US20100134370A1 - Probe and antenna using waveguide - Google Patents
Probe and antenna using waveguide Download PDFInfo
- Publication number
- US20100134370A1 US20100134370A1 US12/629,836 US62983609A US2010134370A1 US 20100134370 A1 US20100134370 A1 US 20100134370A1 US 62983609 A US62983609 A US 62983609A US 2010134370 A1 US2010134370 A1 US 2010134370A1
- Authority
- US
- United States
- Prior art keywords
- waveguide
- probe
- dielectric
- antenna
- conductive elements
- 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
- 239000000523 sample Substances 0.000 title claims abstract description 80
- 239000004020 conductor Substances 0.000 claims abstract description 11
- 239000003990 capacitor Substances 0.000 claims description 15
- 230000005540 biological transmission Effects 0.000 description 7
- 238000005259 measurement Methods 0.000 description 7
- 230000005672 electromagnetic field Effects 0.000 description 6
- 230000035699 permeability Effects 0.000 description 4
- 230000003247 decreasing effect Effects 0.000 description 3
- 239000000758 substrate Substances 0.000 description 3
- 239000006096 absorbing agent Substances 0.000 description 2
- 239000011190 CEM-3 Substances 0.000 description 1
- 239000004593 Epoxy Substances 0.000 description 1
- 239000002131 composite material Substances 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
Images
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P5/00—Coupling devices of the waveguide type
- H01P5/08—Coupling devices of the waveguide type for linking dissimilar lines or devices
- H01P5/10—Coupling devices of the waveguide type for linking dissimilar lines or devices for coupling balanced lines or devices with unbalanced lines or devices
- H01P5/107—Hollow-waveguide/strip-line transitions
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q13/00—Waveguide horns or mouths; Slot antennas; Leaky-waveguide antennas; Equivalent structures causing radiation along the transmission path of a guided wave
- H01Q13/02—Waveguide horns
- H01Q13/0208—Corrugated horns
- H01Q13/0225—Corrugated horns of non-circular cross-section
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q13/00—Waveguide horns or mouths; Slot antennas; Leaky-waveguide antennas; Equivalent structures causing radiation along the transmission path of a guided wave
- H01Q13/02—Waveguide horns
- H01Q13/0275—Ridged horns
Definitions
- Exemplary embodiments of the present invention relates to a probe and an antenna; and, more particularly, to a probe and antenna using a waveguide.
- An antenna is a generic term of devices for transmitting or receiving electromagnetic waves.
- a probe in a wide sense refers to an antenna for receiving electromagnetic waves, and in a narrow sense refers to an electromagnetic wave receiver used for measuring electromagnetic fields.
- a waveguide is a type of transmission lines for transmitting electromagnetic waves or electrical energy.
- a waveguide has a conductive cavity through which electromagnetic waves are transmitted. In general, since a waveguide has low ohmic loss and low dielectric loss, it is widely used in probes and antennas.
- the multiple reflection refers to a phenomenon in which an electromagnetic wave is several times reflected between two specific objects.
- the following description will be made with reference to an example which measures characteristics of an antenna by using a probe to measure an electromagnetic field around the antenna.
- a space electromagnetically influenced by the antenna may be largely divided into a far field and a near field.
- the far field represents a space far away from the antenna by more than several times the wavelength of the electromagnetic wave used in the antenna, generally, more than three to five times.
- the near field represents a space far away from the antenna by less than several times the wavelength of the electromagnetic wave used in the antenna. It can be understood that the far field represents a space farther than a location where the electromagnetic field is completely formed from the antenna and thus it is isolated from the antenna. Also, it can be understood that the near field represents a space covering a location where the electromagnetic field is formed from the antenna.
- an antenna transmits or receives electromagnetic waves by using an electromagnetic field formed in a far field. Therefore, characteristics of an antenna are usually measured in a far field. In some cases, however, characteristics of an antenna may be measured in a near field, and characteristics of an antenna in a far field may be calculated mathematically. Examples of such cases may include a case where a transmission loss is high because a measurement frequency is high, a case where an object to be measured is significantly large compared with the wavelength of an electromagnetic wave, and a case where far field measurement conditions are not met because of limitations in a measurement environment.
- a probe is disposed in a near field space, and characteristics of an antenna are measured.
- an electromagnetic wave reception unit of the probe and a radiator of the antenna become very close to each other. Therefore, the multiple reflection of an electromagnetic wave may occur between the probe and the antenna.
- the probe may accurately measure characteristics of the antenna when it receives only electromagnetic waves radiated directly from the antenna. However, if characteristics of an antenna are measured in a near field, electromagnetic waves radiated from the antenna may be reflected one or more times at the probe or the antenna and then incident into the probe. Such a multiple-reflected electromagnetic wave serves as an error factor in measurement.
- a wavelength of an electromagnetic wave is long and therefore a distance between a probe and an antenna must be large. Since characteristics of an antenna are usually measured inside a shield room or the like, there may be a limitation in increasing the distance between the probe and the antenna. In some cases, due to another limitation in a measurement environment, the distance between the probe and the antenna must be maintained to be narrow. In those cases, the distance between the probe and the antenna may be reduced by decreasing the multiple reflection of an electromagnetic wave.
- An embodiment of the present invention is directed to a probe and an antenna capable of reducing the multiple reflection of electromagnetic waves.
- a probe in accordance with an embodiment of the present invention, includes: a waveguide; and a resonance unit entirely or partially disposed in the inside of the waveguide and comprising a conductor.
- an antenna includes: a waveguide; and a resonance unit entirely or partially disposed in the inside of the waveguide and comprising a conductor.
- FIG. 1 is a perspective view of a probe in accordance with an embodiment of the present invention.
- FIG. 2 is a front view of the probe of FIG. 1 .
- FIG. 3 is a plan view of the probe of FIG. 1 .
- FIG. 4 is a sectional view of a resonance unit in accordance with an embodiment of the present invention.
- FIG. 5 is a sectional view of a resonance unit in accordance with another embodiment of the present invention.
- Exemplary embodiments of the present invention relate to a probe or an antenna using a waveguide and a resonance unit.
- the probe In order to accurately measure characteristics of an antenna, the probe must receive only electromagnetic waves radiated directly from the antenna. However, if characteristics of the antenna are measured in a near field, the multiple reflection may be caused. That is, since an opening side of the probe and a radiator of the antenna are very close to each other, electromagnetic waves multiple-reflected between the opening side of the probe and the radiator of the antenna may be received by the probe. Since the multiple-reflected electromagnetic waves are not electromagnetic waves radiated directly fro the antenna, they serve as an error factor in measuring characteristics of the antenna. Therefore, if the multiple reflection is reduced, characteristics of the antenna may be measured more accurately.
