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Table 1

Cross sections for the partial waves from an analysis where the five (JP,LZ) states (0+,0), (2-,0), (2+,+-2), (2+,0) and (0-,0) are included.

Table 2

Cross section obtained for the three partial waves obtained when the two with smallest amplitude in the previous table are set to zero.

Table 3

Cross sections for the various final states from the 'five partial wave' analysis.

Table 4

Cross sections for the various final states from the 'three partial wave' analysis.

Table 5

Cross sections for the various final states from the 'single partial wave' analysis.

Table 6

Cross sections obtained from the likelihood analysis of the (KS K+ PI- PI0 + CC) final state.

Table 7

Cross sections obtained from the likelihood analysis of the (KS K+ PI- PI0 + CC) final state.

Table 8

Cross section obtained in the analysis of the KS KS PI+ PI- final state.

Table 9

Cross section for the final states (K*0 K*BAR0) AND (K*+ K*-) measured in the final states (KS KS PI0 PI0) and (K+ K- PI0 PI0) respectively. Data are normalized to the appropriate branching ratios (see paper) and have statistical errors only.

Table 10

Cross sections for the final state (K*0 K*BAR0) derived from combining the analysis of the (K+ PI- K- PI+) AND (KS PI0 K+ PI- + CC) final states, and the final state (K*+ K*-) derived from combining the analysis of the (KS PI0 K+ PI- + CC) and (KS KS PI+ PI+) final state. Statistical errors only.

Table 11

Ratio between the (K*+ K*-) and (K*0 K*BAR0) final state.

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Measurement of K* anti-K* production in two-photon interactions.