EP1217644A1 - Short arc high pressure discharge lamp for use in digital projection techniques - Google Patents
Short arc high pressure discharge lamp for use in digital projection techniques Download PDFInfo
- Publication number
- EP1217644A1 EP1217644A1 EP01127159A EP01127159A EP1217644A1 EP 1217644 A1 EP1217644 A1 EP 1217644A1 EP 01127159 A EP01127159 A EP 01127159A EP 01127159 A EP01127159 A EP 01127159A EP 1217644 A1 EP1217644 A1 EP 1217644A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- anode
- cathode
- pressure discharge
- discharge lamp
- lamp
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
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Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J61/00—Gas-discharge or vapour-discharge lamps
- H01J61/84—Lamps with discharge constricted by high pressure
- H01J61/86—Lamps with discharge constricted by high pressure with discharge additionally constricted by close spacing of electrodes, e.g. for optical projection
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J61/00—Gas-discharge or vapour-discharge lamps
- H01J61/02—Details
- H01J61/04—Electrodes; Screens; Shields
- H01J61/06—Main electrodes
- H01J61/073—Main electrodes for high-pressure discharge lamps
Definitions
- the invention is based on a short-arc high-pressure discharge lamp according to the preamble of claim 1. It is in particular a short-arc high-pressure discharge lamp with a xenon filling, as used in cinema projection.
- the well-known xenon short-arc lamps for projection purposes were on Arc lengths and electrode geometries optimized for the 35 to 70 mm Film projection are ideal.
- the screen diagonals of these films are in the range between 28 and 60 mm. If you put such standard lamps in modern ones digital projection systems with DMD, DLP, LCD and D-ILA technology a mismatch between the lamp and the optical system lost a lot of light that does not reach the screen. This lost Light is converted into heat in the projector and leads to additional ones Problems. So far, this problem could only be solved by a larger one Lamp power, which then requires a higher cooling effort, an optimized Mirror design that places high demands on accuracy and the Simulation effort poses and additional double mirrors, which in turn Bring cooling problems in the reflector volume with them, be solved.
- the object of the present invention is a short-arc lamp with xenon filling according to the preamble of claim 1 to provide a optimal focus of light on small cross sections between 10 and 25 mm, corresponding to the diagonals of the integrators, as in digital Projection techniques (DMD, DLP, LCD and D-ILA) are used, enable.
- DMD digital Projection techniques
- the tip of the conical end portion of the cathode to form as a hemisphere
- Larger hemisphere diameters result in a smaller one Luminance, smaller diameters lead to increased cathode erosion.
- the conical end section of the cathode advantageously has a cone angle ⁇ between 36 and 44 °.
- the frustoconical End portion of the anode for optimal operation a cone angle ⁇ between 90 and 105 °. Sharper geometries lead to severe burn-off the electrode tips, while blunt geometries a strong one Result in shadowing in the projector.
- the lamp should have the lamp with a nominal power P between 0 and 5.5 kW with a lamp current I in A of the relation 22 x P + 38 ⁇ I ⁇ 22 x P + 65 and at a nominal power P between 5, 5 and 12 kW with a lamp current I in A with the relation 10 x P + 100 ⁇ I ⁇ 22 x P + 65. While lower currents reduce the light output in the system, increases with higher ones Flowing erosion of the cathode and the maintenance falls below acceptable Values.
- FIG. 1 shows a short-arc high-pressure discharge lamp according to the invention 1 with an Xe filling.
- the lamp 1 with a power consumption of 3000 W consists of a rotationally symmetrical lamp bulb 2 made of quartz glass at its two ends, a lamp shaft 3, 4 also made of quartz glass.
- An electrode rod is in one shaft 3 5 melted from gas-tight tungsten, the inner end of which Cathode 6 carries.
- In the other lamp shaft 4 there is also an electrode rod 7 melted gas-tight from tungsten, at the inner end one Anode 8 is attached.
- Base systems 9, 10 attached for mounting and electrical contacting.
- the cathode 6 is made up of one of the anodes 8 facing conical end portion 6a and one of the electrode rod 5 facing end portion 6b with a circular cylindrical and frustoconical Section together, being between these two sections 6a, 6b, also referred to as a heat accumulation groove circular cylindrical portion 6c of smaller diameter is located.
- the Tip of the conical end section 6a facing the anode 8 a cone angle ⁇ of 40 ° is a hemisphere with a radius R of 0.6 mm trained.
