Introduction

Ultraviolet (UV) photon detection is becoming increasingly important in our quest to understand the fundamental building blocks of our universe. Basic properties of neutrinos and Dark Matter are currently being investigated through interactions with noble elements. Large liquid argon TPC (time projection chamber) detectors exposed to accelerator neutrino beams are being developed for the study of neutrino oscillations at short1,30, ZnS:Mn31,32, CuCy (Copper cysteamine)33,30. The luminescence enhancement is due to the energy transfer from Eu2+ to Mn2+ which has been detailed in our previous publication30.

Baseline response of photosensor with no nanoparticle enhancement

Control data was collected by testing the sensitivity of samples with no nanoparticles in the same configurations and techniques as the nanoparticle tests were done. A scanning monochromator with D2 lamp was used to illuminate the samples with a wavelength range starting as low as 150 nm and increasing in steps of 10 nm (or 5 nm in some cases) to a maximum value of 400 nm. This technique resulted in coverage of the wavelength range defining the turn-on of sensitivity of the MPPCs (Multi-Pixel Photon Counters). Due to the presence of large fluctuations at wavelengths <200 nm, results of the scans will be reported here for wavelengths >190 nm. Figure 3 shows all values of Sigma/Mean for the data taken with different nanoparticle concentrations both histogrammed and as a function of scanning wavelength.

Figure 3
figure 3

(top) Histogrammed values of Sigma/Mean for all LaxCe1−xF3 nanoparticle sample data, (bottom) Sigma/Mean versus wavelength for all samples.

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For the tests of nanoparticles deposited directly on the surface of the MPPCs, response of an uncoated MPPC was used to compare to the coated ones. The uncoated MPPCs were selected to have operating characteristics (as supplied by the manufacturer) very similar to the coated ones. Figure 4 shows the baseline response to the monochromator scan of the uncoated 1 mm × 1 mm MPPC and the 3 mm × 3 mm MPPC. The spot size of the D2 lamp illumination on the MPPCs was set using the 3 mm × 3 mm MPPC. The (round) shape of the lamp spot after focusing and collimation was approximately 1 mm in diameter, so it would fit entirely within the area of the 3 mm × 3 mm MPPC but was slightly greater than the area of the 1 mm × 1 mm MPPC. The baseline signals obtained roughly corresponded to the areas of exposure on the 2 MPPC sensors.

Figure 4
figure 4

Baseline response of 1 mm × 1 mm (red dot), and 3 mm × 3 mm (blue square) MPPCs in the wavelength range from 195 to 400 nm.

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After the data points were normalized to the exposure area of the MPPCs, they show very similar response for wavelengths greater than ~350 nm as expected. Neither of the MPPCs were sensitive at all to light with wavelengths less than ~250 nm. The 3 mm × 3 mm MPPCs are only sensitive to wavelengths greater than ~320 nm, while the response of the 1 mm × 1 mm MPPC turns on ~60 nm lower in wavelength at ~260 nm.

For the measurements of nanoparticle samples deposited on the tape, the baseline response was measured from an area of the tape not coated with nanoparticles. Figure 5 shows the response of the MPPC for a region of uncoated tape. This measurement was taken as backward emission of light from the uncoated tape in the same way as the coated measurements. As confirmation of the method, no reflected or backward emitted light was seen when the tape was irradiated with UV light from a handheld UV light source.

Figure 5
figure 5

Response of 3 mm × 3 mm MPPC to reflected light from uncoated plastic tape.

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For the case of the polystyrene buttons, a button was prepared with 0% (by weight) nanoparticles and was used as the baseline for these tests. The response of the MPPC for a monochromator scan on this button was essentially the same function of wavelength as shown in Fig. 5 for the 3 mm × 3 mm MPPC. No response below the standard MPPC sensitivity range was seen in this test. Also, since this response is nearly identical to the response of the MPPC to light reflected from the plastic tape, this indicates that no sensitivity to low wavelength photons was observed due to the presence of PPO in the transparent button.

These baseline scans clearly show that all of the MPPC testing configurations used in these measurements were not directly sensitive to light with wavelengths less than ~260 nm for the 1 mm × 1 mm MPPC and less than ~320 nm for the 3 mm × 3 mm MPPCs.

Discussion

Light beam alignment from the D2 lamp to the MPPC was eliminated as a systematic effect by fixing the MPPC with respect to the light beam spot. The beam spot size was forced by focusing and collimation to be ~1 mm in diameter and the MPPC was aligned so that the beam spot was centered on the MPPC active area. No stray light could enter the MPPC from either outside the light-tight enclosure or scattered light from the D2 lamp.

