in this abacus are 60 molecules less than 1 nm in diameter positioned on a silicon surface. They can be pushed back and forth with an STM tip in a controlled fashion to count from 1 to 10... [Pg.158]

Tool to close vials 2, arm of the manipulator 3, rod to push vials 4, ball cock 5, exit channel 6, exit container for vials 7, venting valve 8, vacuum valve 9, vacuum pump. [Pg.237]

Fig. 2. Tip height curves during manipulation of (a) a Cu-atom, (b, c) a Pb-atom, (d) a CO molecule and (e—g) a Pb-dimer along step edges on Cu(211). The tip is moved from left to right and respective tunneling resistances are indicated. The vertical dotted lines correspond to fee sites next to the step edge. The initial sites of the manipulated particles are indicated. Notice that in the attractive manipulation modes (a,b,e,f,g pulling and c sliding) the particles first hop towards the tip and then follow it, whereas in the repulsive mode (d pushing) the particle performs hops away from the tip [4] (image supplied by L. Bartels). Fig. 2. Tip height curves during manipulation of (a) a Cu-atom, (b, c) a Pb-atom, (d) a CO molecule and (e—g) a Pb-dimer along step edges on Cu(211). The tip is moved from left to right and respective tunneling resistances are indicated. The vertical dotted lines correspond to fee sites next to the step edge. The initial sites of the manipulated particles are indicated. Notice that in the attractive manipulation modes (a,b,e,f,g pulling and c sliding) the particles first hop towards the tip and then follow it, whereas in the repulsive mode (d pushing) the particle performs hops away from the tip [4] (image supplied by L. Bartels).
This detailed picture of the movement of the atom during manipulation was achieved with the aid of simulations [6]. The atom moves in a local potential minimum on the surface. This potential is the sum of the surface potential and the tip potential. The surface potential can be expressed by the migration barrier while the tip potential describes the direct interaction via chemical or electrostatic forces. The local potential minimum is not identical with the adsorption site, in the limit of close tip-atom separation this minimum always resides below the tip resulting in the sliding mode. The atom is slowly pushed/pulled by the tip out of the adsorption site until it jumps into the next local potential minimum. The jump to the next potential minimum proceeds on a timescale of picoseconds [7,8] whereas typical tip speeds are of the order of 0.5-2.5nm/s. [Pg.188]

Fig. 6. Manipulation curves of C6o molecules on a Si(100)-2 x 1 surface demonstrating (a) pulling and (b) pushing mode, (c) Probability distribution for successful attempts as a function of relative tip-surface separation (initial parameters U = —3V and I = -0.1 nA) [15],... Fig. 6. Manipulation curves of C6o molecules on a Si(100)-2 x 1 surface demonstrating (a) pulling and (b) pushing mode, (c) Probability distribution for successful attempts as a function of relative tip-surface separation (initial parameters U = —3V and I = -0.1 nA) [15],...
A further step towards the implementation of a molecular switch is to use manipulation techniques to reversibly modify the molecular conformation. The switching of a single leg in and out of the porphyrin plane is possible by lateral and vertical movement of the tip to push the leg down. By measuring the current passing through a single leg in real time during its... [Pg.195]

The pumping energy that is invested to overcome the valve differential is wasted energy. The amount of this waste is the difference between the pressure required to "push" (transport) the fluid into the process (see AP in Figure 2.60) and the pump curve of the constant-speed pump. Pumps are selected to be able to meet the maximum possible flow demand, and therefore, most of the time they operate at partial loads. Consequently, using control valves to manipulate the flow of constant-speed pumps wastes energy and thereby increases operating cost. [Pg.211]

What happens if two nucleic acids are partly complementary and partly different In this case, some stretches of the two strands may form base pairs while others don t. The two molecules can be manipulated so that they form a hybrid or separate. The conditions favoring the formation of duplex nucleic acid are low temperature (below the Tm), high salt, and the absence of organic solvents. The latter two conditions raise the Tm of the hybrid duplex so that the DNA would remain more double-stranded. On the other hand, higher temperatures (closer to the Tm of the hybrid) lower salt, and the presence of organic solvents would tend to push the two strands of the DNA apart. [Pg.169]


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See also in sourсe #XX -- [ Pg.360 ]




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