The **Burgers vector**, named after Dutch physicist Jan Burgers, is a vector, often denoted **b**, that represents the magnitude and direction of the lattice distortion of dislocation in a crystal lattice.

The vector's magnitude and direction is best understood when the dislocation-bearing crystal structure is first visualized *without* the dislocation, that is, the *perfect* crystal structure. In this perfect crystal structure, a rectangle whose lengths and widths are integer multiples of "a" (the unit cell length) is drawn *encompassing* the site of the original dislocation's origin. Once this encompassing rectangle is drawn, the dislocation can be introduced. This dislocation will have the effect of deforming, not only the perfect crystal structure, but the rectangle as well. Said rectangle could have one of its sides disjoined from the perpendicular side, severing the connection of the length and width line segments of the rectangle at one of the rectangle's corners, and displacing each line segment from each other. What was once a rectangle before the dislocation was introduced is now an open geometric figure, whose opening defines the direction and magnitude of the Burgers vector. Specifically, the breadth of the opening defines the magnitude of the Burgers vector, and, when a set of fixed coordinates is introduced, an angle between the termini of the dislocated rectangle's length line segment and width line segment may be specified.

The direction of the vector depends on the plane of dislocation, which is usually on the closest-packed plane of unit cell. The magnitude is usually represented by equation:

where *a* is the unit cell length of the crystal, ||**b**|| is the magnitude of Burgers vector and h, k, and l are the components of Burgers vector, **b** =

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