EP0896744A1 - Dual-mode-mikrowellen-bandpassfilter aus hochgüteresonatoren - Google Patents
Dual-mode-mikrowellen-bandpassfilter aus hochgüteresonatorenInfo
- Publication number
- EP0896744A1 EP0896744A1 EP97922878A EP97922878A EP0896744A1 EP 0896744 A1 EP0896744 A1 EP 0896744A1 EP 97922878 A EP97922878 A EP 97922878A EP 97922878 A EP97922878 A EP 97922878A EP 0896744 A1 EP0896744 A1 EP 0896744A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- mode
- dual
- dielectric
- filter according
- pole
- 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
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P7/00—Resonators of the waveguide type
- H01P7/10—Dielectric resonators
- H01P7/105—Multimode resonators
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10—TECHNICAL SUBJECTS COVERED BY FORMER USPC
- Y10S—TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10S505/00—Superconductor technology: apparatus, material, process
- Y10S505/70—High TC, above 30 k, superconducting device, article, or structured stock
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10—TECHNICAL SUBJECTS COVERED BY FORMER USPC
- Y10S—TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10S505/00—Superconductor technology: apparatus, material, process
- Y10S505/825—Apparatus per se, device per se, or process of making or operating same
- Y10S505/866—Wave transmission line, network, waveguide, or microwave storage device
Definitions
- the present invention relates to a dual-mode two-pole filter, such as. B. a bandpass filter for the microwave range, consisting of a resonator for two dipole modes, each with a dielectric, which is arranged on at least one high-temperature superconductor film, with a shielding housing, which is arranged over the high-temperature superconductor film and the dielectric encloses, and with a coupling device for coupling the dipole modes and in particular for coupling microwaves to the electromagnetic fields of the dipole modes used. It also relates to a multi-pole dual-mode filter.
- bandpass filters in the microwave range (4-20GHz) play an important role in the preselection of individual communication channels.
- Analog multiplexers with filters based on cavity resonators are usually used there, in which the quality factors of the individual resonators are in the range of a few 10 4 .
- the mostly circular cylindrical cavity resonators are operated in most cases in so-called “dual modes", ie orthogonal dipole modes with a preferred direction of the electromagnetic fields in the circular area. This means that two poles of a filter can be realized with one resonator, ie an n-pole filter based on "dual-mode" resonators consists of n / 2 resonators.
- REPLACEMENT BLA ⁇ (RULE 26) the high frequency power of the output stages, which is normally generated by tube amplifiers (traveling-wave tube amplifiers), can be reduced.
- Insertion loss decreases with increasing quality factor of the individual resonators.
- a strongly miniaturized "dual-mode M filter based on dielectric resonators is known from US Pat. No. 4,489,293.
- the HE 1 L1 mode of a cylindrical dielectric is used, which splits into two orthogonal dipole modes.
- tan ⁇ is the loss tangent of the material from which the dielectric resonator is made.
- the limitation is caused by losses in the various parts i of the wall of the metallic shielding housing, which are each characterized by the surface resistance of the wall material R s ⁇ and by a geometry factor G ⁇ . The latter results from the distribution of the electromagnetic fields for the respective vibration mode of the resonator.
- WO 93/09575 discloses circular cylindrical dielectric resonators with two end plates made of high-temperature superconductor films. With these, grades in the range of 10 6 were demonstrated, since in the TE 011 vibration mode used there the geometry factor is sufficiently large for the normal conductive outer surface of the cylinder. However, due to the rotational symmetry of the field distribution, this mode is not a dipole mode, so that "dual-mode" operation is not possible here.
- the object of the invention is therefore to create a dual-mode filter in which the quality factors for the individual resonators are 10 5 to 10 6 .
- the object is achieved according to the invention for a two-pole filter in that the dielectric is hemispherical.
- the implementation of more than two-pole filters is solved according to claim 13.
- the curved surfaces of the shielding housing have geometric factors that are large enough to accommodate one or two high-temperature superconductor films (HTS films) to achieve the qualities required in the task.
- HTS films high-temperature superconductor films
- Subclaims 2-5 contain advantageous features for coupling to the electromagnetic fields of the dipole modes to adjust the resonance frequency of the dipole modes and to set the coupling between the dipole modes.
- Fig. La is a schematic side view of a dual-mode two-pole filter according to the present invention.