The stability of response was determined by repeating measurements immediately after the original tests and also several days after the initial trials. Variation in the response of a 3 mm × 3 mm MPPC with no nanoparticle coating was found to be less than 2% in the wavelength range of 200–400 nm with response to wavelengths less than ~320 nm near zero. The variation in the 1 mm × 1 mm MPPC was also found to be less than 2%. For the backwards emitted response measurements in the tested wavelength range, variation in the response for conditions with no nanoparticle deposition was also found to be less than 2% (using the 3 mm × 3 mm MPPC for these tests). Finally, for the measurements of nanoparticle concentrations in polystyrene buttons, the variation in response of the MPPC covered with a button with no nanoparticles was also less than 2%, again using the 3 m × 3 mm MPPC.

The results from tests of MPPCs with nanoparticle coatings applied directly to the protective resin on the face of the sensor are shown in Fig. 6. The 1 mm × 1 mm MPPC was coated with CdTe nanoparticles and showed an enhanced response compared to an uncoated MPPC in the wavelength range of ~200 nm to 240 nm. For the 3 mm × 3 mm MPPC, coated with CdS nanoparticles, no enhanced response was seen. Because the thickness and transparency of the coating was not completely controlled, it is possible that the coating on the 3 mm × 3 mm MPPC was more opaque than that on the 1 mm × 1 mm MPPC, resulting in no transmission of any emitted light. We plan to test these nanoparticles again with more control over the coating thickness and the nanoparticle concentration, which may affect the transparency of the sample. Figure 7 shows the results of backwards emission from nanoparticles deposited on the transparent tape. Three of the 4 samples show significant enhancement, especially in a narrow wavelength range of ~200 to 250 nm. We will investigate these responses further–having a peaked response is very desirable, for example, to detect fast scintillator light response from a crystal in a particular narrow wavelength range with reduced response in other undesirable wavelength regions. Figure 8 shows the results from transparent plastic buttons of constant thickness infused with various concentrations of LaF3:Ce nanoparticles. The largest enhancement was measured for a LaF3:Ce nanoparticle concentration of 10% in PPO/Polystyrene base. The enhanced response has a broad peak from ~240 nm to ~390 nm, making it a good candidate for near-UV applications.

Figure 6
figure 6

Response of Coated (blue dots) and Uncoated (blue circles) sensors for (top left) 1 mm × 1 mm and (top right) 3 mm × 3 mm MPPCs and corresponding ratios of Coated to Uncoated response (bottom).

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Figure 7
figure 7

Ratio of nanoparticle to no nanoparticle response for 4 samples deposited on transparent tape.

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Figure 8
figure 8

Ratio of responses versus wavelength for 6 sample buttons with various concentrations of LaF3:Ce nanoparticles from 2 wt% to 30 wt% (black stars are the 0 wt% ratio).

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To summarize, enhancement of the wavelength response of a 1 mm × 1 mm Hamamatsu MPPC was observed in the wavelength range of 200–240 nm for CdTe nanoparticles deposited directly on the surface of the photosensor when compared to an uncoated MPPC. CdS nanoparticles deposited in a similar manner on a 3 mm × 3 mm MPPC exhibited little or no response in the tested wavelength range of 200–400 nm. For the backward-emitted light from nanoparticle coatings deposited on plastic tape, 3 of the 4 tested nanoparticle samples (ZnS:Mn,Eu, ZnS:Mn, Cu-Cy) exhibited strong enhancement in the range of 200–250 nm. ZnS:Ag nanoparticles showed little enhancement in the tested wavelength range. In tests of variable LaF3:Ce nanoparticle concentrations in constant thickness ~transparent samples, the sample button containing a nanoparticle concentration of 10% showed the best enhanced response over a large wavelength range of 225–375 nm. It appears that for these tested samples, the 10% sample produced an optimal emission-absorption response. Our studies indicate that ZnS:Mn,Eu, ZnS:Mn, Cu-Cy, CdTe and LaF3:Ce nanoparticles have good potential for particle detection to uncover the building blocks of our universe.

Materials and Methods

Preparation of the nanoparticles

The nanoparticles were prepared by methods described in our previous publications ZnS:Mn,Eu30, ZnS:Mn31,32, CuCy (Copper cysteamine)33,30. Briefly, 1.94 g ZnS and 28.6 mg MnCl2 were ground together thoroughly and covered with carbon charcoal in a crucible. The crucible was sintered at 800 °C for 3 h before being cooled to room temperature.

CdTe and CdS nanoparticles were synthesized in aqueous solutions using 3-mercaptopropionic acid (3MPA) as a stabilizing agent. As an example, CdS nanoparticles were synthesized as fellows: Briefly, 0.5 millimole cadmium chloride was dissolved in 50 ml DI water followed by the addition of 110 µl 3-mercaptopropionic acid under vigorous stirring. The pH of the solution was changed to 10 by using 1 M NaOH aqueous solution. Finally, 0.5 millimole thiourea in 10 ml water was added dropwise and reflux at 90 °C for 3.5 hrs. The final product was cooled down to room temperature and the solvent was evaporated using a rotary evaporator. The precipitate was washed with a water-acetone mixture for 3 times and dispersed in 20 ml of de-ionized (DI) water. The as synthesized CdS nanoparticles were highly dispersible in DI water.

