Patent Application
20230113008
Exemplary embodiments of the invention relate to a diamond scanning element, herein also mentioned as diamond scanning probe, especially for imaging application, and a method for its fabrication
Modern material systems, for example those of interest in spintronics, have created a need for imaging techniques with high sensitivity and high spatial resolution. Within this field, the nitrogen-vacancy (NV) center in diamond, particularly when integrated into a scanning probe-based quantum sensor, has attracted much attention due to its high magnetic field sensitivity and spatial resolution on the tens of nanometer scale. These two properties have allowed for the measurement of nanoscale systems such as skyrmions, antiferromagnetic domains, single neuron action potentials and magnetism in 2D materials. This wide range of applications highlights the versatility of the NV center, which can be implemented in a variety of systems and operating temperatures from ambient conditions to cryogenics. The essential requirements of such an NV-based nanoscale sensor are as follows. Firstly, an NV center in close proximity to the diamond surface, to minimize NV-sample separation and thus optimize spatial resolution while enhancing the detected magnetic signal from nanoscale sample volumes. Secondly, a high flux of detected photons for best sensitivity. The high refractive index of the diamond host (n=2.4) presents a challenge for the second requirement, but also offers a natural route to engineer photonic structures to maximize collection efficiency. Many approaches have been taken to optimizing collection efficiency via photonic engineering of diamond, including solid immersion lenses, periodic nanostructuring, dielectric antennas, parabolic reflectors, and waveguiding structures. However, for imaging applications, these approaches have typically suffered from large implantation depths of the NV center, or in the case of traditional scanning probes, non-optimized structures leading to low collection efficiencies. The inventive diamond probe can be used in all the aforementioned applications.
The state-of-the art technology in this field has focused thus far on diamond scanning probes with tapered side walls created by a similar electron beam lithography mask and etching with oxygen (see A. Jenkins, M. Pelliccione, G. Yu, X. Ma, X. Li, K. L. Wang, and A. C. Bleszynski Jayich, Single-spin sensing of domain-wall structure and dynamics in a thin- film skyrmion host, Phys. Rev. Mat. 3, 8 (2019)) and O2/Ar chemistry (see Y. Dovzhenko, F. Casola, S. Schlotter, T. X. Zhou, F. Buttner, R. L. Walsworth, G. S. D. Beach, and A. Yacoby, Magnetostatic twists in room-temperature skyrmions explored by nitrogen-vacancy center spin texture reconstruction, Nature Comm. 9, 1 (2018)). Occasionally, CF4 is introduced to remove residue, but not to produce a curved surface.
Furthermore, alternate masks, such as Aluminum (see: I. Gross, W. Akhtar, A. Hrabec, J. Sampaio, L. J. Martinez, S. Chouaieb, B. J. Shields, P. Maletinsky, A. Thiaville, S. Rohart, and V. Jacques, Skyrmion morphology in ultrathin magnetic films, Phys. Rev. Mat. 2, 2 (2018)) have been used in combination with O2/CF4 dry etching to create diamond nanopillar arrays with straight or tapered walls.
Further prior art relating to the aforementioned application:
Q. Jiang, Large scale fabrication of nitrogen vacancy-embedded diamond nanostructures for single-photon source applications, Chinese Physics B, 25, 11 (2016).
Q. Jiang, Focused-ion-beam overlay-patterning of three-dimensional diamond structures for advanced single photon properties, Journal of Applied Physics, 116, 044308 (2014).
Momenzadeh, S.A, Nanoengineered diamond waveguide as a robust bright platform for nanomagnetometry using shallow nitrogen vacancy centers, Nano Letters, 15, 1 (2015).
S. Ali Momenzadeh et Al: “Nanoengineered Diamond Waveguide as a Robust Bright Platform for Nanomagnetometry Using Shallow Nitrogen Vacancy Centers”, Nano Letters, vol. 15, no. 1, 8. December 2014 (2014–12–08), pages 165-169, XP055716238, US ISSN: 1530-6984, DOI:10.1021/nl503326t
S. Ali Momenzadeh et Al.:”Nano-engineered Diamond Waveguide as a Robust Bright Platform for Nanomagnetometry Using Shallow Nitrogen Vacancy Centers”, 29 August 2014 (2014–08–29), XP055716551, DOI: 10.1021/nl 503326t
Retrieved from the Internet: URL:https://pubs.acs.org/doi/suppl/10.1021/n1503326t/suppl file/nl503326t si 001.pdf
The two aforementioned documents disclose a provision of a diamond material; the deposition of a resist; the formation of an etch mask and an etching process. The mask is made of FOX-material. The etching process uses O2 -plasma for etching the diamond surface and between the oxygen etching step - a O2/CF4-mixture is applied to the surface. The plasma parameters in this process were adjusted by an adjustment of the plasma power and RF bias power.
