Boron doped diamond based electrochemical sensor heads

Abstract

An electrochemical sensor comprising: a boron doped diamond electrode formed of boron doped diamond material; an array of non-diamond carbon sites disposed on a sensing surface of the boron doped diamond electrode; electrochemically active surface groups bonded to the non-diamond carbon sites for generating a redox peak associated with a target species which reacts with the electrochemically active surface groups bonded to the non-diamond carbon sites when a solution containing the target species is disposed in contact with the sensing surface in use; an electrical controller configured to scan the boron doped diamond electrode over a potential range to generate said redox peak; and a processor configured to give an electrochemical reading based on one or both of a position and an intensity of said redox peak.

Claims

1. An electrochemical sensor comprising: a boron doped diamond electrode formed of boron doped diamond material; a patterned array of non-diamond carbon sites disposed on a sensing surface of the boron doped diamond electrode, wherein a size and distribution of the non-diamond carbon sites on the sensing surface of the boron doped diamond electrode is such that a diamond electrochemical sensor head provides a signal to background ratio for current density of a target species in a solution of at least 2.5, and/or a background current density at a peak current density for the target species of no less than −10 mA/cm.sup.2 and no more than 10 mA/cm.sup.2, wherein the non-diamond carbon sites comprise sp2 hybridized carbon; electrochemically active surface groups bonded to the non-diamond carbon sites for generating a redox peak associated with the target species which reacts with the electrochemically active surface groups bonded to the non-diamond carbon sites when the solution containing the target species is disposed in contact with the sensing surface in use; an electrical controller configured to scan the boron doped diamond electrode over a potential range to generate said redox peak; and a processor configured to give an electrochemical reading based on one or both of a position and an intensity of said redox peak.

2. An electrochemical sensor according to claim 1, wherein the electrochemically active surface groups are carbonyl containing groups.

3. An electrochemical sensor according to claim 2, wherein the carbonyl containing groups are quinone groups.

4. An electrochemical sensor according to claim 1, wherein the patterned array of non-diamond carbon sites disposed on the sensing surface of the boron doped diamond electrode is intrinsic non-diamond carbon.

5. An electrochemical sensor according to claim 1, wherein the boron doped diamond electrode is disposed in an electrically insulating diamond support matrix.

6. An electrochemical sensor according to claim 1, wherein the patterned array of non-diamond carbon sites comprises a plurality of isolated non-diamond carbon sites, each having a size in a range of 10 nm to 100 micrometres.

7. A method for determining a pH of a composition, said method comprising: providing the composition, and measuring the pH of said composition with the electrochemical sensor of claim 1.

8. A method for measuring a chlorine concentration of a composition, said method comprising: providing the composition, and measuring the chlorine concentration of said composition with the electrochemical sensor of claim 1.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

(1) For a better understanding of the present invention and to show how the same may be carried into effect, embodiments of the present invention will now be described by way of example only with reference to the accompanying drawings, in which:

(2) FIG. 1 shows a plot of current density versus applied potential for four different types of material: EA grade polycrystalline boron doped diamond material available from Element Six Ltd which has a very low non-diamond carbon content; EP grade polycrystalline boron doped diamond material available from Element Six Ltd which has a higher non-diamond carbon content than EA grade; glassy carbon; and platinum;

(3) FIG. 2 show the response of low non-diamond carbon content polycrystalline boron doped diamond material in 13% NaOCl indicating that no signal is provided by the high quality boron doped diamond material without any functionalization (although a signal can be generated close to the edge of the solvent window, the signal being pushed outwards due to the fact that the surface is so electrochemically inert);

(4) FIG. 3 shows a Raman spectrum for polycrystalline boron doped diamond material which has been deliberately grown to contain small amounts of non-diamond carbon;

(5) FIG. 4 shows a Raman spectrum for low non-diamond carbon content polycrystalline boron doped diamond material which has treated by laser patterning to introduce controlled amounts of non-diamond carbon onto the surface of the material;

(6) FIG. 5 shows the response to the target species ClO.sup.− for five different types of electrode: polycrystalline boron doped diamond material which has been deliberately grown to contain controlled amounts of non-diamond carbon; low non-diamond carbon content polycrystalline boron doped diamond material which has treated by laser patterning to introduce controlled amounts of non-diamond carbon onto the surface of the material; glassy carbon; nanodiamond which contains significant quantities of non-diamond carbon; and graphite paste which contains large amounts of non-diamond carbon—FIG. 5 illustrates that the signal to background ratio is 5 for the polycrystalline boron doped diamond electrode which has been deliberately grown to contain controlled amounts of non-diamond carbon;

(7) FIG. 6 shows the same data as FIG. 5 and illustrates that the signal to background ratio is 8.3 for the low non-diamond carbon content polycrystalline boron doped diamond material which has treated by laser patterning to introduce controlled amounts of non-diamond carbon onto the surface of the material;

(8) FIG. 7 shows the same data as FIG. 5 and illustrates that the signal to background ratio is 0.8 for the glassy carbon electrode;

