CN112763768B - Driving method, system and controller for direct-current quantum small voltage - Google Patents

Driving method, system and controller for direct-current quantum small voltage Download PDF

Info

Publication number
CN112763768B
CN112763768B CN202011517649.2A CN202011517649A CN112763768B CN 112763768 B CN112763768 B CN 112763768B CN 202011517649 A CN202011517649 A CN 202011517649A CN 112763768 B CN112763768 B CN 112763768B
Authority
CN
China
Prior art keywords
quantum
superconducting
small voltage
voltage
microwave
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Active
Application number
CN202011517649.2A
Other languages
Chinese (zh)
Other versions
CN112763768A (en
Inventor
朱珠
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Beijing Institute of Radio Metrology and Measurement
Original Assignee
Beijing Institute of Radio Metrology and Measurement
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Beijing Institute of Radio Metrology and Measurement filed Critical Beijing Institute of Radio Metrology and Measurement
Priority to CN202011517649.2A priority Critical patent/CN112763768B/en
Publication of CN112763768A publication Critical patent/CN112763768A/en
Application granted granted Critical
Publication of CN112763768B publication Critical patent/CN112763768B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R1/00Details of instruments or arrangements of the types included in groups G01R5/00 - G01R13/00 and G01R31/00
    • G01R1/28Provision in measuring instruments for reference values, e.g. standard voltage, standard waveform

Abstract

The invention discloses a driving method, a system and a controller for direct current quantum small voltage, belonging to the technical field of voltage driving; the invention adopts microwave drive frequency adjustment and combines with a bias current drive control technology, and simultaneously changes the frequency of microwave drive signals applied to the superconducting array junctions and the number of the superconducting array junctions driven by the bias current, thereby obtaining accurate direct current quantum small voltage signals and greatly reducing the deviation between the programmable Josephson voltage standard output direct current small voltage signals (1 mV-10 mV) and a nominal value.

Description

Driving method, system and controller for direct-current quantum small voltage
Technical Field
The invention relates to the technical field of voltage driving, in particular to a driving method, a driving system and a driving controller for direct-current quantum small voltage.
Background
The programmable Josephson quantum voltage standard is used as the highest standard to carry out magnitude transmission on an alternating current voltage parameter and a direct current voltage parameter, can realize the output of the direct current quantum voltage, can also realize the output of the alternating current voltage through dynamic scanning, and has wide application in the aspects of electrical metering, aerospace and high-end measurement of the alternating current voltage and the direct current voltage of a weapon system.
The minimum output of the dc quantum voltage realized by the programmable josephson quantum voltage standard is the first quantum voltage step of a superconducting junction. The prior driving method for the direct current quantum voltage is that a microwave source is adopted to carry out irradiation driving on a superconducting array junction in liquid helium, so that the superconducting array junction is in a zero-step state, and then a bias current driving signal is applied to the superconducting array junction, so that the superconducting array junction generates a first quantum voltage step, and at the moment, a direct current quantum voltage signal can be obtained; and driving the programmable Josephson array junctions with different numbers to obtain different direct current quantum voltage outputs. The driving method is a common driving method of the current programmable Josephson, the driving is simple and convenient, but because the voltage magnitude of the quantum voltage step is a non-integer, the output direct current quantum voltage has certain deviation with the required magnitude, and particularly when a direct current small voltage signal (1 mV-10 mV) is output, the relative numerical value of the deviation is larger.
Disclosure of Invention
The invention aims to provide a driving method, a driving system and a driving controller for a direct current quantum small voltage, so that the difference value between the actual output voltage magnitude and the nominal value is close to 0, and the accuracy of the direct current small voltage signal output is improved.
In order to achieve the purpose, the invention provides the following scheme:
a driving method for dc quantum small voltage, the method comprising:
acquiring a nominal value V of a direct-current quantum small voltage, a quantum voltage step number n of a superconducting junction and a microwave frequency f;
according to the nominal value V of the direct current quantum small voltage, the quantum voltage step number N of the superconducting junction and the microwave frequency f, N is utilized1=V*KJCalculating the number N of the superconducting array junctions applying the bias current driving signals by using a/nf model1(ii) a The number N of the superconducting array junctions applying the bias current drive signal1Taking an integer; wherein KJIs the josephson constant;
according to the nominal value V of the direct current quantum small voltage and the number N of the superconducting array junctions applying the bias current driving signal1Using f1=V*KJ/N1Obtaining the microwave driving frequency f by model calculation1
According to the number N of the superconducting array junctions applying the bias current driving signal1And a microwave drive frequency f1Using V1=N1*nf1/KJThe model obtains the actual output DC quantum small voltage value V1
Optionally, the quantum voltage step number n of the superconducting junction is 1.
Optionally, the Josephson constant KJ=483597.848416984GHz/V。
A drive system for dc quantum small voltages, the system comprising:
the parameter acquisition module is used for acquiring a nominal value V of the direct-current quantum small voltage, the quantum voltage step number n of the superconducting junction and the microwave frequency f;
a superconducting array junction number calculation module for utilizing N according to the DC quantum small voltage nominal value V, the quantum voltage step number N of the superconducting junction and the microwave frequency f1=V*KJCalculating the number N of the superconducting array junctions applying the bias current driving signal by the nf model1(ii) a The number N of the superconducting array junctions applying the bias current drive signal1Taking an integer; wherein KJIs the josephson constant;
a microwave drive frequency calculation module for calculating a frequency based onThe nominal value V of the direct current quantum small voltage and the number N of the superconducting array junctions applying the bias current driving signal1Using f1=V*KJ/N1Obtaining the microwave driving frequency f by model calculation1
A DC quantum small voltage output module for applying bias current drive signal to the superconducting array junction number N1And a microwave drive frequency f1Using V1=N1*nf1/KJThe model obtains the actual output DC quantum small voltage value V1
Optionally, the quantum voltage step number n of the superconducting junction is 1.
Optionally, the Josephson constant KJ=483597.848416984GHz/V。
A drive controller for dc quantum small voltages, the controller comprising:
the input device is used for inputting a nominal value V of the direct current quantum small voltage, the quantum voltage step number n of the superconducting junction and the microwave frequency f;
calculating the number of superconducting array junctions N for applying a bias current drive signal1The first computing device of (1); the first computing device utilizes N according to the nominal value V of the direct current quantum small voltage, the quantum voltage step number N of the superconducting junction and the microwave frequency f1=V*KJCalculating the number N of the superconducting array junctions applying the bias current driving signals by using a/nf model1(ii) a The number N of the superconducting array junctions applying the bias current drive signal1Taking an integer; wherein KJIs the josephson constant;
for calculating the microwave drive frequency f1The second computing device of (1); the second computing device applies a bias current drive signal to the superconducting array junction according to the nominal value V of the direct current quantum small voltage and the number N of the superconducting array junctions1Using f1=V*KJ/N1Obtaining the microwave driving frequency f by model calculation1
The output device is used for outputting the direct current quantum small voltage; the output device drives the super of the signal according to the applied bias currentNumber of conducting array junctions N1And a microwave drive frequency f1Using V1=N1*nf1/KJModel output DC quantum small voltage magnitude V1
Optionally, the quantum voltage step number n of the superconducting junction is 1.
Optionally, the Josephson constant KJ=483597.848416984GHz/V。
According to the specific embodiment provided by the invention, the invention discloses the following technical effects: the invention adopts microwave drive frequency adjustment and combines with a bias current drive control technology, and simultaneously changes the frequency of microwave drive signals applied to the superconducting array junctions and the number of the superconducting array junctions driven by the bias current, thereby obtaining accurate direct current quantum small voltage signals and greatly reducing the deviation between the programmable Josephson voltage standard output direct current small voltage signals (1 mV-10 mV) and a nominal value.
Drawings
In order to more clearly illustrate the embodiments of the present invention or the technical solutions in the prior art, the drawings needed in the embodiments will be briefly described below, and it is obvious that the drawings in the following description are only some embodiments of the present invention, and it is obvious for those skilled in the art to obtain other drawings without creative efforts.
Fig. 1 is a schematic flow diagram of a driving method for dc quantum small voltage provided by the present invention;
FIG. 2 is a schematic diagram of a driving system for DC quantum small voltage provided by the present invention;
fig. 3 is a schematic diagram of a driving controller for dc quantum small voltage provided by the present invention.
Detailed Description
The technical solutions in the embodiments of the present invention will be clearly and completely described below with reference to the drawings in the embodiments of the present invention, and it is obvious that the described embodiments are only a part of the embodiments of the present invention, and not all of the embodiments. All other embodiments, which can be derived by a person skilled in the art from the embodiments given herein without making any creative effort, shall fall within the protection scope of the present invention.
The invention aims to provide a driving method, a system and a controller for direct current quantum small voltage, which can obtain accurate direct current quantum small voltage signals.
In order to make the aforementioned objects, features and advantages of the present invention comprehensible, embodiments accompanied with figures are described in further detail below.
Fig. 1 is a schematic flow chart of a driving method for a dc quantum small voltage provided by the present invention, and the method includes:
step 101: and acquiring a nominal value V of the direct current quantum small voltage, the quantum voltage step number n of the superconducting junction and the microwave frequency f.
Step 102: according to the nominal value V of the direct current quantum small voltage, the quantum voltage step number N of the superconducting junction and the microwave frequency f, N is utilized1=V*KJCalculating the number N of the superconducting array junctions applying the bias current driving signal by the nf model1(ii) a Number N of superconducting array junctions to which bias current drive signals are applied1Taking an integer; wherein KJIs the josephson constant.
Step 103: according to the nominal value V of the direct current quantum small voltage and the number N of the superconducting array junctions for applying the bias current driving signal1Using f1=V*KJ/N1Obtaining the microwave driving frequency f by model calculation1
Step 104: according to the number N of the superconducting array junctions applying the bias current drive signal1And a microwave drive frequency f1Using V1=N1*nf1/KJThe model obtains the actual output DC quantum small voltage value V1
The quantum voltage step number n of the superconducting junction generally takes the first step in practical use, so n takes 1.
KJJosephson constant K, according to resolution # 1 of the 26 th International conference on year 5, 20/2019J=483597.848416984GHz/V。
The method combines microwave drive frequency adjustment and bias current drive control technology, and simultaneously changes the frequency of the microwave drive signals applied to the superconducting array junctions and the number of the superconducting array junctions driven by the bias current, thereby obtaining accurate direct current quantum small voltage signals.
Fig. 2 is a schematic diagram of a driving system for dc quantum small voltage provided by the present invention, the system includes: the device comprises a parameter acquisition module 201, a superconducting array junction number calculation module 202, a microwave driving frequency calculation module 203 and a direct current quantum small voltage output module 204.
The parameter obtaining module 201 is configured to obtain a nominal value V of a dc quantum small voltage, a quantum voltage step number n of the superconducting junction, and a microwave frequency f.
The superconducting array junction number calculating module 202 is configured to utilize N according to the nominal value V of the dc quantum small voltage, the quantum voltage step number N of the superconducting junction, and the microwave frequency f1=V*KJCalculating the number N of the superconducting array junctions applying the bias current driving signal by the nf model1(ii) a The number N of the superconducting array junctions applying the bias current drive signal1Taking an integer; wherein KJIs the josephson constant.
The microwave driving frequency calculation module 203 is configured to calculate the number N of the superconducting array junctions based on the nominal value V of the dc quantum small voltage and the bias current driving signal1Using f1=V*KJ/N1Obtaining the microwave driving frequency f by model calculation1
The direct current quantum small voltage output module 204 is used for applying the number N of the superconducting array junctions of the bias current driving signal according to1And a microwave drive frequency f1Using V1=N1*nf1/KJThe model obtains the actual output DC quantum small voltage value V1
The quantum voltage step number n of the superconducting junction is 1.
Josephson constant KJ=483597.848416984GHz/V。
Fig. 3 is a schematic diagram of a driving controller for dc quantum small voltage provided by the present invention, the controller includes:
and the input device 301 is used for inputting a nominal value V of the direct current quantum small voltage, the quantum voltage step number n of the superconducting junction and the microwave frequency f.
Calculating the number of superconducting array junctions N for applying a bias current drive signal1The first computing device 302; the first computing device 302 utilizes N according to the nominal value V of the DC quantum small voltage, the quantum voltage step number N of the superconducting junction and the microwave frequency f1=V*KJCalculating the number N of the superconducting array junctions applying the bias current driving signal by the nf model1(ii) a The number N of the superconducting array junctions applying the bias current drive signal1Taking an integer; wherein KJIs the josephson constant.
For calculating the microwave drive frequency f1The second computing device 303; the second computing device 303 applies a bias current drive signal to the superconducting array junction according to the nominal value V of the DC quantum small voltage and the number N of the superconducting array junctions1By using f1=V*KJ/N1Obtaining the microwave driving frequency f by model calculation1
An output device 304 for outputting a small dc quantum voltage; the output device 304 applies the bias current driving signal to the superconducting array junction number N1And a microwave drive frequency f1Using V1=N1*nf1/KJModel output DC quantum small voltage magnitude V1
The quantum voltage step number n of the superconducting junction is 1.
Josephson constant KJ=483597.848416984GHz/V。
The invention takes the example of outputting 1mV direct current quantum voltage as an example, and introduces the method for driving the direct current quantum small voltage again in detail:
firstly, according to the required quantum voltage nominal value V is 1mV, the microwave frequency f is 70GHz and N is 1, and the formula N is followed1=V*KJN is obtained from nf17, i.e. to obtain a quantum voltage of nominally 1mV, 7 superconducting array junctions driven by a bias current source are required.
Then according to the formula f1=V*KJ/N1Calculating the required microwave driving frequency f1And is approximately equal to 69.0854 GHz. Adopting 69.0854GHz microwave to perform irradiation drive on the superconducting array junction in liquid helium to enable the superconducting array junction to be in a zero-step state, applying bias current drive signals to 7 superconducting array junctions to enable the superconducting array junction to generate a first quantum voltage step, and then generating a first quantum voltage step according to V1=N1*nf1/KJThe direct current quantum voltage of 0.9999999mV can be obtained.
Actual output voltage magnitude V1Difference from nominal value V:
ΔV=V1-V=-0.0000001mV=-0.1nV。
the invention adopts microwave driving frequency adjustment and a bias current driving control technology to realize the output of precise direct current quantum small voltage, can realize the micro change of the output quantum voltage value by a method of finely adjusting the microwave driving frequency under the drive of fixed bias current, and realizes the resolution test of a high-accuracy digital voltmeter.
The embodiments in the present description are described in a progressive manner, each embodiment focuses on differences from other embodiments, and the same and similar parts among the embodiments are referred to each other. For the system and the controller disclosed by the embodiment, the description is simple because the system and the controller correspond to the method disclosed by the embodiment, and the relevant points can be referred to the method part for description.
The principles and embodiments of the present invention have been described herein using specific examples, which are provided only to help understand the method and the core concept of the present invention; meanwhile, for a person skilled in the art, according to the idea of the present invention, the specific embodiments and the application range may be changed. In view of the foregoing, the description is not to be taken in a limiting sense.

Claims (9)

1. A driving method for a dc quantum small voltage, the method comprising:
acquiring a nominal value V of a direct current quantum small voltage, a quantum voltage step number n of a superconducting junction and a microwave frequency f;
according to the nominal value V of the direct current quantum small voltage, the quantum voltage step number N of the superconducting junction and the microwave frequency f, N is utilized1=V*KJCalculating the number N of the superconducting array junctions applying the bias current driving signal by the nf model1(ii) a The number N of the superconducting array junctions applying the bias current drive signal1Taking an integer; wherein KJIs the josephson constant;
according to the nominal value V of the direct current quantum small voltage and the number N of the superconducting array junctions applying the bias current driving signal1By using f1=V*KJ/N1Obtaining the microwave driving frequency f by model calculation1
According to the number N of the superconducting array junctions applying the bias current driving signal1And a microwave drive frequency f1Using V1=N1*nf1/KJThe model obtains the actual output DC quantum small voltage value V1
2. The driving method for direct current quantum small voltage according to claim 1, wherein the quantum voltage step number n of the superconducting junction takes 1.
3. Driving method for direct current quantum small voltages according to claim 1 or 2, characterized in that the Josephson constant KJ=483597.848416984GHz/V。
4. A drive system for dc quantum small voltages, the system comprising:
the parameter acquisition module is used for acquiring a nominal value V of the direct current quantum small voltage, the quantum voltage step number n of the superconducting junction and the microwave frequency f;
the superconducting array junction number calculation module is used for calculating the number of the microwave junctions according to the nominal value V of the direct current quantum small voltage, the quantum voltage step number n of the superconducting junctions and the microwaveFrequency f, using N1=V*KJCalculating the number N of the superconducting array junctions applying the bias current driving signal by the nf model1(ii) a The number N of the superconducting array junctions applying the bias current drive signal1Taking an integer; wherein KJIs the josephson constant;
a microwave drive frequency calculation module for calculating the number N of the superconducting array junctions based on the nominal value V of the DC quantum small voltage and the bias current drive signal1Using f1=V*KJ/N1Obtaining the microwave driving frequency f by model calculation1
A DC quantum small voltage output module for applying bias current drive signal to the superconducting array junction number N1And a microwave drive frequency f1Using V1=N1*nf1/KJThe model obtains the actual output DC quantum small voltage value V1
5. The driving system for direct current quantum small voltage according to claim 4, wherein the quantum voltage step number n of the superconducting junction takes 1.
6. Driving system for direct current quanta of small voltages according to claim 4 or 5, characterized in that the Josephson constant KJ=483597.848416984GHz/V。
7. A drive controller for dc quantum small voltage, the controller comprising:
the input device is used for inputting a nominal value V of the direct current quantum small voltage, the quantum voltage step number n of the superconducting junction and the microwave frequency f;
calculating the number of superconducting array junctions N for applying a bias current drive signal1The first computing device of (1); the first computing device utilizes N according to the nominal value V of the direct current quantum small voltage, the quantum voltage step number N of the superconducting junction and the microwave frequency f1=V*KJCalculating by a/nf model to obtain a driving signal for applying bias currentNumber of superconducting array junctions N1(ii) a The number N of the superconducting array junctions applying the bias current drive signal1Taking an integer; wherein KJIs the josephson constant;
for calculating the microwave drive frequency f1The second computing device of (1); the second computing device is used for computing the number N of the superconducting array junctions according to the nominal value V of the direct current quantum small voltage and the bias current driving signal1Using f1=V*KJ/N1Obtaining the microwave driving frequency f by model calculation1
The output device is used for outputting the direct current quantum small voltage; the output device is used for applying a bias current drive signal according to the number N of the superconducting array junctions1And a microwave drive frequency f1By using V1=N1*nf1/KJModel output DC quantum small voltage magnitude V1
8. The driving controller for dc quantum small voltage according to claim 7, wherein the quantum voltage step number n of the superconducting junction takes 1.
9. The drive controller for dc quantumsmall voltages according to claim 7 or 8, characterised in that the josephson constant K isJ=483597.848416984GHz/V。
CN202011517649.2A 2020-12-21 2020-12-21 Driving method, system and controller for direct-current quantum small voltage Active CN112763768B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202011517649.2A CN112763768B (en) 2020-12-21 2020-12-21 Driving method, system and controller for direct-current quantum small voltage

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202011517649.2A CN112763768B (en) 2020-12-21 2020-12-21 Driving method, system and controller for direct-current quantum small voltage

Publications (2)

Publication Number Publication Date
CN112763768A CN112763768A (en) 2021-05-07
CN112763768B true CN112763768B (en) 2022-06-24

Family

ID=75695083

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202011517649.2A Active CN112763768B (en) 2020-12-21 2020-12-21 Driving method, system and controller for direct-current quantum small voltage

Country Status (1)

Country Link
CN (1) CN112763768B (en)

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN202443043U (en) * 2012-03-09 2012-09-19 北京无线电计量测试研究所 Programmable bias source for quantum alternating-current voltage standard
CN106575667A (en) * 2014-07-02 2017-04-19 哥本哈根大学 A semiconductor josephson junction and a transmon qubit related thereto
CN111367344A (en) * 2020-04-09 2020-07-03 中国计量大学 Direct current voltage characteristic simulation circuit and method for series connection Josephson junction
CN111628072A (en) * 2020-05-22 2020-09-04 中国计量科学研究院 Josephson junction array bias combination calculation method, electronic device and medium

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP3834635B2 (en) * 2002-11-18 2006-10-18 独立行政法人産業技術総合研究所 Voltage standard equipment

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN202443043U (en) * 2012-03-09 2012-09-19 北京无线电计量测试研究所 Programmable bias source for quantum alternating-current voltage standard
CN106575667A (en) * 2014-07-02 2017-04-19 哥本哈根大学 A semiconductor josephson junction and a transmon qubit related thereto
CN111367344A (en) * 2020-04-09 2020-07-03 中国计量大学 Direct current voltage characteristic simulation circuit and method for series connection Josephson junction
CN111628072A (en) * 2020-05-22 2020-09-04 中国计量科学研究院 Josephson junction array bias combination calculation method, electronic device and medium

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
基于约瑟夫森结效应的电压标准研究;朱珠等;《宇航计测技术》;20120615;第32卷(第3期);全文 *

Also Published As

Publication number Publication date
CN112763768A (en) 2021-05-07

Similar Documents

Publication Publication Date Title
Burroughs et al. Error and transient analysis of stepwise-approximated sine waves generated by programmable Josephson voltage standards
DE102017206177A1 (en) Operating method for an oversampling data converter
US4109168A (en) Current-to-frequency converter
CN108459647A (en) The calibration mistuned circuit and method of electronic load constant current control loop
Jeanneret et al. Josephson-voltage-standard-locked sine wave synthesizer: Margin evaluation and stability
CN112763768B (en) Driving method, system and controller for direct-current quantum small voltage
Ihlenfeld et al. A digital four terminal-pair impedance bridge
US3612975A (en) Electronic data-processing apparatus
CN108732385B (en) Drift correction device and automatic correction method of scanning probe microscopic imaging system
US3786350A (en) Linear input ohmmeter
CN105717393B (en) A kind of parameter test system and test method for electronic component
Ehtesham et al. Development of an automated precision direct current source for generation of pa currents based on capacitance charging method at csir-npl
Tapashetti et al. Design and simulation of op amp integrator and its applications
CN111273203B (en) Feedback control device with magnetic gradient measurement and suspended superconducting ball position
CN114384307A (en) Driving method and system for nano-volt level direct current quantum small voltage
CN203387496U (en) A simulation apparatus for a signal source
CN115347896B (en) High-precision DC signal source
Reymann et al. Limits to the accuracy of 10-V Josephson standards revealed by BIPM on-site comparisons
JPH09181604A (en) Semiconductor integrated circuit device and its noise reduction method
JP2014215048A (en) Power supply device and test device using the same
RU2790350C1 (en) Method for extending the range of current measured by an analogue signal converter
JP3189866B2 (en) Resistance meter calibration device
Yang et al. Design of multi-channel signal acquisition system based on LTC2325
CN113325226B (en) Method for testing voltage drop of low-voltage linear voltage stabilizer
Chabchoub et al. New time-domain conditioning circuit for resistive sensor: Behavioral modelling for simulation and optimization

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant