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Dot size

Fig. 2. Effect of deposition time and deposition pressure on (a) dot size (inset shows atomic force micrograph of dots formed at O.STorr) (b) dot density. Fig. 2. Effect of deposition time and deposition pressure on (a) dot size (inset shows atomic force micrograph of dots formed at O.STorr) (b) dot density.
Figure 17.8 (A) Photoluminescence spectra of CdSe quantum dots in CHCI3 in the presence of polybutadiene at different times under photoactivation at 400 nm. The blue shift of the photoluminescence spectra is due to a gradual decrease in quantum dot size. (B) Schematic... Figure 17.8 (A) Photoluminescence spectra of CdSe quantum dots in CHCI3 in the presence of polybutadiene at different times under photoactivation at 400 nm. The blue shift of the photoluminescence spectra is due to a gradual decrease in quantum dot size. (B) Schematic...
FIGURE 9.6 The peptide and small protein map from a 100 pL human plasma injection. Columns sample preparation SCX RAM analytical column chromolith performance RP-18, 100 x 0.1 mm I.D. Minute fractions were analyzed using MALDI-TOF MS. Fraction numbers correspond to the time scale. Dot size is related to signal intensity. [Pg.217]

In a study that addressed the effect of doping on quantum dots, the donor and acceptor levels were found to be practically independent of particle size [De3]. In other words, shallow impurities become deep ones if the dot size is reduced. Experimental observations show that the luminescence is not affected by doping if a thermal diffusion process, for example using a POCl3 source, is used [Ell]. Implantation, in contrast, is observed to effectively quench the PL [Tal4]. If the pores are filled with a medium of a large low-frequency dielectric constant, such as water or any other polar solvent, it is found that deep impurity states still exist,... [Pg.154]

Measured D/H ratios in five bulk Stardust particles (black dots sizes represent relative particle sizes), and in micron-size subareas in one particle (open circles enclosed by oval) measured by ion microprobe. The particle compositions overlap D/H ratios in comets, IDPs, and the insoluble organic matter in chondrites. Modified from McKeegan et al. (2006). [Pg.430]

Numerous hydrophilic as well as hydrophobic quantum dots are now commercially available as suspensions in organic or aqueous solvents, yet for a specific coating motif or quantum dot size researchers have the choice between organome-tallic syntheses commonly based on a high-temperature thermolysis [99] of a precursor or sol-gel type aqueous phase syntheses [100]. [Pg.337]

Fig. 1 A series of hexadecylamine-stabilized CdSe quantum dots (sizes range from 2.5 on the far left to 5.2 nm on the far right) excited at 2CXC = 366 nm (image provided by B. Kinkead)... Fig. 1 A series of hexadecylamine-stabilized CdSe quantum dots (sizes range from 2.5 on the far left to 5.2 nm on the far right) excited at 2CXC = 366 nm (image provided by B. Kinkead)...
Fig. 6 Osmotic coefficient 0 versus reduced density n/a3 for monovalent counterions. Heavy dots mark the measurements, while the solid lines are fits which merely serve to guide the eye. The dotted lines are the prediction of PB theory. From top to bottom the Bjerrum length lB/o varies as 1,2,3. The errors in the measurement are roughly as big as the dot size [29]... Fig. 6 Osmotic coefficient 0 versus reduced density n/a3 for monovalent counterions. Heavy dots mark the measurements, while the solid lines are fits which merely serve to guide the eye. The dotted lines are the prediction of PB theory. From top to bottom the Bjerrum length lB/o varies as 1,2,3. The errors in the measurement are roughly as big as the dot size [29]...
In Fig. 4(A) it can be seen that the AFM dot size is almost independent on the dwell time (e-beam irradiation time) while the magnetic dot diameter (MFM) increases almost linearly with the square root of the dwell time. [Pg.267]

Figure 4. (A) Time dependence of AFM (open circle) and magnetic (solid circle) dot size and (B) TEM micrograph of a patterned Co-C film with direct laser lithography. Figure 4. (A) Time dependence of AFM (open circle) and magnetic (solid circle) dot size and (B) TEM micrograph of a patterned Co-C film with direct laser lithography.
The right part of Fig. 5 shows an array of 800 nm Co dots, spaced from each other by 800 nm. Also smaller dot size (150 nm) has been prepared. The improvement is achieved mostly due the selection of a proper substrate that minimizes surface diffusion and mixing within the surface region. Further optimizations may lead to dot sizes with a factor 2-5 smaller [24]. [Pg.269]

In [55] a large-area fabrication of hexagonally ordered metal dot arrays with an area density of 10u/cm2 was demonstrated. The metal dots were produced by an electron beam evaporation followed by a lift-off process. The dots size was 20 nm dots with a 40 nm period by combining block copolymer nanolithography and a trilayer resist technique. A self-assembled spherical-phase block copolymer top layer spontaneously generated the pattern, acting as a template. The pattern was first transferred to a silicon nitride middle layer by reactive ion etch, producing holes. The nitride layer was then used as a mask to further etch into a polyamide bottom layer. [Pg.279]