Preparation of nanoparticle samples for testing

The CdTe and CdS nanoparticles were deposited in solution on the surface resin coating of a Hamamatsu MPPC. CdTe nanoparticles were deposited on a 1 mm × 1 mm square MPPC and CdS nanoparticles were deposited on a larger 3 mm × 3 mm MPPC. The droplets of nanoparticles in solution were deposited on the surface of the MPPC and the liquid was allowed to evaporate, leaving a dry nanoparticle deposition. For these tests, control of the uniformity of nanoparticle concentration over the surface of the MPPC was not attempted. It was noticed that surface tension effects tended to sweep the nanoparticles to the edges of the surface as the liquid solution evaporated, resulting in a non-uniform distribution of the nanoparticles over the resin surface. Nevertheless, tests were performed on these devices using a similar setup as used in our earlier publication28 – in this case no plastic film was needed since the nanoparticles were deposited directly on the MPPC resin surface. The resin coating acted as the plastic film, effectively blocking photons of wavelength less than ~320 nm from impacting on the silicon of the MPPC.

Nanoparticle samples of ZnS:Mn,Eu, ZnS:Mn, CuCy, and ZnS:Ag were deposited on clear plastic tape in ~3 mm × ~3 mm square areas. The thickness and light transmission of each of these samples was such that the samples were opaque to visible and UV light. In our standard setup for testing, looking for light to be transmitted through the samples, no light was seen. Since these samples showed clear luminescence in the presence of a handheld UV light, a slightly different test was done with the monochromator setup. Instead of placing the MPPC behind the samples to collect transmitted light, the detector was positioned in front of and off to one side of the samples. In this way, emitted light at angles backwards to the direction of the incoming photons and also any reflected light was detected by the MPPC.

Finally, samples were prepared in which the visible light transmission through the sample was kept high by varying the concentration of nanoparticles in a transparent medium. Samples of LaxCe1−xF3 nanoparticles in PPO/polystyrene buttons were prepared as discussed in a previous work44. The thickness of the button was kept approximately constant while varying the nanoparticle concentration from 0% to 30% by weight (0%, 2%, 5%, 10%, 20%, and 30% concentrations) in the polystyrene base which also included a small amount (1%) of 2,5-diphenyloxazole (PPO). These samples were designed to determine if an optimal nanoparticle concentration would emerge, while kee** the base material transparent enough to transmit any emitted visible light.

These tests were all designed to test absorption of the nanoparticles with at least some emission of absorbed light in the visible range seen by a photosensor with no sensitivity for wavelengths less than ~320 nm. No attempt was made to tune the nanoparticle sizes to get an optimal emitted wavelength for the MPPC photosensor. Future tests will be done comparing the results of like nanoparticles of different sizes. The optimal wavelength sensitivity of the MPPC used in these tests is characterized by a broad peak centered at ~425 nm. For those samples for which no enhancement was observed, it may be that there was indeed enhancement, but the emitted light was not detected by the photosensor – this will be investigated in future tests in which the emitted wavelength spectrum will be determined using a spectrophotometer device.

Experimental set up for emission measurement

The experimental setup consisted of a scanning monochromator equipped with a Deuterium lamp/fused silica window combination which produced light with wavelengths >150 nm. Transmission of UV light from the lamp to the test setup was done inside a black box in the room air atmosphere. This resulted in light measurements which sometimes were dominated by large fluctuations, especially at wavelengths <200 nm or so. In the future, we will control this by enclosing the entire setup in a N2 atmosphere, reducing the signal fluctuations at low wavelengths. Lenses and a collimator system were focused and formed the light into an approximately 1 mm diameter spot: (1) at the surface of the MPPC, which has an active area of 1 mm2 (9 mm2) for the 1 mm × 1 mm (3 mm × 3 mm) directly coated MPPCs, (2) into a similar 1 mm diameter spot centered on the nanoparticle coatings on tape, each of which had an area of ~9 mm2, and (3) also the same spot size centered on one of the polystyrene buttons which was then placed directly in front of the MPPC. The MPPC was not powered with a bias voltage but was operated in photovoltaic mode – current generated from incident light was amplified and measured with a picoammeter at each scanned wavelength step. The data acquisition program stepped the monochromator in 5 or 10 nm steps, accumulating 100 data samples at each wavelength step, reporting the average response and calculating the standard deviation of the 100 responses at each point.