Abstract

The receiver is a signal receiving device in a radio telescope system. As an important parameter to characterize the receiver performance, noise temperature is very practical to calibrate accurately. The traditional receiver noise temperature calibration method is the cold and ambient load method. Through the establishment of K-band ambient receiver, and its amplitude calibration test platform of the cold and ambient load method, chopper wheel method, and ambient and hot load method, comparison and analysis of the above three methods were carried out. The test and calculation results show that the test accuracy of the cold and ambient load method is about 1.3%, that of the chopper wheel method (nonlow elevation) is about 3%, and that of the ambient and hot load method is about 9%. The test accuracy of the ambient and hot load method is slightly lower than that of the above two methods. The analysis is mainly due to the uncertainty of the hot load temperature and the small temperature difference between the two loads, which leads to the deterioration of the overall accuracy. But the advantage is that the method can perform real-time calibration in the process of observation, and it is easier to implement than the traditional cold and ambient load method. The results of noise temperature measurement are compared with those of theoretical calculation, the error is basically within 10%, and it can satisfy the demand of the noise temperature test. In the future, we expect that on the basis of increasing the hot load temperature, further experiments were carried out on the thermostatic treatment of hot load and the accuracy of temperature acquisition, and finally we hope that this method can better meet the testing requirements of receiver noise temperature and radio source amplitude calibration.

Highlights

  • IntroductionEreinto, Vamb is the power output of ambient load, Vcold is the power output of cold load, Tamb is the temperature of ambient load, and Tcold is the temperature of cold load

  • Under the premise that the sky temperature can be accurately obtained by the chopper wheel method, the error of 90° elevation is between 0.6% and 4%, the error of 30° elevation is between 3.2% and 7.7%, and the error of 5° elevation is between 21.4% and 30.3%. e test error of the ambient and hot load method is between 0.9% and 10.7%

  • Through the establishment of the K-band ambient receiver and its cold and ambient load method, chopper wheel method, and ambient and hot load method amplitude calibration test platform, comparison and analysis of the above three methods are carried out. e results show that the test accuracy of the cold and ambient load method is about 1.3%, the test accuracy of the chopper method is about 3%, and the test accuracy of the ambient and hot load method is about 9%

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Summary

Introduction

Ereinto, Vamb is the power output of ambient load, Vcold is the power output of cold load, Tamb is the temperature of ambient load, and Tcold is the temperature of cold load Combined with this amplitude and temperature response ratio g, we can control the telescope to point on the radio source and point off, and we can get the equivalent temperature value of the radio source TA (equation (2)). In order to reduce the noise temperature of the receiver, the first stage amplifier with lower noise coefficient is usually used in the design of the centimeter band receiver On this basis, if the sensitivity is expected to be further improved, it is generally used to cool the low noise amplifier and its prestage microwave devices (partly or wholly) below 20 K to reduce the noise temperature of the whole receiver system. In view of the fact that the noise temperature calibration of the receiver is the basis of the amplitude calibration of the whole telescope system and the key process to characterize the performance of the receiver, it is of great practical significance to carry out relevant calibration research in the corresponding band

Amplitude Calibration Method
System Construction and Test
Discussion
Conclusions
Full Text
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