(9) FIG. 8 shows the same data as FIG. 5 and illustrates that the signal to background ratio is 2 for the nanodiamond electrode which contains significant quantities of non-diamond carbon;

(10) FIG. 9 shows the same data as FIG. 5 and illustrates that the signal to background ratio is 1.8 for the graphite paste electrode which contains large amounts of non-diamond carbon;

(11) FIG. 10 shows how the speciation of NaOCl changes with pH;

(12) FIG. 11(a) shows an x-ray photoelectron spectrum of the surface of an alumina polished, oxygen terminated polycrystalline boron doped diamond material and the contributions made by different surface groups;

(13) FIG. 11(b) shows an x-ray photoelectron spectrum of the surface of an alumina polished, oxygen terminated polycrystalline boron doped diamond material which has been further treated by polarizing in 0.1 M H.sub.2SO.sub.4 at +3 V for 60 seconds;

(14) FIG. 12(a) shows data for open circuit potential measurements of boron doped diamond electrodes which have been alumina polished;

(15) FIG. 12(b) shows data for open circuit potential measurements of boron doped diamond electrodes which have been polarised in 0.1 M H.sub.2SO.sub.4 at +3 V for 60 seconds;

(16) FIG. 13 shows various surface functional groups which are present on glassy carbon electrodes including various types of carbonyl containing groups;

(17) FIG. 14 shows an open circuit potential measurement for glassy carbon polarised at +3 V for 10 seconds in 0.1 M H.sub.2SO.sub.4 with the inset showing a plot of pH vs open circuit potential;

(18) FIG. 15 shows laser features introduced into a glass sealed polycrystalline boron doped diamond macroelectrode;

(19) FIGS. 16(a) and 16(b) also show laser patterns in a 1 mm polycrystalline boron doped diamond electrode;

(20) FIG. 16(c) shows interferometry data on the boron doped diamond electrodes indicating lasered pits of approximately 45 micrometres wide and approximately 50 micrometres deep;

(21) FIGS. 17(a) and 17(b) show the solvent window and capacitance of three different types of electrode: a lasered polycrystalline boron doped diamond electrode; an unlasered polycrystalline boron doped diamond electrode; and a glassy carbon electrode;

(22) FIG. 18(a) shows the OCP response for a lasered and acid cleaned electrode;

(23) FIG. 18(b) shows the OCP response after the electrode was polarised at +3 V for 10 s in 0.1 M H.sub.2SO.sub.4;

(24) FIG. 19 illustrates pH sensitive electron transfer characteristics of quinones;

(25) FIGS. 20(a) and 20(b) show the results of performing square wave voltammetry in different pH solutions on a bare glassy carbon electrode illustrating a Nernstian pH response for the quinone reduction peak;

(26) FIG. 21 shows the results of performing x-ray photoelectron spectroscopy to analyse the top 3 nm of polycrystalline boron doped diamond material before and after laser patterning indicating the emergence of an sp2 peak after lasering;

(27) FIG. 22 shows high resolution x-ray photoelectron spectroscopic imaging for C═O groups on a laser patterned boron doped diamond electrode with a data point resolution of 3 micrometres shows that C═O groups are more prevalent in laser pits and thus there is a highly likelihood for more quinone groups;

(28) FIG. 23 shows a Raman spectra analysis of the laser pits compared with the unlasered boron doped diamond material indicating no obvious increase in sp2 and thus indicating that the bulk of the electrode remains as sp3 diamond even in the laser patterned regions;

(29) FIG. 24 shows the results of square wave voltammetry of quinone reduction on a laser patterned polycrystalline boron doped diamond surface indicate a deviation from a Nernstian response for acidic pH solutions;

(30) FIG. 25 shows the results of square wave voltammetry of quinone reduction on a laser patterned and anodically polarized polycrystalline boron doped diamond surface indicating a Nernstian pH response across at least a pH range of 2 to 10;

(31) FIG. 26 shows results for a number of polycrystalline boron doped diamond macroelectrodes of 1 mm diameter, laser patterned and anodically polarised at 7 mA for 60 s in 0.1 M sulphuric acid indicating repeatability with all electrodes showing a similar pH response;

(32) FIG. 27 shows a pH measurement at pH 2 for twenty repeat measurements on a single electrode illustrating that once polarised the diamond based pH sensing electrode is stable;

(33) FIG. 28 shows the pH response in the presence of dissolved lead (Pb.sup.2) for a glassy carbon electrode (FIGS. 28(a), 28(c), 28(e)) and a diamond based electrode (FIGS. 28(b), 28(d), 28(f)) at pH values of 3, 7, and 11 indicating that signal to noise and peak stability is much improved in this environment for a diamond based electrode compared with a glassy carbon electrode;

(34) FIG. 29 shows the pH response in the presence of dissolved cadmium (Cd.sup.2) for a glassy carbon electrode (FIGS. 29(a), 29(c)) and a diamond based electrode (FIGS. 29(b), 29(d)) at pH values of 3 and 11 indicating that signal to noise and peak stability is also improved in this environment for a diamond based electrode compared with a glassy carbon electrode.