- Fig. Lb is a schematic plan view of the dual-mode ⁇ two-pole filter from Fig. La;
- FIG. 2 shows a schematic top view of a dual-mode four-pole filter according to the present invention
- 3a shows a schematic side view of a calculated example of a distribution of the electric field in a resonator according to the present invention
- FIG. 3b shows a schematic top view of the example from FIG. 3a;
- 4a is a schematic side view of a calculated example of a distribution of the magnetic field in a resonator according to the present
- FIG. 4b shows a schematic top view of the example from FIG. 4a.
- a dual-mode two-pole filter 1 according to the invention is shown schematically in a side view in FIG.
- a dielectric 3 (for example made of LaA10 3 ) designed as a dielectric hemisphere is arranged on a high-temperature superconductor film 5 (hereinafter referred to as HTS film).
- HTS film high-temperature superconductor film 5
- the invention is not limited to the arrangement of a single HTS film; rather, in another embodiment, another HTS film 5 can also be provided as the upper end plate of a cylindrical shielding housing 7.
- the metallic shield housing 7 can be rectangular, cylindrical or hemispherical and consists, for. B. preferably made of a highly conductive metal such as copper.
- the coupling to the two dipole modes of the "dual mode" is carried out by a coupling device, the coupling elements 9 of which are either linear coaxial antennas (FIGS. 1 a and 1 b) for coupling to the electric field or coaxial loops (not shown) for coupling to the magnetic field .
- the coupling elements 9 are passed through holes 11 in the superconducting films 5.
- the coupling between the dipole modes is set via a further adjustable dielectric rod 15 (FIG. 1b), which is preferably arranged at an angle of 45 ° with respect to the orientation of the dipole modes.
- 2 shows a four-pole filter consisting of two “dual-mode” resonators 1, 1.
- the coupling between the two resonators 1, 1 is defined by the distance between the two hemispheres and can optionally be adjusted by means of a further adjustable dielectric rod between the hemispheres become.
- several hemispheres can be arranged next to one another in the manner shown in FIG. The hemispheres do not necessarily have to be arranged in a row.
- the metallic shielding housing 7 should have at least a distance from the hemisphere surface corresponding to the diameter of the hemisphere at all points so that the losses in the shielding housing do not become too high.
- the loss contribution of the curved surface of the metallic shielding housing is very small. This is because, in contrast to the arrangement described in the prior art, the electric fields in the Hemisphere run mainly parallel to the surface of the sphere (Fig. 3a).
- calculation example s is the half-sphere diameter 9.6mm, the dielectric constant of the material hemisphere 23.4 (LaAlO ß). Diameter / height of the circular cylindrical shielding housing are 26 / 14mm.
- the calculation results in a resonance frequency of 6.58GHz, the mode is the fundamental mode (lowest resonance frequency) o of the resonator.
- the calculated geometry factors are 114 ⁇ for the lower end face (superconducting film), 16300 ⁇ for the upper end face and 10400 ⁇ for the outer surface.
Landscapes
- Control Of Motors That Do Not Use Commutators (AREA)
Abstract
Description
Claims
Applications Claiming Priority (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE19617698 | 1996-05-03 | ||
DE19617698A DE19617698C1 (de) | 1996-05-03 | 1996-05-03 | Dual-mode-Zweipolfilter |
PCT/DE1997/000857 WO1997042679A1 (de) | 1996-05-03 | 1997-04-26 | Dual-mode-mikrowellen-bandpassfilter aus hochgüteresonatoren |
Publications (2)
Publication Number | Publication Date |
---|---|
EP0896744A1 true EP0896744A1 (de) | 1999-02-17 |
EP0896744B1 EP0896744B1 (de) | 2000-05-31 |
Family
ID=7793177
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP97922878A Expired - Lifetime EP0896744B1 (de) | 1996-05-03 | 1997-04-26 | Dual-mode-mikrowellen-bandpassfilter aus hochgüteresonatoren |
Country Status (7)
Country | Link |
---|---|
US (1) | US6484043B1 (de) |
EP (1) | EP0896744B1 (de) |
