Alles um Liebe?

Schwander, Hans-Peter

doi:10.1007/978-3-322-90307-5

1997

DOI: 10.1007/978-3-322-90307-5

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Alles um Liebe?

Hans-Peter Schwander¹

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1998

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“…This means The goal of this brief note is to present an iterative algorithm for that each column contains at most one 0 followed by a 1, solving discrete tomography problems which arise in electron ( 0 1 ); and at most one 1 followed by a 0, ( 1 0 ). microscopy of crystals [1]. Here, we consider crystals with an 2.…”

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Iterative algorithm for discrete tomography

Patch¹

1998

Int. J. Imaging Syst. Technol.

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The general limited-angle problem is underdetermined. This in discrete tomography. However, electron microscopy of crystals is a terminology is used in the following theorem. much more specific problem, and is subject to stringent mathematical conditions. Using a constructive argument, we show that under these APPENDIX Matlab Routines. Two Matlab .m files are listed below. The first, gendata.m, takes a matrix (like any of the three phantoms shown in Section II) and the tangent of the angle at which the diagonals are measured. (See Fig. 1 in main text.) gendata.m Phantom 2.returns the diagonal data in a column vector.

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confidence: 99%

Iterative algorithm for discrete tomography

Patch¹

1998

Int. J. Imaging Syst. Technol.

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Alles um Liebe?

Cited by 1 publication

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Iterative algorithm for discrete tomography

Iterative algorithm for discrete tomography

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