# Fibre Optic Readout of Microcantilever Arrays for Fast Microorganism Growth Detection

Authors: N. Maloney; G. Lukacs; N. Nugaeva; W. Grange; J. P. Ramseyer; J. Jensen; M. Hegner
Journal: Journal of Sensors
 (2012)

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## Abstract

We present a fibre-optic-based device for the automated readout of microcantilever arrays for fast microorganism growth detection. We determined the ability of our device to track shifts in resonance frequency due to an increase in mass on the cantilever surface or changes in mechanical stiffness. The resonance frequency response of 7μm thick agarose-functionalised cantilevers was tracked as humidity levels were varied revealing a mass responsivity of ~51±1 pg/Hz. The resonance response of microcantilevers coated with Aspergillus niger (A. niger) spores was monitored for >48 h revealing a growth detection time of >4 h. The growth of mycelium along the cantilevers surface is seen to result in an increase in resonance frequency due to the reinforcement of the cantilever structure. The use of our fibre optic detection technique allows data to be recorded continuously and faster than previously reported.


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## Body

## 1. Introduction

Microbial infection through contamination still poses a threat in areas such as the pharmaceutical, cosmetic, and food industries. For this reason, quality control tests are performed to ensure that microbial contamination does not occur and that preservatives are functional. The survival of a microbial population is dependent on the provision of suitable nutrition and environmental conditions (relative humidity > 93%, temperature = 25°C–37°C). Conventional methods to date rely on contaminating a sample containing preservatives with prescribed inocula of microorganism on a petri dish, followed by counting the colonies present. An example of this would be a preservative efficacy test for a pharmaceutical product [1] where, under the effect of the preservative living bacteria should show a log reduction of 3 after 24 h and fungi should show a log reduction of 2 after 7 days. These inexpensive manual methods provide the desired sensitivity and growth information but are time consuming and require highly skilled personnel to perform them. For this reason, there is a need for the development of automated, highly sensitive, label-free and real-time detection systems.The reported use of microcantilever resonators as biosensors has risen in recent years. Typically, detection is based on either (i) tracking the deflection caused by induced surface stress changes on the cantilever surface by adsorption of target biomolecules (static mode) [2, 3] or (ii) tracking the resonance frequency changes caused by mass adsorption on the cantilever surface (dynamic mode). Using static mode, single base pair mismatches have been detected in DNA hybridization experiments [4] while the detection of Escherichia coli(E. coli) has also been reported using an antibody-immobilized microcantilever with a detection limit of 1×106 cfu/mL [5]. Using dynamic mode, a mass resolution of 1 attogram (10-18 g) has been achieved [6], while the detection of bacterial cells [7], virus particles [8, 9], and biomolecules [10] has also been described. The use of microcantilever arrays for the detection of viable microorganism growth has previously been reported in [11–14]. These measurements, based on the optical beam deflection method [15], were performed using a scanning probe MultiMode head operated in a controlled environment. Manual manipulation of the laser spot was required for the readout of several cantilevers. This paper presents the development and successful application of an automatised fibre-optic-based readout technique of cantilever arrays for microorganism growth detection. The principle of operation relies on the modulation of the optical signal, by an oscillating cantilever, carried by the optic fibres to a photodiode detector. The mechanism of detection is similar to that used in [11, 12] where the absorption of water on the functionalised cantilever surface due to microorganism growth results in a resonance frequency shift.


## 2. Materials and Methods

### 2.1. Chemicals and Reagents

All chemicals and reagents are of analytical grade and were purchased from Sigma-Aldrich (Arklow, Ireland), unless otherwise stated.


### 2.2.Aspergillus niger Culture Method

Aspergillus niger (A. niger, CIP 1431.83) spores were obtained from Institut Pasteur (Paris, France). Spores were cultured on potato dextrose agar (PDA) (Oxoid, Basel, Switzerland) slants at 35°C for five days and then stored at 4°C until required. Spores were suspended in 4 mL of malt extract broth (ME). Spores were harvested by centrifugation (10,000 rpm, 5 min) (Genofuge 16M, Techne) of 3 mL of this suspension. The resulting pellet was resuspended in a 200 μL solution of ME and deionised water (1 : 10). These steps take an average of 20 mins to complete after which the spore suspension is used for cantilever functionalisation (Section 2.3).


