DocumentCode
954932
Title
On some aspects of superconducting quantum interferometer optimization
Author
Vasiliev, B.V. ; Danilov, V.V. ; Likharev, K.K.
Author_Institution
IEEE TMAG
Volume
11
Issue
2
fYear
1975
fDate
3/1/1975 12:00:00 AM
Firstpage
743
Lastpage
748
Abstract
A problem is considered of optimizing the following parameters of the single-junction quantum superconducting fluxmeter: 1. The full range output signal of the magnitometer ΔA. 2. The derivative of the signal characteristic
3. The minimum detected flux change δφ For the hysteresis case (
) the following results have been obtained. In the resistive mode (
) the maximum value ΔA equals (
where the maximum value of the function
is about unity, when
. A satisfactory agreement has been obtained between the measured and calculated dependences of ΔA on k and CT parameters for the fluxmeter having a pumping frequency of about 10 MHz and the high-Q circuit. With detuning
conditioning either a triangular or trapezoidal waveform pattern, γ is as usually given by
If the detuning is great and negative a signal amplitude may take a rectangular form, and γ in this case is much more larger than γo . The experimentally obtained value
Gs.cm2is near enough to the known theoretical estimation. Calculations indicate that for a nonhysteresis case one may have the following formulae:
and
giving
Gs.cm2/
when
,
H (not taking into account the noise of the amplifier). The magnetometers were employed to search for the electrical dipole moment of the electron in the macroscopic experiment, in low temperature paramagnetic thermometry and also to test the degree of magnetic field shielding with a hollow superconducting screen.
3. The minimum detected flux change δφ For the hysteresis case (
) the following results have been obtained. In the resistive mode (
) the maximum value ΔA equals (
where the maximum value of the function
is about unity, when
. A satisfactory agreement has been obtained between the measured and calculated dependences of ΔA on k and C
conditioning either a triangular or trapezoidal waveform pattern, γ is as usually given by
If the detuning is great and negative a signal amplitude may take a rectangular form, and γ in this case is much more larger than γ
Gs.cm2is near enough to the known theoretical estimation. Calculations indicate that for a nonhysteresis case one may have the following formulae:
and
giving
Gs.cm2/
when
,
H (not taking into account the noise of the amplifier). The magnetometers were employed to search for the electrical dipole moment of the electron in the macroscopic experiment, in low temperature paramagnetic thermometry and also to test the degree of magnetic field shielding with a hollow superconducting screen.Keywords
Magnetometers, superconducting; Circuits; Electrons; Estimation theory; Frequency measurement; Hysteresis; Magnetic noise; Magnetometers; Paramagnetic materials; Superconducting device noise; Temperature;
fLanguage
English
Journal_Title
Magnetics, IEEE Transactions on
Publisher
ieee
ISSN
0018-9464
Type
jour
DOI
10.1109/TMAG.1975.1058688
Filename
1058688
Link To Document