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Table 1.

Eclipsing binaries in the MASCARA sample that exhibit the O’Connell effect.

ASCC Identifier V RA (J2000) Dec (J2000) Period (days) Amplitude (mag) Δm (mmag) Previous detection
307947 V376 And 7.77 02h35′11.6″ +49°51′37″ 0.79867(6) 0.29 44 (1)
449928 HD 219561a 8.40 23h16′21.2″ +41°33′43″ 0.56660(5) 0.28 21
513514 V556 Lyr 8.14 19h25′08.3″ +35°59′58″ 1.4901(3) 0.13 13 (2)
521078 V448 Cyg 8.14 20h06′09.9″ +35°23′10″ 6.519(2) 0.37 18 (3)
558695 V600 Per 7.86 03h19′01.4″ +32°41′16″ 1.4697(1) 0.39 26 (4)
725559 ER Vul 7.35 21h02′25.9″ +27°48′26″ 0.69810(5) 0.13 13 (5)
1017908 V1392 Ori 7.76 06h16′17.9″ +09°01′40″ 1.3881(1) 0.20 24

Notes. Periods include a 3σ confidence interval. The amplitude is that of the full oscillation in the MASCARA band. Δm is the difference in magnitude between the primary (after primary minimum) and secondary (before primary minimum) maxima in the binned light curve. No previous detections of the O’Connell effect in HD 219561 and V1392 Ori were found.

(a)

Identified as NSVS 6156390 in the ASCC-VSX cross-match; identified as TYC 3225-1270-1 in the ASCC catalogue.

References. (1) Djurašević et al. (2008); (2) Hartman et al. (2004); (3) Djurašević et al. (2009); (4) Campos-Cucarella et al. (1997); (5) Olah et al. (1994).

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