A General Method for Single-Stranded DNA Probe Generation

1997 ◽  
Vol 249 (1) ◽  
pp. 114-117 ◽  
Author(s):  
Daniel S. Millican ◽  
Ian M. Bird
RSC Advances ◽  
2021 ◽  
Vol 11 (35) ◽  
pp. 21796-21804
Author(s):  
Seo Won Cho ◽  
Hyun Jeong Lim ◽  
Beelee Chua ◽  
Ahjeong Son

Principle of an ssDNA paired aptasensor where extra dye binding sites are created to enhance its fluorescence response.


Gene ◽  
1986 ◽  
Vol 42 (1) ◽  
pp. 113-117 ◽  
Author(s):  
Jingzhong Liu ◽  
Kenneth D. Lanclos ◽  
Titus H.J. Huisman

2007 ◽  
Vol 126 (2) ◽  
pp. 655-663 ◽  
Author(s):  
Kavita Arora ◽  
Nirmal Prabhakar ◽  
Subhash Chand ◽  
B.D. Malhotra

2014 ◽  
Vol 50 (69) ◽  
pp. 9846-9848 ◽  
Author(s):  
Wenbo Zhao ◽  
Zhen Qin ◽  
Chengsen Zhang ◽  
Meiping Zhao ◽  
Hai Luo

A label-free double amplification system has been developed by using a ternary DNA probe containing the poly(adenine-thymine) sequence assisted by exonuclease III degradation.


Author(s):  
J. R. Fields

The energy analysis of electrons scattered by a specimen in a scanning transmission electron microscope can improve contrast as well as aid in chemical identification. In so far as energy analysis is useful, one would like to be able to design a spectrometer which is tailored to his particular needs. In our own case, we require a spectrometer which will accept a parallel incident beam and which will focus the electrons in both the median and perpendicular planes. In addition, since we intend to follow the spectrometer by a detector array rather than a single energy selecting slit, we need as great a dispersion as possible. Therefore, we would like to follow our spectrometer by a magnifying lens. Consequently, the line along which electrons of varying energy are dispersed must be normal to the direction of the central ray at the spectrometer exit.


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