SQUID detector with flux feedback coil sized and located to produce uniform feedback flux

Claim 2

A high critical temperature (high-T C ), superconducting quantum interference device (SQUID) magnetometer for measuring a subject magnetic field in which the SQUID magnetometer is positioned, the magnetometer including: a SQUID chip having a non-super conducting region threaded by a first magnetic flux produced by the subject magnetic field and energized by an excitation circuit, a separate feedback coil positioned adjacent to the SQUID chip, and a flux-locked loop for producing a feedback signal to energize the feedback coil, the flux-locked loop driving the feedback coil to produce a feedback magnetic flux which adds to, or subtracts from, the first magnetic flux to produce a resultant total magnetic flux threading the SQUID chip, and the feedback coil having a size relative to the SQUID chip to cause the resultant total magnetic flux to be substantially uniform over the SQUID chip, the feedback signal thereby being indicative of the magnitude of the first magnetic flux and the subject magnetic field which produces it.

Claim 3

The magnetometer of claim 1 wherein the feedback coil includes a cylindrical coil mounted co-axially with and in close proximity to the SQUID chip.

Claim 4

The magnetometer of claim 2 wherein the diameter of the cylindrical coil is greater than the maximum dimension of the SQUID chip.

Claim 5

The magnetometer of claim 1 wherein: the SQUID has a single weak link and is configured as a radio frequency SQUID, and the excitation circuit comprises a tuned circuit including a radio frequency coil.

Claim 6

The magnetometer of claim 4 wherein the SQUID chip is formed as a thin film of ceramic superconducting material on a suitable substrate.

Claim 7

The magnetometer of claim 5 wherein the superconducting material is YBa 2 Cu 3 O 7 .

Claim 8

The magnetometer of claim 5 wherein the weak link includes a step in the substrate to cause a misalignment of crystals of the superconducting material in the region of the step.

Claim 9

The magnetometer of claim 5 wherein the weak link is a junction selected from a group comprising: a step edge junction, a grain boundary junction, a bicrystal junction, a step-SNS junction, a multi-layer junction and a ramp junction.

Claim 10

The magnetometer of claim 4 wherein the rf coil is mounted in close proximity to the chip.

Claim 11

The magnetometer of claim 9 wherein the rf coil is a spiral coil mounted co-axially with and parallel to the SQUID chip.

Claim 12

The magnetometer of claim 9 wherein the rf circuit is driven by a radio frequency constant current source.

Claim 13

The magnetometer of claim 11 wherein the radio frequency current source has a frequency of at least 1 MHz.

Claim 14

The magnetometer of claim 12 wherein the radio frequency current source has a frequency in the range of from 150 MHz to 200 MHz.

Claim 15

The magnetometer of claim 4 including a single interconnecting cable and a crossover network for connecting the rf coil and the feedback coil to the flux-locked loop.

Claim 16

The magnetometer of claim 14 wherein the cross-over network comprises an LC network, the rf coil and feedback coil being connected in parallel with one another, an inductor of the LC network being connected in series with the feedback coil and a capacitor of the LC network being connected in series with the rf coil.

Claim 17

The magnetometer of claim 1 wherein: the SQUID has two weak links and is configured as a dc SQUID, and the excitation circuit comprises a dc constant current source.

Claim 18

The magnetometer of claim 16 wherein the SQUID chip is formed as a thin film of ceramic superconducting material on a suitable substrate.

Claim 19

The magnetometer of claim 17 wherein the superconducting material is YBa 2 Cu 3 O 7 .

Claim 20

The magnetometer of claim 17 wherein the weak links include two steps in the substrate to cause a misalignment of crystals of the superconducting material in the region of the steps.

Claim 21

The magnetometer of claim 17 wherein the weak links include a single step extending across the substrate and the superconducting material is located on the substrate such that two regions of the superconducting material, corresponding to the locations of two weak links, pass over the step to cause a misalignment of crystals of the superconducting material in each of those regions.

Claim 22

The magnetometer of claim 17 wherein each of the weak links is a junction selected from a group comprising: a step edge junction, a grain boundary junction, a bicrystal junction, a step-SNS junction, a multi-layer junction and a ramp junction.

Claim 23

The magnetometer as claimed in claim 1 wherein a probe containing the SQUID chip and coils magnetically coupled to the chip are shielded by a thin-walled, non-magnetic stainless steel shield.

Claim 24

The magnetometer of claim 22 wherein the shield includes a housing containing the SQUID chip and the coupled coils, the housing having a wall thickness of 0.1 mm to 0.5 mm.

Claim 25

The magnetometer of claim 22 wherein the wall thickness is 0.3 mm.

Claim 26

The magnetometer as in claim 22 wherein cables connected to said coupled coils are shielded in respectively associated thin-walled, non-magnetic stainless steel tubes.

Claim 27

The magnetometer of claim 25 wherein the wall thickness of the tube is in the range of 0.1 mm to 0.5 mm.