### 2.3. Cantilever Array Preparation and Functionalisation

Cantilever arrays used were obtained from the microfabrication group located in the IBM Zurich Research Laboratory. Each array consists of eight cantilevers separated by a pitch of 250μm with length, width, and thickness dimensions of 500 μm, 100 μm, and 7 μm, respectively. Two types of array (array A and array B) were prepared. Array type A were cleaned for 10 min in Piranha solution (H2SO4 : H2O2; 1 : 1) and subsequently washed in a solution of nanopure water and ethanol (1 : 1) and then nanopure water. This procedure was repeated twice, and the array was then washed using HPLC grade isopropanol. Array type B was cleaned by exposing it to 0.3 mbar O2 plasma for 3 min (PICO Barrel Asher; Diener electronic GmbH + Co. KG, Nagolderstrasse 61, D-72224 Ebhausen, Germany). After cleaning, a self-assembled monolayer was formed on the arrays by immersion in a silane solution (3-glycidyloxypropyl-trimethoxysilane : N-ethyldiisopropylamine : water free toluene; 1 : 1 : 100) for 45 min and then washed twice in water-free toluene for 15 min. The array was dried using nitrogen gas and then stored under vacuum. This step provides an epoxy-activated surface which is reactive, in alkali conditions, towards primary hydroxyl groups (e.g., agarose).Seakem Gold Agarose (Bioconcept; NH, USA) was dissolved in nanopure water at a concentration of 1% (wt/vol) and stored at 4°C. Prior to use the agarose gel solution was melted. The pH of the agarose solution was adjusted to~11.9 by adding 2 M NaOH. Glass capillaries (King Precision Glass, Inc.; Calif, USA) were used to agarose functionalise the cantilever arrays as described in [16]. In order to prevent gelatinisation of the agarose solution in the capillary tubes, they were preheated using a radiation lamp (Osram; 8401 Winterthur, Switzerland). In the case of array type A, cantilevers were exposed to the agarose solution for 1 second. In the case of array type B, cantilevers were exposed to the agarose solution for 1, 5, or 10 seconds to obtain a different agarose thickness on each cantilever. The nutritional soaking of the agarose layer and deposition of A. niger spores on the cantilever were performed in parallel using glass capillaries as previously mentioned. The spore suspension used was prepared as discussed in Section 2.2. Cantilevers on array type A were immersed in the spore suspension for 10 min. The in situ reference cantilever was immersed in 10% ME broth without spores for 10 min. The array was immediately placed inside the test chamber at 94% RH and 30°C.