- the multiple reflection of the electromagnetic waves may be reduced by decreasing an area of the opening area of the probe. Since the opening area of the probe is a region where electromagnetic waves can be reflected, the reflection of the electromagnetic waves may be reduced by decreasing the opening area of the probe. However, the opening area of the probe is closely associated with an operating frequency of the probe. Generally, if the opening area of the probe is small, the operating frequency of the probe is low. Therefore, in accordance with the embodiments of the present invention, the probe is designed to receive electromagnetic waves of a desired operating frequency band by using a resonance unit.
- the resonance unit is entirely or partially disposed in the inside of the waveguide, and includes a conductor. The conductor included in the resonance unit may resonate at the operating frequency band of the probe.
- the probe or the antenna using the waveguide and the resonance unit may further reduce the multiple reflection than other probe or antenna that operates at the same operating frequency band.
- the probe in accordance with the embodiment of the present invention includes a waveguide and a resonance unit.
- the resonance unit is entirely or partially disposed inside the waveguide and includes a conductor.
- the waveguide is used as a transmission line through which electromagnetic waves or signals are transmitted, and it has a conductive cavity.
- the waveguide transmits electromagnetic waves confined inside, and has low ohmic loss because no current directly flows through the surrounding conductor.
- a section of the waveguide may have various shapes. Generally, the section of the waveguide may be rectangular or circular. The lowest frequency that can be transmitted through the waveguide is determined by the size of the section of the waveguide. As an operating frequency increases, the section of the waveguide decreases.
- the resonance unit may include a dielectric and a conductive resonance element attached to the dielectric.
- the resonance element resonates in an operating frequency band of the probe.
- the probe may receive electromagnetic waves of desired frequencies through the resonance unit.
- the dielectric supports the resonance element and may be formed in a type of a dielectric substrate.
- the dielectric substrate may be formed of Frame Retadent 1 (FR1), FR2, FR4, Composite Epoxy Material-1 (CEM-1), CEM-3, or the like.
- the probe may further include a ridge attached to the inside of the waveguide and connected to the dielectric.
- the ridge is an elongated conductor and increases the electromagnetic-wave transmission efficiency of the probe.
- the ridge may be disposed in a direction in which an electromagnetic wave is transmitted, or may be attached to an inner side of the waveguide.
- a pair of ridges may be disposed.
- a pair of ridges facing each other may be attached to opposite sides of the waveguide, respectively.
- two pairs of ridges may be used.
- the ridges may be connected to the dielectric, and the dielectric may be formed to protrude at the connection portion where the dielectric and the ridges are connected together. Electromagnetic waves received through the resonance unit are guided and transmitted by the ridges connected to the dielectric. The protrusion of the dielectric matches impedance between the dielectric and the ridge and thus increases the efficiency of electromagnetic wave transmission.
- the resonance element included in the resonance unit may be formed in a ring shape with a cut portion. That is, the resonance element may have a shape similar to alphabet āCā.
- the resonance element resonates at a specific frequency band according to its material and shape.
- the resonance frequency of the resonance unit is most affected by the length of the resonance element.
- the resonance frequency becomes lower as the length of the resonance element becomes longer, and the resonance frequency becomes higher as the length of the resonance element becomes shorter.
- the ring-shaped resonance element with a cut portion may have a long length in a relatively small space. Therefore, such a ring type resonance element may occupy a small space and resonate at a low frequency.
- the ring-shaped resonance element with a cut portion may include a capacitor attached to the cut portion.
- the capacitor shifts the resonance frequency of the resonance element.
- the capacitor may be a variable capacitor.
- the variable capacitor if a capacitance of the variable capacitor is changed, the resonance frequency of the resonance element is also changed. Consequently, the operating frequency of the probe may be changed using the variable capacitor.
- the resonance element included in the resonance unit may include a plurality of conductive elements electrically isolated from one another.
- electrically isolated means that no current can flow because the conductive elements are not directly connected together, and does mean āelectromagnetically isolated.ā Therefore, the plurality of conductive elements can transmit electromagnetic waves because they are electrically isolated from one another but electromagnetically coupled to one another.
- the dielectric of the resonance unit may support the conductive elements.
- the conductive elements may be attached to one side or both sides of the dielectric. In a case where the conductive elements are attached to both sides of the dielectric, two conductive elements may be attached to one side of the dielectric, and the conductive elements attached to the other side of the dielectric may be arranged between the two conductive elements. Such an arrangement strengthens the electromagnetic coupling between the conductive elements. Therefore, such an arrangement may reduce the loss generated when the conductive elements transmit the electromagnetic waves.
- the conductive elements may be arranged in a direction perpendicular to an opening side of the waveguide. Since the conductive elements transmit the electromagnetic waves, the loss during transmission is reduced when the conductive elements are arranged in a direction in which the electromagnetic waves are transmitted. In the waveguide, the electromagnetic waves are transmitted in a direction perpendicular to the opening side of the waveguide, that is, an extending direction of the waveguide. Therefore, the conductive elements may be arranged in this direction.
- FIGS. 1 to 3 are a perspective view, a front view, and a plane view of a probe 100 in accordance with an embodiment of the present invention, respectively.
- the probe 100 includes a first waveguide 10 , a second waveguide 20 , and a third waveguide 30 .
- the probe 100 may be used to measure the electromagnetic field of a near field.
- the first waveguide 10 , the second waveguide 20 , and the third waveguide 30 have a rectangular section, and the height and width of their insides are constant in an extending direction of the waveguides.
- the second waveguide 20 has a smaller section than the first waveguide 10
- the third waveguide 30 has a smaller section than the second waveguide 20 . Since the third waveguide 30 has the smallest section, it is possible to reduce the multiple reflection that may be caused when measuring the electromagnetic waves. Moreover, the measurement distance may become closer by as much as the reduced multiple reflection.
- the waveguide functions as a high-pass filter (HPF). As the size of the section of the waveguide becomes smaller, a cutoff frequency of the waveguide becomes higher. If the third waveguide 30 is formed to have a small section in order to reduce the multiple reflection, the cutoff frequency of the third waveguide 30 may be much higher than the operating frequency band of the probe 100 . Even in this case, the probe 100 may receive electromagnetic waves of the operating frequency band by using the resonance element 45 . Further detailed description will be made below in conjunction with the resonance element 45 .
- the electromagnetic waves are transmitted from the third waveguide 30 through the second waveguide 20 to the first waveguide 10 .
- the second waveguide 20 matches impedance between the first waveguide 30 and the third waveguide 10 .
- the probe 100 may include an electromagnetic wave absorber at the outer sides of the waveguides 10 , 20 and 30 .