DETAILED DESCRIPTION OF CERTAIN EMBODIMENTS

(35) FIG. 1 illustrates why high quality, low non-diamond carbon content diamond material is advantageous over other materials for electrochemical analysis. As can be seen from the plot of current density versus applied potential, such a material has a wide, flat solvent window when compared to lower grades of boron doped diamond material, glassy carbon, or metal electrodes such as platinum. This provides a large detecting window, low background currents, and excellent signal resolution as well resistance to corrosion and fouling and the ability to operate in harsh environments.

(36) However, the downside to this stability and inert nature is a lack of electrocatalytic activity such that the electrode material is unable to detect certain target species such as OCL. This is illustrated by the lack of response shown in FIG. 2 for low non-diamond carbon content polycrystalline boron doped diamond material in 13% NaOCl which indicates that no signal is provided by the high quality boron doped diamond material without any functionalization (although a signal can be generated close to the edge of the solvent window, the signal being pushed outwards due to the fact that the surface is so electrochemically inert).

(37) It is known that during diamond growth non-diamond carbon can be incorporated into the diamond lattice. FIG. 3 shows a Raman spectrum for polycrystalline boron doped diamond material which has been deliberately grown to contain small amounts of non-diamond carbon. Peaks attributable to the sp3 diamond lattice, the boron doping, and the non-diamond carbon are clearly visible.

(38) It is also known that non-diamond carbon can be introduced onto the surface of a diamond material by post-synthesis treatments such as laser patterning. FIG. 4 shows a Raman spectrum for low non-diamond carbon content polycrystalline boron doped diamond material which has treated by laser patterning to introduce controlled amounts of non-diamond carbon onto the surface of the material. The diamond trace shows a large sp3 carbon peak while the overlying trace shows a non-diamond carbon peak attributable to surface graphitization by laser action. In this regard, it may be noted that acid cleaning after laser patterning can reduce the non-diamond carbon peak by removing sp2 carbon with the remaining non-diamond carbon being robustly bonded to the diamond electrode.

(39) It is also known that boron doped diamond electrodes can detect species such as ClO.sup.− as described, for example, in Murata et al., “Electrochemical detection of free chlorine at highly boron-doped diamond electrodes”, Journal of Electroanalytical Chemistry, Volume 612, Issue 1, 1 Jan. 2008, Pages 29-36. Here, the generation of a signal for ClO.sup.− can be attributed to non-diamond carbon in the boron doped diamond electrode as it is clear from FIG. 2 that if a high quality, low non-diamond carbon content boron doped diamond material is used for the electrode then the electrode is inert to such a target species due to lack of catalytic activity.

(40) The present inventors have noted that although a signal can be generated for species such as ClO.sup.− using a boron doped diamond electrode which comprises significant quantities of non-diamond carbon, a significant background signal is also generated due to the presence of the non-diamond carbon and this leads to a reduced sensitivity to the detection and measurement of such target species. Surprisingly, the present inventors have found that if a very low and controlled amount of non-diamond carbon is provided at the sensing surface of a boron-doped diamond electrode then sufficient non-diamond carbon can be provided to produce a good signal for species such as ClO.sup.− while not unduly increasing the background. That is, there is an optimum range of non-diamond carbon content for such sensing applications where the target species is not detectable by a high quality, low non-diamond carbon content boron doped diamond material. It has also been found that oxidative pretreatments (e.g. electrochemical oxidative treatments) aid in obtaining a stable and reproducible signal for such non-diamond carbon functionalized boron doped diamond electrodes by providing suitable electrochemically active surface groups on the non-diamond carbon at the sensing surface.

(41) An alternative way of viewing how the present invention works is in terms of the effect of non-diamond carbon on the solvent window of a boron doped diamond electrode. As shown in FIG. 1, the solvent window of a boron doped diamond material is reduced in width, as well as being made less flat, as the concentration of non-diamond carbon is increased. For target species which have an electrochemical peak near the edge of the solvent window, if too much non-diamond carbon is provided at the sensing surface of the boron doped diamond material then the solvent window is reduced too much and the signal for the target species is lost in the background signal for water electrolysis. Conversely, if too little non-diamond carbon is provided then the solvent window will be sufficient wide but no signal will be generated for target species which are inert to boron doped diamond material which has little or no non-diamond carbon. For target species which are only a little more reactive than water, such as ClO.sup.−, there is a delicate balance to be struck between increasing the reactivity of the boron doped diamond electrode to the target species without increasing the reactivity of the boron diamond electrode too much that it reacts with water at the same potential thus masking the signal from the target species.

(42) The specific amount of non-diamond carbon required at the sensing surface to achieve an optimized signal to background ratio will depend on the specific target species to be detected and measured. The required amount of non-diamond carbon for a particular target species can be readily determined by fabricating boron doped diamond materials with a range of different concentrations of non-diamond carbon at the sensing surface and testing these to determine the optimum composition for the target species of interest. For example, the signal to background ratio and the background current density may be measured using a concentration of the target species in solution of 0.1%, 1%, 2%, 3%, 4%, 7%, or 13%. While such test solutions of the target species can be used to characterize the functionality of the boron doped diamond electrodes as described herein, it should be noted that functionalized boron doped diamond electrodes as described herein can reliably detect and measure target species down to parts-per-million and even parts-per-billion concentration levels. As such, in real applications the functionalized boron doped diamond electrodes as described herein may conform to the background signal levels and signal-to-background ratios at concentrations for the target species of 10 ppb, 100 ppb, 1 ppm, 10 ppm, or 100 ppm with a range between 0 and 10 ppm being of particular interest for many applications.

(43) FIG. 5 shows the response to the target species ClO.sup.− for five different types of electrode: polycrystalline boron doped diamond material which has been deliberately grown to contain controlled amounts of non-diamond carbon; low non-diamond carbon content polycrystalline boron doped diamond material which has treated by laser patterning to introduce controlled amounts of non-diamond carbon onto the surface of the material; glassy carbon; nanodiamond which contains significant quantities of non-diamond carbon; and graphite paste which contains large amounts of non-diamond carbon. The signal to background ratio can be calculated as illustrated in FIG. 5 and it is found that the signal to background ratio is 5 for the polycrystalline boron doped diamond electrode which has been deliberately grown to contain controlled amounts of non-diamond carbon. It may also be noted that the polycrystalline boron doped diamond material may be further optimized to increase the signal to background ratio to higher values. It should also be noted that ClO.sup.− is an example of a very challenging target species for which it is difficult to obtain a reasonable signal-to-noise ratio using traditional sensing systems.

(44) FIG. 6 shows the same data as FIG. 5 and illustrates that the signal to background ratio is 8.3 for the low non-diamond carbon content polycrystalline boron doped diamond material which has treated by laser patterning to introduce controlled amounts of non-diamond carbon onto the surface of the material.

(45) As such, FIGS. 5 and 6 illustrated that a high signal to background ratio can be achieved via intrinsic non-diamond carbon introduced into the boron doped diamond material during synthesis or by post-synthesis treatment to provide controlled quantities of non-diamond carbon on the sensing surface of a low non-diamond carbon content boron doped diamond material.

(46) In contrast, FIGS. 7 to 9 show the same data as FIG. 5 and illustrate that the signal to background ratio is only 0.8 for a glassy carbon electrode, 2 for a nanodiamond electrode which contains significant quantities of non-diamond carbon, and 1.8 for the graphite paste electrode which contains large amounts of non-diamond carbon.

(47) In light of the above, it is evident that by controlling the non-diamond carbon content at the sensing surface of a boron doped diamond electrode it is possible to provide a much improved signal to background ratio and thus achieve a higher sensitivity for target species such as ClO.sup.−. While diamond with a significant amount of carbon can achieve a signal to background ratio of 2, by providing low and controlled amounts of non-diamond it is possible to achieve a signal to background ratio of at least 2.5 and more preferably at least 3, 4, 5, 6, 7, or 8. Furthermore, while the background signal and peak current density is greater than ±10 mA/cm.sup.2 for other electrode materials, by providing low and controlled amounts of non-diamond it is possible to achieve a background current density at the peak current density for the target species which is no more than ±10 mA/cm.sup.2, ±8 mA/cm.sup.2, ±6 mA/cm.sup.2, ±4 mA/cm.sup.2, or ±3 mA/cm.sup.2.

(48) The effect as described above has been illustrated for the target species ClO.sup.−. Traditionally, free chlorine detection involves titrimetric or UV analysis which is slow, involves multiple steps, and is performed off-line. In contrast, electrochemical detection can be performed online and is cheap, fast and reliable. In principle free chlorine is easily electrochemically detected via the reaction:
OCl.sup.−+H.sub.2O+2e.sup.−.fwdarw.Cl.sup.−+2OH.sup.−

(49) However, traditional electrode materials are not suitable as oxides form on simple contact with free chlorine in solution and the electrodes are prone to passivation and fouling. Furthermore, reduction of naturally present oxygen can also be problematic. In contrast, the functionalized boron-doped diamond electrodes of the present invention are not prone to such problems and have been shown to produce excellent signal to background responses if the non-diamond carbon content of such electrodes is suitably controlled.

(50) It will be appreciate that while the effect as described above has been illustrated for the target species ClO.sup.−, and particularly utilizing a single peak of this species at between −0.5 and −1.5 volts, the effect can also be utilized for other target species which are catalysed by non-diamond carbon but which are inert to boron doped diamond material which has little or no non-diamond carbon.

