Difference between revisions of "Lattice:HCP"
KevinYager (talk | contribs) (→Canonical HCP) |
KevinYager (talk | contribs) (→Reciprocal-space Peaks) |
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− | '''HCP''' ('''Hexagonal close-packed''') is a [[Lattice:Hexagonal|hexagonal]] [[Lattices|lattice]]. It is notable (along with [[Lattice:FCC| | + | '''HCP''' ('''Hexagonal close-packed''') is a [[Lattice:Hexagonal|hexagonal]] [[Lattices|lattice]]. It is notable (along with [[Lattice:FCC|FCC]]) because it achieves the densest possible packing of spheres. It thus arises naturally in many atomic crystals, as well as in colloidal crystals and nanoparticles [[superlattice]]s. |
==Canonical HCP== | ==Canonical HCP== | ||
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\frac{c}{a} = 2 \sqrt{ \frac{2}{3} } = \frac{2\sqrt{6}}{3} \approx 1.633 | \frac{c}{a} = 2 \sqrt{ \frac{2}{3} } = \frac{2\sqrt{6}}{3} \approx 1.633 | ||
</math> | </math> | ||
+ | |||
+ | ===Symmetry=== | ||
+ | * Crystal Family: Hexagonal | ||
+ | * Particles per unit cell: <math>n=2</math> | ||
+ | ** 'inner' particles: <math>1</math> | ||
+ | ** 'corner' particles: <math>1</math> | ||
+ | * Volume of unit cell: <math>V_d=a^2 c \sin(60^{\circ}) = a^2 c \frac{\sqrt{3}}{2}</math> | ||
+ | * Dimensionality: <math>d=3</math> | ||
+ | |||
+ | ===Particle Positions (basis vectors)=== | ||
+ | There are 9 positions, with 2 particles in the unit cell | ||
+ | |||
+ | ====Particle A: corners==== | ||
+ | These are the corners of the hexagonal frame. There are 8 corner positions, which contributes a total of 1 particle. | ||
+ | * <math> 8 \, \mathrm{corners}: \frac{1}{12} + \frac{1}{6} + \frac{1}{12} + \frac{1}{6} + \frac{1}{12} + \frac{1}{6} + \frac{1}{12} + \frac{1}{6} = 1</math> | ||
+ | ** <math>\left(0,0,0\right), \, (0,0,1), \, (0,1,0), \, (1,0,0), \, (0,1,1), \, (1,0,1), \, (1,1,0), \, (1,1,1)</math> | ||
+ | |||
+ | ====Particle B: inner==== | ||
+ | * <math> 1 \, \mathrm{inner} \, \times \, 1 = 2</math> | ||
+ | ** <math>\left(\frac{1}{3},\frac{1}{3},\frac{1}{2} \right) </math> | ||
+ | |||
+ | ===Particle Positions (Cartesian coordinates)=== | ||
+ | |||
+ | ====Particle A: corners==== | ||
+ | * <math>\left(0,0,0\right), \, (0,0,c), \, \left(\frac{b}{2},\frac{\sqrt{3}b}{2},0 \right), \, (a,0,0), \, \left(\frac{b}{2},\frac{\sqrt{3}b}{2},c \right), \, (a,0,c), \, \left(a+\frac{b}{2},\frac{\sqrt{3}b}{2},0 \right), \, \left(a+\frac{b}{2},\frac{\sqrt{3}b}{2},c \right)</math> | ||
+ | |||
+ | ====Particle B: inner==== | ||
+ | * <math>\left(\frac{a}{3}+\frac{b}{6},\frac{\sqrt{3}b}{6},\frac{c}{2} \right)</math> | ||
+ | |||
+ | ===[[Reciprocal-space]] Peaks=== | ||
+ | * Allowed reflections: | ||
+ | ** <math>l</math> even | ||
+ | ** <math>h+2k \neq 3 n</math> | ||
+ | * Peak positions: | ||
+ | *: <math>q_{hkl}=2\pi\left( \frac{(h^2 + hk + k^2)^2}{a^2} + \frac{l^2}{c^2} \right)^{1/2}</math> | ||
===Examples=== | ===Examples=== | ||
====Elemental==== | ====Elemental==== | ||
+ | [http://en.wikipedia.org/wiki/Periodic_table_%28crystal_structure%29 Many elements pack into HCP]. E.g.: | ||
: 4. [http://en.wikipedia.org/wiki/Beryllium Beryllium (Be)] (''a'' = ''b'' = 2.290 Å, ''c'' = 3.588, ''c''/''a'' = 1.567) | : 4. [http://en.wikipedia.org/wiki/Beryllium Beryllium (Be)] (''a'' = ''b'' = 2.290 Å, ''c'' = 3.588, ''c''/''a'' = 1.567) | ||
: 27. [http://en.wikipedia.org/wiki/Cobalt Cobalt (Co)] (''a'' = ''b'' = 2.5071 Å, ''c'' = 4.0695, ''c''/''a'' = 1.623) | : 27. [http://en.wikipedia.org/wiki/Cobalt Cobalt (Co)] (''a'' = ''b'' = 2.5071 Å, ''c'' = 4.0695, ''c''/''a'' = 1.623) | ||
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====Nano==== | ====Nano==== | ||
− | * | + | * Gold nanoparticles |
+ | ** Stoeva et al. [http://pubs.acs.org/doi/abs/10.1021/jp030013%2B Face-Centered Cubic and Hexagonal Closed-Packed Nanocrystal Superlattices of Gold Nanoparticles Prepared by Different Methods] ''J. Phys. Chem. B'' '''2003''', 107 (30), 7441-7448 [http://dx.doi.org/10.1021/jp030013+ doi: 10.1021/jp030013+] | ||
==See Also== | ==See Also== | ||
* [http://en.wikipedia.org/wiki/Close-packing_of_equal_spheres Wikipedia: Close-packing of equal spheres] | * [http://en.wikipedia.org/wiki/Close-packing_of_equal_spheres Wikipedia: Close-packing of equal spheres] | ||
+ | * [[Lattice:AlB2]] |
Latest revision as of 18:31, 10 November 2014
HCP (Hexagonal close-packed) is a hexagonal lattice. It is notable (along with FCC) because it achieves the densest possible packing of spheres. It thus arises naturally in many atomic crystals, as well as in colloidal crystals and nanoparticles superlattices.
Contents
Canonical HCP
In the canonical HCP, the ratio between the a and c distances is:
- Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \frac{c}{a} = 2 \sqrt{ \frac{2}{3} } = \frac{2\sqrt{6}}{3} \approx 1.633 }
Symmetry
- Crystal Family: Hexagonal
- Particles per unit cell: Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle n=2}
- 'inner' particles: Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle 1}
- 'corner' particles: Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle 1}
- Volume of unit cell: Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle V_d=a^2 c \sin(60^{\circ}) = a^2 c \frac{\sqrt{3}}{2}}
- Dimensionality: Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle d=3}
Particle Positions (basis vectors)
There are 9 positions, with 2 particles in the unit cell
Particle A: corners
These are the corners of the hexagonal frame. There are 8 corner positions, which contributes a total of 1 particle.
- Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle 8 \, \mathrm{corners}: \frac{1}{12} + \frac{1}{6} + \frac{1}{12} + \frac{1}{6} + \frac{1}{12} + \frac{1}{6} + \frac{1}{12} + \frac{1}{6} = 1}
- Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \left(0,0,0\right), \, (0,0,1), \, (0,1,0), \, (1,0,0), \, (0,1,1), \, (1,0,1), \, (1,1,0), \, (1,1,1)}
Particle B: inner
- Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle 1 \, \mathrm{inner} \, \times \, 1 = 2}
- Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \left(\frac{1}{3},\frac{1}{3},\frac{1}{2} \right) }
Particle Positions (Cartesian coordinates)
Particle A: corners
- Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \left(0,0,0\right), \, (0,0,c), \, \left(\frac{b}{2},\frac{\sqrt{3}b}{2},0 \right), \, (a,0,0), \, \left(\frac{b}{2},\frac{\sqrt{3}b}{2},c \right), \, (a,0,c), \, \left(a+\frac{b}{2},\frac{\sqrt{3}b}{2},0 \right), \, \left(a+\frac{b}{2},\frac{\sqrt{3}b}{2},c \right)}
Particle B: inner
- Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \left(\frac{a}{3}+\frac{b}{6},\frac{\sqrt{3}b}{6},\frac{c}{2} \right)}
Reciprocal-space Peaks
- Allowed reflections:
- Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle l} even
- Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle h+2k \neq 3 n}
- Peak positions:
- Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle q_{hkl}=2\pi\left( \frac{(h^2 + hk + k^2)^2}{a^2} + \frac{l^2}{c^2} \right)^{1/2}}
Examples
Elemental
Many elements pack into HCP. E.g.:
- 4. Beryllium (Be) (a = b = 2.290 Å, c = 3.588, c/a = 1.567)
- 27. Cobalt (Co) (a = b = 2.5071 Å, c = 4.0695, c/a = 1.623)
- 48. Cadmium (Cd) (a =b = 2.9794 Å, c = 5.6186 Å, c/a = 1.886)
Atomic
- TBD
Nano
- Gold nanoparticles
- Stoeva et al. Face-Centered Cubic and Hexagonal Closed-Packed Nanocrystal Superlattices of Gold Nanoparticles Prepared by Different Methods J. Phys. Chem. B 2003, 107 (30), 7441-7448 doi: 10.1021/jp030013+