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Advanced Metallization & Interconnect Systems for Ulsi by Robert Havemann, John Schmitz, Hiroshi Komiyama, Kazuo PDF

By Robert Havemann, John Schmitz, Hiroshi Komiyama, Kazuo Tsubouchi

ISBN-10: 1558993851

ISBN-13: 9781558993853

The MRS Symposium continuing sequence is an across the world acknowledged reference appropriate for researchers and practitioners.

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Extra info for Advanced Metallization & Interconnect Systems for Ulsi Applications in 1996: Materials Research Society Conference Proceedings

Example text

5(a), either a transmission photograph or back-reflection photograph may be taken, and the pattern of spots which are produced lie on ellipses in the transmission case or hyperbolae in the back-reflection case. e. where all the lattice planes are parallel to a common direction, the zone axis) and, consequently, the Laue pattern is able to indicate the symmetry of the crystal. For example, if the beam is directed along a [111] or [100] direction in the crystal, the Laue pattern will show three-fold or four-fold symmetry respectively.

C. reciprocal lattice, and vice versa. A simple geometrical construction using the reciprocal lattice gives the conditions that correspond to Bragg reflection. Thus, if a beam of wavelength λ is incident on the origin of the reciprocal lattice, then a sphere of radius l/λ drawn through the origin will intersect those points which correspond to the reflecting planes of a stationary crystal. 12 in which the reflecting plane AB has a reciprocal point at d*. 14) and the Bragg law is satisfied; the line joining the origin to the operating reciprocal lattice spot is usually referred to as the g-vector.

The reciprocal lattice therefore corresponds to the diffraction spectrum possible from a particular crystal lattice and, since a particular lattice type is characterized by 'absent' reflections the corresponding spots in the reciprocal lattice will also be missing. c. c. reciprocal lattice, and vice versa. A simple geometrical construction using the reciprocal lattice gives the conditions that correspond to Bragg reflection. Thus, if a beam of wavelength λ is incident on the origin of the reciprocal lattice, then a sphere of radius l/λ drawn through the origin will intersect those points which correspond to the reflecting planes of a stationary crystal.

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Advanced Metallization & Interconnect Systems for Ulsi Applications in 1996: Materials Research Society Conference Proceedings by Robert Havemann, John Schmitz, Hiroshi Komiyama, Kazuo Tsubouchi


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