This step of a short O2/CF4-treatment was presumably done to remove small resputtered particles of FOX from the diamond surface as a cleaning procedure.
Wan, N.H. Efficient extraction of light from a nitrogen-vacancy center in a diamond parabolic reflector. Nano Letters, 18, 5 (2018).
The US 2018/0246143 A1 and WO 2018/169997 A1 should also be cited as state of the art.
Also, in WO 2018/169997 A1, just as disclosed by Momenzadeh et al., the plasma parameters were adjusted by an adjustment of the plasma power and the RF bias power.
Varying the plasma power will affect both the diamond and the mask etch rates, a controlled formation of a surface structure with a tapered geometry with increasing taper angle towards a flat end facet however is not disclosed by the aforementioned documents.
Momenzadeh et al. as well as WO 2018/169997 A1 disclose different taper angles in different devices, but do not show an increasing series of taper angles in a single device. Further to this the range of taper angles considered in the simulations in Momenzadeh et al. only extends up to 33 degrees, and the optimal angle is found to be 20 degrees. Momenzadeh et al. also disclose a diameter of 400 nm.
The production method disclosed by Momenzadeh et al as well as WO 2018/169997 A1 does not allow further modification of the lateral section of the pillar because the variation of the power of the plasma treatment during the etching process will attack the diamond structure as well as the mask structure. An independent control of an etching of either the one or the other material is not possible
Qianqing et al. disclose two taper angles, but they are not independently controlled.
A further relevant document in the state of the art is US 2012/292590 A1. This document discloses that the taper angles are achieved by etching along certain crystal directions of the diamond, up to a taper angle of 35 degrees. There is also one mention of a taper angle up to 40 degrees in that document, but not higher. The method in D4 allows for only certain discrete angles. Further to this the diameter given in this document is between 200 nm and 1um. Further to this, this document discloses in claim 1 a specific dipole orientation.
Exemplary embodiments of the invention are directed to a scanning element with high collection efficiency and to minimize the depth of the defect.
Exemplary embodiments of the invention are also directed to a method for manufacturing a scanning element, where the control of the design is achieved during the etching process.
The inventive diamond scanning element can be suitable for the use in an imaging application. It comprises a support and a pillar extending from the support. The support can be a diamond slab. The pillar is tapered and the tapered diamond pillar is preferably monolithically attached at its base to the diamond slab.
The pillar is provided with a longitudinal axis and the pillar further comprises a tip with a tapered lateral section with a, preferably constantly, increasing curvature. The curvature might preferably have the form of a paraboloidal section. The range of taper angles comprised the curvature can preferably be in the range of 12-50 degree.
The tip is further provided with a flat end facet, also referred to as a tapered end facet, extending at least toward the axis (X), with a gradient of less than 10%. The flat end facet might be plane, in which case the gradient is 0%. The gradient should be preferably less than 8%, more preferably less than 5% and even more preferably less than 2%.
A gradient of 100% would define an angle of 90°, which would be a surface parallel to the longitudinal axis of the pillar. At a gradient of less than 10% the flat facet can be tilted away from the plane perpendicular to the axis by an angle of preferably less than 9 degrees.
The flat facet at the end is essential in order to minimize the distance between the tip and preferably of the defect at the tip, which is considered as a sensor element in the context of the current invention, and the sample to be measured.
The diamond scanning element can be considered as a sensor in the context of the current invention.
The curvature, also referred to by an increasing taper angle towards the tip, is essential in order to achieve a high collection efficiency across a broad spectral band, without making the tip radius too large because larger tip radius impairs performance as a scanning probe.
The tapered end facet can have a preferred diameter of at least 30 nm, preferably at least 50 nm, more preferably between 100-300 nm.
The tapered end facet can have a diameter which is at least 1% of the length of the pillar. The length of the pillar can be less than 10.0 µm, preferably between 3.0 and 6.0 µm.
