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Analysis of the input noise contribution in the noise temperature measurements

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IEEE MICROWAVE AND WIRELESS COMPONENTS LETTERS, VOL. 15, NO. 3, MARCH 2005 141

Analysis of the Input Noise Contribution

in the Noise Temperature Measurements

Robert Hu

Abstract—In measuring the noise temperature of a cryogenic microwave low-noise amplifier (LNA), the noise from the input thermal buffer, i.e., the coaxial cable that connects the noise source to the amplifier, needs to be correctly accounted for. With the amplifier’s noise temperature approaching just a few Kelvins, the postulate used in calculating the cable’s noise temperature, that the cable is homogeneous and has a linear temperature profile, commands a further inspection. This letter analyzes these assumptions and clarifies the situations in which they hold. To substantiate this Kelvin-level discretion, a LNA is designed and measured.

Index Terms—Noise temperature measurement.

I. INTRODUCTION

M

ICROWAVE low-noise amplifier (LNA) is widely used in radio-astronomy receivers and its noise temperature can be just a few kelvins [1], [2]. To carry out accurate mea-surements both at room temperature and cryogenically, the noise from the input coaxial cable, which serves as a thermal buffer between the LNA and the noise source, needs to be known ac-curately. Ideally, by treating the cable as a uniform, i.e., homo-geneous, medium with constant thermal conductivity, tempera-ture along the cable can be assumed linear [3]. However, since a coaxial cable comprises inner conductor, outer conductor and dielectric insulator in between, and, even worse, thermal con-ductivity is in general a function of temperature, this linear as-sumption seems susceptible and should be reexamined. Knowl-edge of this input thermal buffer’s noise will be even critical in the more demanding areas, such as cryogenic on-wafer noise measurements [4], [5].

In this letter, by modeling the coaxial cable as a two-port thermal transmission line, it is proved that the temperature of the inner conductor does follow that of the outer conductor, except at the very boundaries. So, with caution, linear temperature pro-file can be adopted and a close-form expression for the coaxial cable is therefore derived. If the cable is low-loss, a further sim-plification ensues.

II. CABLE’STEMPERATUREPROFILE

To obtain the temperature profile along the coaxial cable, a thermal model needs to be constructed first (see Figs. 1 and 2).

Manuscript received March 24, 2004; revised October 28, 2004. The review of this letter was arranged by Associate Editor A. Stelzer.

The author is with the Department of Electronics Engineering, National Chiao Tung University (NCTU), Hsinchu, Taiwan, R.O.C.

Digital Object Identifier 10.1109/LMWC.2004.842832

Fig. 1. Cryogenic noise-temperature measurement using variable-temperature load method. The temperature of the 50- resistors, as indicated, can be changed and monitored during the measurement. The input 5-in coaxial cable on the LNA branch works as a thermal buffer to prevent the LNA from heating up by the variable-temperature 50- resistor. The other 5-in coaxial cable, as directly connecting to the switch, is for calibration purpose.

Fig. 2. Coaxial cable modeling. This distributed cable model comprises the inner and outer thermal resistanceR , R , and the radial (shunt) thermal conductanceG . Radii r to r , as indicated by the arrowed lines, are the radii of the boundary of the inner stainless steel, inner copper, Teflon, optional outer copper, outer stainless steel and jacket, respectively.

The cable, as discussed throughout this letter, is the 5-in se-ries- cable made by SSI Cable Corporation, which can be modeled thermally with

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142 IEEE MICROWAVE AND WIRELESS COMPONENTS LETTERS, VOL. 15, NO. 3, MARCH 2005

where , , , and are the temperatures and heat flows along the inner and outer conductors. The three constants ,

, and are linked to the cable’s geometry

(2)

The thermal conductivity of the stainless steel at room tem-perature is, according to Goodfellow, around 16.3, pure copper

has 401, alloy copper such as has

be-tween 60 and 120, and Teflon has 0.25, all with unit of W m K . Therefore, this SSI coaxial cable has

m K W, m K W, and

W m K .

At first glance, since the shunt thermal conductance is large as compared with and , the temperature differ-ence between the inner and outer conductors on the same cross section should be very small except at the boundaries, which is defined by the characteristic distance with

(3) Mathematically, the solution of (1), i.e., the temperature distri-bution on the cable with length , is

(4) The four unknowns , , , and can be easily decided from the four end-point constrains , , , and on the inner and outer conductors. If the inner and outer conductors are

ther-mally connected, i.e., 0, then , ,

and their corresponding temperature profiles must be linear and identical. If , such as air line, then the inner and outer temperature profiles are linear but unrelated.

As for the intended coaxial cable, its characteristic distance at room temperature is 0.18 in (4.57 mm) which is a small fraction of the total cable length; therefore, a linear temperature profile holds (Fig. 3). As temperature decreases, thermal con-ductivities of both stainless steel and Teflon decrease while that of copper will increase. The composite effects will cause the cable’s cryogenic characteristic distance to increase but is still far less than the cable’s total length. In short, the coaxial cable can be treated as a uniform medium in most cryogenic noise measurements.

Another implication of the simulated results is that, even the heater and temperature sensor in Fig. 1 are attached to the out-side of the 50- termination, temperature inside the termination does follow that on the outside and the temperature sensor can record correctly.

Fig. 3. Simulated temperature profile and power transfer along the 5-in coaxial cable. (a) The inner and outer temperature profiles. The four end-point temperatures of this cable are set to be 300, 300, 300, and 250 K. The large radial thermal conductivity of the cable means the temperature of the inner conductor is following that of the outer conductor on most part of the cable. (b) The corresponding inner and outer heat transfers. Most of the heat is flowing in the radial direction and is confined at one end.

III. CABLE’SNOISETEMPERATURECALCULATION

For a two-port lumped passive component, that is reciprocal and has no input reflection, its noise temperature is

where is the power gain, or , and is the ambient temperature. By dividing the cable into infini-tesimal sections where the th section has power gain

and physical temperature , the cable’s noise tem-perature is

(5) where and are the end-point temperatures and a linear temperature profile along the cable is assumed. Of course, if

, then . Otherwise, since

(6) or

(7) there is

(8) If the cable is low-loss, i.e., and , then, as , the above expression can be simplified as

(9) In this situation, the cable can be treated as a lumped element with equivalent physical temperature of .

However, since thermal conductivity is in general a function of temperature rather than a constant, the real temperature pro-file along the cable is more complicated. As an example, in the cryogenic noise temperature measurement in the liquid Helium (LHe) cryostat where one end of the coaxial cable is heated from 4 to 20 K while the other end is kept at 4 K, a copper cable with

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HU: ANALYSIS OF THE INPUT NOISE CONTRIBUTION IN THE NOISE TEMPERATURE MEASUREMENTS 143

Fig. 4. Temperature profile of the coaxial cable used in the cryogenic noise-temperature measurements. (a) The assumed thermal conductivity of pure copper from 4 to 300 K. (b) The temperature profile along the 5-in cable made with copper that has end-point temperatures of 4 and 20 K. The solid curve is the simulated result while the dashed curve is its linear counterpart.

Fig. 5. LNA circuit. (a) This is a three-stage amplifier with common drain and gate biases, and is fabricated by Raytheon. The layout has dimensions of 20002 750 2 75 m . (b) In the schematic, the capacitance is in fentofarads and the resistance is in.

0.5-dB loss should have, through simulation, equivalent phys-ical temperature of 13.5 K rather than from 12 K (Fig. 4). Nonetheless, the cable’s output noise-temperature dif-ference, which is directly related to the measured noise-tem-perature uncertainty of the LNA, is a mere

0.185 K. In other words, except in the ultra-low-noise cryogenic LNA measurements or in the more demanding noise-parameter measurements, the use of the above noise expression is acceptable. As an illustration, a 10-K cryo-genic amplifier is designed and tested (Figs. 5 and 6), where the aforementioned 0.185 K offset appears to be tolerable.

So far, the other noise-temperature measurement method, the so-called cold-attenuator method where the input coaxial cable is connecting the commercial noise source at room temperature to the cold attenuator inside the cryostat [6], is left undiscussed. This is because, from the above analysis, it is obvious that the

Fig. 6. Noise temperatureT and gain of the LNA inside the 4 K liquid Helium dewar. The solid curves correspond to bias condition ofV = 0.8 V and I = 23 mA while the dashed curves are withV = 0.5 V and I = 10 mA.

cable’s noise contribution cannot be accurately retrieved. And quite often, the resulting noise temperature of a sensitive am-plifier measured using the cold-attenuator method is negative, which apparently is due to an over-estimation of the cable’s noise. It is too bold assuming the equivalent physical tempera-ture of a cable stretching from room temperatempera-ture (around 296 K) to 4 K is simply (296 4)/2 150 K. Practically, cold-attenuator method needs to be calibrated with the help of variable-temper-ature-load method.

IV. CONCLUSION

In this letter, the noise of the input coaxial cable used in the noise-temperature measurements has been analyzed, and the condition where close-form expressions hold is clarified. As an illustration, a cryogenic amplifier is designed and tested. Its low noise temperature justifies this letter’s kelvin-level discretion.

ACKNOWLEDGMENT

The author wishes to thank Dr. S. Weinreb and T. Vayonakis, Caltech, and J. Ward, JPL, for their suggestions.

REFERENCES

[1] S. Weinreb, D. L. Fensternmacher, and R. W. Harris, “Ultra-low-noise 1.2- to 1.7-GHz cooled GaAsFET amplifier,” IEEE Trans. Microw.

Theory Tech., vol. 82, no. 6, pp. 847–853, Jun. 1982.

[2] N. Wadefalk et al., “Cryogenic wide-band ultra-low-noise IF amplifiers operating at ultra-low DC power,” IEEE Trans. Microw. Theory Tech., vol. 51, no. 6, pp. 1705–1711, Jun. 2003.

[3] J. Ward, “Observation of Carbon Monoxide in the Starburst Galaxy M82 With a 690 GHz Wide Receiver,” Ph.D. dissertation, California Inst. Technol., Pasadena, CA, 2002.

[4] J. Laskar, J. J. Bautista, M. Nishimoto, M. Hamai, and R. Lai, “Develop-ment of accurate on-wafer, cryogenic characterization technique,” IEEE

Trans. Microw. Theory Tech., vol. 44, no. 7, pp. 1178–1183, Jul. 1996.

[5] A. Caddemi and N. Donato, “Characterization techniques for temper-ature-dependent experimental analysis of microwave transistor,” IEEE

Trans. Instrum. Meas., vol. 52, no. 1, pp. 85–91, Feb. 2003.

[6] J. D. Gallego, “Definition of measurements of performance of X band cryogenic amplifiers,” Technical Note ESA/CAY-01 TN01, Centro As-tronomico de yebes Observatorio AsAs-tronomico Nacional, Madrid, Spain, 2000.

數據

Fig. 1. Cryogenic noise-temperature measurement using variable-temperature load method
Fig. 3. Simulated temperature profile and power transfer along the 5-in coaxial cable
Fig. 6. Noise temperature T and gain of the LNA inside the 4 K liquid Helium dewar. The solid curves correspond to bias condition of V = 0.8 V and I = 23 mA while the dashed curves are with V = 0.5 V and I = 10 mA.

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