EP0941496A1 - Lame de phase annulaire pour la realisation d'un contraste de phase positif - Google Patents
Lame de phase annulaire pour la realisation d'un contraste de phase positifInfo
- Publication number
- EP0941496A1 EP0941496A1 EP98948715A EP98948715A EP0941496A1 EP 0941496 A1 EP0941496 A1 EP 0941496A1 EP 98948715 A EP98948715 A EP 98948715A EP 98948715 A EP98948715 A EP 98948715A EP 0941496 A1 EP0941496 A1 EP 0941496A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- phase
- layer
- substrate
- putty
- refractive index
- 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.)
- Withdrawn
Links
- 239000000758 substrate Substances 0.000 claims abstract description 24
- 239000010409 thin film Substances 0.000 claims abstract description 8
- 239000004568 cement Substances 0.000 claims abstract description 5
- 230000010363 phase shift Effects 0.000 claims description 28
- BQCADISMDOOEFD-UHFFFAOYSA-N Silver Chemical compound [Ag] BQCADISMDOOEFD-UHFFFAOYSA-N 0.000 claims description 10
- 229910052709 silver Inorganic materials 0.000 claims description 10
- 239000004332 silver Substances 0.000 claims description 10
- 239000003989 dielectric material Substances 0.000 claims description 3
- 239000011159 matrix material Substances 0.000 claims description 3
- 239000005304 optical glass Substances 0.000 claims description 3
- 239000013078 crystal Substances 0.000 claims description 2
- 229920003023 plastic Polymers 0.000 claims description 2
- 239000004033 plastic Substances 0.000 claims description 2
- OGIDPMRJRNCKJF-UHFFFAOYSA-N titanium(II) oxide Chemical class [Ti]=O OGIDPMRJRNCKJF-UHFFFAOYSA-N 0.000 claims description 2
- 239000006117 anti-reflective coating Substances 0.000 claims 1
- 230000007423 decrease Effects 0.000 claims 1
- 239000010408 film Substances 0.000 abstract 1
- 230000001105 regulatory effect Effects 0.000 abstract 1
- 230000005540 biological transmission Effects 0.000 description 16
- 239000011521 glass Substances 0.000 description 4
- 238000000034 method Methods 0.000 description 3
- 229910018072 Al 2 O 3 Inorganic materials 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 230000000149 penetrating effect Effects 0.000 description 1
- 238000007740 vapor deposition Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B21/00—Microscopes
- G02B21/06—Means for illuminating specimens
- G02B21/08—Condensers
- G02B21/14—Condensers affording illumination for phase-contrast observation
Definitions
- the invention relates to a phase ring for realizing a positive phase contrast.
- the microscopic phase contrast method has been known since Zernike.
- so-called phase rings are produced by vapor deposition of one or more thin layers on a substrate base, for example made of optical glass.
- a clever choice of the layer thickness succeeds in delaying the phase of the direct light - i.e. the light beam that passes through the vapor-deposited phase ring - compared to the phase of the diffracted light - i.e. the light beam not penetrating the phase ring - for example by ⁇ / 2 or to accelerate ⁇ / 2.
- the latter case is a so-called "positive" phase contrast.
- FIG. 1 b a reduced top view of that shown in FIG. 1 a;
- 5b shows a graphical representation of the transmission of an uncemented phase ring as a function of the wavelength ⁇ , specifically for an Ag layer thickness of 34.5 nm;
- 6b a graphical representation of the course of the transmission as a function of the wavelength ⁇ for a thin-layer system according to FIG. 6a; 7a: a graphical representation of a phase shift as a function of the wavelength ⁇ for a putty for which the following applies: n putty ⁇ n ⁇
- FIG. 1a The layer sequence of a cemented phase ring according to the invention is shown schematically in FIG. 1a.
- a ring made of silver (Ag) is vapor-deposited on a substrate - for example on a glass plate or a glass lens - and a dielectric layer with a refractive index n H is placed on it .
- n H a refractive index
- FIG. 1b shows a plan view - in a reduced form - of what is shown in FIG. 1a, the two areas (direct
- FIG. 2 shows a non-cemented embodiment.
