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Since <math>\mathbf{a}</math> is generally not known, <math>\mathbf{P}_a^{\perp}</math> can be constructed using the eigen-decomposition of <math>\mathbf{R}</math>, in particular the matrix containing an orthonormal basis of the noise subspace, which is the orthogonal complement of <math>\mathbf{a}</math>. The disadvantages to this approach include altering the visibilities covariance matrix and coloring the white noise term.<ref>{{cite journal
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| title = Spatial Filtering of RF Interference in Radio Astronomy
| journal = IEEE Signal Processing Letters
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This approach requires much more computationally intensive matrix manipulations, and again the visibilities covariance matrix is altered.<ref>{{cite journal
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| title = Radio astronomical imaging in the presence of strong radio interference
| journal = IEEE Transactions on Information Theory
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where <math>\lambda_1(2 \alpha - \alpha^2) \approx \sigma_s^2</math> by selecting the appropriate <math>\alpha</math>. This scheme requires an accurate estimation of the interference term, but does not alter the noise or sources term.<ref>{{cite journal
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| title = Multichannel Interference Mitigation Techniques in Radio Astronomy
| journal = Astrophysical Journal Supplement Series
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