- the electromagnetic wave absorber increases an electromagnetic-wave measurement accuracy by absorbing electromagnetic waves radiated from the outside of the probe 100 .
- the probe 100 includes a first double ridge 25 attached to the inside of the second waveguide 20 , and a second double ridge 35 attached to the inside of the third waveguide 30 .
- the first double ridge 25 is provided with a pair of ridges facing each other and attached to the inside of the second waveguide 20 .
- the first double ridge 25 matches impedance between the first waveguide 10 and the third waveguide 30 .
- the first double ridge 25 lowers a cutoff frequency of the second waveguide 20 .
- the second double ridge 35 is provided with a pair of ridges and attached to the inside of the third waveguide 30 .
- the second double ridge 35 lowers a cutoff frequency of the third waveguide 30 .
- the first double ridge 25 and the second double ridge 35 narrow the inside of the waveguides and guide electromagnetic waves transmitted through the inside of the waveguides.
- the probe 100 includes a dielectric 50 , a portion of which is disposed in the inside of the third waveguide 30 , and a resonance element 45 attached to the dielectric 50 . As illustrated in FIGS. 1 to 3 , the resonance element 45 and the dielectric 50 are disposed at one side of the third waveguide 30 . The resonance element 45 and the dielectric 50 constitute a resonance unit of the probe 100 .
- the resonance element 45 includes a plurality of ring-shaped conductive elements with a cut portion.
- the resonance element 45 resonates at an operating frequency band of the probe 100 .
- the probe 100 may receive electromagnetic waves of a desired frequency through the resonance element 45 .
- the multiple reflection may be further reduced.
- the cutoff frequency of the third waveguide 30 may be higher than the operating frequency of the probe 100 .
- a transverse permeability of the waveguide is negative at a frequency band lower than the cutoff frequency.
- a permittivity of the resonance element is negative at the resonant frequency band. Therefore, a transverse permeability of the third waveguide 30 and a permittivity of the resonance element 45 are negative at the operating frequency band of the probe 100 .
- both the permeability and the permittivity are negative, the electromagnetic waves travel in the same manner as when both the permeability and the permittivity are positive. Due to this principle, the probe 100 may receive electromagnetic waves at the operating frequency band, while reducing the section of the third waveguide 30 .
- the resonance element 45 includes a plurality of C-shaped conductive elements arranged in a row. As the third waveguide 30 becomes longer, the multiple reflection is further reduced. If the number of the conductive elements included in the resonance element 45 increases, the length of the third waveguide 30 increases. At this time, as the number of the conductive elements increases, the conductive and dielectric loss increases. However, the second double ridge 35 minimizes the conductive and dielectric loss. The second double ridge 35 may reduce the conductive and dielectric loss and lower the cutoff frequency of the third waveguide 30 . It can be easily understood by those skilled in the art that a single conductive element may be used as the resonance element 45 .
- the dielectric 50 has a substrate shape and supports the resonance element 45 .
- FIG. 3 which illustrates a plan view of the probe 100
- the dielectric 50 is disposed in the center of the third waveguide 30 .
- the dielectric 50 includes a protrusion 40 at a connection portion where the dielectric 50 and the second double ridge 35 are connected together.
- the protrusion 40 matches impedance between the third waveguide 30 and the dielectric 50 .
- FIG. 4 is a sectional view of the resonance unit in accordance with the embodiment of the present invention.
- the resonance unit includes the protrusion 40 , the resonance element 45 , and the dielectric 50 .
- the resonance element 45 includes a plurality of C-shaped conductive elements.
- the plurality of conductive elements are arranged on both sides of the dielectric 50 in a row.
- the conductive elements arranged on the front side of the dielectric 50 are indicated by solid lines, and the conductive elements arranged on the rear side of the dielectric 50 are indicated by dotted lines.
- the conductive elements on the rear side of the dielectric 50 are arranged in the intervals of the conductive elements on the front side of the dielectric 50 . This arrange of the conductive elements increases the electromagnetic-wave transmission efficiency.
- FIG. 5 is a sectional view of a resonance unit in accordance with another embodiment of the present invention.
- the plurality of conductive elements constituting the resonance element 45 include capacitors 42 , respectively.
- the capacitors 42 shift the resonant frequency of the resonance element 45 .
- the resonant frequency of the resonance element 45 is changed to a certain value.
- the capacitors 42 are variable capacitors, the resonant frequency of the resonance element 45 may be changed by adjusting the capacitances of the capacitors 42 .
- An antenna in accordance with an embodiment of the present invention includes a waveguide and a resonance unit.
- the resonance unit is entirely or partially disposed in the inside of the waveguide.
- the resonance unit may include a dielectric and a conductive resonance element attached to the dielectric.
- the antenna may further include a ridge attached to the inside of the waveguide and connected to the dielectric.
- the dielectric may be formed to protrude at a connection portion where the dielectric and the ridge are connected together.
- the resonance element may be formed in a ring shape with a cut portion, and may include a capacitor attached to the cut portion. Furthermore, the resonance element may include a plurality of conductive elements electrically isolated from one another. The conductive elements may be attached to one side of the dielectric and arranged in a direction perpendicular to an opening side of the waveguide. Meanwhile, the conductive elements may include two conductive elements attached to one side of the dielectric, and conductive elements attached the other side of the dielectric and arranged between the two conductive elements, and may be arranged in a direction perpendicular to an opening side of the waveguide.
- the probe and the antenna in accordance with the embodiments of the present invention may reduce the multiple reflection of electromagnetic waves.
Landscapes
- Waveguide Aerials (AREA)
- Control Of Motors That Do Not Use Commutators (AREA)
Abstract
Description
- The present application claims priority of Korean Patent Application No(s). 10-2008-0121833, filed on Dec. 3, 2008, which is incorporated herein by reference in its entirety.
- 1. Field of the Invention
- Exemplary embodiments of the present invention relates to a probe and an antenna; and, more particularly, to a probe and antenna using a waveguide.
- 2. Description of Related Art
- An antenna is a generic term of devices for transmitting or receiving electromagnetic waves. A probe in a wide sense refers to an antenna for receiving electromagnetic waves, and in a narrow sense refers to an electromagnetic wave receiver used for measuring electromagnetic fields.
- Probes or antennas using waveguides have been known. A waveguide is a type of transmission lines for transmitting electromagnetic waves or electrical energy. A waveguide has a conductive cavity through which electromagnetic waves are transmitted. In general, since a waveguide has low ohmic loss and low dielectric loss, it is widely used in probes and antennas.
- Meanwhile, in probes and antennas, multiple reflection is frequently problematic. The multiple reflection refers to a phenomenon in which an electromagnetic wave is several times reflected between two specific objects. The following description will be made with reference to an example which measures characteristics of an antenna by using a probe to measure an electromagnetic field around the antenna.