### 2.4. Apparatus and Measurement

All components were purchased from Thorlabs (Cambridgeshire CB7 4EX, UK), unless otherwise stated.  Experiments were performed using a custom built device (Figure1) based on the optical beam deflection method. The deflected optical beam is captured using optic fibres. When actuated at its resonance frequency, the motion of a cantilever results in a modulation in the intensity of the optical beam captured by the optic fibres. By recording the intensity modulation, the resonance frequency of a cantilever can be determined and tracked. The optical axis of the device is maintained using 16 mm cage plates (SP03) and cage rods (SR3) which are mounted on two gothic-arch XYZ translation stages (9061 XYZ, Newport, Calif, USA). A collimated laser beam (beam diameter = 3.4 mm) is provided to the system using a pig-tailed laser diode (LPS-830-FC, λ=830 nm, maximum power 12 mW) which is accompanied by a collimator (F280FC-B). The laser diode is driven with an external module (ITC502-Benchtop Laser Diode and Temperature Controller ±200 mA/16 W) and is temperature controlled (TCLDM9-TE-Cooled Mount). The collimated beam is focused into a line, with a width of ~6 μm, along a cantilever array using a convex cylindrical lens (47764, f=20 mm; Edmund Optics, UK). The reflection from each cantilever is directed into eight pick-up fibres (BFL48-200, core diameter = 0.2 mm), one corresponding to each cantilever in the array, via a concave cylindrical lens (LK1363L1-B, f=-7.7 mm). Figure 2 shows an illustration of this setup. The pick-up fibres are coupled to a custom built photodetector device where a voltage is produced proportional to the intensity of the detected light. The voltage generated is amplified using a low-noise voltage preamplifier (SR560, Stanford Research Systems, Calif, USA). Actuation of the cantilever array is performed using a custom made stage containing a 15 mm × 15 mm × 1 mm piezo ceramic plate (EBL#2, EBL Products Inc.; Conn, USA).Figure 1
Photograph of fibre optic cantilever device. A collimated laser beam is focused into a line along a cantilever array using a convex cylindrical lens. The deflected signal from each cantilever is directed into one of eight optic fibres (one for each cantilever) using a concave cylindrical lens. The optical axis is maintained using two cage systems, which are mounted on two gothic arch XYZ translation stages. Horizontal distance from hole to hole is 25 mm on breadboard.Figure 2
Illustration outlining optics of fibre optic cantilever device. Description is given in Section2.4.LabVIEW (National Instruments, Tex, USA) is used to control our instrument and to measure the resonance frequencies of cantilevers in an array in a time multiplexed fashion. Three boards, NI PCI-5412 (100 MS/s, 14-Bit Arbitrary Waveform Generator; National Instruments, Tex, USA), NI PCI-6010 (16-Bit, 200 kS/s, 16 Analog Input Multifunction DAQ; National Instruments, Tex, USA), and NI 5112 (High speed digitiser; National Instruments, Tex, USA), allow us (i) to output voltages on the before-mentioned piezo plate, (ii) to acquire and process voltages from the custom built photodetector device, and (iii) to control the current applied to the pigtailed laser diode.In order to obtain suitable conditions for microorganism growth, a custom environmental chamber (5500-8139 A; Electro Tech Systems Inc., Pa, USA) is used to regulate temperature and humidity. Temperature is generated using a heating element housed inside the chamber. Humid air is pumped into the chamber using an ultrasonic humidification system (5472-3; Electro Tech Systems Inc.; PA 19038 USA). Humidity and temperature are regulated using a temperature-compensated humidity sensor (554; Electro Tech Systems Inc, Pa, USA) in conjunction with a microprocessor controller (5200 441-431; Electro Tech Systems Inc., Pa, USA).


## 2.1. Chemicals and Reagents

All chemicals and reagents are of analytical grade and were purchased from Sigma-Aldrich (Arklow, Ireland), unless otherwise stated.


## 2.2.Aspergillus niger Culture Method

Aspergillus niger (A. niger, CIP 1431.83) spores were obtained from Institut Pasteur (Paris, France). Spores were cultured on potato dextrose agar (PDA) (Oxoid, Basel, Switzerland) slants at 35°C for five days and then stored at 4°C until required. Spores were suspended in 4 mL of malt extract broth (ME). Spores were harvested by centrifugation (10,000 rpm, 5 min) (Genofuge 16M, Techne) of 3 mL of this suspension. The resulting pellet was resuspended in a 200 μL solution of ME and deionised water (1 : 10). These steps take an average of 20 mins to complete after which the spore suspension is used for cantilever functionalisation (Section 2.3).


