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States-TPPI technique achieves two effects for a given indirect dimension (say, dimension F1): '''(1)''' signal frequency discrimination and '''(2)''' displacement of the unmodulated artefact signal from an inconvenient location in the middle of spectrum to the edge.

'''(1)''' is achieved by recording two data sets at each t1 point - with orthogonal phases of the preparation pulse and same receiver phase - and storing them in a separate memory location. These two fid measurements yield one complex data point in F1.

'''(2)''' - by inverting phase of the preparation pulse and the receiver each time when t1 is incremented. The result of this is that the artefact signal at  F1=0 Hz appears at F1=&#177;SW/2 Hz

For example to get two sequential complex data points - on at the evolution delay t1 and the next one at evolution delay t1 + 1/SW four fid's are recoreded:

{|border=1
|-
|complex point #||fid#||phase of prep. pulse||receiver phase
|-
|rowspan=2|1
|1||x||x
|-
|2||y||x
|-
|rowspan=2|2
|3||-x||-x
|-
|4||-y||-x
|}

The data is subsequently processed by the complex Fourier transformation.
===Reference===
<bibtex>
@article{marion1989rrn,
  title={Rapid recording of 2D NMR spectra without phase cycling. Application to the study of hydrogen exchange in proteins},
  author={Marion, D. and Ikura, M. and Tschudin, R. and Bax, A.},
  journal={J. Magn. Reson},
  volume={85},
  number={2},
  pages={393--399},
  year={1989},
  url={http://spin.niddk.nih.gov/bax/lit/spdf/129.pdf}
}
</bibtex>
[[Category:NMR Bibliography]]

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