- An optical glass or another transparent medium - for example crystals, plastics - is used as the substrate material.
- Layer system is a layer sequence of silver and a dielectric material, e.g. B. a titanium-oxygen compound.
- a dielectric material e.g. B. a titanium-oxygen compound.
- Layer system it is also possible that Layer system to be additionally provided with a reflection-reducing layer.
- the application of these structures is known for example from DE-PS 2 261 780. A so-called Menzel three-slit is used to measure the specific phase shift.
- Fig. 3 is another embodiment of a cemented
- 4a shows the phase shift of a cemented phase ring as a function of the wavelength ⁇ in a graphic representation. It can be seen that the four measured values in the range between 425 nm and 600 nm are between 50 ° and 55 °.
- the transmission values determined for this example (the thickness of the
- the transmission of the overall system is first determined via the thickness of the silver layer. This is associated with a phase shift.
- the layer with the thickness n 2 primarily protects the silver; it consists z. B. from an oxide (Al 2 O 3 ) of suitable thickness, for. B. 5 nm.
- the setting of the desired phase shift ⁇ takes place primarily with the n layer. The relationship applies to this:
- ⁇ s (n Kltt - n 1 ) - d 1 .
- FIG. 5a graphically illustrates how, in the case of an uncondensed phase ring according to FIG. 2, the phase shift as a function of the
- FIG. 6a shows a graphical representation of the phase shift as a function of the wavelength ⁇ for a putty with the refractive index n Kltt > n.
- the phase shift is 59% at a ⁇ of 437 nm and at a ⁇ of 482 nm at 71%, at a ⁇ of 546 nm at 64% and at a ⁇ of 585 nm at 72%.
- the course of the transmission T is shown as a function of the wavelength ⁇ in FIG. 6b, with a transmission of 28% at a ⁇ value of 425 nm and a transmission T of approximately 12 at a ⁇ of approximately 600 nm % is achieved.
- the present invention it is therefore possible to achieve a positive phase contrast with a largely constant phase shift of 50 ° to 55 ° in the wavelength range between 425 nm and 600 nm with a transmission characteristic of T (at 425 nm) of approx. 35% to T (at 600 nm) between 15-20%.
- T at 425 nm
- the present invention enables any positive phase shift to be set between 40 ° and 60 °.
Landscapes
- Physics & Mathematics (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Polarising Elements (AREA)
- Microscoopes, Condenser (AREA)
- Optical Modulation, Optical Deflection, Nonlinear Optics, Optical Demodulation, Optical Logic Elements (AREA)
Abstract
Applications Claiming Priority (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE19743027 | 1997-09-29 | ||
DE19743027A DE19743027A1 (de) | 1997-09-29 | 1997-09-29 | Phasenring zur Realisierung eines positiven Phasenkontrastes |
PCT/DE1998/002228 WO1999017145A1 (fr) | 1997-09-29 | 1998-08-03 | Lame de phase annulaire pour la realisation d'un contraste de phase positif |
Publications (1)
Publication Number | Publication Date |
---|---|
EP0941496A1 true EP0941496A1 (fr) | 1999-09-15 |
Family
ID=7844023
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP98948715A Withdrawn EP0941496A1 (fr) | 1997-09-29 | 1998-08-03 | Lame de phase annulaire pour la realisation d'un contraste de phase positif |
Country Status (6)
Country | Link |
---|---|
US (1) | US6212009B1 (fr) |
EP (1) | EP0941496A1 (fr) |
JP (1) | JP4199833B2 (fr) |
CN (2) | CN1267761C (fr) |
DE (1) | DE19743027A1 (fr) |