## 2.3. Cantilever Array Preparation and Functionalisation

Cantilever arrays used were obtained from the microfabrication group located in the IBM Zurich Research Laboratory. Each array consists of eight cantilevers separated by a pitch of 250μm with length, width, and thickness dimensions of 500 μm, 100 μm, and 7 μm, respectively. Two types of array (array A and array B) were prepared. Array type A were cleaned for 10 min in Piranha solution (H2SO4 : H2O2; 1 : 1) and subsequently washed in a solution of nanopure water and ethanol (1 : 1) and then nanopure water. This procedure was repeated twice, and the array was then washed using HPLC grade isopropanol. Array type B was cleaned by exposing it to 0.3 mbar O2 plasma for 3 min (PICO Barrel Asher; Diener electronic GmbH + Co. KG, Nagolderstrasse 61, D-72224 Ebhausen, Germany). After cleaning, a self-assembled monolayer was formed on the arrays by immersion in a silane solution (3-glycidyloxypropyl-trimethoxysilane : N-ethyldiisopropylamine : water free toluene; 1 : 1 : 100) for 45 min and then washed twice in water-free toluene for 15 min. The array was dried using nitrogen gas and then stored under vacuum. This step provides an epoxy-activated surface which is reactive, in alkali conditions, towards primary hydroxyl groups (e.g., agarose).Seakem Gold Agarose (Bioconcept; NH, USA) was dissolved in nanopure water at a concentration of 1% (wt/vol) and stored at 4°C. Prior to use the agarose gel solution was melted. The pH of the agarose solution was adjusted to~11.9 by adding 2 M NaOH. Glass capillaries (King Precision Glass, Inc.; Calif, USA) were used to agarose functionalise the cantilever arrays as described in [16]. In order to prevent gelatinisation of the agarose solution in the capillary tubes, they were preheated using a radiation lamp (Osram; 8401 Winterthur, Switzerland). In the case of array type A, cantilevers were exposed to the agarose solution for 1 second. In the case of array type B, cantilevers were exposed to the agarose solution for 1, 5, or 10 seconds to obtain a different agarose thickness on each cantilever. The nutritional soaking of the agarose layer and deposition of A. niger spores on the cantilever were performed in parallel using glass capillaries as previously mentioned. The spore suspension used was prepared as discussed in Section 2.2. Cantilevers on array type A were immersed in the spore suspension for 10 min. The in situ reference cantilever was immersed in 10% ME broth without spores for 10 min. The array was immediately placed inside the test chamber at 94% RH and 30°C.


## 2.4. Apparatus and Measurement

All components were purchased from Thorlabs (Cambridgeshire CB7 4EX, UK), unless otherwise stated.  Experiments were performed using a custom built device (Figure1) based on the optical beam deflection method. The deflected optical beam is captured using optic fibres. When actuated at its resonance frequency, the motion of a cantilever results in a modulation in the intensity of the optical beam captured by the optic fibres. By recording the intensity modulation, the resonance frequency of a cantilever can be determined and tracked. The optical axis of the device is maintained using 16 mm cage plates (SP03) and cage rods (SR3) which are mounted on two gothic-arch XYZ translation stages (9061 XYZ, Newport, Calif, USA). A collimated laser beam (beam diameter = 3.4 mm) is provided to the system using a pig-tailed laser diode (LPS-830-FC, λ=830 nm, maximum power 12 mW) which is accompanied by a collimator (F280FC-B). The laser diode is driven with an external module (ITC502-Benchtop Laser Diode and Temperature Controller ±200 mA/16 W) and is temperature controlled (TCLDM9-TE-Cooled Mount). The collimated beam is focused into a line, with a width of ~6 μm, along a cantilever array using a convex cylindrical lens (47764, f=20 mm; Edmund Optics, UK). The reflection from each cantilever is directed into eight pick-up fibres (BFL48-200, core diameter = 0.2 mm), one corresponding to each cantilever in the array, via a concave cylindrical lens (LK1363L1-B, f=-7.7 mm). Figure 2 shows an illustration of this setup. The pick-up fibres are coupled to a custom built photodetector device where a voltage is produced proportional to the intensity of the detected light. The voltage generated is amplified using a low-noise voltage preamplifier (SR560, Stanford Research Systems, Calif, USA). Actuation of the cantilever array is performed using a custom made stage containing a 15 mm × 15 mm × 1 mm piezo ceramic plate (EBL#2, EBL Products Inc.; Conn, USA).Figure 1
Photograph of fibre optic cantilever device. A collimated laser beam is focused into a line along a cantilever array using a convex cylindrical lens. The deflected signal from each cantilever is directed into one of eight optic fibres (one for each cantilever) using a concave cylindrical lens. The optical axis is maintained using two cage systems, which are mounted on two gothic arch XYZ translation stages. Horizontal distance from hole to hole is 25 mm on breadboard.Figure 2
Illustration outlining optics of fibre optic cantilever device. Description is given in Section2.4.LabVIEW (National Instruments, Tex, USA) is used to control our instrument and to measure the resonance frequencies of cantilevers in an array in a time multiplexed fashion. Three boards, NI PCI-5412 (100 MS/s, 14-Bit Arbitrary Waveform Generator; National Instruments, Tex, USA), NI PCI-6010 (16-Bit, 200 kS/s, 16 Analog Input Multifunction DAQ; National Instruments, Tex, USA), and NI 5112 (High speed digitiser; National Instruments, Tex, USA), allow us (i) to output voltages on the before-mentioned piezo plate, (ii) to acquire and process voltages from the custom built photodetector device, and (iii) to control the current applied to the pigtailed laser diode.In order to obtain suitable conditions for microorganism growth, a custom environmental chamber (5500-8139 A; Electro Tech Systems Inc., Pa, USA) is used to regulate temperature and humidity. Temperature is generated using a heating element housed inside the chamber. Humid air is pumped into the chamber using an ultrasonic humidification system (5472-3; Electro Tech Systems Inc.; PA 19038 USA). Humidity and temperature are regulated using a temperature-compensated humidity sensor (554; Electro Tech Systems Inc, Pa, USA) in conjunction with a microprocessor controller (5200 441-431; Electro Tech Systems Inc., Pa, USA).