- the anode 8 consists of a circular cylindrical middle section 8a with a Diameter D of 22 mm and two frustoconical end sections 8b, 8c facing the cathode 6 or the electrode rod 7 are.
- the frustoconical end portion 8c facing the cathode 6 has a plateau AP with a diameter of 6 mm. All sections of the two electrodes 6, 8 are made of tungsten.
- the two electrodes 6, 8 are so opposite in the axis of the lamp bulb 2 attached that there is an electrode gap when the lamp is hot or an arc length of 3.5 mm.
- This lamp can be used in a digital projection system compared to conventional short-arc high-pressure discharge lamps Xenon filling achieve an increase of up to 50%.
Landscapes
- Discharge Lamps And Accessories Thereof (AREA)
- Discharge Lamp (AREA)
- Projection Apparatus (AREA)
- Circuit Arrangements For Discharge Lamps (AREA)
Abstract
Bei einer Kurzbogen-Hochdruckentladungslampe (1) mit einer Xenonfüllung für digitale Projektionszwecke ist der Abstand L in mm der beiden einander zugewandten Endabschnitte (6a, 8c) von Kathode (6) und Anode (8) im Heißzustand der Lampe durch die Relation 0,8 x P <= L <= 1 x P + 1 gegeben, wobei P die Lampenleistung in kW ist. Außerdem folgt der Durchmesser D des kreiszylindrischen Mittelabschnitts (8a) der Anode (8) in mm der Relation D >= 2,1 x L + 10. <IMAGE>In the case of a short-arc high-pressure discharge lamp (1) with a xenon filling for digital projection purposes, the distance L in mm of the two mutually facing end sections (6a, 8c) of the cathode (6) and anode (8) is 0.8 when the lamp is hot x P <= L <= 1 x P + 1, where P is the lamp power in kW. In addition, the diameter D of the circular cylindrical central section (8a) of the anode (8) in mm follows the relation D> = 2.1 x L + 10. <IMAGE>
Description
Die Erfindung geht aus von einer Kurzbogen-Hochdruckentladungslampe
gemäß dem Oberbegriff des Anspruchs 1. Es handelt sich dabei insbesondere
um eine Kurzbogen-Hochdruckentladungslampe mit einer Xenonfüllung,
wie sie in der Kinoprojektion verwendet wird.The invention is based on a short-arc high-pressure discharge lamp
according to the preamble of
Die bekannten Xenon-Kurzbogenlampen für Projektionszwecke wurden auf Bogenlängen und Elektrodengeometrien optimiert, die für die 35 bis 70 mm Filmprojektion ideal sind. Die Bilddiagonalen dieser Filme liegen im Bereich zwischen 28 und 60 mm. Setzt man solche Standard-Lampen in die modernen digitalen Projektionssysteme mit DMD-, DLP-, LCD- und D-ILA-Technik ein, so geht durch die Fehlanpassung zwischen Lampe und optischem System viel Licht verloren, das die Leinwand nicht erreicht. Dieses verlorengegangene Licht wird im Projektor in Wärme umgewandelt und führt zu zusätzlichen Problemen. Bisher konnte diese Problem nur durch eine größere Lampenleistung, die dann einen höhern Kühlaufwand erfordert, ein optimiertes Spiegeldesign, das hohe Anforderungen an die Genauigkeit und den Simulationsaufwand stellt und zusätzliche Doppelspiegel, die wiederum Kühlprobleme im Reflektorvolumen mit sich bringen, gelöst werden. The well-known xenon short-arc lamps for projection purposes were on Arc lengths and electrode geometries optimized for the 35 to 70 mm Film projection are ideal. The screen diagonals of these films are in the range between 28 and 60 mm. If you put such standard lamps in modern ones digital projection systems with DMD, DLP, LCD and D-ILA technology a mismatch between the lamp and the optical system lost a lot of light that does not reach the screen. This lost Light is converted into heat in the projector and leads to additional ones Problems. So far, this problem could only be solved by a larger one Lamp power, which then requires a higher cooling effort, an optimized Mirror design that places high demands on accuracy and the Simulation effort poses and additional double mirrors, which in turn Bring cooling problems in the reflector volume with them, be solved.