WO (1) | WO1999017145A1 (fr) |
Families Citing this family (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP5285306B2 (ja) * | 2008-03-06 | 2013-09-11 | 豊 末永 | 光学部品及び光学部品を用いた位相差顕微鏡 |
DE102011006018A1 (de) | 2011-03-24 | 2012-09-27 | Hilti Aktiengesellschaft | Befestigungssystem |
JP7031740B2 (ja) * | 2018-06-05 | 2022-03-08 | 株式会社ニコン | 位相板、対物レンズ、及び観察装置 |
Family Cites Families (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE45855C (de) * | TH. OTTO in Schkeuditz | Selbstthätiger Kuppelungsapparat mit Daumen für Seilbahnen | ||
US2427689A (en) * | 1942-08-28 | 1947-09-23 | American Optical Corp | Microscope with special light modifiers |
US2616334A (en) | 1947-11-25 | 1952-11-04 | Zernike Frits | Phase microscopy |
AT180745B (de) * | 1953-06-17 | 1955-01-10 | Optische Werke C Reichert Ag | Kontrastmikroskop |
AT187704B (de) * | 1953-09-23 | 1956-11-26 | Optische Werke C Reichert Ag | Phasenkontrastmikroskop |
DE2261780C2 (de) * | 1972-12-16 | 1979-09-20 | Ernst Leitz Wetzlar Gmbh, 6330 Wetzlar | Verfahren zur Herstellung von unmittelbar nebeneinander liegenden Strukturen |
DE3412958A1 (de) * | 1984-04-06 | 1985-10-17 | Dr. Johannes Heidenhain Gmbh, 8225 Traunreut | Phasengitter |
US5144362A (en) * | 1990-11-14 | 1992-09-01 | Mitsubishi Denki Kabushiki Kaisha | Projection aligner |
JP3413238B2 (ja) | 1993-03-31 | 2003-06-03 | オリンパス光学工業株式会社 | 位相制御膜構造体 |
-
1997
- 1997-09-29 DE DE19743027A patent/DE19743027A1/de not_active Ceased
-
1998
- 1998-08-03 JP JP51955399A patent/JP4199833B2/ja not_active Expired - Fee Related
- 1998-08-03 WO PCT/DE1998/002228 patent/WO1999017145A1/fr not_active Application Discontinuation
- 1998-08-03 EP EP98948715A patent/EP0941496A1/fr not_active Withdrawn
- 1998-08-03 US US09/308,855 patent/US6212009B1/en not_active Expired - Lifetime
- 1998-08-03 CN CN200410031776.6A patent/CN1267761C/zh not_active Expired - Fee Related
- 1998-08-03 CN CNB988019884A patent/CN1179226C/zh not_active Expired - Fee Related
Non-Patent Citations (1)
Title |
---|
See references of WO9917145A1 * |
Also Published As
Publication number | Publication date |
---|---|
WO1999017145A1 (fr) | 1999-04-08 |
DE19743027A1 (de) | 1999-05-12 |
CN1267761C (zh) | 2006-08-02 |
JP4199833B2 (ja) | 2008-12-24 |
CN1534324A (zh) | 2004-10-06 |
CN1179226C (zh) | 2004-12-08 |
JP2001508557A (ja) | 2001-06-26 |
CN1244264A (zh) | 2000-02-09 |
US6212009B1 (en) | 2001-04-03 |
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Legal Events
Date | Code | Title | Description |
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PUAI | Public reference made under article 153(3) epc to a published international application that has entered the european phase |
Free format text: ORIGINAL CODE: 0009012 |
|
17P | Request for examination filed |
Effective date: 19990518 |
|
AK | Designated contracting states |
Kind code of ref document: A1 Designated state(s): CH DE FR GB LI |
|
RIN1 | Information on inventor provided before grant (corrected) |
Inventor name: GUNKEL, CLAUS Inventor name: ALT-NEDVIDEK, SABINE |
|
17Q | First examination report despatched |
Effective date: 20040414 |
|
RAP1 | Party data changed (applicant data changed or rights of an application transferred) |
Owner name: LEICA MICROSYSTEMS CMS GMBH |
|
17Q | First examination report despatched |
Effective date: 20040414 |
|
STAA | Information on the status of an ep patent application or granted ep patent |
Free format text: STATUS: THE APPLICATION IS DEEMED TO BE WITHDRAWN |
|
18D | Application deemed to be withdrawn |
Effective date: 20071026 |