top of page

Faith Group

Public·16 members

Neon Lines | 4K

The Neon NxT Electroporation System is an electroporation instrument that offers up to 90% transfection and gene-editing efficiency in extremely difficult-to-transfect cells, including immune, primary, and stem cells. Over 150 cell lines have been tested with optimized ready-to-use conditions for efficiency and viability.

Neon Lines | 4K

Avoid the hassle of searching for a buffer kit that will work with your cell line. We have simplified the process with one buffer kit that is compatible with over 150 mammalian cell lines. We recommend using Invitrogen Neon NxT Resuspension R Buffer at voltages below 1,900 V and Invitrogen Neon NxT Resuspension T Buffer at higher voltages.

Figure 5. Performance of the Neon NxT Electroporation System and the Neon Transfection System. Performance was evaluated by transfecting different mammalian cell lines with GFP plasmid DNA or GFP mRNA. (A) GFP plasmid DNA transfection efficiency reported as the percentage of GFP-positive cells. (B) Viability of cells after transfection with GFP plasmid DNA. (C) GFP mRNA transfection efficiency reported as the percentage of GFP-positive cells. (D) Viability of cells after transfection with GFP mRNA.

Larson wanted to hide the triangle just behind the wrist. To hide parts of your neon shape, set the Brush tool to black, select the mask (the white icon on the layer), and brush to remove those sections. To reverse the effect, simply change the brush color to white and paint on the mask to reveal detail again.

The table below contains a listing of the cell lines and primary cells successfully electroporated with the Neon Transfection System (or the predecessor instrument the Microporator MP-100). The hyperlinked cell line names take you to a PDF that gives:

This is an attempt to give a reasonable accurate picture of the appearance of the neon spectrum, but both the images are composite images. The image below is composed of segments of three photographs to make the yellow and green lines more visible along with the much brighter red lines. Then the image below was reduced and superimposed on the image above, because with the exposure reasonable for the bright tube, only the red lines were visible on the photograph.

The prominent mercury lines are at 435.835 nm (blue), 546.074 nm (green), and a pair at 576.959 nm and 579.065 nm (yellow-orange). There are two other blue lines at 404.656 nm and 407.781 nm and a weak line at 491.604 nm.

Neon color spreading (also referred to as neon-like color spreading) is an optical illusion in the category of transparency effects, characterized by fluid borders between the edges of a colored object and the background in the presence of black lines. The illusion was first documented in 1971 and was eventually rediscovered in 1975 by Van Tuijl.[2]

The exact causes of the neon color spreading illusion are not known. It seems to occur most often when black lines are substituted with colored lines on a white background. One theory as to why this happens is that the simultaneous stimulation between the visual processing of lines and the color receptors in the eyes are not congruent. For this reasoning to work neon effects would only be possible if all black lines and colored lines were in contact, however there are illusions where this is not the case.

Other theories about reasons for the effect have proposed that it occurs within non-random patterns. Others state that it is necessary for there to be straight lines for the effect to occur. This is not the case as many neon effects happen within random patterns and on curved lines.

The neon color spreading effect works in a similar way to another illusion: illusory contours. Illusory contours are characterized by the appearance of contours due to the implication that they are there. Neon color spreading is better characterized by the generation of contours by the changing color of black lines. They can both create the perception of contours where there are none.

Illusory contours and neon color spreading are often difficult to differentiate. Neon color spreading is characterized by the color being used to create the visual phenomena. This tricks the visual system into thinking that there is color where there is not. Illusory contours cause a similar fooling of the visual system into perceiving contours by causing effects where the contours should be. They are both fooling the visual system in similar ways, but are characterized differently.

Another aspect of neon color spreading that can affect the magnitude of the illusion are the colors used within the illusion. Different colors tend to cause a less or more intense illusion. Changing the color of the background can also enhance or inhibit the effect. If contrasting colors are used, such as a yellow background with blue and black lines, the effect will be enhanced. If similar colors are used, the effect will be inhibited.

Long and short wavelength light, where the human eye is less sensitive to spatial detail, seem to enhance the effect. This means that if the illusion is created with red or blue lines, black lines, and a white background, the effect will be more intense.[1] This is particularly notable when the colors are more saturated. In contrast to this, green and yellow tend to suppress the effect of neon color spreading when used in the same way.

Another important factor is the luminance of the color causing the effect. Studies have shown that the color should be higher in luminance than the dark lines supporting the effect and it should be lower in luminance than the background.[4]

Ehrenstein figures are a good way of easily making persistent color spreading effects. They are good for showing both the neon color spreading illusion and illusory contours. They are also good for showing examples of differences in hue between inner and outer lines and how they affect the neon color spreading illusion.

Select the new shape with the Selection tool. Go to Object>Path>Simplify. In the Simplify menu, click the Preview option, then experiment with the Curve Precision percentage till your shape is smooth like neon tubing. In this example, I set the Curve Precision to 60%.

The image continuously pops with an amazing degree of fine detail and every aspect of the presentation feels absolutely surreal with the amazing aesthetic of the presentation. Though this release is presented without HDR the image is still stunning from beginning to end. Colors are as impressive as what one will find on the standard high-definition 1080p presentation of the film and the neon-infused style of the cinematography is downright amazing. This film is a great example of how much a filmmaker's creative use of cinematography can help to enhance a filmmakers vision and the rich use of the bright, deep, and creative color tones highlighted in the film enhance every scene. This highly-stylized genre experience is one which has received an excellent 4K transfer that will greatly satisfy viewers, even without the inclusion of high dynamic range.

Options include mercury-argon (253-923 nm), krypton (427-893 nm), neon (540-754 nm), argon (696-1704 nm) and xenon (916-1984 nm) gas-discharge emission sources. With multiple wavelength options and emission lines to utilize, users can more readily choose a source, or combination of sources, to match analytical wavelengths of interest within the measurement range.

A two-crystal X-ray spectrometer system has been implemented in the EAST tokamak to simultaneously diagnose high- and low-temperature plasmas using He- and H-like argon spectra. But for future fusion devices like ITER and Chinese Fusion Engineering Test Reactor (CFETR), argon ions become fully stripped in the core and the intensity of the H-like lines will be significantly at high temperatures (Te > 5 keV). With increasing auxiliary heating power on EAST, the core plasma temperature could also reach 5 keV and higher. In such conditions, the use of a xenon puff becomes an appropriate choice for both ion-temperature and flow-velocity measurements. A new two-crystal system using a quartz 110 crystal (2d = 4.913 Å) to view He-like argon lines and a quartz 011 crystal (2d = 6.686 Å) to view Ne-like xenon spectra has been deployed on a poloidal X-ray crystal spectrometer. While the He-like argon spectra will be used to measure the plasma temperature in the edge plasma region, the Ne-like xenon spectra will be used for measurement in the hot core. The new crystal arrangement allows a wide temperature measurement ranging from 0.5 to 10 keV or even higher, being the first tests for burning plasmas like ITER and CFETR. The preliminary result of lab-tests, Ne-like xenon lines measurement will be presented. 041b061a72


Welcome to the group! You can connect with other members, ge...
bottom of page