Es ist Aufgabe der vorliegenden Erfindung, eine Kurzbogenlampe mit Xenonfüllung
gemäß dem Oberbegriff des Anspruchs 1 bereitzustellen, die eine
optimale Fokussierung des Lichts auf kleine Querschnitte zwischen 10 und
25 mm, entsprechend den Diagonalen der Integratoren, wie sie bei digitalen
Projektionstechniken (DMD, DLP, LCD und D-ILA) Verwendung finden,
ermöglichen.The object of the present invention is a short-arc lamp with xenon filling
according to the preamble of
Diese Aufgabe wird durch die kennzeichnenden Merkmale des Anspruchs 1
gelöst. Besonders vorteilhafte Ausgestaltungen finden sich in den abhängigen
Ansprüchen. Die Lampe ist außerdem vorteilhaft mit einem Lampenstrom
zu betreiben der den Merkmalen des Anspruchs 6 genügt.This object is achieved by the characterizing features of
Durch die Festlegung des Abstands L in mm der beiden einander zugewandten Endabschnitte von Anode und Kathode im Heißzustand der Lampe gemäß der Relation 0,8 x P ≤ L ≤ 1 x P + 1, wobei P die Lampenleistung in kW ist, wird eine optimale Ausleuchtung des Bildfensters erreicht. Bei größeren Bogenlängen geht die Effizienz des Systems, d. h. das Verhältnis von abgegebenem Lichtstrom zu aufgenommener Leistung deutlich nach unten. Ist der Abstand Anode - Kathode kürzer als in der Relation, so sinkt die Lebensdauer der Lampe unter akzeptable Werte.By defining the distance L in mm of the two facing each other End sections of the anode and cathode when the lamp is hot according to the relation 0.8 x P ≤ L ≤ 1 x P + 1, where P is the lamp power in kW, optimal illumination of the picture window is achieved. For larger ones Arc lengths affects the efficiency of the system, i. H. the ratio of delivered Luminous flux to power consumed significantly down. is the anode - cathode distance is shorter than in the relation, so the service life decreases the lamp below acceptable values.
Die stärkere Aufheizung der Anodenvorderfläche (Anodenplateau) bei kürzeren Bögen erfordert auch eine Anpassung der Anodengeometrie. So muss der Durchmesser D der Anode in mm der Relation D ≥ 2,1 x L + 10 genügen, wobei L der Abstand der einander zugewandten Endabschnitte von Anode und Kathode in mm im Heißzustand der Lampe ist.The stronger heating of the anode front surface (anode plateau) with shorter ones Arches also require anode geometry adjustment. So must the diameter D of the anode in mm satisfies the relation D ≥ 2.1 x L + 10, where L is the distance between the facing end sections of the anode and cathode in mm when the lamp is hot.
Vorteilhaft sollte für eine optimale Lichtausbeute bei hoher Lebensdauer der der Kathode zugewandte kegelstumpfförmige Endabschnitt der Anode ein Plateau AP mit einem Durchmesser in mm besitzen, das der Relation 1,8 x L - 1 ≤ AP ≤ 1,8 x L + 1 genügt, wobei L wiederum der Abstand der einander zugewandten Enden von Anode und Kathode in mm im Heißzustand ist. Bei Abweichungen des Anodenplateaudurchmessers nach unten kommt es aufgrund starker Erosion (Kraterbildung) am Anodenplateau zu einer Lebensdauerverkürzung. Im Falle eines größeren Anodenplateaus als durch die Relation gegeben, geht die Systemeffizienz aufgrund der Abschattung zurück.It should be advantageous for an optimal light yield with a long lifespan the frustoconical end portion of the anode facing the cathode Have plateau AP with a diameter in mm that corresponds to the relation 1.8 x L - 1 ≤ AP ≤ 1.8 x L + 1 is sufficient, where L is the distance between each other facing ends of the anode and cathode in mm is hot. at Deviations in the anode plateau diameter downward are due to severe erosion (crater formation) on the anode plateau to shorten the service life. In the case of a larger anode plateau than the relation given the system efficiency decreases due to the shadowing.
Für eine optimale Leuchtdichteverteilung über die gesamte Lebensdauer ist weiterhin vorteilhaft die Spitze des kegelförmigen Endabschnitts der Kathode als Halbkugel auszubilden, wobei der Radius R der Halbkugel in mm der Relation 0,12 x P + 0,1 ≤ R ≤ 0,12 x P + 0,5 mit P als Lampenleistung in kW genügt. Größere Durchmesser der Halbkugel resultieren in einer geringeren Leuchtdichte, kleinere Durchmesser führen zu einem verstärkten Kathodenabbrand.For an optimal luminance distribution over the entire service life further advantageously the tip of the conical end portion of the cathode to form as a hemisphere, the radius R of the hemisphere in mm of Relation 0.12 x P + 0.1 ≤ R ≤ 0.12 x P + 0.5 with P as lamp power in kW enough. Larger hemisphere diameters result in a smaller one Luminance, smaller diameters lead to increased cathode erosion.