(51) The aforementioned finding is an important contribution in itself to the art of electrochemical sensing. In addition, the present inventors have also found that the functionality of boron-doped diamond electrodes comprising low and controlled non-diamond carbon content as described herein can degrade over time and can be variable from electrode to electrode. In particular, these problems have been observed for functionalized boron doped diamond electrodes mounted in a glass or epoxy sealed sensor configuration. It would appear that in use the glass or epoxy mounting material can degrade around the edge of a functionalized boron doped diamond electrode exposing more non-diamond carbon around the edge of the functionalized boron doped diamond electrode. It is difficult to co-planar seal a boron doped diamond electrode in a non-diamond support and repeated polishing and/or strong etching solutions lead to more of the side walls of the boron doped diamond electrode being exposed. Since the amount of non-diamond carbon required to achieve the optimized response is small, this can lead to a significant deviation from the optimum quantity of exposed non-diamond carbon at the sensing surface and leads to a degradation in the signal to background ratio. As such, the present inventors have realized that to avoid this problem it is advantageous to mount the functionalized boron doped diamond electrode in an electrically insulating diamond support matrix. The electrically insulating diamond support matrix does not degrade with respect to boron doped diamond electrode material and thus the quantity of exposed non-diamond carbon remains stable.

(52) Methods for mounting boron doped diamond electrodes in an electrically insulating diamond support matrix are known in the art (see, for example, WO2005/012894 and WO2012/156203). Ideally the boron doped diamond electrodes are mounted so as to be co-planar with the electrically insulating diamond support matrix. Non-diamond sp2 bonded carbon has been shown to achieve catalytic activation in diamond enabling the detection of species such as persulphates, ozone, hypochlorous acid, and hypochlorite. What is new here is the finding that a low and controlled non-diamond carbon content at the sensing surface of a boron doped diamond electrode in combination with diamond encapsulation can provide an electrode configuration which is capable of reliably detecting and measuring low concentrations of such target species. For example, the present diamond sensor head configuration can be used to detect free chlorine in the range 0 to 10 ppm. Furthermore, it has been found that such functionalized boron doped diamond electrodes are stable in use.

(53) A variety of fabrication technique can be utilized to fabricate the diamond electrochemical sensor heads as described herein including one or more of the following: 1. Micro arrays of NDC dots, bands, or other shapes may be provided within a supporting matrix of high quality boron doped diamond to maximise signal current by, for example, laser patterning. The functionalized area may be controlled to maximise analyte signal against background reactions. 2. Areas of sp2 rich diamond can be provided by forming indents or trenches into a boron doped diamond electrode, overgrowing an sp2 rich diamond layer, and then processing back the sp2 rich diamond layer to leave isolated areas of sp2 rich diamond within the original indents or trenches formed in the boron doped diamond electrode. 3. Diamond synthesis conditions, morphology, and methane concentration can be controlled to achieve regions of sp2 rich diamond which are intrinsic to the grade of diamond material. 4. Regions of sp2 carbon within a boron doped diamond material can be exposed to controlled post-synthesis surface processing. 5. Post-synthesis graphitisation techniques such as thermal treatments, laser micro-machining, or hot metal treatments (e.g. deposition of metal nano particles and subsequent heating to induce graphitisation) may be applied to a base boron doped diamond material. 6. Post-synthesis oxidation treatments can be applied to remove excess none bonded sp2 carbon if the starting material has too much exposed non-diamond carbon and/or to remove sp2 carbon which is only loosely bound to the diamond electrode such that the remaining non-diamond carbon is robust.

(54) While some of the aforementioned methods utilize boron doped diamond materials which comprising some intrinsic non-diamond carbon formed during synthesis, certain methods start with a base boron doped diamond material which has a high boron content and a low sp2 carbon content material as described in WO2013/135783 as this enables one to then introduce a low and controlled amount of non-diamond carbon in a reproducible manner and de-couples the required amount of non-diamond carbon from the diamond synthesis process. As such, the bulk of the boron doped diamond electrode on which the non-diamond carbon surface pattern is disposed may comprise boron doped diamond material which has a boron content in a range 1×10.sup.20 boron atoms cm.sup.−3 to 7×10.sup.21 boron atoms cm.sup.−3 and an sp2 carbon content which is sufficiently low as to not exhibit non-diamond carbon peaks in a Raman spectrum of the material.

(55) An additional advantage of starting with an inert boron doped diamond material which has little or no non-diamond carbon content is that the material can then be patterned with non-diamond carbon such that the spacing between areas of non-diamond carbon is well controlled in addition to controlling the concentration of non-diamond carbon. For example, regions of non-diamond carbon can be spaced apart with a spacing approximately equal to the diffusion path length such that the regions of non-diamond carbon function as a microelectrode array. This is possible if the base boron doped diamond material does not interact with the target species but isolated regions of non-diamond carbon do interact with the target species. In this respect, patterning regions of non-diamond carbon into an inert boron doped diamond material is advantageous over a less controlled non-diamond carbon distribution such as one provided by the diamond synthesis process.