The tip, preferably the flat end facet, comprises the sensor element which is a defect according to the invention, more preferably a nitrogen-vacancy. The defect can be positioned at center of the tip, especially at the center of the flat end facet.
In a preferred embodiment of the invention the defect provides one or more dipoles, especially an s-polarized and a p-polarized dipole, that are oriented perpendicular and parallel to the pillar axis respectively.
One preferred advantage of the current invention contributes to a reduced suppression of the emission. Therefore, the dipole source is preferably oriented perpendicular to the longitudinal axis of the pillar such that the dipole can be located very close to the flat end facet of the pillar (much less than a wavelength separation) without significant suppression of emission.
This is of special advantage for sensing nano-scale objects external to the diamond. The suppression of dipole emission in the case of a dipole oriented parallel to the axis increases dramatically as the dipole approaches the surface of the diamond. So, in the current device, the parallel component of the dipole does not contribute to the collected photons, and the dipole should therefore be substantially orthogonal to the axis.
A second benefit of the orthogonal dipole orientation is that the emission from the device will have an approximately Gaussian intensity profile, which matches well to the modes of an optical fiber, which is commonly used to collect the light and channel it to a detector. The parallel dipole orientation results in an emission pattern that is donut-shaped and is radially polarized, which has very poor overlap with the optical fiber modes. So, it is very problematic to use a dipole oriented parallel or inclined to the axis as it is claimed by US 2012/292590 A1.
The depth of the defect from the surface of the flat end facet can be less than 40 nm, preferably less than 25 nm.
In a preferred embodiment the pillar comprises a waveguide or can be designed as a waveguide. The diamond scanning element may further preferably comprise an aperture at the base of the pillar.
In a preferred embodiment of the invention the reflection occurs at normal incidence, or nearly normal incidence, to the backside, which minimizes the reflection. Alternatively, or additionally, the backside of the slab could be coated with a film of material having an index of refraction less than 2.4, preferably close to 1.5, which could serve as an antireflection coating to minimize the reflection.
The divergence of the light could preferably be below the angle of total reflection for a diamond-air interface. Said angle of total reflection could preferably be about 24.5 degrees.
In the case of an NV-center as a defect the minimum aperture at the base of the pillar might be at least 0.8 µm.
At the tip of the diamond pillar, the rate of tapering can be steadily increased. The angle of tapering at the tip should be close to 45 degrees or more, in order to obtain a device that efficiently collects light from a broad band of wavelengths.
The taper does not continue to a radius of zero, but rather the tip radius is finite and may preferably be greater than approximately 50 nm. Most preferably in this context the diameter of the tip might greater than approximately 50 nm.
As mentioned before, the defect, especially provided as a NV center, is placed in the tip of the pillar, at the focal point of the paraboloid and just inside the plane of the flat facet of the tip. The defect can also be misplaced offset from the focal point in any direction. In this case the device will still work but not as efficiently.
The defect is preferably sensitive to external fields produced by a sample that is brought in close proximity to the flat facet.
The invention further comprises a method for the fabrication of a diamond scanning element comprising a support and a pillar extending from said support, wherein the method comprises the following steps:
Consequently, the relative etch rate of the mask vs. the diamond is variably controlled by adjusting the etch chemistry. This distinguishes it from other methods for curved or angled surfaces and allows for much more control over the shape of the wall, beyond even the parabolic shape.
It is pointed out that the method can preferably be used for the fabrication of the inventive diamond scanning element. However, other designs can also be realized with the current method of fabrication. Therefore, the method is not limited for the production of the inventive diamond scanning element only.
With the inventive method a range of angles up to 50 degrees can be achieved which is far more than known methods comprising the said method steps in the state of the art.
The first chemical compound is O2 and the second chemical compound can preferably be CF4.
According to the invention the amount of etching of mask material and/or diamond material during the formation of the diamond scanning element can be controlled by the ratio between the first and the second chemical compound that are added and/or adjusted during the etching process. The ratio can be controlled and adapted by a control unit for controlling the dosage of each compound.
Varying the plasma power according to the disclosure of the state of the art is fundamentally different from varying the CF4-concentration, because a variation of the plasma power will affect both the diamond and the mask etch rates, while the latter affects primarily just the mask etch rate (there is a slight influence on the diamond etch rate), allowing for the diamond and mask etch rates to be controlled independently.
