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    • 34. 发明专利
    • DE602005006436D1
    • 2008-06-12
    • DE602005006436
    • 2005-12-15
    • KONINKL PHILIPS ELECTRONICS NV
    • TUKKER TEUNIS WVREHEN JORIS JHENDRIKS BERNARDUS HKUIPER STEIN
    • G02B3/02G02B3/12G11B7/135
    • An optical scanning device for scanning optical record carriers having cover layers of different thicknesses. The scanning device has a first mode for scanning a first optical record carrier, a second mode for scanning a second optical record carrier and a third mode for scanning third optical record carrier. The device comprises an objective lens system and a switchable optical element having a first discrete state and a different, second discrete state. The element comprises: a fluid system including a first fluid and a different, second fluid (19); a wavefront modifier (17); and a fluid system switch for acting on the fluid system to switch between the first and second discrete states of the element. When the element is in the first discrete state, the wavefront modifier (17) is substantially covered by the first fluid, and when the element is in the second discrete state, the wavefront modifier (17) is substantially covered by the second fluid (19). The wavefront modifier includes a non-periodic phase structure including a plurality of stepped annular zones separated by steps, the zones forming a non-periodic radial pattern, and is characterized in that the wavefront modifier further includes an aspherical surface. The scanning device is arranged to operate using the element in the second state to generate spherical aberration when in the second mode, the aspherical surface of the element in the second state compensating for more than half of the spherical aberration due to the objective lens system and second record carrier in combination.
    • 35. 发明专利
    • DK1516323T3
    • 2007-05-14
    • DK03730434
    • 2003-06-11
    • KONINKL PHILIPS ELECTRONICS NV
    • HELLMIG JOACHIM WSTALLINGA SJOERDMIJIRITSKII ANDREITUKKER TEUNIS W
    • G11B7/24038G11B7/241
    • A dual-stack optical data storage medium (20) is described for read out using a focused radiation beam (29) with a wavelength of 400 - 410 nm and a Numerical Aperture (NA) of 0.84 - 0.86. The medium has a substrate (21) and a first stack of layers named L0 (22) comprising a first information layer and a second stack of layers named L1 (23), comprising a second information layer. A radiation beam (29) transparent spacer layer (24) is present between L0 and L1. A transmission stack named TS0 with a thickness d TS0 and an effective refractive index n TS0 contains all layers between L0 and an entrance face (26) of the medium (20). A transmission stack named TS1 with a thickness d TS1 and an effective refractive index n TS1 containing all layers between L1 and the entrance face (26). The spacer layer (24) has a thickness selected from the range 20 - 30 µm, the thickness D TS0 in dependence on the refractive index n TS0 and the thickness D TS1 in dependence on the refractive index n TS0 are within a specified area. In this way a reliable read out of both the first and the second information layer of respectively L0 and L1 is achieved.
    • 36. 发明专利
    • AT350749T
    • 2007-01-15
    • AT03730434
    • 2003-06-11
    • KONINKL PHILIPS ELECTRONICS NV
    • HELLMIG JOACHIM WMIJIRITSKII ANDREITUKKER TEUNIS WSTALLINGA SJOERD
    • G11B7/24038G11B7/241G11B7/24
    • A dual-stack optical data storage medium (20) is described for read out using a focused radiation beam (29) with a wavelength of 400 - 410 nm and a Numerical Aperture (NA) of 0.84 - 0.86. The medium has a substrate (21) and a first stack of layers named L0 (22) comprising a first information layer and a second stack of layers named L1 (23), comprising a second information layer. A radiation beam (29) transparent spacer layer (24) is present between L0 and L1. A transmission stack named TS0 with a thickness d TS0 and an effective refractive index n TS0 contains all layers between L0 and an entrance face (26) of the medium (20). A transmission stack named TS1 with a thickness d TS1 and an effective refractive index n TS1 containing all layers between L1 and the entrance face (26). The spacer layer (24) has a thickness selected from the range 20 - 30 µm, the thickness D TS0 in dependence on the refractive index n TS0 and the thickness D TS1 in dependence on the refractive index n TS0 are within a specified area. In this way a reliable read out of both the first and the second information layer of respectively L0 and L1 is achieved.
    • 40. 发明专利
    • ΜΕΣO ΑΠΟΘΗΚΕΥΣΕΩΣ ΟΠΤΙΚΩΝ ΔΕΔΟΜΕΝΩΝ ΣΕ ΔΥΟ ΣΤΟΙΒΕΣ ΚΑΙ Η ΧΡΗΣΙΜΟΠΟΙΗΣΗ ΕΝΟΣ ΤΕΤΟΙΟΥ ΜΕΣΟΥ
    • CY1107587T1
    • 2013-03-13
    • CY071100429
    • 2007-03-28
    • KONINKL PHILIPS ELECTRONICS NV
    • HELLMIG JOACHIM WMIJIRITSKII ANDREITUKKER TEUNIS WSTALLINGA SJOERD
    • G11B7/24G11B7/24038G11B7/241
    • Έναμέσοαποθηκεύσεωςοπτικώνδεδομένωνδιπλήςστοιβάδος (20) περιγράφεταιδιαανάγνωσημεχρησιμοποίησημιαςεστιασμένηςδέσμηςμέσου (29) μεέναμήκοςκύματος 400-410 nm καιενόςαριθμητικούανοίγματος (ΝΑ) 0.84-0.86. Τομέσοέχειέναυπόστρωμα (21) καιμιαπρώτηστοιβάδαστρώσεωνπουονομάζεται L0 (22) καιπεριέχουνμιαπρώτηστρώσηπληροφορίαςκαιμιαδευτέραστοιβάδαστρώσεωνπουονομάζεται L1 (24), καιπεριέχειμιαδευτέραστρώσηπληροφορίας. Μιαδιαφανήςπαρεμβαλλoμένηστοιβάς (24) δέσμηςακτινοβολίας (29) ευρίσκεταιμεταξύ L0 και L1. Μιαστοιβάςμεταδόσεωςπουονομάζεται TS0 μεπάχος dTso καιαποτελεσματικόδείκτηδιαθλάσεως nTso πουπεριέχειόλεςτιςστρώσειςμεταξύ L0 καιμιαςόψεωςεισόδου (26) τουμέσου (20). Μιαστοίβαςμεταδόσεωςπουονομάζεται TS1 μεπάχος dTs1 καιαποτελεσματικόδείκτηδιαθλάσεως nsτ1 πουπεριέχειόλεςτιςστρώσειςμεταξύ L1 καιτηςόψεωςεισόδου (26). Ηπαρεμβαλλομένηστρώση (24) έχειέναπάχοςπουεκλέγεταιαπότηνπεριοχή 20-30 μm, τοπάχος dTS0 αναλόγωςτουδείκτουδιαθλάσεως nTS1 εμπίπτειεντόςτηςορισθείσηςπεριοχής. Κατάτοντρόποαυτόεπιτυγχάνεταιμιααξιόπιστοςανάγνωσηκαιτηςπρώτηςκαιτηςδευτέραςστρώσεωςπληροφορίαςτηςαντιστοίχου L0 και L1.