(56) Another advantage of starting with an inert boron doped diamond material which has little or no non-diamond carbon content is that exposure of side edges using such a base electrode material will not significantly increase the amount of exposed non-diamond carbon (unless coated with sp2 carbon due to laser cutting). That is, if the base boron doped diamond electrode is inert to a target species of interest and a pattern of non-diamond carbon is introduced onto the sensing surface of such an inert boron doped diamond electrode, then such an electrode does not necessarily need to be encapsulated in an electrically insulating support matrix. As such, a diamond electrochemical sensor head can be provided which does not necessarily require a diamond support matrix. Such a diamond electrochemical sensor head comprises: a boron doped diamond electrode formed of boron doped diamond material which is electrochemically inert to a target species in solution; and an array of non-diamond carbon sites disposed on a sensing surface of the boron doped diamond electrode, wherein the size and distribution of the non-diamond carbon sites on the sensing surface of the boron doped diamond electrode is such that the diamond electrochemical sensor head provides one or both of: a signal to background ratio for current density of the target species in solution of at least 2.5, 3, 4, 5, 6, 7, or 8; and a background current density at a peak current density for the target species of no more than ±10 mA/cm.sup.2, ±8 mA/cm.sup.2, ±6 mA/cm.sup.2, ±4 mA/cm.sup.2, or ±3 mA/cm.sup.2.

(57) For example, the bulk of the boron doped diamond electrode on which the non-diamond carbon surface pattern is disposed may comprise boron doped diamond material which has a boron content in a range 1×10.sup.20 boron atoms cm.sup.−3 to 7×10.sup.21 boron atoms cm.sup.−3 and an sp2 carbon content, at least at exposed surfaces, which is sufficiently low as to not exhibit non-diamond carbon peaks in a Raman spectrum of the material. Edges of such a boron doped diamond material may be polished in addition to the provision of a polished main sensing surface. The array of non-diamond carbon sites disposed on the sensing surface of such a base electrode material may comprise a plurality of isolated non-diamond carbon sites each having a size in a range 10 nm to 100 micrometres.

(58) The diamond electrochemical sensor heads as described herein may also comprise one or more further boron doped diamond electrodes. For example, the diamond electrochemical sensor heads may comprise one or more further boron doped diamond electrodes which comprise less non-diamond carbon than the boron doped diamond electrode which is functionalized with non-diamond carbon. A non-functionalized electrode can be used to generate target species to be sensed by the functionalized electrode and/or to change the pH of the local environment to optimize the concentration of target species to be sensed. For example, FIG. 10 shows how the speciation of NaOCl changes with pH and indicates that ClO.sup.− is generated at high pH. As such, for ClO.sup.− sensing it is advantageous to increase the pH to more than 10 as the ClO.sup.− form is electrochemically active. In this regard, a secondary non-functionalized electrode, such as a ring electrode around a functionalized disc electrode, can be used to change the pH over the functionalized sensing electrode.

(59) The sensor technology can be used in a variety of applications and for a variety of target species of interest. For example, the diamond sensor technology as described herein can be used as part of a sanitation dosing system to maintain concentrations of chlorine in a tight range of, for example, 1±0.5 ppm in a ballast water treatment system. Furthermore, the sensor technology can be utilized for pH sensing as indicated in the summary of invention section and discussed in more detail below.

(60) pH is fundamental to the study of chemical environments and is therefore prevalent in many industries including medicine, waste management, water and environmental monitoring. The most prevalent pH sensor is the glass pH sensor which has a pH range from −1 to 12. The glass pH sensor has a number of advantageous features including high sensitivity to protons, a large analysable pH range, a quick response time, and is readily commercially available. However, the glass pH sensor does have a number of disadvantages including fragility, potential drift over time, and alkali errors where interfering ions such as Na+ and Li+ affect pH response (which is particularly problematic in sea water for example).

(61) The present inventors have investigated whether boron doped diamond electrodes could be used as a pH sensor. In particular, the present inventors have identified that the presence of carbonyls on the surface of oxygen-terminated boron doped diamond is a possible way to use boron doped diamond as a pH sensor, as carbonyls, such as quinones, can interact with hydrogen ions and show a pH dependent redox response. In this regard, FIG. 11(a) shows an x-ray photoelectron spectrum of the surface of an alumina polished, oxygen terminated polycrystalline boron doped diamond material and the contributions made by different surface groups. FIG. 11(b) shows an x-ray photoelectron spectrum of the surface of an alumina polished, oxygen terminated polycrystalline boron doped diamond material which has been further treated by polarizing in 0.1 M H.sub.2SO.sub.4 at +3 V for 60 seconds. Both spectra shown in FIGS. 11(a) and 11(b) are C 1 s XPS spectra on 1 mm polycrystalline boron doped diamond electrodes with a 50 micrometre spot size. The spectra show that anodic polarisation increases the number of carbonyl groups.