- With regard to characteristics of the antenna, a space electromagnetically influenced by the antenna may be largely divided into a far field and a near field. The far field represents a space far away from the antenna by more than several times the wavelength of the electromagnetic wave used in the antenna, generally, more than three to five times. The near field represents a space far away from the antenna by less than several times the wavelength of the electromagnetic wave used in the antenna. It can be understood that the far field represents a space farther than a location where the electromagnetic field is completely formed from the antenna and thus it is isolated from the antenna. Also, it can be understood that the near field represents a space covering a location where the electromagnetic field is formed from the antenna.
- Generally, an antenna transmits or receives electromagnetic waves by using an electromagnetic field formed in a far field. Therefore, characteristics of an antenna are usually measured in a far field. In some cases, however, characteristics of an antenna may be measured in a near field, and characteristics of an antenna in a far field may be calculated mathematically. Examples of such cases may include a case where a transmission loss is high because a measurement frequency is high, a case where an object to be measured is significantly large compared with the wavelength of an electromagnetic wave, and a case where far field measurement conditions are not met because of limitations in a measurement environment.
- In such cases, a probe is disposed in a near field space, and characteristics of an antenna are measured. In those cases, an electromagnetic wave reception unit of the probe and a radiator of the antenna become very close to each other. Therefore, the multiple reflection of an electromagnetic wave may occur between the probe and the antenna. The probe may accurately measure characteristics of the antenna when it receives only electromagnetic waves radiated directly from the antenna. However, if characteristics of an antenna are measured in a near field, electromagnetic waves radiated from the antenna may be reflected one or more times at the probe or the antenna and then incident into the probe. Such a multiple-reflected electromagnetic wave serves as an error factor in measurement.
- Furthermore, in a case where a frequency band of a signal to be measured is low, a wavelength of an electromagnetic wave is long and therefore a distance between a probe and an antenna must be large. Since characteristics of an antenna are usually measured inside a shield room or the like, there may be a limitation in increasing the distance between the probe and the antenna. In some cases, due to another limitation in a measurement environment, the distance between the probe and the antenna must be maintained to be narrow. In those cases, the distance between the probe and the antenna may be reduced by decreasing the multiple reflection of an electromagnetic wave.
- Therefore, there is a need for methods which are capable of reducing the multiple reflection of electromagnetic waves in probes or antennas.
- An embodiment of the present invention is directed to a probe and an antenna capable of reducing the multiple reflection of electromagnetic waves.
- Other objects and advantages of the present invention can be understood by the following description, and become apparent with reference to the embodiments of the present invention. Also, it is obvious to those skilled in the art to which the present invention pertains that the objects and advantages of the present invention can be realized by the means as claimed and combinations thereof.
- In accordance with an embodiment of the present invention, a probe includes: a waveguide; and a resonance unit entirely or partially disposed in the inside of the waveguide and comprising a conductor.
- In accordance with another embodiment of the present invention, an antenna includes: a waveguide; and a resonance unit entirely or partially disposed in the inside of the waveguide and comprising a conductor.
-
FIG. 1 is a perspective view of a probe in accordance with an embodiment of the present invention. -
FIG. 2 is a front view of the probe ofFIG. 1 . -
FIG. 3 is a plan view of the probe ofFIG. 1 . -
FIG. 4 is a sectional view of a resonance unit in accordance with an embodiment of the present invention. -
FIG. 5 is a sectional view of a resonance unit in accordance with another embodiment of the present invention. - Exemplary embodiments of the present invention will be described below in more detail with reference to the accompanying drawings. The present invention may, however, be embodied in different forms and should not be constructed as limited to the embodiments set forth herein. Rather, these embodiments are provided so that this disclosure will be thorough and complete, and will fully convey the scope of the present invention to those skilled in the art. Throughout the disclosure, like reference numerals refer to like parts throughout the various figures and embodiments of the present invention. The drawings are not necessarily to scale and in some instances, proportions may have been exaggerated in order to clearly illustrate features of the embodiments.
- Exemplary embodiments of the present invention relate to a probe or an antenna using a waveguide and a resonance unit.
- The principle of the invention will be described, taking an example that measures characteristics of an antenna in a near field by using a probe. In order to accurately measure characteristics of an antenna, the probe must receive only electromagnetic waves radiated directly from the antenna. However, if characteristics of the antenna are measured in a near field, the multiple reflection may be caused. That is, since an opening side of the probe and a radiator of the antenna are very close to each other, electromagnetic waves multiple-reflected between the opening side of the probe and the radiator of the antenna may be received by the probe. Since the multiple-reflected electromagnetic waves are not electromagnetic waves radiated directly fro the antenna, they serve as an error factor in measuring characteristics of the antenna. Therefore, if the multiple reflection is reduced, characteristics of the antenna may be measured more accurately.
- In this case, the multiple reflection of the electromagnetic waves may be reduced by decreasing an area of the opening area of the probe. Since the opening area of the probe is a region where electromagnetic waves can be reflected, the reflection of the electromagnetic waves may be reduced by decreasing the opening area of the probe. However, the opening area of the probe is closely associated with an operating frequency of the probe. Generally, if the opening area of the probe is small, the operating frequency of the probe is low. Therefore, in accordance with the embodiments of the present invention, the probe is designed to receive electromagnetic waves of a desired operating frequency band by using a resonance unit. The resonance unit is entirely or partially disposed in the inside of the waveguide, and includes a conductor. The conductor included in the resonance unit may resonate at the operating frequency band of the probe.
- As such, the probe or the antenna using the waveguide and the resonance unit may further reduce the multiple reflection than other probe or antenna that operates at the same operating frequency band.
- Hereafter, embodiments of the present invention will be described in detail with reference to the accompanying drawings.
- <Probe>
- A probe in accordance with an embodiment of the present invention will be described below in detail.
- The probe in accordance with the embodiment of the present invention includes a waveguide and a resonance unit. The resonance unit is entirely or partially disposed inside the waveguide and includes a conductor. The waveguide is used as a transmission line through which electromagnetic waves or signals are transmitted, and it has a conductive cavity. The waveguide transmits electromagnetic waves confined inside, and has low ohmic loss because no current directly flows through the surrounding conductor. A section of the waveguide may have various shapes. Generally, the section of the waveguide may be rectangular or circular. The lowest frequency that can be transmitted through the waveguide is determined by the size of the section of the waveguide. As an operating frequency increases, the section of the waveguide decreases.
- The resonance unit may include a dielectric and a conductive resonance element attached to the dielectric. The resonance element resonates in an operating frequency band of the probe. Thus, the probe may receive electromagnetic waves of desired frequencies through the resonance unit. The dielectric supports the resonance element and may be formed in a type of a dielectric substrate. In this case, the dielectric substrate may be formed of Frame Retadent 1 (FR1), FR2, FR4, Composite Epoxy Material-1 (CEM-1), CEM-3, or the like.