A preferred embodiment step A comprises the generation of a defect, preferably a nitrogen-vacancy, most preferably at the tip of the pillar, most preferably at center at the tip of the pillar.
The resist can preferably be an inorganic polymer layer, preferably formed by a flowable oxide material, most preferably Fox-16 by Dow Corning.
The formation of the etch mask in step C may be provided by an electron beam lithography.
In step D the diamond can preferably be exposed to an Inductively Coupled Plasma, which causes the diamond to be etched in a Reactive Ion Etch process, wherein the reactive ions are formed from said first and second chemical compound.
The etching process can be controlled such that the inclination of the sidewalls of the mask is adapted to a 45 degree angle with a deviation of less than 5 degrees, preferably less than 2 degrees.
By control of the ratio between the first and the second chemical compound the range of angles, which are preferably etched in the diamond material for the formation of the tip, can be varied between 10 and 50 degrees, preferably between 12 and 50 degrees.
During the first part of the etch process, an etch chemistry, preferably O2, is used that primarily attacks the diamond, forming a tapered conical pillar of diamond. The taper angle of this section is less than 12 degrees. Simultaneously the mask is eroded at the edge to form a trapezoidal cross section. The sidewalls of the mask are inclined at an approximately 45 degree angle (the angle need not be precisely 45 degrees, but should be substantially inclined from the vertical direction).
During the second part of the etch, the etch chemistry is modified by adding an agent that etches the mask material, preferably CF4. By changing the concentration of CF4 relative to O2, the angle of the resulting diamond sidewall is changed.
Multiple CF4:O2 ratios are used according to the invention sequentially to obtain a curved surface profile. The range of angles we have achieved with this process is between 12 and 50 degrees.
The plasma power and preferably also the RF bias power can be kept constant over the time period when multiple CF4:O2 ratios are applied in order to form the curved surface profile. This way a better control of the etching process with high precision is possible by controlling the CF4:O2 ratios over the time without interference of secondary effects such as a power-variation.
The better control is especially achieved because the diamond etch rate can be controlled independently to the mask etching process. Changing the plasma power, the etching process would affect both the mask etching and the diamond etching.
The etching-treatment of CF4:O2 with different ratios may be longer than at least 5 minutes, more preferably at least 10 minutes, wherein the ration between sccm CF4 and sccm O2 may vary between 1:30 and 1:3.
The time period of application might be more than 2 minutes for sccm-ratios of CF4 compared to O2 lower than 1:10.
The time period of application might be less than 1 minute for sccm-ratios of CF4 compared to O2 higher than 1.4:10.
The design of the diamond scanning element of the current invention may require a control over multiple, preferably at least two, different taper angles in a single device.
As mentioned, the diamond and mask etch rates to be controlled independently due to the application of different CF4:O2 ratios.
The current diamond scanning element may comprise an increasing series of taper angles in a single device respectively a single element.
The current inventive method allows a continuous tuning of the angle within the range 10-50 degrees.
The diameter of the end facet specified in the current application is ideally between 100-300 nm. Achieving a small diameter is of advantage for the contact with the sample for ideal scanning conditions.
Some advantageous embodiments for inventive diamond scanning element and an inventive embodiment of a method for fabrication are further explained in detail below together with drawings. Specific parts of the different embodiments can be understood as separate features that can also be realized in other embodiments of the invention. The combination of features described by the embodiment shall not be understood as a limitation for the invention.
The parabolic tip shape yields a median saturation count rate of 2.1 MHz, the highest recorded count rate for scanning probes to date. At the same time, the structures remain highly broadband and produce directed emission.
Furthermore, the truncation shifts the diamond surface towards the focus of the parabola, allowing for small NV-sample spacings, which leads to ideal scanning conditions.
The truncation can preferably be a distal flattening of the parabolic form of the tip. The flattening of the probe at the tip may preferably be a planar surface. This geometry adapts to the concept of a diamond parabolic reflector in combination with a pillar slab geometry that was incorporated into an atomic force microscope probe for scanning magnetic field imaging.
Rather than using the typically cylindrical or tapered pillar structure, the current geometry of the tip of the probe consists of a diamond paraboloid with an NV at the focus. The truncated parabolic design comprises with a flat, preferably planar, end face, also referred to as a flat end facet, which minimizes the depth of the NV, and hence the distance to the sample.