(62) The boron doped diamond electrodes were tested as potential pH sensors by taking open circuit potential measurements in different pH buffers. Different types of boron doped diamond electrodes were investigated and various polarisation times were investigated. However, no obvious pH sensitivity was observed and the data was not repeatable even with anodically treated boron doped diamond. In this regard, FIGS. 12(a) and 12(b) show data for open circuit potential measurements of boron doped diamond electrodes which have been alumina polished (FIG. 12(a)) and polarised in 0.1 M H.sub.2SO.sub.4 at +3 V for 60 seconds (FIG. 12(b)). As such, it has been concluded that this open circuit measurement approach to pH sensing using boron doped diamond electrodes is not a viable route, at least using these types of boron doped diamond material.

(63) In contrast to boron doped diamond material, the literature suggests that non diamond carbon in the form of glassy carbon electrodes can be used as a pH sensor. In this regard, various surface functional groups are present on glassy carbon electrodes including various types of carbonyl containing groups as shown in FIG. 13 (see, for example, Lu, M., Compton, G. R., Analyst, 2014, 139, 2397 and Lu, M., Compton, G. R., Analyst, 2014, 139, 4599-4605). FIG. 14 shows an OCP for glassy carbon polarised at +3 V for 10 s in 0.1 M H.sub.2SO.sub.4 with the inset showing a plot of pH vs OCP. In this regard, the Nernst theory equation dictates that at 298 K, 1 change in pH unit=59 mV. For glassy carbon, the gradient is 58 mV indicating a Nernstian response.

(64) Since non-diamond carbon in the form of glassy carbon can be used as a pH sensor, the present inventors have investigated what effect introducing sp.sup.2 carbon to a boron doped diamond electrode will have in sensing pH. In this regard, laser ablation has been investigated as a means of introducing intentional sp.sup.2 carbon into a boron doped diamond electrode in order to measure pH. FIG. 15 shows laser features introduced into a glass sealed polycrystalline boron doped diamond macroelectrode. FIGS. 16(a) and 16(b) also show laser patterns in a 1 mm polycrystalline boron doped diamond electrode. A hexagonal array of laser features are formed followed by acid cleaning and sonication after laser patterning to remove any loose sp.sup.2 from the surface of the diamond material. A hot acid treatment may also function to activate the non-diamond carbon surface as well as removing loose sp.sup.2 carbon. FIG. 16(c) shows interferometry data collected showing pits of approximately 45 micrometres wide and approximately 50 micrometres deep.

(65) The electrochemistry of the laser patterned polycrystalline boron doped diamond electrodes was then tested versus un-modified polycrystalline boron doped diamond and glassy carbon. FIGS. 17(a) and 17(b) show the solvent window and capacitance of the three different types of electrode (the solvent window range is specified between ±0.4 mA cm.sup.−2). It can be seen that the laser patterned boron doped diamond electrodes have a solvent window and capacitance response which is intermediate between bare boron doped diamond material and glassy carbon. It can be seen that laser patterned polycrystalline boron doped diamond exhibits the benefits of higher catalytic activity associated with glassy carbon, along with the advantageous lower background currents attributed to boron doped diamond.

(66) The open circuit potential of the laser patterned boron doped diamond electrode was then investigated. FIG. 18(a) shows the OCP response for a laser ablated and acid cleaned electrode whereas FIG. 18(b) shows the OCP response after the electrode was polarised at +3 V for 10 s in 0.1 M H.sub.2SO.sub.4. A more linear response is obtained when compared to bare boron doped diamond material. However, issues still exist in that the OCP response takes a long time to stabilized and the electrodes are still not achieving a Nernstian response although polarisation does lead to an improvement (only a 43 mV gradient is achieved for OCP vs pH as illustrated in the inset of FIG. 18(b)). It has been postulated that there may be insufficient C═O groups on the electrode surface to achieve the desired Nernstian response.

(67) In light of the failure to achieve a satisfactory method of measuring pH using an open circuit potential route with boron doped diamond electrodes even when laser patterned to introduce sp2 carbon, other electrochemical methods of pH detection have been considered. In this regard, as previously indicated, quinones are present on sp.sup.2 surfaces, the electron transfer characteristics of which are [H.sup.+] dependent as illustrated in FIG. 19. It has been shown that the reduction potential of quinone on the surface of a glassy carbon electrode is pH dependent and that this case be used to measure pH. FIGS. 20(a) and 20(b) show the results of performing square wave voltammetry in different pH solutions on a bare glassy carbon electrode illustrating a Nernstian pH response (59 mV) for the quinone reduction peak. The present inventors have thus considered that if similar functionalization could be applied to a boron doped diamond electrode then this could provide a route to a diamond based pH sensor.