## 3. Results and Discussion

The detection ofE. coli and A. nigergrowth using cantilever arrays has been reported in [11–14]. However, as mentioned previously, this work was performed manually using a scanning probe MultiMode head with NanoScope control software (Digital Instruments, Santa Barbara, Calif, USA). For our fibre optic device, the following tests were performed to ensure that continuous resonance frequency changes, due to increasing mass on the cantilever surface, can be detected.


### 3.1. Response of Agarose-Functionalised Cantilevers in Varying Humidity Conditions

Figures3 and 4 show the resonance frequency response of cantilevers, from array types A and B, to changes in humidity, respectively. Agarose-functionalised cantilevers show an increased response to changes in humidity. This is due to an increase in mass on the cantilever surface caused by the absorption of water by the agarose layer. Increasing the incubation time in agarose solution during functionalisation results in a thicker layer and hence a greater response to humidity fluctuations (Figure 4). There is seen to be a correlation between frequency noise levels in the device and the incubation time of the cantilevers in the agarose solution during functionalisation. For incubation times of 1, 5, and 10 seconds, noise levels are found to be in the order of 4, 5.5, and 7 Hz, respectively, at experimental conditions (94% RH, 30°C) (data not shown). The mass responsivity of our sensor when operated in its first resonance mode is ~51±1 pg/Hz. It should be noted that the minimal detectable mass increases with the thickness of agarose on the cantilever surface due to increased noise levels.Figure 3
Resonance frequency response of agarose functionalised cantilevers. Agarose functionalized cantilevers show an increased response to changes in humidity. Zero point on right hand axis corresponds to 44% RH.Figure 4
Resonance frequency response of agarose-functionalised cantilevers. The thin, medium and thick agarose sensors correspond to 1-, 5-, and 10-second incubation times during functionalisation, respectively. The response to humidity changes increases with increasing layer thickness. Frequency noise levels are also seen to increase slightly with increasing layer thickness. Zero point on right hand axis corresponds to 36% RH.


