Robert Lehmensiek
Research Subjects
Robert Lehmensiek has a total of 7 co-authors. Here are the top co-authors by number of shared publications:
- Dirk I. L. de Villiers
Department of Electrical and Electronic Engineering, Stellenbosch University, Stellenbosch, South Africa
3 shared publications - Isak P. Theron
EMSS Antennas (Pty) Ltd,Stellenbosch,South Africa
3 shared publications Alexander Krebs
EMSS Antennas (Pty) Ltd,Stellenbosch,South Africa
1 shared publicationEvan C. Knox-Davies
EMSS Antennas (Pty) Ltd, Stellenbosch
1 shared publication- Nianhua Jiang
National Research Council Canada (Canada)
1 shared publication Ockert B. Jacobs
EMSS Antennas (Pty) Ltd, Stellenbosch
1 shared publication
Latest Publications
- 5 September 2022
- Published by Institute of Electrical and Electronics Engineers (IEEE)
- Vol. 580, 307-310
Aspects of the Feed Production and Support for MeerKAT and SKA – a Retrospective View
This paper highlights some of the lessons learned during the design, production, and operation of the MeerKAT and SKA feeds and the design of the reflector surfaces.
- 5 September 2022
- Published by Institute of Electrical and Electronics Engineers (IEEE)
- Vol. 580, 307-310
Aspects of the Feed Production and Support for MeerKAT and SKA – a Retrospective View
This paper highlights some of the lessons learned during the design, production, and operation of the MeerKAT and SKA feeds and the design of the reflector surfaces.
- 5 September 2022
- Published by Institute of Electrical and Electronics Engineers (IEEE)
- p. 374
The optics and feed design of the 18 metre reflector antenna for the ngVLA
A new radio astronomy interferometer called the Next Generation Very Large Array (ngVLA), a project of the National Radio Astronomy Observatory (NRAO), is envisaged to be built on the Plains of San Agustin in New Mexico, USA [1]. The instrument consists of offset Gregorian dual reflector antennas with approximately 244 antennas with an 18 meter aperture diameter and 19 antennas with 6 meter aperture diameter. At the reflector system’s focus is a suite of cryogenic feeds mounted on an indexer mechanism which cover the frequency range from 1.2 GHz to 116 GHz with a gap at the atmospheric absorption band between 50.5 GHz and 70 GHz.
- 5 September 2022
- Published by Institute of Electrical and Electronics Engineers (IEEE)
- p. 374
The optics and feed design of the 18 metre reflector antenna for the ngVLA
A new radio astronomy interferometer called the Next Generation Very Large Array (ngVLA), a project of the National Radio Astronomy Observatory (NRAO), is envisaged to be built on the Plains of San Agustin in New Mexico, USA [1]. The instrument consists of offset Gregorian dual reflector antennas with approximately 244 antennas with an 18 meter aperture diameter and 19 antennas with 6 meter aperture diameter. At the reflector system’s focus is a suite of cryogenic feeds mounted on an indexer mechanism which cover the frequency range from 1.2 GHz to 116 GHz with a gap at the atmospheric absorption band between 50.5 GHz and 70 GHz.
- 28 January 2022
- Published by Institute of Electrical and Electronics Engineers (IEEE) in IEEE Transactions on Antennas and Propagation
- Vol. 70 (6) , 4784-4793
Multi-Level Approximations for Fast and Accurate Antenna Noise Temperature Calculation of Dual-Reflector Antennas
Antenna noise temperature calculation for a reflector antenna system can be a computationally expensive operation if the structure is electrically large. Several approximate methods have been suggested to speed up the calculation. These rely on removing one or more of the reflecting surfaces from the calculation domain and compensating for the effect through geometric optics arguments. This article presents a unified multilevel approximation formalism, which allows the user the freedom to tradeoff the simulation time, implementation complexity, and result accuracy as required for a specific application. As part of the formalism, a strategy to reliably remove both reflectors in a dual-reflector system from the calculation domain and rely on ray tracing to correct the background temperature is developed. It is shown that this new method reduces calculation time by several orders of magnitude while maintaining accuracy in the final antenna temperature result of the order of 1%. It is fast and accurate enough to be used in numerical optimization loops. The method requires the implementation of a ray tracing algorithm, and thus, may present some unnecessary complexity if only rough temperature estimates are required. To this end, a simplified method is also presented requiring no ray tracing and only simple postprocessing of readily available feed pattern data. Though not as accurate as of the ray tracing-based method, temperatures may be estimated with around 10% accuracy over bandwidths well in excess of a decade.