The parabolic sides of the tip may define an imaginary parabolic plane, wherein the flat end facet preferably defines a planar surface perpendicular to the normal of the parabolic plane.
The geometry of the tip may provide total internal reflection at the parabolic surface which collimates the emission into a unidirectional output mode, resulting in improved waveguiding of the NV emission.
A further simulating of a cylindrical design was performed with a finite-difference time-domain solver (Lumerical), taking a cylindrical pillar waveguide as a basis of comparison.
Both cylindrical and parabolic devices have a facet diameter of 200 nm, approximately the minimal diameter that still supports an optical mode with strong confinement to the diamond. It was considered that dipoles are oriented both perpendicular (s-polarized) to the pillar axis, and assess the device performance on the basis of two key metrics: outcoupled power Ina within the 0.8 numerical aperture cone of our objective (Ina) and directionality of emission. Note that Ina is related to the collection efficiency η of the parabolic reflector, but also includes the near-field effect of the parabolic surface and the Purcell effect due to reflection off the back side of the holding slab, which modify the radiative decay rate of the dipole. All powers are normalized to the power radiated by a dipole in uniform bulk diamond, Ibd.
As a result, an s-polarized dipole in the cylindrical device leads to a value of Ina/Ibd = 0.18 (averaged across the 630 nm to 800 nm NV emission band), while the same dipole in the parabolic device gives Ina/Ibd = 0.68. The nearly factor of four increase in waveguided emission shows the strength of the parabolic design, even when taking into account the interference due to the holding slab and exit aperture. To isolate the contribution of the parabola from this interference, a second simulation has been performed in which the waveguide section is terminated in the perfectly absorbing wall of the simulation space. The waveguided power Iwg was measured and it could be demonstrated that the parabolic design shows a consistently higher collected power over the NV emission band. If the actual fabricated device shown in
A further full structure simulation has been performed to determine the far-field emission pattern for each device. By plotting the emission intensity as a function of polar angle, it has been observed that the larger aperture of the parabolic device concentrates the far field emission within a small numerical aperture (NA) of 0.25. The cylindrical pillar, on the other hand, due to its wavelength-scale aperture undergoes significant diffraction, resulting in a much larger NA = 0.65.
It has been noted that in the case of a p-polarized dipole outcoupled power is in all cases suppressed by a factor ≥ 7, due to the near-field diamond-air interface, and poor overlap with the waveguide mode. It is clear from these findings that an s-polarized dipole is optimal, which would be the case if the NV axis were aligned to the pillar axis.
For the development of the parabolic diamond tips, we begin with a high-purity type-IIa diamond (Element Six, [N]< 5 ppb, (100) surface), implanted with 2 × 1011 cm-214N at 12 keV and 7° tilt to the sample normal. The diamond is then annealed. More information for the annealing process can be found in the following document: Y. Chu, et al., Coherent optical transitions in implanted nitrogen vacancy centers, Nano Lett., 14, 4 (2014)
The annealing treatment will result in an estimated NV depth of 20 nm. ~1-µm diameter discs where used, patterned via electron beam lithography in a ~300-nm thick, flowable oxide resist (FOX-16, Dow-Corning) as an etch mask.
The following fabrication process then comprises of two dry-etching stages. The first, which is used to fabricate the waveguide portion, consists of an inductively coupled plasma reactive ion etch (ICP-RIE, Sentech) with primarily O2 etch chemistry, and short steps of O2 and CF4 to clean off resputtered material from the walls of the device.
The two etch steps may be repeated a total of nine times to achieve a ~6 µm pillar. At the end of this stage, the mask has a trapezoidal cross section with a base diameter of 900 µm.
For the second stage, CF4 was induced for the full duration of the etch at increasing flow rates for successive steps, which erodes the FOX mask in proportion to CF4 concentration. This, along with the trapezoidal cross section, allows to tune the angle of the walls by controlling the relative etch rate of FOX mask and diamond. A typical final device is shown in
The established procedures can be derived from the following document: P. Appel, E. Neu, M. Ganzhorn, A. Barfuss, M. Batzer, M. Gratz, A. Tscho p̈e, and P. Maletinsky. Fabrication of all diamond scanning probes for nanoscale magnetome- try, Rev. Sci. Instrum. 87, 6 (2016).
The different steps of fabrication are shown in
The fabrication can be described as a method for the dry etching of curved surfaces in diamond.