Claim 28

The magnetometer of claim 25 wherein the wall thickness of the tube is 0.3 mm.

Claim 29

A high critical temperature (high-T C ) radio frequency superconducting quantum interference device rf (SQUID) magnetometer for measuring a subject magnetic field in which the SQUID magnetometer is positioned, the magnetometer including: a SQUID chip having a single weak link and a non-superconducting region threaded by a first magnetic flux produced by the subject magnetic field and energized by a radio frequency excitation circuit having a radio frequency tuned circuit including a radio frequency coil, a separate feedback coil positioned adjacent to the SQUID chip, a flux-locked loop for producing a feedback signal to energize the feedback coil, and a single interconnecting cable and a cross over network for connecting the rf coil and the feedback coil to the flux-locked loop, the flux-locked loop driving the feedback coil to produce a feedback magnetic flux which adds to, or subtracts from, the first magnetic flux to produce a resultant total magnetic flux threading the SQUID chip, the feedback coil having a size relative to the SQUID chip to cause the resultant total magnetic flux to be substantially uniform over the SQUID chip, the feedback signal thereby being indicative of the magnitude of the first magnetic flux and the subject magnetic field which produces it.

Claim 30

A high critical temperature (high-T C ) radio frequency superconducting quantum interference device rf (SQUID) magnetometer for measuring a subject magnetic field in which the SQUID magnetometer is positioned, the magnetometer including: a SQUID chip having a single weak link and a non-superconducting region threaded by a first magnetic flux produced by the subject magnetic field and energized by a radio frequency excitation circuit having a radio frequency tuned circuit including a radio frequency coil, a separate feedback coil positioned adjacent to the SQUID chip, a flux-locked loop for producing a feedback signal to energize the feedback coil, and a single interconnecting cable and a cross over network for connecting the rf coil and the feedback coil to the flux-locked loop, the flux-locked loop driving the feedback coil to produce a feedback magnetic flux which adds to, or subtracts from, the first magnetic flux to produce a resultant total magnetic flux threading the SQUID chip, the feedback coil having a size relative to the SQUID chip to cause the resultant total magnetic flux to be substantially uniform over the SQUID chip, the feedback signal thereby being indicative of the magnitude of the first magnetic flux and the subject magnetic field which produces it.

Claim 31

The magnetometer of claim 28 wherein the feedback coil includes a cylindrical coil mounted co-axially with and in close proximity to the SQUID chip.

Claim 32

The magnetometer of claim 29 wherein the diameter of the cylindrical coil is greater than the maximum dimension of the SQUID chip.

Claim 33

The magnetometer of claim 28 wherein the SQUID chip is formed a as thin film of ceramic superconducting material on a suitable substrate.

Claim 34

The magnetometer of claim 31 wherein the superconducting material is YBa 2 Cu 3 O 7 .

Claim 35

The magnetometer of claim 31 wherein the weak link includes a step in the substrate to cause a misalignment of crystals of the superconducting material in the region of the step.

Claim 36

The magnetometer of claim 31 wherein the weak link is a junction selected from a group comprising: a grain boundary junction, a bicrystal junction, a step-SNS junction, a multi-layer junction and a ramp junction.

Claim 37

The magnetometer of claim 28 wherein the rf coil is mounted in close proximity to the chip.

Claim 38

The magnetometer of claim 35 wherein the rf coil is a spiral coil mounted co-axially with and parallel to the SQUID chip.

Claim 39

The magnetometer of claim 35 wherein the rf circuit is driven by a radio frequency constant current source.

Claim 40

The magnetometer of claim 37 wherein the radio frequency current source has a frequency of at least 1 Mhz.

Claim 41

The magnetometer of claim 37 wherein the radio frequency current source has a frequency in the range of from 150 MHZ to 200 MHZ.

Claim 42

The magnetometer of claim 28 wherein the cross-over network comprises an LC network, the rf coil and feedback coil being connected in parallel with one another, an inductor of the LC network being connected in series with the feedback coil and a capacitor of the LC network being connected in series with the rf coil.

Claim 43

A high-T C SQUID magnetometer for TEM comprising: a SQUID chip having an RF excitation field coil disposed thereon; and a feedback electromagnetic coil dimensioned and disposed to provide a substantially uniform magnetic flux over the entire SQUID chip when electrical current is passed through the feedback coil.

Claim 44

A high-T C SQUID magnetometer for TEM comprising: a SQUID chip having an RF excitation field coil disposed thereon; and a feedback electromagnetic coil dimensioned and disposed to provide a substantially uniform magnetic flux over the entire SQUID chip when electrical current is passed through the feedback coil.

Claim 45

A magnetometer as in claim 41 wherein said feedback coil includes a solenoidal coil mounted co-axially and in close proximity with said SQUID chip.

Claim 46

A magnetometer as in claim 42 wherein the feedback coil has a diameter that is greater than the maximum dimension of said SQUID chip.