- The probe may further include a ridge attached to the inside of the waveguide and connected to the dielectric. Generally, the ridge is an elongated conductor and increases the electromagnetic-wave transmission efficiency of the probe. The ridge may be disposed in a direction in which an electromagnetic wave is transmitted, or may be attached to an inner side of the waveguide. In another embodiment, a pair of ridges may be disposed. For example, a pair of ridges facing each other may be attached to opposite sides of the waveguide, respectively. In other embodiment, two pairs of ridges may be used.
- In this case, the ridges may be connected to the dielectric, and the dielectric may be formed to protrude at the connection portion where the dielectric and the ridges are connected together. Electromagnetic waves received through the resonance unit are guided and transmitted by the ridges connected to the dielectric. The protrusion of the dielectric matches impedance between the dielectric and the ridge and thus increases the efficiency of electromagnetic wave transmission.
- Meanwhile, the resonance element included in the resonance unit may be formed in a ring shape with a cut portion. That is, the resonance element may have a shape similar to alphabet āCā. The resonance element resonates at a specific frequency band according to its material and shape. In particular, the resonance frequency of the resonance unit is most affected by the length of the resonance element. Generally, the resonance frequency becomes lower as the length of the resonance element becomes longer, and the resonance frequency becomes higher as the length of the resonance element becomes shorter. Compared with other resonance elements, the ring-shaped resonance element with a cut portion may have a long length in a relatively small space. Therefore, such a ring type resonance element may occupy a small space and resonate at a low frequency.
- The ring-shaped resonance element with a cut portion may include a capacitor attached to the cut portion. The capacitor shifts the resonance frequency of the resonance element. In this case, the capacitor may be a variable capacitor. In a case where the variable capacitor is used, if a capacitance of the variable capacitor is changed, the resonance frequency of the resonance element is also changed. Consequently, the operating frequency of the probe may be changed using the variable capacitor.
- Meanwhile, the resonance element included in the resonance unit may include a plurality of conductive elements electrically isolated from one another. The expression āelectrically isolatedā means that no current can flow because the conductive elements are not directly connected together, and does mean āelectromagnetically isolated.ā Therefore, the plurality of conductive elements can transmit electromagnetic waves because they are electrically isolated from one another but electromagnetically coupled to one another.
- The dielectric of the resonance unit may support the conductive elements. The conductive elements may be attached to one side or both sides of the dielectric. In a case where the conductive elements are attached to both sides of the dielectric, two conductive elements may be attached to one side of the dielectric, and the conductive elements attached to the other side of the dielectric may be arranged between the two conductive elements. Such an arrangement strengthens the electromagnetic coupling between the conductive elements. Therefore, such an arrangement may reduce the loss generated when the conductive elements transmit the electromagnetic waves.
- Furthermore, the conductive elements may be arranged in a direction perpendicular to an opening side of the waveguide. Since the conductive elements transmit the electromagnetic waves, the loss during transmission is reduced when the conductive elements are arranged in a direction in which the electromagnetic waves are transmitted. In the waveguide, the electromagnetic waves are transmitted in a direction perpendicular to the opening side of the waveguide, that is, an extending direction of the waveguide. Therefore, the conductive elements may be arranged in this direction.
- Hereafter, a probe in accordance with a specific embodiment of the present invention will be described with reference to the accompanying drawings.
-
FIGS. 1 to 3 are a perspective view, a front view, and a plane view of a probe 100 in accordance with an embodiment of the present invention, respectively. Referring toFIGS. 1 to 3 , the probe 100 includes afirst waveguide 10, asecond waveguide 20, and athird waveguide 30. - The probe 100 may be used to measure the electromagnetic field of a near field.
- The
first waveguide 10, thesecond waveguide 20, and thethird waveguide 30 have a rectangular section, and the height and width of their insides are constant in an extending direction of the waveguides. Thesecond waveguide 20 has a smaller section than thefirst waveguide 10, and thethird waveguide 30 has a smaller section than thesecond waveguide 20. Since thethird waveguide 30 has the smallest section, it is possible to reduce the multiple reflection that may be caused when measuring the electromagnetic waves. Moreover, the measurement distance may become closer by as much as the reduced multiple reflection. - Generally, the waveguide functions as a high-pass filter (HPF). As the size of the section of the waveguide becomes smaller, a cutoff frequency of the waveguide becomes higher. If the
third waveguide 30 is formed to have a small section in order to reduce the multiple reflection, the cutoff frequency of thethird waveguide 30 may be much higher than the operating frequency band of the probe 100. Even in this case, the probe 100 may receive electromagnetic waves of the operating frequency band by using theresonance element 45. Further detailed description will be made below in conjunction with theresonance element 45. - When the probe 100 measures the electromagnetic waves, the electromagnetic waves are transmitted from the
third waveguide 30 through thesecond waveguide 20 to thefirst waveguide 10. Thesecond waveguide 20 matches impedance between thefirst waveguide 30 and thethird waveguide 10. - The probe 100 may include an electromagnetic wave absorber at the outer sides of the
waveguides - The probe 100 includes a first
double ridge 25 attached to the inside of thesecond waveguide 20, and a seconddouble ridge 35 attached to the inside of thethird waveguide 30. - Referring to