JP (1) | JP2000509584A (de) |
CA (1) | CA2252659A1 (de) |
DE (2) | DE19617698C1 (de) |
ES (1) | ES2148978T3 (de) |
WO (1) | WO1997042679A1 (de) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US9138317B2 (en) | 2013-03-14 | 2015-09-22 | Osteoceramics, Inc | Conduits for enhancing tissue regeneration |
Families Citing this family (11)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE19824997C2 (de) * | 1998-06-05 | 2003-01-09 | Forschungszentrum Juelich Gmbh | Mehrpol-Bandpaßfilter mit elliptischer Filtercharakteristik |
DE19927798A1 (de) * | 1999-06-18 | 2001-01-04 | Forschungszentrum Juelich Gmbh | Dieelektrische Resonatorkonfiguration für Mikrowellen-Mehrpol-Bandpaßfilter |
DE10034338C2 (de) * | 2000-07-14 | 2002-06-20 | Forschungszentrum Juelich Gmbh | Mehrpoliges kaskadierendes Quardrupel-Bandpaßfilter auf der Basis dielektrischer Dual-Mode-Resonatoren |
US7068127B2 (en) * | 2001-11-14 | 2006-06-27 | Radio Frequency Systems | Tunable triple-mode mono-block filter assembly |
US7042314B2 (en) * | 2001-11-14 | 2006-05-09 | Radio Frequency Systems | Dielectric mono-block triple-mode microwave delay filter |
DE10353104A1 (de) * | 2003-11-12 | 2005-06-09 | Tesat-Spacecom Gmbh & Co.Kg | Anordnung zur Justage der Kopplung bei dielektrischen Filtern |
US6954122B2 (en) * | 2003-12-16 | 2005-10-11 | Radio Frequency Systems, Inc. | Hybrid triple-mode ceramic/metallic coaxial filter assembly |
DE102007027371A1 (de) * | 2007-06-11 | 2008-12-18 | Cognis Oleochemicals Gmbh | Verfahren zur Herstellung einer Verbindung aufweisend mindestens eine Ester-Gruppe |
DE102007027372A1 (de) * | 2007-06-11 | 2008-12-18 | Cognis Oleochemicals Gmbh | Verfahren zur Hydrierung von Glycerin |
US8111115B2 (en) * | 2008-07-21 | 2012-02-07 | Com Dev International Ltd. | Method of operation and construction of dual-mode filters, dual band filters, and diplexer/multiplexer devices using half cut dielectric resonators |
US8954125B2 (en) | 2011-07-28 | 2015-02-10 | International Business Machines Corporation | Low-loss superconducting devices |
Family Cites Families (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4489293A (en) * | 1981-05-11 | 1984-12-18 | Ford Aerospace & Communications Corporation | Miniature dual-mode, dielectric-loaded cavity filter |
JPS62204601A (ja) * | 1986-03-04 | 1987-09-09 | Murata Mfg Co Ltd | 二重モ−ドフイルタ |
DE69020195T2 (de) * | 1989-03-14 | 1995-11-30 | Fujitsu Ltd | Schaltung mit dielektrischem Resonator im TE01-Mode. |
US5179074A (en) * | 1991-01-24 | 1993-01-12 | Space Systems/Loral, Inc. | Hybrid dielectric resonator/high temperature superconductor filter |
US5324713A (en) * | 1991-11-05 | 1994-06-28 | E. I. Du Pont De Nemours And Company | High temperature superconductor support structures for dielectric resonator |
US5585331A (en) * | 1993-12-03 | 1996-12-17 | Com Dev Ltd. | Miniaturized superconducting dielectric resonator filters and method of operation thereof |
-
1996
- 1996-05-03 DE DE19617698A patent/DE19617698C1/de not_active Expired - Fee Related
-
1997
- 1997-04-26 US US09/180,160 patent/US6484043B1/en not_active Expired - Fee Related
- 1997-04-26 DE DE59701819T patent/DE59701819D1/de not_active Expired - Fee Related
- 1997-04-26 EP EP97922878A patent/EP0896744B1/de not_active Expired - Lifetime
- 1997-04-26 ES ES97922878T patent/ES2148978T3/es not_active Expired - Lifetime
- 1997-04-26 CA CA002252659A patent/CA2252659A1/en not_active Abandoned
- 1997-04-26 WO PCT/DE1997/000857 patent/WO1997042679A1/de active IP Right Grant
- 1997-04-26 JP JP9539421A patent/JP2000509584A/ja active Pending
Non-Patent Citations (1)
Title |
---|
See references of WO9742679A1 * |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US9138317B2 (en) | 2013-03-14 | 2015-09-22 | Osteoceramics, Inc | Conduits for enhancing tissue regeneration |
Also Published As
Publication number | Publication date |
---|---|
CA2252659A1 (en) | 1997-11-13 |
US6484043B1 (en) | 2002-11-19 |
ES2148978T3 (es) | 2000-10-16 |
DE19617698C1 (de) | 1997-10-16 |
JP2000509584A (ja) | 2000-07-25 |
WO1997042679A1 (de) | 1997-11-13 |
DE59701819D1 (de) | 2000-07-06 |
EP0896744B1 (de) | 2000-05-31 |
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