- 28 January 2022
- Published by Institute of Electrical and Electronics Engineers (IEEE) in IEEE Transactions on Antennas and Propagation
- Vol. 70 (6) , 4784-4793
Multi-Level Approximations for Fast and Accurate Antenna Noise Temperature Calculation of Dual-Reflector Antennas
Antenna noise temperature calculation for a reflector antenna system can be a computationally expensive operation if the structure is electrically large. Several approximate methods have been suggested to speed up the calculation. These rely on removing one or more of the reflecting surfaces from the calculation domain and compensating for the effect through geometric optics arguments. This article presents a unified multilevel approximation formalism, which allows the user the freedom to tradeoff the simulation time, implementation complexity, and result accuracy as required for a specific application. As part of the formalism, a strategy to reliably remove both reflectors in a dual-reflector system from the calculation domain and rely on ray tracing to correct the background temperature is developed. It is shown that this new method reduces calculation time by several orders of magnitude while maintaining accuracy in the final antenna temperature result of the order of 1%. It is fast and accurate enough to be used in numerical optimization loops. The method requires the implementation of a ray tracing algorithm, and thus, may present some unnecessary complexity if only rough temperature estimates are required. To this end, a simplified method is also presented requiring no ray tracing and only simple postprocessing of readily available feed pattern data. Though not as accurate as of the ray tracing-based method, temperatures may be estimated with around 10% accuracy over bandwidths well in excess of a decade.
- Open Access
- 22 October 2021
- Published by SPIE-Intl Soc Optical Eng in Journal of Astronomical Telescopes, Instruments, and Systems
- Vol. 8 (01) , 011002-15
L-band cryogenic radio astronomy receiver front-end of the Square Kilometre Array
Receiving sensitivity, arguably the most important metric for astronomical radio telescopes, is defined as the ratio of effective aperture area to system noise temperature (). The system noise temperature is the sum of the antenna noise temperature, determined by the feed horn and reflector system’s combined radiation characteristics, and the receiver noise temperature, determined by resistive losses in the receiver chain plus the low-noise amplifier’s (LNA) noise contribution. The antenna noise temperature includes the emission from water vapor and dry air in the atmosphere, the apparent temperature due to the cosmic microwave background and galactic emissions as seen through the atmosphere, and the ground emission. Since the sensitivity scales linearly with the total collecting area of the system, any improvement to the noise temperature of a single dish in an interferometric array leads to a corresponding reduction in the total number of dishes required to achieve the same system sensitivity. With a 15 K system temperature, a 0.5 K improvement in the system temperature allows removing one dish in thirty, saving about 7% in operational time for each science experiment, highlighting the importance of a carefully optimized antenna system and cryogenic receiver front-end.- 22 October 2021
- Published by SPIE-Intl Soc Optical Eng in Journal of Astronomical Telescopes, Instruments, and Systems
- Vol. 8 (01) , 011002-15
Open AccessL-band cryogenic radio astronomy receiver front-end of the Square Kilometre Array
Receiving sensitivity, arguably the most important metric for astronomical radio telescopes, is defined as the ratio of effective aperture area to system noise temperature (). The system noise temperature is the sum of the antenna noise temperature, determined by the feed horn and reflector system’s combined radiation characteristics, and the receiver noise temperature, determined by resistive losses in the receiver chain plus the low-noise amplifier’s (LNA) noise contribution. The antenna noise temperature includes the emission from water vapor and dry air in the atmosphere, the apparent temperature due to the cosmic microwave background and galactic emissions as seen through the atmosphere, and the ground emission. Since the sensitivity scales linearly with the total collecting area of the system, any improvement to the noise temperature of a single dish in an interferometric array leads to a corresponding reduction in the total number of dishes required to achieve the same system sensitivity. With a 15 K system temperature, a 0.5 K improvement in the system temperature allows removing one dish in thirty, saving about 7% in operational time for each science experiment, highlighting the importance of a carefully optimized antenna system and cryogenic receiver front-end. - 25 June 2021