Vorteilhaft besitzt der kegelförmige Endabschnitt der Kathode einen Kegelwinkel α zwischen 36 und 44°. Außerdem weist der kegelstumpfförmige Endabschnitt der Anode für einen optimalen Betrieb einen Kegelwinkel β zwischen 90 und 105° auf. Spitzere Geometrien führen zu einem starken Abbrand der Elektrodenspitzen, während stumpfere Geometrien eine starke Abschattung im Projektor zur Folge haben.The conical end section of the cathode advantageously has a cone angle α between 36 and 44 °. In addition, the frustoconical End portion of the anode for optimal operation a cone angle β between 90 and 105 °. Sharper geometries lead to severe burn-off the electrode tips, while blunt geometries a strong one Result in shadowing in the projector.
Für einen optimalen Betrieb mit einer ausreichend hohen Effizienz (Lumen/W) und einem akzeptablen Lichtstromrückgang über die Lebensdauer der Lampe sollte die Lampe bei einer Nennleistung P zwischen 0 und 5,5 kW mit einem Lampenstrom I in A der Relation 22 x P + 38 ≤ I ≤ 22 x P + 65 und bei einer Nennleistung P zwischen 5, 5 und 12 kW mit einem Lampenstrom I in A der Relation 10 x P + 100 ≤ I ≤ 22 x P + 65 betrieben werden. Während geringere Ströme die Lichtausbeute im System herabsetzen, steigt bei höheren Strömen die Erosion der Kathode und die Maintenance unterschreitet akzeptable Werte. For optimal operation with a sufficiently high efficiency (lumens / W) and an acceptable decrease in luminous flux over the lifetime The lamp should have the lamp with a nominal power P between 0 and 5.5 kW with a lamp current I in A of the relation 22 x P + 38 ≤ I ≤ 22 x P + 65 and at a nominal power P between 5, 5 and 12 kW with a lamp current I in A with the relation 10 x P + 100 ≤ I ≤ 22 x P + 65. While lower currents reduce the light output in the system, increases with higher ones Flowing erosion of the cathode and the maintenance falls below acceptable Values.
Mit den folgenden Figuren soll die Erfindung anhand eines Ausführungsbeispiels
näher erläutert werden:
In Figur 1 ist eine erfindungsgemäße Kurzbogen-Hochdruckentladungslampe
1 mit einer Xe-Füllung dargestellt. Die Lampe 1 mit einer Leistungsaufnahme
von 3000 W besteht aus einem rotationssymmetrischen Lampenkolben
2 aus Quarzglas an dessen beiden Enden je ein Lampenschaft 3, 4 ebenfalls
aus Quarzglas angesetzt ist. In den einen Schaft 3 ist ein Elektrodenstab
5 aus Wolfram gasdicht eingeschmolzen, dessen inneres Ende eine
Kathode 6 trägt. In den anderen Lampenschaft 4 ist ebenfalls ein Elektrodenstab
7 aus Wolfram gasdicht eingeschmolzen, an dessen innerem Ende eine
Anode 8 befestigt ist. An den äußeren Enden der Elektrodenschäfte 3, 4 sind
Sockelsysteme 9, 10 zur Halterung und zur elektrischen Kontaktierung angebracht.FIG. 1 shows a short-arc high-pressure discharge lamp according to the
Wie aus der Figur 2 ersichtlich setzt sich die Kathode 6 aus einem der Anode
8 zugewandten kegelförmigen Endabschnitt 6a und einem dem Elektrodenstab
5 zugewandten Endabschnitt 6b mit einem kreiszylindrischen und kegelstumpfförmigen
Teilabschnitt zusammen, wobei sich zwischen diesen
beiden Abschnitten 6a, 6b ein, als Wärmestaunut bezeichneter, ebenfalls
kreiszylindrischer Abschnitt 6c von kleinerem Durchmesser befindet. Die
Spitze des der Anode 8 zugewandten kegelförmigen Endabschnitts 6a mit
einem Kegelwinkel α von 40° ist als Halbkugel mit einem Radius R von 0,6
mm ausgebildet. As can be seen from FIG. 2, the
Die Anode 8 besteht aus einem kreiszylindrischen Mittelabschnitt 8a mit einem