FIGS. 2 and 3 , the firstdouble ridge 25 is provided with a pair of ridges facing each other and attached to the inside of thesecond waveguide 20. The firstdouble ridge 25 matches impedance between thefirst waveguide 10 and thethird waveguide 30. The firstdouble ridge 25 lowers a cutoff frequency of thesecond waveguide 20. The seconddouble ridge 35 is provided with a pair of ridges and attached to the inside of thethird waveguide 30. The seconddouble ridge 35 lowers a cutoff frequency of thethird waveguide 30. The firstdouble ridge 25 and the seconddouble ridge 35 narrow the inside of the waveguides and guide electromagnetic waves transmitted through the inside of the waveguides. - Furthermore, the probe 100 includes a dielectric 50, a portion of which is disposed in the inside of the
third waveguide 30, and aresonance element 45 attached to the dielectric 50. As illustrated inFIGS. 1 to 3 , theresonance element 45 and the dielectric 50 are disposed at one side of thethird waveguide 30. Theresonance element 45 and the dielectric 50 constitute a resonance unit of the probe 100. - As illustrated in
FIGS. 1 to 3 , theresonance element 45 includes a plurality of ring-shaped conductive elements with a cut portion. Theresonance element 45 resonates at an operating frequency band of the probe 100. The probe 100 may receive electromagnetic waves of a desired frequency through theresonance element 45. - As the section of the
third waveguide 30 becomes smaller, the multiple reflection may be further reduced. If the section of thethird waveguide 30 is small, the cutoff frequency of thethird waveguide 30 may be higher than the operating frequency of the probe 100. Generally, a transverse permeability of the waveguide is negative at a frequency band lower than the cutoff frequency. On the other hand, a permittivity of the resonance element is negative at the resonant frequency band. Therefore, a transverse permeability of thethird waveguide 30 and a permittivity of theresonance element 45 are negative at the operating frequency band of the probe 100. When both the permeability and the permittivity are negative, the electromagnetic waves travel in the same manner as when both the permeability and the permittivity are positive. Due to this principle, the probe 100 may receive electromagnetic waves at the operating frequency band, while reducing the section of thethird waveguide 30. - Meanwhile, the
resonance element 45 includes a plurality of C-shaped conductive elements arranged in a row. As thethird waveguide 30 becomes longer, the multiple reflection is further reduced. If the number of the conductive elements included in theresonance element 45 increases, the length of thethird waveguide 30 increases. At this time, as the number of the conductive elements increases, the conductive and dielectric loss increases. However, the seconddouble ridge 35 minimizes the conductive and dielectric loss. The seconddouble ridge 35 may reduce the conductive and dielectric loss and lower the cutoff frequency of thethird waveguide 30. It can be easily understood by those skilled in the art that a single conductive element may be used as theresonance element 45. - As illustrated in
FIGS. 1 to 5 , the dielectric 50 has a substrate shape and supports theresonance element 45. Referring toFIG. 3 , which illustrates a plan view of the probe 100, the dielectric 50 is disposed in the center of thethird waveguide 30. The dielectric 50 includes aprotrusion 40 at a connection portion where the dielectric 50 and the seconddouble ridge 35 are connected together. Theprotrusion 40 matches impedance between thethird waveguide 30 and the dielectric 50. -
FIG. 4 is a sectional view of the resonance unit in accordance with the embodiment of the present invention. The resonance unit includes theprotrusion 40, theresonance element 45, and the dielectric 50. - As illustrated in
FIG. 4 , theresonance element 45 includes a plurality of C-shaped conductive elements. In this embodiment, the plurality of conductive elements are arranged on both sides of the dielectric 50 in a row. InFIG. 4 , the conductive elements arranged on the front side of the dielectric 50 are indicated by solid lines, and the conductive elements arranged on the rear side of the dielectric 50 are indicated by dotted lines. The conductive elements on the rear side of the dielectric 50 are arranged in the intervals of the conductive elements on the front side of the dielectric 50. This arrange of the conductive elements increases the electromagnetic-wave transmission efficiency. -
FIG. 5 is a sectional view of a resonance unit in accordance with another embodiment of the present invention. In this embodiment, the plurality of conductive elements constituting theresonance element 45 includecapacitors 42, respectively. - The
capacitors 42 shift the resonant frequency of theresonance element 45. When the capacitances of thecapacitors 42 are determined, the resonant frequency of theresonance element 45 is changed to a certain value. Meanwhile, when thecapacitors 42 are variable capacitors, the resonant frequency of theresonance element 45 may be changed by adjusting the capacitances of thecapacitors 42. - <Antenna>
- An antenna in accordance with an embodiment of the present invention includes a waveguide and a resonance unit. The resonance unit is entirely or partially disposed in the inside of the waveguide.
- The resonance unit may include a dielectric and a conductive resonance element attached to the dielectric. The antenna may further include a ridge attached to the inside of the waveguide and connected to the dielectric. The dielectric may be formed to protrude at a connection portion where the dielectric and the ridge are connected together.
- Meanwhile, the resonance element may be formed in a ring shape with a cut portion, and may include a capacitor attached to the cut portion. Furthermore, the resonance element may include a plurality of conductive elements electrically isolated from one another. The conductive elements may be attached to one side of the dielectric and arranged in a direction perpendicular to an opening side of the waveguide. Meanwhile, the conductive elements may include two conductive elements attached to one side of the dielectric, and conductive elements attached the other side of the dielectric and arranged between the two conductive elements, and may be arranged in a direction perpendicular to an opening side of the waveguide.
- The foregoing description of the probe may be applied to the antenna.
- The probe and the antenna in accordance with the embodiments of the present invention may reduce the multiple reflection of electromagnetic waves.
- While the present invention has been described with respect to the specific embodiments, it will be apparent to those skilled in the art that various changes and modifications may be made without departing from the spirit and scope of the invention as defined in the following claims.
