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== | ||
In the canonical HCP, the ratio between the ''a'' and ''c'' distances is: | In the canonical HCP, the ratio between the ''a'' and ''c'' distances is: | ||
:<math> | :<math> | ||
− | \frac{c}{a} = \sqrt{ \frac{ | + | \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 17:31, 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:
Symmetry
- Crystal Family: Hexagonal
- Particles per unit cell:
- 'inner' particles:
- 'corner' particles:
- Volume of unit cell:
- Dimensionality:
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.
Particle B: inner
Particle Positions (Cartesian coordinates)
Particle A: corners
Particle B: inner
Reciprocal-space Peaks
- Allowed reflections:
- even
- Peak positions:
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+