Durchmesser D von 22 mm und zwei kegelstumpfförmigen Endabschnitten
8b, 8c die der Kathode 6 bzw. dem Elektrodenstab 7 zugewandt
sind. Das der Kathode 6 zugewandte kegelstumpfförmige Endabschnitt 8c
besitzt ein Plateau AP mit einem Durchmesser von 6 mm. Alle Abschnitte
der beiden Elektroden 6, 8 bestehen aus Wolfram.The
Die beiden Elektroden 6, 8 sind in der Achse des Lampenkolbens 2 so gegenüberstehend
angebracht, dass sich im Heißzustand der Lampe ein Elektrodenabstand
bzw. eine Bogenlänge von 3, 5 mm ergibt.The two
Mit dieser Lampe lässt sich bei Einsatz in einem digitalen Projektionssystem gegenüber den herkömmlichen Kurzbogen-Hochruckentladungslampen mit Xenon-Füllung eine Steigerung von bis zu 50 % erzielen.This lamp can be used in a digital projection system compared to conventional short-arc high-pressure discharge lamps Xenon filling achieve an increase of up to 50%.
Claims (6)
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE10063938A DE10063938A1 (en) | 2000-12-20 | 2000-12-20 | Short arc high pressure discharge lamp for digital projection techniques |
DE10063938 | 2000-12-20 |
Publications (2)
Publication Number | Publication Date |
---|---|
EP1217644A1 true EP1217644A1 (en) | 2002-06-26 |
EP1217644B1 EP1217644B1 (en) | 2009-01-07 |
Family
ID=7668251
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP01127159A Expired - Lifetime EP1217644B1 (en) | 2000-12-20 | 2001-11-15 | Short arc high pressure discharge lamp for use in digital projection techniques |
Country Status (8)
Country | Link |
---|---|
US (1) | US6573657B2 (en) |
EP (1) | EP1217644B1 (en) |
JP (1) | JP4261795B2 (en) |
KR (1) | KR20020050177A (en) |
CN (1) | CN1316550C (en) |
CA (1) | CA2365357C (en) |
DE (2) | DE10063938A1 (en) |
TW (1) | TW527623B (en) |
Cited By (3)
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WO2009121400A1 (en) * | 2008-04-01 | 2009-10-08 | Osram Gesellschaft mit beschränkter Haftung | Method for producing a high-pressure discharge lamp, method for producing light using a high-pressure discharge lamp and digital video projector |
DE102010003381A1 (en) * | 2010-03-29 | 2011-09-29 | Osram Gesellschaft mit beschränkter Haftung | A method for providing an AC gas discharge lamp, method for providing light by means of this AC gas discharge lamp and illumination device with this AC gas discharge lamp |
EP2390902A1 (en) * | 2010-05-03 | 2011-11-30 | Osram Gesellschaft mit Beschränkter Haftung | Noble gas short arc discharge lamp |
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---|---|---|---|---|
US6578970B2 (en) * | 2001-09-19 | 2003-06-17 | Advanced Radiation Corporation | Point-like lamp with anode chimney |
DE10209426A1 (en) * | 2002-03-05 | 2003-09-18 | Patent Treuhand Ges Fuer Elektrische Gluehlampen Mbh | Short-arc high pressure discharge lamp |
JP4042605B2 (en) * | 2003-03-31 | 2008-02-06 | ウシオ電機株式会社 | Xenon lamp |
JP4259282B2 (en) * | 2003-11-07 | 2009-04-30 | ウシオ電機株式会社 | High pressure discharge lamp |
JP4556656B2 (en) * | 2004-12-14 | 2010-10-06 | ウシオ電機株式会社 | Short arc type mercury lamp |
US20060175973A1 (en) * | 2005-02-07 | 2006-08-10 | Lisitsyn Igor V | Xenon lamp |
WO2008074361A1 (en) * | 2006-12-18 | 2008-06-26 | Osram Gesellschaft mit beschränkter Haftung | Electrode for a discharge lamp |
EP2201594A1 (en) * | 2007-09-21 | 2010-06-30 | Osram Gesellschaft mit beschränkter Haftung | Direct-current discharge lamp |
DE102008062677A1 (en) | 2008-12-17 | 2010-06-24 | Osram Gesellschaft mit beschränkter Haftung | discharge lamp |