- Published by Institute of Electrical and Electronics Engineers (IEEE) in IEEE Transactions on Antennas and Propagation
- Vol. 69 (12) , 8282-8290
An Optimal 18 m Shaped Offset Gregorian Reflector for the ngVLA Radio Telescope
This paper describes the design of the 18-meter shaped offset Gregorian reflector system for the Next Generation Very Large Array (ngVLA) radio interferometer and the associated 1.66:1 axially corrugated conical horn antennas. A parametric sweep determined feed horns with the goal of pattern symmetry and low spillover efficiency. Given these feeds, a mapping function for the shaped offset Gregorian reflector system was then determined, by a full factorial design, to achieve maximum receiving sensitivity with secondary parameters such as plate scale, scan loss, sidelobe, and cross-polarization at acceptable levels. A sub-reflector extension is included in a feed-down tipping configuration with improved performance over the feed-up case. The resultant optics and feeds achieve very symmetrical patterns with an aperture efficiency of around 95 %, a plate scale of 15 arcsec/mm, and first and second sidelobe levels of -18 dB and -24 dB respectively. The receiving sensitivity at 30 GHz is 8.7 m2/K and increases to above 12 m2/K at 12.3 GHz, and reduces to 1.5 m2/K at 116 GHz (ignoring efficiency loss due to non-ideal reflector surfaces). These sensitivities are close to the theoretical optimum.
- 25 June 2021
- Published by Institute of Electrical and Electronics Engineers (IEEE) in IEEE Transactions on Antennas and Propagation
- Vol. 69 (12) , 8282-8290
An Optimal 18 m Shaped Offset Gregorian Reflector for the ngVLA Radio Telescope
This paper describes the design of the 18-meter shaped offset Gregorian reflector system for the Next Generation Very Large Array (ngVLA) radio interferometer and the associated 1.66:1 axially corrugated conical horn antennas. A parametric sweep determined feed horns with the goal of pattern symmetry and low spillover efficiency. Given these feeds, a mapping function for the shaped offset Gregorian reflector system was then determined, by a full factorial design, to achieve maximum receiving sensitivity with secondary parameters such as plate scale, scan loss, sidelobe, and cross-polarization at acceptable levels. A sub-reflector extension is included in a feed-down tipping configuration with improved performance over the feed-up case. The resultant optics and feeds achieve very symmetrical patterns with an aperture efficiency of around 95 %, a plate scale of 15 arcsec/mm, and first and second sidelobe levels of -18 dB and -24 dB respectively. The receiving sensitivity at 30 GHz is 8.7 m2/K and increases to above 12 m2/K at 12.3 GHz, and reduces to 1.5 m2/K at 116 GHz (ignoring efficiency loss due to non-ideal reflector surfaces). These sensitivities are close to the theoretical optimum.
- 1 September 2007
- Published by Institute of Electrical and Electronics Engineers (IEEE)
- No. 21530025,p. 1-5
On the design of the feed horns for the karoo array telescope dish antennas
This paper describes the design of the feed horns for the Karoo array telescope (KAT) experimental prototype dish. The feed horn is a dual polarized circular horn with a linearly polarized circular pattern operating from 1414 to 1670 MHz. The horn is excited with a quad-ridged ortho-mode transducer (OMT).
- 1 September 2007
- Published by Institute of Electrical and Electronics Engineers (IEEE)
- No. 21530025,p. 1-5
On the design of the feed horns for the karoo array telescope dish antennas
This paper describes the design of the feed horns for the Karoo array telescope (KAT) experimental prototype dish. The feed horn is a dual polarized circular horn with a linearly polarized circular pattern operating from 1414 to 1670 MHz. The horn is excited with a quad-ridged ortho-mode transducer (OMT).