### 3.2.Aspergillus niger Growth Detection

Figure5 shows resonance frequency shift (Δω=ω0-ω1) versus time for two A. nigerspore-coated cantilevers. The observed shift is as a result of spores starting to germinate and spread mycelium along the cantilever. To put this into context, the mass of an individual spore (diameter ~4 μm) is ~34 pg, which increases to ~270 pg due to swelling before germination (diameter ~8 μm). This value is well within our detection limits indicated earlier.  The growing mycelium assimilates nutrients and mostly water from the nutritive layer, which then absorbs water to remain in equilibrium with its surroundings. The detection of vital fungal growth is possible in less than 4 h. This value is in agreement with that reported in [13, 14]. The use of our fibre optic detection technique allows data to be recorded continuously. The use of an automated system allows experiments to be run over longer periods of time (>48 h) which provides further insight into the dynamics of mycelium growth. Approximately 28 h after the start of the experiment, an increase in resonance frequency, and hence most likely a rise in stiffness (k), was observed. We believe this increase to be as a result of the reinforcement of the cantilever by the growth of mycelium along its length (Figure 6). The effect of adsorbed mass stiffness and its position along the cantilever have been reported in [17, 18]. These effects may apply here; however, further work is required to clarify this as the online imaging of spore growth would be required. We believe the jumps in resonance frequency observed at ~33 and 42 h for the cantilever with the denser spore coating (Figure 6(A); black curve) could be interpreted as a temporary buckling of the strained mycelium. Different magnitudes of response can be linked to a higher number of viable spores on one cantilever than the other as can be seen in Figure 6. One point to note is that the rate of growth is the same on both cantilevers as the individual sensor response seems to scale with the number of viable spores deposited.Figure 5
Differential nanomechanical response ofA. nigerfunctionalised cantilevers. The black and red curves correspond to Figure 6 (A and B, resp.). The agarose reference sensor remained stable with a standard deviation of ~15 Hz. Vital spore growth, which is manifested by a resonance frequency shift, is detected in less than 4 h. An increase in resonance frequency is also observed after ~28 h. This is due to reinforcement of cantilevers caused by the growth of mycelium along their lengths. Different numbers of viable spores on each cantilever result in different magnitudes of response; however, growth rates are the same.Figure 6
Optical microscope images of the front and backside of twoA. nigercoated cantilevers. Figure 6 (A and B) show the front and backsides of cantilevers which correspond to the black and red curves from Figure 5, respectively. Figure C shows an SEM image of mycelium on the surface of a cantilever. Mycelium thicknesses (~2 μm) are of the same order of magnitude when compared to the cantilever thickness (7 μm). The growth of mycelium proceeds at a rate of ~9 μm/h along the length of cantilevers.


## 3.1. Response of Agarose-Functionalised Cantilevers in Varying Humidity Conditions

Figures3 and 4 show the resonance frequency response of cantilevers, from array types A and B, to changes in humidity, respectively. Agarose-functionalised cantilevers show an increased response to changes in humidity. This is due to an increase in mass on the cantilever surface caused by the absorption of water by the agarose layer. Increasing the incubation time in agarose solution during functionalisation results in a thicker layer and hence a greater response to humidity fluctuations (Figure 4). There is seen to be a correlation between frequency noise levels in the device and the incubation time of the cantilevers in the agarose solution during functionalisation. For incubation times of 1, 5, and 10 seconds, noise levels are found to be in the order of 4, 5.5, and 7 Hz, respectively, at experimental conditions (94% RH, 30°C) (data not shown). The mass responsivity of our sensor when operated in its first resonance mode is ~51±1 pg/Hz. It should be noted that the minimal detectable mass increases with the thickness of agarose on the cantilever surface due to increased noise levels.Figure 3
Resonance frequency response of agarose functionalised cantilevers. Agarose functionalized cantilevers show an increased response to changes in humidity. Zero point on right hand axis corresponds to 44% RH.Figure 4
Resonance frequency response of agarose-functionalised cantilevers. The thin, medium and thick agarose sensors correspond to 1-, 5-, and 10-second incubation times during functionalisation, respectively. The response to humidity changes increases with increasing layer thickness. Frequency noise levels are also seen to increase slightly with increasing layer thickness. Zero point on right hand axis corresponds to 36% RH.