The method can be described as following
A preparation of the surface, such as cleaning or other preparations may be included in this step. Also, the preparation of the defect at the surface may be included in the step A. In the case of an NV-defect - nitrogen is implanted to a controlled depth below the diamond surface and the diamond is annealed, forming NV centers.
As a preferred ebeam resist a flowable oxide mask can be used. A preferred material for such an oxide mask may be an inorganic polymer layer. Most preferred as material may be FOx-16 from Dow Corning in the composition delivered in the year 2019.
An etch mask may be formed from the layer by a treatment by the electron beam lithography such that the resist can be developed to form the etch mask.
The diamond may be exposed to an inductively coupled plasma, which causes the diamond to be etched in a reactive ion etch process.
During the first part of the etch process, an etch chemistry, preferably O2401, is used that primarily attacks the diamond, forming a tapered conical pillar of diamond. The taper angle of this section may preferably be less than 12 degrees.
Simultaneously the mask may be eroded at the edge to form a trapezoidal cross section.
The sidewalls of the mask are inclined at an approximately 45 degree angle. Note that the angle need not be precisely 45 degrees, but should be substantially inclined from the vertical direction.
During the second part of the etch, the etch chemistry is modified by adding an agent that etches the mask material, preferably CF4402. By changing the concentration of CF4 relative to O2, the angle of the resulting diamond sidewall is changed.
Multiple CF4:O2 ratios can be used sequentially to obtain a curved surface profile. The range of angles achieved with this process can be between 10 and 50 degrees, preferably between 12 and 50 degrees. The ratio can be controlled by a control unit 403 which can control the volume of CF4 and/or O2 introduced in the etching process.
The relative etch rate of the mask vs. the diamond is variably controlled by adjusting the etch chemistry. This distinguishes it from other methods for curved or angled surfaces, i.e., “grey-scale” lithography or mask erosion under fixed conditions. Therefore, the inventive method allows for much more control over the shape of the wall, beyond even the parabolic shape.
As mentioned above etching can be performed as a reactive ion etching of the mask in oxygen plasma to form an inclined cross-section at the edge of the mask, such that the mask tapers from a uniform thickness section to a point at the edge.
The reactive ion etching of the mask can be provided with a combination of oxygen and CF4 plasma. The oxygen plasma primarily attacks the diamond, while the CF4 plasma primarily attacks the FOx-16 mask. Thus, by varying the relative concentration of oxygen vs. CF4, the angle of the wall of the diamond can be controlled. With such a technique it is possible to achieve angles between 10 degrees and 50 degrees.
The etching method allows for etching of curved surfaces, in particular for nano-optical devices.
This technique can be used for the fabrication of parabolic-shaped diamond scanning probes with flat end facets. It is possible to etch sidewalls with angles between 10 and 50 degrees from vertical, and by varying the concentration of gases during the etch curved surfaces can be obtained. By change of the concentration of the said gases the mask erosion can be controlled.
Various nanopillar shapes have been achieved through a combination of an electron beam lithography mask and oxygen etching, but without use of the mask erosion to control the angle of the etch.
The main alternative technique for producing curved surfaces is to create a greyscale mask (i.e., of varying thickness) by “reflowing” the resist after it is deposited. Reflow involves carefully heating the resist until it becomes fluid and forms a bubble on the surface. The resist is then etched, typically in a single etch step with uniform etch conditions, so that the curvature of the bubble is transferred into the substrate.
Within our search, we have found only one other resource in which the angle of diamond pillars within a large array is linked to a hard mask (such as what we use) erosion, while two techniques: one with a similar mask, and one with a lift-off procedure and Cr mask, both of which then use a CHF3/O2 etch chemistry. Here, they propose that the angle does appear due to the erosion of the mask, but only study the angle dependence on the pillar period and diameter.
The technique described above is extendable to arbitrary geometries, although a further focus might be on a circularly symmetric geometries. The technique relatively easy to implement in that it requires etching of a single mask.
For the production of the planar end facet, different techniques can be used. The produced diamond scanning probes have improved photonic performance relative to the existing commercially available scanning probes.
The scanning probes fabricated with this method collect data about 5-10 times faster than the existing probes thanks to an improved sensitivity resulting from the curvature of the diamond.