Figure 16. (A). The virgin curve and full AHE curve of a patterned Co/Pt multilayer with a dot size is 120 nm. The loop is measured form about 200 dots in the area of the Hall cross, (B) SEM image of a 60 nm FePt dot (bright spot) covered with a Pt cross-shaped electrode, (C) AHE loops for 10 and 300 K with an inset of the unpatterned FePt film at 300 K. Figure 16. (A). The virgin curve and full AHE curve of a patterned Co/Pt multilayer with a dot size is 120 nm. The loop is measured form about 200 dots in the area of the Hall cross, (B) SEM image of a 60 nm FePt dot (bright spot) covered with a Pt cross-shaped electrode, (C) AHE loops for 10 and 300 K with an inset of the unpatterned FePt film at 300 K.
The distribution of geochemical data may be presented, in their most basic form, through the use of dot maps in which dots, or other symbols selected by the operator, of a size proportional to concentration are plotted at geographical coordinates for each sampled site. Dot sizes may be classified by means of concentration intervals based on percentiles or other statistical methods. Dot maps are often the most suitable method to represent isolated points of a discrete set of geochemical data. [Pg.162]

One can say that the obtained by us experimental results upon 2D exciton localization (taking place due to the growth of the crystal dielectric permeability anisotropy parameter) with o are very close to [27] where the behaviour of polaron excitons in parabolic quantum dots were considered and shown that the dot size decrease results in increasing the exciton binding energy. [Pg.338]

Figure 7.11 A schematic view of kem dependence on quantum dot size in the case of cadmium selenide... Figure 7.11 A schematic view of kem dependence on quantum dot size in the case of cadmium selenide...
The effect of temperature on dot size is demonstrated in Table 1 ink viscosity is 8cPs, drop volume is 22pl and substrate is grained anodized aluminum plate. [Pg.87]

Fig. 2.16. Adiabatic compressibility of aqueous sodium chloride solutions as a function of salt mole fraction, at various temperatures. The solid line is the calculated compressibility. The expected error is on the order of the dot size. (Reprinted from G. Onori, J. Chem. Phys. 89 510, 1988.)... Fig. 2.16. Adiabatic compressibility of aqueous sodium chloride solutions as a function of salt mole fraction, at various temperatures. The solid line is the calculated compressibility. The expected error is on the order of the dot size. (Reprinted from G. Onori, J. Chem. Phys. 89 510, 1988.)...
Figure 1. Relative PL intensity and PL peak wavelength (Xmax) of CdSe/ZnS (ca. 4x25 nm) film at different applied electric fields in comparison with quantum dots size of 4 nm. Figure 1. Relative PL intensity and PL peak wavelength (Xmax) of CdSe/ZnS (ca. 4x25 nm) film at different applied electric fields in comparison with quantum dots size of 4 nm.
We have studied EB drawing to form very fine dot arrays with fine pitch for 20-30 nm pitched dot arrays pattern using EB drawing with calixarene resist [2] on silicon wafer as the ideal substrate [3-7]. Furthermore, we have to form the fine dot arrays with fine pitch on practical material and substrate because there is a substrate dependence on the formed dot size and dot array pitch because various element dependence on primary electron scattering and charge-up occur as known well. [Pg.456]

Figure 2. SEM image of ultrahigh packed dot arrays resist pattern (a) and resist dot size variations (b) using calixarene (28-44 mC/cm 30 kV, a pitch of 25 nm x 25 nm). Figure 2. SEM image of ultrahigh packed dot arrays resist pattern (a) and resist dot size variations (b) using calixarene (28-44 mC/cm 30 kV, a pitch of 25 nm x 25 nm).
Fig. Spatial distribution of soil gas hydrocarbons at Filo Morado, Argentina (arbitrary coordinates) dot size indicates ethane concentration dot colour indicates Ci/Q ratio, such that green = low (oil), yellow = intermediate, red = high (gas). Fig. Spatial distribution of soil gas hydrocarbons at Filo Morado, Argentina (arbitrary coordinates) dot size indicates ethane concentration dot colour indicates Ci/Q ratio, such that green = low (oil), yellow = intermediate, red = high (gas).
Series of M1-M4 are square dot arrays of various sizes of edge and dot thickness. Media of M5-M9 have the same edge size of but different sizes of with the same thickness of 5 nm except M5 of 10 nm for comparison. Series of MIO-M13 are for investigation of the elongation effect with an increased Dj. The dot size variety is from 7 nm to 22.5 nm, and the thickness is from 2.5 nm to 10 nm. [Pg.121]


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See also in sourсe #XX -- [ Pg.166 ]




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Effects of Pressure and Time on Dot Size

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