JP4706779B2 (en) * | 2008-12-19 | 2011-06-22 | ウシオ電機株式会社 | Super high pressure mercury lamp |
JP5276485B2 (en) * | 2009-03-13 | 2013-08-28 | 株式会社オーク製作所 | Short arc type discharge lamp |
DE102009054670A1 (en) | 2009-12-15 | 2011-06-16 | Osram Gesellschaft mit beschränkter Haftung | Electrode i.e. anode, for use in e.g. xenon- or mercury-vapor short-arc lamp, has core extending in longitudinal direction and partially surrounded by cylindrical shell that is made of material, where material consists of carbon |
DE102010030992A1 (en) | 2010-07-06 | 2012-01-12 | Osram Gesellschaft mit beschränkter Haftung | Short arc lamp discharge lamp |
JP6292431B2 (en) * | 2012-08-24 | 2018-03-14 | 河北ライティングソリューションズ株式会社 | Cathode for discharge lamp |
JP5812053B2 (en) * | 2013-04-24 | 2015-11-11 | ウシオ電機株式会社 | Short arc type discharge lamp |
JP6361905B2 (en) * | 2013-09-12 | 2018-07-25 | 河北ライティングソリューションズ株式会社 | Cathode for discharge lamp |
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-
2000
- 2000-12-20 DE DE10063938A patent/DE10063938A1/en not_active Withdrawn
-
2001
- 2001-11-15 DE DE50114638T patent/DE50114638D1/en not_active Expired - Lifetime
- 2001-11-15 EP EP01127159A patent/EP1217644B1/en not_active Expired - Lifetime
- 2001-11-22 TW TW090128906A patent/TW527623B/en not_active IP Right Cessation
- 2001-12-13 US US10/013,503 patent/US6573657B2/en not_active Expired - Lifetime
- 2001-12-17 JP JP2001382587A patent/JP4261795B2/en not_active Expired - Fee Related
- 2001-12-18 CA CA2365357A patent/CA2365357C/en not_active Expired - Fee Related
- 2001-12-20 CN CNB011433604A patent/CN1316550C/en not_active Expired - Fee Related
- 2001-12-20 KR KR1020010081627A patent/KR20020050177A/en not_active Application Discontinuation
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DE3716485C1 (en) * | 1987-05-16 | 1988-11-24 | Heraeus Gmbh W C | Xenon short-arc discharge lamp |
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PATENT ABSTRACTS OF JAPAN vol. 1996, no. 01 31 January 1996 (1996-01-31) * |
PATENT ABSTRACTS OF JAPAN vol. 1997, no. 08 29 August 1997 (1997-08-29) * |
PATENT ABSTRACTS OF JAPAN vol. 1997, no. 10 31 October 1997 (1997-10-31) * |
PATENT ABSTRACTS OF JAPAN vol. 2000, no. 02 29 February 2000 (2000-02-29) * |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
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WO2009121400A1 (en) * | 2008-04-01 | 2009-10-08 | Osram Gesellschaft mit beschränkter Haftung | Method for producing a high-pressure discharge lamp, method for producing light using a high-pressure discharge lamp and digital video projector |
DE102010003381A1 (en) * | 2010-03-29 | 2011-09-29 | Osram Gesellschaft mit beschränkter Haftung | A method for providing an AC gas discharge lamp, method for providing light by means of this AC gas discharge lamp and illumination device with this AC gas discharge lamp |
EP2390902A1 (en) * | 2010-05-03 | 2011-11-30 | Osram Gesellschaft mit Beschränkter Haftung | Noble gas short arc discharge lamp |
Also Published As
Publication number | Publication date |
---|---|
CA2365357C (en) | 2010-10-26 |
KR20020050177A (en) | 2002-06-26 |
CA2365357A1 (en) | 2002-06-20 |
CN1360333A (en) | 2002-07-24 |
CN1316550C (en) | 2007-05-16 |
US6573657B2 (en) | 2003-06-03 |
TW527623B (en) | 2003-04-11 |
DE10063938A1 (en) | 2002-07-04 |
US20020074943A1 (en) | 2002-06-20 |
JP2002260589A (en) | 2002-09-13 |
EP1217644B1 (en) | 2009-01-07 |
JP4261795B2 (en) | 2009-04-30 |
DE50114638D1 (en) | 2009-02-26 |
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