The effectiveness of the previously described parabolic tip with the planar surface can be shown for scanning magnetometry by performing measurements of an out-of-plane magnetized ferromagnet, specifically a 1 nm thick, 0.73 µm wide stripe of CoFeB capped by a 5 nm layer of Ta. A single scanning probe is mounted in a home-built confocal scanning setup and a small external field along the NV axis to split the spin states has been applied. Linescans were performed across the stripe, recording an ODMR spectrum every 20 nm. The frequency position of the lower ODMR resonance has been recorded, and thereby the field along the NV axis has been extracted by comparing it to the out-of-contact zero-field splitting.
Based on a fit of the measurement signals, one can extract a sample magnetization of (1.0 ± 0.2) mA and a separation of (45 ± 5) nm between the NV and the CoFeB stripe. Since the CoFeB is capped by a 5 nm layer of Ta, the effective separation between NV and Ta surface is (40 ± 5) nm is done. This provides an excellent spatial sensitivity.
In conclusion the parabolic diamond scanning probe containing single NV centers and demonstrated their use for nanoscale magnetic field imaging. The parabolic design is ideal for sensing applications, as it yields a high rate of detected photons from a near- surface NV. The devices could be further improved by incorporating an antireflection coating to the back surface of the slab, through the use of (111) oriented diamond to achieve optimal mode overlap with the NV optical transition dipoles, and better lateral NV placement via deterministic alignment to pre-selected NVs. The design is versatile and can be applied to many systems of interest, including scanning probe sensing of magnetic and electric fields or temperature, as well as NMR sensing of molecules or materials attached to the diamond surface.
The design of the inventive diamond scanning element 1 according to
The tip 2 can be preferably formed as a tapered diamond pillar preferably monolithically attached at its base to a diamond slab as a support 5.
At the tip of the diamond pillar, the rate of tapering is steadily increased, such that the profile of the pillar approximates a paraboloidal lateral surface 3. It is not strictly necessary that the shape be paraboloidal, but the rate of tapering should increase towards the tip. The angle of tapering at the tip should be close to 45 degrees or more, in order to obtain a device that efficiently collects light from a broad band of wavelengths.
The taper does not continue to a radius of zero, but rather the tip radius is finite and greater than approximately 50 nm. i.e., the tip of the pillar is a flat facet.
A defect 6 (NV center) is placed in the tip of the pillar, at the focal point of the paraboloid and just inside the plane of the flat facet of the tip. The defect can also be misplaced, offset from the focal point in any direction; the device will still work but not as efficiently.
The defect is sensitive to external fields, such as magnetic or electric fields, produced by a sample that is brought in close proximity to the flat facet.
The pillar constitutes a waveguide 7 for light emitted by the defect, and the base 5 of the pillar constitutes an aperture 10 through which the light emitted by the defect passes. The backside 9 of the diamond slab reflects this light, so the divergence of the light should be below the angle of total internal reflection for a diamond-air interface, preferably 24.3 - 24.7 degrees, more preferably about 24.5 degrees. For the NV center this implies a minimum aperture preferably between 0.9 and 1.1 µm, more preferably about 1 µm.
The flat facet at the end is provided in order to minimize the distance between the NV defect, which is the sensor and the sample to be measured.
Further to this the increasing taper angle towards the tip is provided in order to achieve a high collection efficiency across a broad spectral band, without making the tip diameter or radius too large because a larger tip radius impairs performance as a scanning probe.
Although the invention has been illustrated and described in detail by way of preferred embodiments, the invention is not limited by the examples disclosed, and other variations can be derived from these by the person skilled in the art without leaving the scope of the invention. It is therefore clear that there is a plurality of possible variations. It is also clear that embodiments stated by way of example are only really examples that are not to be seen as limiting the scope, application possibilities or configuration of the invention in any way. In fact, the preceding description and the description of the figures enable the person skilled in the art to implement the exemplary embodiments in concrete manner, wherein, with the knowledge of the disclosed inventive concept, the person skilled in the art is able to undertake various changes, for example, with regard to the functioning or arrangement of individual elements stated in an exemplary embodiment without leaving the scope of the invention, which is defined by the claims and their legal equivalents, such as further explanations in the description.
| Number | Date | Country | Kind |
|---|---|---|---|
| 20154950.8 | Jan 2020 | EP | regional |
| Filing Document | Filing Date | Country | Kind |
|---|---|---|---|
| PCT/EP2021/051477 | 1/22/2021 | WO |