Claims (10)
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
KR1020080121833A KR101133743B1 (en) | 2008-12-03 | 2008-12-03 | Probe and antenna |
KR10-2008-0121833 | 2008-12-03 |
Publications (2)
Publication Number | Publication Date |
---|---|
US20100134370A1 true US20100134370A1 (en) | 2010-06-03 |
US8373611B2 US8373611B2 (en) | 2013-02-12 |
Family
ID=42222342
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
US12/629,836 Expired - Fee Related US8373611B2 (en) | 2008-12-03 | 2009-12-02 | Probe and antenna using waveguide |
Country Status (2)
Country | Link |
---|---|
US (1) | US8373611B2 (en) |
KR (1) | KR101133743B1 (en) |
Cited By (19)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20120194399A1 (en) * | 2010-10-15 | 2012-08-02 | Adam Bily | Surface scattering antennas |
US20160184563A1 (en) * | 2011-01-27 | 2016-06-30 | Medtronic Xomed, Inc. | Adjustment for hydrocephalus shunt valve |
US9385435B2 (en) | 2013-03-15 | 2016-07-05 | The Invention Science Fund I, Llc | Surface scattering antenna improvements |
WO2016140377A1 (en) * | 2015-03-02 | 2016-09-09 | ķźµģ źø°ģ°źµ¬ģ | Slit antenna probe, and apparatus and method for inspecting defects of multi-junction semiconductor using same |
US9448305B2 (en) | 2014-03-26 | 2016-09-20 | Elwha Llc | Surface scattering antenna array |
US9647345B2 (en) | 2013-10-21 | 2017-05-09 | Elwha Llc | Antenna system facilitating reduction of interfering signals |
US9711852B2 (en) | 2014-06-20 | 2017-07-18 | The Invention Science Fund I Llc | Modulation patterns for surface scattering antennas |
US9825358B2 (en) | 2013-12-17 | 2017-11-21 | Elwha Llc | System wirelessly transferring power to a target device over a modeled transmission pathway without exceeding a radiation limit for human beings |
US9843103B2 (en) | 2014-03-26 | 2017-12-12 | Elwha Llc | Methods and apparatus for controlling a surface scattering antenna array |
US9853361B2 (en) | 2014-05-02 | 2017-12-26 | The Invention Science Fund I Llc | Surface scattering antennas with lumped elements |
US9882288B2 (en) | 2014-05-02 | 2018-01-30 | The Invention Science Fund I Llc | Slotted surface scattering antennas |
US9923271B2 (en) | 2013-10-21 | 2018-03-20 | Elwha Llc | Antenna system having at least two apertures facilitating reduction of interfering signals |
US9935375B2 (en) | 2013-12-10 | 2018-04-03 | Elwha Llc | Surface scattering reflector antenna |
US9971970B1 (en) * | 2015-04-27 | 2018-05-15 | Rigetti & Co, Inc. | Microwave integrated quantum circuits with VIAS and methods for making the same |
US10361481B2 (en) | 2016-10-31 | 2019-07-23 | The Invention Science Fund I, Llc | Surface scattering antennas with frequency shifting for mutual coupling mitigation |
US10446903B2 (en) | 2014-05-02 | 2019-10-15 | The Invention Science Fund I, Llc | Curved surface scattering antennas |
US11121301B1 (en) | 2017-06-19 | 2021-09-14 | Rigetti & Co, Inc. | Microwave integrated quantum circuits with cap wafers and their methods of manufacture |
US11276727B1 (en) | 2017-06-19 | 2022-03-15 | Rigetti & Co, Llc | Superconducting vias for routing electrical signals through substrates and their methods of manufacture |
WO2024036171A1 (en) * | 2022-08-12 | 2024-02-15 | Raytheon Company | Microwave cavity resonator and fixed-geometry probe |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4990870A (en) * | 1989-11-06 | 1991-02-05 | The United States Of America As Represented By The Secretary Of The Navy | Waveguide bandpass filter having a non-contacting printed circuit filter assembly |
US20020027483A1 (en) * | 2000-09-06 | 2002-03-07 | Murata Manufacturing Co., Ltd. | Filter, multiplexer, and communication apparatus |
US20040017272A1 (en) * | 2002-02-19 | 2004-01-29 | Smith Stephanie L. | Low cost dielectric tuning for E-plane filters |
US20070024399A1 (en) * | 2003-09-25 | 2007-02-01 | Universitat Autonoma De Barcelona | Filters and antennas for microwaves and millimetre waves, based on open-loop resonators and planar transmission lines |
Family Cites Families (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2002100912A (en) | 2000-09-22 | 2002-04-05 | Matsushita Electric Ind Co Ltd | Method for manufacturing waveguide circuit and waveguide circuit |
KR100834422B1 (en) | 2007-05-31 | 2008-06-04 | ķźµģ ģķµģ ģ°źµ¬ģ | Probe |
-
2008
- 2008-12-03 KR KR1020080121833A patent/KR101133743B1/en not_active Expired - Fee Related
-
2009
- 2009-12-02 US US12/629,836 patent/US8373611B2/en not_active Expired - Fee Related
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4990870A (en) * | 1989-11-06 | 1991-02-05 | The United States Of America As Represented By The Secretary Of The Navy | Waveguide bandpass filter having a non-contacting printed circuit filter assembly |
US20020027483A1 (en) * | 2000-09-06 | 2002-03-07 | Murata Manufacturing Co., Ltd. | Filter, multiplexer, and communication apparatus |
US20040017272A1 (en) * | 2002-02-19 | 2004-01-29 | Smith Stephanie L. | Low cost dielectric tuning for E-plane filters |
US20070024399A1 (en) * | 2003-09-25 | 2007-02-01 | Universitat Autonoma De Barcelona | Filters and antennas for microwaves and millimetre waves, based on open-loop resonators and planar transmission lines |
Cited By (38)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US9450310B2 (en) * | 2010-10-15 | 2016-09-20 | The Invention Science Fund I Llc | Surface scattering antennas |
US10320084B2 (en) | 2010-10-15 | 2019-06-11 | The Invention Science Fund I Llc | Surface scattering antennas |
US10062968B2 (en) | 2010-10-15 | 2018-08-28 | The Invention Science Fund I Llc | Surface scattering antennas |
US20120194399A1 (en) * | 2010-10-15 | 2012-08-02 | Adam Bily | Surface scattering antennas |
US20160184563A1 (en) * | 2011-01-27 | 2016-06-30 | Medtronic Xomed, Inc. | Adjustment for hydrocephalus shunt valve |
US10512762B2 (en) * | 2011-01-27 | 2019-12-24 | Medtronic Xomed, Inc. | Adjustment for hydrocephalus shunt valve |
US9385435B2 (en) | 2013-03-15 | 2016-07-05 | The Invention Science Fund I, Llc | Surface scattering antenna improvements |
US10090599B2 (en) | 2013-03-15 | 2018-10-02 | The Invention Science Fund I Llc | Surface scattering antenna improvements |
US9923271B2 (en) | 2013-10-21 | 2018-03-20 | Elwha Llc | Antenna system having at least two apertures facilitating reduction of interfering signals |
US10673145B2 (en) | 2013-10-21 | 2020-06-02 | Elwha Llc | Antenna system facilitating reduction of interfering signals |
US9647345B2 (en) | 2013-10-21 | 2017-05-09 | Elwha Llc | Antenna system facilitating reduction of interfering signals |
US9935375B2 (en) | 2013-12-10 | 2018-04-03 | Elwha Llc | Surface scattering reflector antenna |
US10236574B2 (en) | 2013-12-17 | 2019-03-19 | Elwha Llc | Holographic aperture antenna configured to define selectable, arbitrary complex electromagnetic fields |