(68) Following the above, x-ray photoelectron spectroscopy has been performed to analyse the top 3 nm of polycrystalline boron doped diamond material before and after laser patterning along the lines previously described. FIG. 21 shows the results indicating the emergence of an sp2 peak after laser patterning. High resolution XPS imaging for C═O groups on a laser patterned boron doped diamond electrode with a data point resolution of 3 micrometres shows that C═O groups are more prevalent in laser pits and thus there is a highly likelihood for more quinone groups (see FIG. 22). However, a Raman spectra analysis of the laser pits compared with the un-modified boron doped diamond material indicates no obvious increase in sp2 (G peak) as illustrated in FIG. 23. This can be understood as Raman is a bulk measurement with a penetration depth of several 100 nanometres and indicates that even though pits have been laser ablated containing amorphous carbon, the bulk of the electrode is still sp3 diamond. This also illustrates why the lasered boron doped diamond has electrochemical characteristics which are intermediate between glassy carbon and bare boron doped diamond.

(69) Quinone reduction was then investigated on a polycrystalline boron doped diamond surface. The results of square wave voltammetry of quinone reduction on a polycrystalline boron doped diamond surface are illustrated in FIG. 24. The results indicate that while a Nernstian pH response at alkaline pH was observed, there is a deviation from the Nernstian response for acidic pH solutions. This implies that not enough quinones are present on functionalized boron doped diamond surface for pH sensing. The laser patterned polycrystalline boron doped diamond electrodes were then anodically polarized at 7 mA (approximately +3 V) for 60 seconds. The quinone reduction measurements at different pH were then re-measured. The results of square wave voltammetry of quinone reduction on an acid treated and anodically polarized polycrystalline boron doped diamond surface are illustrated in FIGS. 25(a) and 25(b). A Nernstian pH response (about 59 mV) is observed across at least a pH range of 2 to 10.

(70) The repeatability of the above described results has been tested by preparing a number of polycrystalline boron doped diamond macroelectrodes of 1 mm diameter, laser patterning the electrodes, and polarising the electrodes at 7 mA for 60 s in 0.1 M sulphuric acid. pH measurements were then performed for all the electrodes and the results are illustrated in FIG. 26. As can be seen from FIG. 26, all the electrodes show a similar pH response indicating good repeatability.

(71) As previously described, the present diamond based pH sensor approach effectively combines the advantageous properties of glassy carbon electrodes in terms of reactivity with those of diamond electrodes in terms of inertness, and achieves an electrode which is sufficiently active to perform pH measurements without being too active that interferences in the pH measurement are problematic. For example, in both of the Compton papers (Lu, M., Compton, G. R., Analyst, 2014, 139, 2397 and Lu, M., Compton, G. R., Analyst, 2014, 139, 4599-4605) in order to make accurate measurements using glassy carbon degassing of the solution is required for at least 20 minutes. For the diamond based electrodes as described herein, due to their lower catalytic activity oxygen reduction is not favoured within the region of interest (where quinone reduction occurs). Furthermore, once polarised the diamond based pH sensing electrodes as described herein have a stable response. For example, FIG. 27 shows a pH measurement at pH 2 for twenty repeat measurements illustrating that the response is stable even for a pH value which has a smaller peak than for higher pH readings.

(72) Following the above, the possibility of redox active metal interference has been investigated and compared to glassy carbon electrodes. FIG. 28 shows the pH response in the presence of dissolved lead (Pb.sup.2+) for a glassy carbon electrode (FIGS. 28(a), 28(c), 28(e)) and a diamond based electrode fabricated in accordance with the present invention (FIGS. 28(b), 28(d), 28(f)) at pH values of 3, 7, and 11. As can be seen from the results, signal to noise and peak stability is much improved in this environment for a diamond based electrode compared with a glassy carbon electrode.

(73) FIG. 29 shows the pH response in the presence of dissolved cadmium (Cd.sup.2+) for a glassy carbon electrode (FIGS. 29(a), 29(c)) and a diamond based electrode fabricated in accordance with the present invention (FIGS. 29(b), 29(d)) at pH values of 3 and 11. As can be seen from the results, signal to noise and peak stability is also improved in this environment for a diamond based electrode compared with a glassy carbon electrode.

(74) In light of the above, it has been determined that by providing controlled amounts of sp2 carbon at the sensing surface of a boron doped diamond electrode (e.g. by controlled diamond growth or by post-synthesis processing such as by laser patterning) it is possible to increase the catalytic activity of a boron doped diamond electrode while retaining, at least to some degree, the inert properties of the basic boron doped diamond material. This can be used for sensing target species such as chlorine which are not detectable using boron doped diamond material with low sp2 carbon content and so long as not too much sp2 carbon is provided at the sensing surface then a low background signal can be retained. In addition, by treating such a diamond electrode (e.g. by anodically polarizing the electrode) to provide a particular type of surface termination, and particular providing carbonyl containing groups such as quinone, it is also possible to provide further sensing capability such as pH sensing. In this case the sensor can be calibrated to give a pH reading based on the potential of a redox peak of the carbonyl containing surface species which shifts in a reproducible manner according to the pH of the solution in which the diamond electrode is placed.

(75) While this invention has been particularly shown and described with reference to embodiments, it will be understood to those skilled in the art that various changes in form and detail may be made without departing from the scope of the invention as defined by the appending claims.