Difference between revisions of "Paper:DNA-nanoparticle superlattices formed from anisotropic building blocks"

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(Created page with "This is a summary/discussion of the results from: * Matthew R. Jones, Robert J. Macfarlane, Byeongdu Lee, Jian Zhang, Kaylie L. Young, Andrew J. Senesi, and Chad A. Mirkin [ht...")
 
(Summary of Mathematics)
 
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* Matthew R. Jones, Robert J. Macfarlane, Byeongdu Lee, Jian Zhang, Kaylie L. Young, Andrew J. Senesi, and Chad A. Mirkin [http://www.nature.com/nmat/journal/v9/n11/full/nmat2870.html DNA-nanoparticle superlattices formed from anisotropic building blocks] ''Nature Materials'' '''2010''', ''9'', 913-917 [http://dx.doi.org/10.1038/nmat2870 doi: 10.1038/nmat2870]
 
* Matthew R. Jones, Robert J. Macfarlane, Byeongdu Lee, Jian Zhang, Kaylie L. Young, Andrew J. Senesi, and Chad A. Mirkin [http://www.nature.com/nmat/journal/v9/n11/full/nmat2870.html DNA-nanoparticle superlattices formed from anisotropic building blocks] ''Nature Materials'' '''2010''', ''9'', 913-917 [http://dx.doi.org/10.1038/nmat2870 doi: 10.1038/nmat2870]
  
This paper describes the formation of nanoparticle [[superlattices] from anisotropic nano-objects. In the [http://www.nature.com/nmat/journal/v9/n11/extref/nmat2870-s1.pdf Supplementary Information] information, the authors describe how to model x-ray scattering data from [[lattice]]s of anisotropic nanoparticles.
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This paper describes the formation of nanoparticle [[superlattices]] from anisotropic nano-objects. In the [http://www.nature.com/nmat/journal/v9/n11/extref/nmat2870-s1.pdf Supplementary Information] information, the authors describe how to model x-ray scattering data from [[lattice]]s of anisotropic nanoparticles.
  
 
===Summary of Mathematics===
 
===Summary of Mathematics===
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</math>
 
</math>
  
Where the '''structure factor''' is defined by an orientational average (randomly oriented crystal(s)):
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Where the '''[[structure factor]]''' is defined by an orientational average (randomly oriented crystal(s)):
 
:<math>
 
:<math>
 
S(q) \equiv \left\langle \frac{|F(\mathbf{q})|^2}{P(q)} S(\mathbf{q}) \right\rangle  
 
S(q) \equiv \left\langle \frac{|F(\mathbf{q})|^2}{P(q)} S(\mathbf{q}) \right\rangle  
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Where ''c'' is a constant, and ''L'' is the [[X-ray peak shape|peak shape]].
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Where ''c'' is a constant, and ''L'' is the [[peak shape|peak shape]]; such as:
 +
:<math>
 +
L = \frac{\sigma_L/(2\pi)}{(q-q_{hkl})^2 + (\sigma_L/2)^2}
 +
</math>
  
The (isotropic) '''form factor intensity''' is an average over all possible particle orientations:
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Note that the presented form of <math>\scriptstyle S(q)</math> is closely-related to the [[lattice factor]]. The (isotropic) '''[[form factor]] intensity''' is an average over all possible particle orientations:
 
:<math>
 
:<math>
 
\begin{alignat}{2}
 
\begin{alignat}{2}
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\end{alignat}
 
\end{alignat}
 
</math>
 
</math>
 +
 +
==Form Factors==
 +
The SI also provides form factors for a variety of nano-object shapes:
 +
* [[Form Factor:Pyramid|Pyramid]]
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* [[Form Factor:Cube|Cube]]
 +
* [[Form Factor:Cylinder|Cylinder]]
 +
* [[Form Factor:Octahedron|Octahedron]]
 +
* Rhombic dodecahedron (RD)
 +
* Triangular prism

Latest revision as of 16:49, 14 January 2015

This is a summary/discussion of the results from:

This paper describes the formation of nanoparticle superlattices from anisotropic nano-objects. In the Supplementary Information information, the authors describe how to model x-ray scattering data from lattices of anisotropic nanoparticles.

Summary of Mathematics

Randomly oriented crystals give scattering intensity:

Where the structure factor is defined by an orientational average (randomly oriented crystal(s)):

and can be computed by:


Where c is a constant, and L is the peak shape; such as:

Note that the presented form of is closely-related to the lattice factor. The (isotropic) form factor intensity is an average over all possible particle orientations:

The form factor amplitude is computed via:

Form Factors

The SI also provides form factors for a variety of nano-object shapes: