IP Library Granted Patent US 12,411,025
Granted Patent B2
US 12,411,025 · App. 17/774,741 · Granted Sep 9, 2025

Methods and apparatuses for measuring magnetic flux density and other parameters by means of a plurality of NV centers, and applications thereof

Inventors: Bernd Burchard (Essen, DE); Jan Meijer (Bochum, DE)
Assignees: QUANTUM TECHNOLOGIES GMBH; ELMOS SEMICONDUCTOR SE
G01D5/266G01D5/2451G01D5/30
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Quick Facts
Patent No.
US 12,411,025
App. No.
17/774,741
Granted
Sep 9, 2025
Kind
B2
Abstract

A sensor system includes a quantum dot including one or more paramagnetic centers. It comprises a control and evaluation device including a pump radiation source, a radiation receiver and which irradiates the quantum dot depending on a transmission signal. The quantum dot emits fluorescence radiation upon irradiation with the pump radiation, which depends on the magnetic flux density and/or on another physical parameter. The control and evaluation device generates an output signal including a measured value as a function of the fluorescence radiation. The control and evaluation device compensatingly readjusts the sensitivity of the quantum dot for the magnetic flux density and/or the other physical parameter by means of one or more compensation coils.

Claims (56)

1. A sensor system (NVMS) comprising:

a quantum dot with a plurality of paramagnetic centers (NV 1 ), wherein two or more paramagnetic centers (NV 1 ) of the plurality of paramagnetic centers are couple to each other; and

a drive and evaluation device (AWV);

wherein:

the drive and evaluation device (AWV) comprises:

a first pump radiation source (PL 1 );

a first radiation receiver (PD 1 );

a sub-device including one or more compensation coils;

a first multiplier (M 1 );

a second multiplier (M 2 );

a subtractor (A 1 );

a filter (TP); and

a controller (RG), the controller being a PI controller or functionally equivalent controller;

the drive and evaluation device (AWV) irradiates the quantum dot with pump radiation (LB) at least temporarily using the first pump radiation source (PL 1 );

the pump radiation (LB) of the first pump radiation source (PL 1 ) depends on a transmission signal (S 5 ) of the drive and evaluation device (AWV);

the quantum dot emits fluorescence radiation (FL) upon irradiation with the pump radiation (LB);

the fluorescence radiation (FL) depends on a magnetic flux density (B) at a location of the quantum dot and/or another physical parameter;

the drive and evaluation device (AWV) generates a first output signal (out) with a signal component representing a measured value as a function of the fluorescence radiation (FL);

the measured value depends on the value of the magnetic flux density (B) and/or the other physical parameter;

the drive and evaluation device (AWV) readjusts a sensitivity of the quantum dot for the magnetic flux density (B) and/or the other physical parameter using a sub-device including the one or more compensation coils (LC);

the second multiplier (M 2 ) multiplies the first output signal (out) by a transmitted signal (S 5 ) and thus reconstructs an amplified component of the transmitted signal (S 5 ) in the receiver output signal (S 0 ) as a feedback signal (S 6 );

the subtractor (A 1 ) subtracts the feedback signal (S 6 ) from the receiver output signal (S 0 ), thus forming a reduced receiver output signal (S 1 );

the first multiplier (M 1 ) multiplies the reduced receiver output signal (S 1 ) by the transmitted signal (S 5 ) and generates a filter input signal (S 3 );

the filter (TP) filters the filter input signal (S 3 ) to the first output signal (out);

the controller (RG) derives an operating point control signal (S 9 ) from the first output signal (out);

the control is performed by the controller (RG) with a first time constant τ 1 ;

the compensation control is performed using the filter (TP) with a second time constant τ 2 ;

the first time constant τ 1 of the controller (RG) is greater than the second time constant τ 2 of the filter (TP);

in event of a change in the value of the magnetic flux density (B) or a change in the value of another of the physical parameters at the location of the plurality (NVC) of paramagnetic centers (NV 1 ), the controller (RG) shifts the magnetic flux density (B) at the location of the plurality (NVC) of paramagnetic centers (NV 1 ) in a direction of an operating point by subtracting or adding a coil current of the compensation coil (LC) supplied by the controller (RG), and

the control and evaluation device (AWV) thus carries out the readjustment via the feedback signal (S 6 ) in a compensating manner, such that the reduced receiver output signal (S 1 ) no longer has any component of the transmitted signal (S 5 ) in the reduced receiver output signal (S 1 ) except for signal noise and control errors.

2. A sensor system (NVMS) comprising:

a quantum dot with a plurality of paramagnetic centers (NV 1 ), wherein two or more paramagnetic centers (NV 1 ) of the plurality (NVC) of paramagnetic centers (NV 1 ) couple to each other, wherein the plurality of paramagnetic centers (NV 1 ) is included in multiple nanodiamonds, the multiple nanodiamonds having different respective crystal orientations; and

a drive and evaluation device (AWV);

wherein:

the drive and evaluation device comprises:

a first pump radiation source (PL 1 );

a first radiation receiver (PD 1 );

a correlator (CORR), wherein the correlator includes;

a sub-device including one or more compensation coils;

a controller (RG), the controller being a PI controller or functionally equivalent controller;

the drive and evaluation device (AWV) irradiates the quantum dot with pump radiation (LB) at least temporarily by means of the first pump radiation source (PL 1 );

the pump radiation (LB) of the first pump radiation source (PL 1 ) depends on a transmission signal (S 5 ) of the drive and evaluation device (AWV);

the quantum dot emits fluorescence radiation (FL) upon irradiation with the pump radiation (LB);

the fluorescence radiation (FL) depends on a magnetic flux density (B) at a location of the quantum dot and/or another physical parameter;

the drive and evaluation device (AWV) generates, as a function of the fluorescence radiation (FL), by means of a correlator (CORR) which determines a component of a transmitted signal (S 5 ) in a receiver output signal (S 0 ) of the first radiation receiver (PD 1 ), the component of the transmitted signal (S 5 ) in the receiver output signal (S 0 ) being a first output signal (out) which represents a measured value, wherein the correlator includes a synchronous demodulator, an optimal filter, or a matched filter;

the measured value depends on the value of the magnetic flux density (B) and/or the other physical parameter;

the drive and evaluation device (AWV) readjusts a sensitivity of the quantum dot for the magnetic flux density (B) and/or the other physical parameter by means of a sub-device in a form of one or more compensation coils (LC);

a current flow of the compensation coil (LC) depends on the fluorescence radiation (FL) of the quantum dot (NV 1 );

the drive and evaluation device (AWV) controls the sensitivity of the quantum dot;

the drive and evaluation device (AWV) compensatingly readjusting the sensitivity of the quantum dot by means of a dividing device as a function of a control signal of the control and evaluation device (AWV) by means of a controller (RG);

the compensation coils (LC), as a result of a change in an intensity of the fluorescence radiation (FL) in event of a change in the value of the magnetic flux density (B) or in the event of a change in the value of another physical parameter at the location of the plurality (NVC) of paramagnetic centers (NV 1 ), shift the magnetic flux density (B) at the location of the plurality (NVC) of paramagnetic centers (NV 1 ) in a direction of an operating point by means of a subtraction and/or addition of a coil current; and

the drive and evaluation device (AWV) carries out this readjustment in a compensating manner, such that the receiver output signal (S 0 ) of the first radiation receiver (PD 1 ) no longer has any component of the transmitted signal (S 5 ) in the receiver output signal (S 0 ) except for signal noise and control errors, which means that the receiver output signal (S 0 ) of the first radiation receiver (PD 1 ) has a component of the transmission signal (S 5 ) in the receiver output signal (S 0 ) with an amplitude that is smaller than a predetermined amplitude bandwidth amount.

3. The sensor system according to claim 2 , wherein the different respective crystal orientations are random.

4. The sensor system according to claim 2 , wherein the correlator includes the synchronous demodulator.

5. The sensor system according to claim 2 , wherein the correlator includes the optimal filter.

6. The sensor system according to claim 2 , wherein the correlator includes the matched filter.

Assignments (5)
CHANGE OF ADDRESS Recorded Jan 4, 2026
From: ELMOS SEMICONDUCTOR SE
To: ELMOS SEMICONDUCTOR SE
Reel/Frame 074853/0001 →
CHANGE OF NAME Recorded Sep 26, 2022
From: QUANTUM TECHNOLOGIES UG (HAFTUNGSBESCHRÄNKT)
To: QUANTUM TECHNOLOGIES GMBH
Reel/Frame 061536/0095 →
CORRECTIVE ASSIGNMENT TO CORRECT THE CORRESPONDENT ADDRESS PREVIOUSLY RECORDED AT REEL: 060091 FRAME: 0678. ASSIGNOR(S) HEREBY CONFIRMS THE ASSIGNMENT . Recorded Jun 17, 2022
From: BURCHARD, BERND; MEIJER, JAN
To: QUANTUM TECHNOLOGIES UG (HAFTUNGSBESCHRÄNKT)
Reel/Frame 060452/0420 →
CORRECTIVE ASSIGNMENT TO CORRECT THE ADD THE SECOND ASSIGNEE PREVIOUSLY RECORDED AT REEL: 060091 FRAME: 0678. ASSIGNOR(S) HEREBY CONFIRMS THE ASSIGNMENT. Recorded Jun 13, 2022
From: BURCHARD, BERND; MEIJER, JAN
To: QUANTUM TECHNOLOGIES UG (HAFTUNGSBESCHRÄNKT); ELMOS SEMICONDUCTOR SE
Reel/Frame 060364/0256 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Jun 2, 2022
From: BURCHARD, BERND; MEIJER, JAN
To: QUANTUM TECHNOLOGIES UG (HAFTUNGSBESCHRÄNKT)
Reel/Frame 060091/0678 →
Priority Claims (1)
DE 10 2019 130 114.9 · Nov 7, 2019 · national
Continuity (1)
Related Publication 20220397429A1 · Dec 15, 2022
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