Noise Thermometry with Conventional Electronics

1978 ◽  
pp. 240-248
Author(s):  
L. Storm
Keyword(s):  
2021 ◽  
Vol 92 (1) ◽  
pp. 014904
Author(s):  
A. V. Talanov ◽  
J. Waissman ◽  
T. Taniguchi ◽  
K. Watanabe ◽  
P. Kim

1999 ◽  
Vol 9 (2) ◽  
pp. 4408-4411 ◽  
Author(s):  
D.A. Peden ◽  
J.C. Macfarlane ◽  
Ling Hao ◽  
R.P. Reed ◽  
J.C. Gallop

Author(s):  
Nathan E. Flowers-Jacobs ◽  
Alessio Pollarolo ◽  
Kevin J. Coakley ◽  
Adam C. Weis ◽  
Anna E. Fox ◽  
...  

In preparation for the redefinition of the International System of Units (SI), five different electronic measurements of the Boltzmann constant have been performed using different Johnson noise thermometry (JNT) systems over the past seven years. In this paper, we describe in detail the JNT system and uncertainty components associated with the most recent National Institute of Standards and Technology (NIST) determination of the Boltzmann constant: k = 1.380642 9(69) × 10−23 J/K, with a relative standard uncertainty of 5.0 × 10−6 and relative offset of −4.05 × 10−6 from the Committee on Data for Science and Technology (CODATA) 2014 recommended value. We discuss the input circuits and the approach we used to match the frequency response of two noise sources. We present new measurements of the correlated noise of the 4 K on-chip resistors in the quantum-accurate, pseudorandom, voltage-noise source, which we used to estimate the correlated, frequency-dependent, nonthermal noise in our system. Finally, we contrast our system with those used in other measurements and speculate on future improvements.


1986 ◽  
pp. 1263-1268
Author(s):  
Q. S. Shu ◽  
J. P. Harrison ◽  
S. Idziak ◽  
A. Sachrajda ◽  
T. Seeto
Keyword(s):  

2004 ◽  
pp. 159-168
Author(s):  
Yaakov Kraftmakher
Keyword(s):  

2020 ◽  
Vol 201 (5-6) ◽  
pp. 803-824
Author(s):  
A. Fleischmann ◽  
A. Reiser ◽  
C. Enss

AbstractIn recent years, current-sensing dc-SQUIDs have enabled the application of noise thermometry at ultralow temperatures. A major advantage of noise thermometry is the fact that no driving current is needed to operate the device and thus the heat dissipation within the thermometer can be reduced to a minimum. Such devices can be used either in primary or relative primary mode and cover typically several orders of magnitude in temperature extending into the low microkelvin regime. Here we will review recent advances of noise thermometry for ultralow temperatures.


Sign in / Sign up

Export Citation Format

Share Document