## 3.2.Aspergillus niger Growth Detection

Figure5 shows resonance frequency shift (Δω=ω0-ω1) versus time for two A. nigerspore-coated cantilevers. The observed shift is as a result of spores starting to germinate and spread mycelium along the cantilever. To put this into context, the mass of an individual spore (diameter ~4 μm) is ~34 pg, which increases to ~270 pg due to swelling before germination (diameter ~8 μm). This value is well within our detection limits indicated earlier.  The growing mycelium assimilates nutrients and mostly water from the nutritive layer, which then absorbs water to remain in equilibrium with its surroundings. The detection of vital fungal growth is possible in less than 4 h. This value is in agreement with that reported in [13, 14]. The use of our fibre optic detection technique allows data to be recorded continuously. The use of an automated system allows experiments to be run over longer periods of time (>48 h) which provides further insight into the dynamics of mycelium growth. Approximately 28 h after the start of the experiment, an increase in resonance frequency, and hence most likely a rise in stiffness (k), was observed. We believe this increase to be as a result of the reinforcement of the cantilever by the growth of mycelium along its length (Figure 6). The effect of adsorbed mass stiffness and its position along the cantilever have been reported in [17, 18]. These effects may apply here; however, further work is required to clarify this as the online imaging of spore growth would be required. We believe the jumps in resonance frequency observed at ~33 and 42 h for the cantilever with the denser spore coating (Figure 6(A); black curve) could be interpreted as a temporary buckling of the strained mycelium. Different magnitudes of response can be linked to a higher number of viable spores on one cantilever than the other as can be seen in Figure 6. One point to note is that the rate of growth is the same on both cantilevers as the individual sensor response seems to scale with the number of viable spores deposited.Figure 5
Differential nanomechanical response ofA. nigerfunctionalised cantilevers. The black and red curves correspond to Figure 6 (A and B, resp.). The agarose reference sensor remained stable with a standard deviation of ~15 Hz. Vital spore growth, which is manifested by a resonance frequency shift, is detected in less than 4 h. An increase in resonance frequency is also observed after ~28 h. This is due to reinforcement of cantilevers caused by the growth of mycelium along their lengths. Different numbers of viable spores on each cantilever result in different magnitudes of response; however, growth rates are the same.Figure 6
Optical microscope images of the front and backside of twoA. nigercoated cantilevers. Figure 6 (A and B) show the front and backsides of cantilevers which correspond to the black and red curves from Figure 5, respectively. Figure C shows an SEM image of mycelium on the surface of a cantilever. Mycelium thicknesses (~2 μm) are of the same order of magnitude when compared to the cantilever thickness (7 μm). The growth of mycelium proceeds at a rate of ~9 μm/h along the length of cantilevers.


## 4. Conclusions

A new home-built cantilever array device for fast microorganism growth detection has been successfully set up. Measurements involving growth of microorganisms require high humidity and elevated temperatures that are regulated with high precision.  A fibre optic detection scheme was chosen to prevent adverse humidity effects to electronic parts which would have to be placed close by the cantilever structure under these environmental conditions.  The nanomechanical change, induced by the viable growth of spores on cantilever sensors, can be continuously tracked.  We demonstrated that the use of fibre optic beam injection and fibre optic beam modulation readout can be used to track the resonance frequency of cantilevers in microcantilever arrays over an extended period of time under high humidity and temperature. The resonance frequency of agarose-functionalised cantilevers in varying humidity conditions was instantaneously tracked revealing a mass responsivity for the thin agarose-coated sensors of~51±1 pg/Hz. Frequency noise levels were also found to have a dependence on the thickness of the agarose layer favouring thin layers produced during 1 second functionalisations. The detection of growth of viable A. nigerspores was recorded in less than 4 h. The use of an automated integrated detection system allowed nanomechanical data to be recorded continuously and growth of viable species to be monitored for >48 h, revealing additional insight into the dynamics of mycelium growth.  We postulate that extended growth of micron-sized mycelium along the longitudinal axis of micron-sized cantilevers is inducing a reinforcement of the nanomechanical properties of the micron thin cantilever structures.  It was observed that micromycelia are able to grow with a speed of up to ~9 μm/h under optimal growth conditions and therefore have comparable dimensions to the sensors on which they are grown.  The fast detection of viable microorganism, as demonstrated in this paper, is important for routine quality control tests which are required to ensure that microbial contamination does not occur and that preservatives are functional.



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*Source: 405281-2011-09-13.xml*