US9871291B2 (en) | 2013-12-17 | 2018-01-16 | Elwha Llc | System wirelessly transferring power to a target device over a tested transmission pathway |
US9825358B2 (en) | 2013-12-17 | 2017-11-21 | Elwha Llc | System wirelessly transferring power to a target device over a modeled transmission pathway without exceeding a radiation limit for human beings |
US9843103B2 (en) | 2014-03-26 | 2017-12-12 | Elwha Llc | Methods and apparatus for controlling a surface scattering antenna array |
US9448305B2 (en) | 2014-03-26 | 2016-09-20 | Elwha Llc | Surface scattering antenna array |
US9853361B2 (en) | 2014-05-02 | 2017-12-26 | The Invention Science Fund I Llc | Surface scattering antennas with lumped elements |
US9882288B2 (en) | 2014-05-02 | 2018-01-30 | The Invention Science Fund I Llc | Slotted surface scattering antennas |
US10727609B2 (en) | 2014-05-02 | 2020-07-28 | The Invention Science Fund I, Llc | Surface scattering antennas with lumped elements |
US10446903B2 (en) | 2014-05-02 | 2019-10-15 | The Invention Science Fund I, Llc | Curved surface scattering antennas |
US9711852B2 (en) | 2014-06-20 | 2017-07-18 | The Invention Science Fund I Llc | Modulation patterns for surface scattering antennas |
US10998628B2 (en) | 2014-06-20 | 2021-05-04 | Searete Llc | Modulation patterns for surface scattering antennas |
US9806416B2 (en) | 2014-06-20 | 2017-10-31 | The Invention Science Fund I Llc | Modulation patterns for surface scattering antennas |
US9806415B2 (en) | 2014-06-20 | 2017-10-31 | The Invention Science Fund I Llc | Modulation patterns for surface scattering antennas |
US9812779B2 (en) | 2014-06-20 | 2017-11-07 | The Invention Science Fund I Llc | Modulation patterns for surface scattering antennas |
US9806414B2 (en) | 2014-06-20 | 2017-10-31 | The Invention Science Fund I Llc | Modulation patterns for surface scattering antennas |
WO2016140377A1 (en) * | 2015-03-02 | 2016-09-09 | ķźµģ źø°ģ°źµ¬ģ | Slit antenna probe, and apparatus and method for inspecting defects of multi-junction semiconductor using same |
US10769546B1 (en) | 2015-04-27 | 2020-09-08 | Rigetti & Co, Inc. | Microwave integrated quantum circuits with cap wafer and methods for making the same |
US9971970B1 (en) * | 2015-04-27 | 2018-05-15 | Rigetti & Co, Inc. | Microwave integrated quantum circuits with VIAS and methods for making the same |
US10068181B1 (en) | 2015-04-27 | 2018-09-04 | Rigetti & Co, Inc. | Microwave integrated quantum circuits with cap wafer and methods for making the same |
US11574230B1 (en) | 2015-04-27 | 2023-02-07 | Rigetti & Co, Llc | Microwave integrated quantum circuits with vias and methods for making the same |
US10361481B2 (en) | 2016-10-31 | 2019-07-23 | The Invention Science Fund I, Llc | Surface scattering antennas with frequency shifting for mutual coupling mitigation |
US11121301B1 (en) | 2017-06-19 | 2021-09-14 | Rigetti & Co, Inc. | Microwave integrated quantum circuits with cap wafers and their methods of manufacture |
US11276727B1 (en) | 2017-06-19 | 2022-03-15 | Rigetti & Co, Llc | Superconducting vias for routing electrical signals through substrates and their methods of manufacture |
US11770982B1 (en) | 2017-06-19 | 2023-09-26 | Rigetti & Co, Llc | Microwave integrated quantum circuits with cap wafers and their methods of manufacture |
US12207569B1 (en) | 2017-06-19 | 2025-01-21 | Rigetti & Co, Llc | Microwave integrated quantum circuits with cap wafers and their methods of manufacture |
WO2024036171A1 (en) * | 2022-08-12 | 2024-02-15 | Raytheon Company | Microwave cavity resonator and fixed-geometry probe |
Also Published As
Publication number | Publication date |
---|---|
KR20100063353A (en) | 2010-06-11 |
KR101133743B1 (en) | 2012-04-09 |
US8373611B2 (en) | 2013-02-12 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US8373611B2 (en) | Probe and antenna using waveguide | |
JP6482456B2 (en) | Millimeter wave antenna and millimeter wave sensor using the same | |
US9627772B2 (en) | Passive repeater for wireless communications | |
JP5555087B2 (en) | Radar equipment | |
US20210234279A1 (en) | Circularly polarized antenna | |
US8810461B2 (en) | Antenna coupler | |
JP2015043562A (en) | Suppressing modes in antenna feed including coaxial waveguide | |
US7495630B2 (en) | Feed point adjustable planar antenna | |
ITRM20120003A1 (en) | LOW NOISE OPENING ANTENNA | |
Daniyan et al. | Horn antenna design: the concepts and considerations | |
JP4511406B2 (en) | Antenna equipment | |
JP2009060403A (en) | Radio apparatus and antenna provided in radio apparatus | |
US9912037B2 (en) | Planar inverted-F wing antenna for wireless culinary appliances | |
KR100834422B1 (en) | Probe | |
US20130194144A1 (en) | Multi-resonance tunable antenna | |
RU2402843C1 (en) | Waveguide transition | |
CN202444041U (en) | High-pass strip line filter based on spiral stub | |
JP5978180B2 (en) | Millimeter wave filter and method for preventing leakage of electromagnetic wave | |
CN202474163U (en) | Stripline high-pass filter based on folding shorting stubs | |
RU2153742C1 (en) | Broad-band aerial | |
CN103311621A (en) | Strip line high-pass filter based on fine line stub | |
US9385410B2 (en) | Radio wave half mirror for millimeter wave band and method of flattening transmittance thereof | |
US9893422B2 (en) | Antenna with the eighth of the wavelength | |
CN110011042A (en) | Small-sized linear polarization transceiver common-frequency aerial | |
CN202487729U (en) | Strip line high-pass filter based on fine line stub |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
AS | Assignment |
Owner name: ELECTRONICS AND TELECOMMUNICATIONS RESEARCH INSTIT Free format text: ASSIGNMENT OF ASSIGNORS INTEREST;ASSIGNORS:OH, SOON-SOO;MOON, JUNG-ICK;KIM, JOUNG-MYOUN;AND OTHERS;REEL/FRAME:023596/0831 Effective date: 20091116 |
|
FEPP | Fee payment procedure |
Free format text: PAYOR NUMBER ASSIGNED (ORIGINAL EVENT CODE: ASPN); ENTITY STATUS OF PATENT OWNER: SMALL ENTITY |
|
STCF | Information on status: patent grant |
Free format text: PATENTED CASE |
|
REMI | Maintenance fee reminder mailed | ||
FPAY | Fee payment |
Year of fee payment: 4 |
|
SULP | Surcharge for late payment | ||
FEPP | Fee payment procedure |
Free format text: MAINTENANCE FEE REMINDER MAILED (ORIGINAL EVENT CODE: REM.); ENTITY STATUS OF PATENT OWNER: SMALL ENTITY |
|
LAPS | Lapse for failure to pay maintenance fees |
Free format text: PATENT EXPIRED FOR FAILURE TO PAY MAINTENANCE FEES (ORIGINAL EVENT CODE: EXP.); ENTITY STATUS OF PATENT OWNER: SMALL ENTITY |
|
STCH | Information on status: patent discontinuation |
Free format text: PATENT EXPIRED DUE TO NONPAYMENT OF MAINTENANCE FEES UNDER 37 CFR 1.362 |
|
FP | Lapsed due to failure to pay maintenance fee |
Effective date: 20210212 |