Crystal

Crystal
ID	OSW0bb3b43473aa428fb4e82a2468648e19
UUID	0bb3b434-73aa-428f-b4e8-2a2468648e19
Label	Crystal
Machine compatible name	Crystal
Statements (outgoing)

Statements (incoming)

Description

A material is a crystal if it has essentially a sharp diffraction pattern.

A solid is a crystal if it has essentially a sharp diffraction pattern. The word essentially means that most of the intensity of the diffraction is concentrated in relatively sharp Bragg peaks, besides the always present diffuse scattering. In all cases, the positions of the diffraction peaks can be expressed by

H=∑ni=1hia∗i (n≥3)

Category (Class)

OWL Class
Imported fromA prefixed IRI defining this entry as a imported term. In OSW the prefix must be a registered imported ontology.<br>Definition: OWL Class	https://w3id.org/emmo#EMMO 0bb3b434 73aa 428f b4e8 2a2468648e19
OntologiesOntologies that contain this term<br>Definition: OWL Class	Materials

EmmoClass
Supercategories<br>Definition: Category (Class), OWL Class, EmmoClass	CrystallineMaterial
metaclass<br>Definition: Category (Class), EmmoClass	EmmoClass

Graph

Attachments

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jsondata

rdf_type

"owl:Class"

uuid

"0bb3b434-73aa-428f-b4e8-2a2468648e19"

iri

"https://w3id.org/emmo#EMMO_0bb3b434_73aa_428f_b4e8_2a2468648e19"

name

"Crystal"

label

text	"Crystal"
lang	"en"

description

text

"A material is a crystal if it has essentially a sharp diffraction pattern. A solid is a crystal if it has essentially a sharp diffraction pattern. The word essentially means that most of the intensity of the diffraction is concentrated in relatively sharp Bragg peaks, besides the always present diffuse scattering. In all cases, the positions of the diffraction peaks can be expressed by H=∑ni=1hia∗i (n≥3)"

lang

"en"

text

"A material is a crystal if it has essentially a sharp diffraction pattern. A solid is a crystal if it has essentially a sharp diffraction pattern. The word essentially means that most of the intensity of the diffraction is concentrated in relatively sharp Bragg peaks, besides the always present diffuse scattering. In all cases, the positions of the diffraction peaks can be expressed by H=∑ni=1hia∗i (n≥3)"

lang

"en"