Design of the LEA AMS System

Figure 1 shows the schematic layout of the new LEA system. Basic elements such as the ion source, injection magnet, and the fast beam bouncing system are copied from the MICADAS design, while the mass spectrometer following the acceleration stage has been modified according to the reduced ion energy. As a consequence, the beam curve radius of the high energy magnet is reduced from 350 mm (MICADAS) to 250 mm (LEA) and the curve radius for the electrostatic deflector is reduced from 380 mm (MICADAS) to 250 mm (LEA) (De Maria Reference De Maria2021). This leads to a reduction of the overall footprint of the system to just 2.0 × 3.0 m², which is 1.5 m² less than the footprint of MICADAS.

Figure 1

Schematic representation of the LEA AMS system operating at ETH Zurich. This compact AMS instrument has an overall footprint of just 3 m x 2 m. The beam injector (LE-side) reproduces the one of the MICADAS system. The size of the HE-side has been reduced due to the new design of the accelerator unit and the lower energy of the ions after the tandem acceleration stage (terminal voltage around 50 kV).

Accelerator Unit of LEA

Detailed view of the HE (High Energy) end of the LEA AMS system is shown in Figure 2. The geometry of the stripper tube defines the phase space volume that matches the geometric acceptance of the following HE spectrometer. The areal density of the stripper medium (He at $ \approx 0.5\;$ μg/cm²) enables the reduction of the molecular component of the injected mass 14 ion beam below the detection limit of the instrument. However, molecular break up products such as ¹²C and ¹³C ions will emerge partly from the stripper tube in charge state 2⁺. These ions will gain more energy during their passage through the HE acceleration gap than the 1⁺ ions.

Figure 2

Schematic view of the high energy end of the LEA AMS system. The stripper housing is differentially pumped and the conductance limiting aperture is separated from the acceleration section. The following magnetic (p/q) and the electrostatic (E/q) filtering elements are combined to enable an achromatic image of the ions emerging form the stripper tube to the final ion detector. Red: ion trajectories of ¹⁴C ions, blue trajectories of ¹²C and ¹³C ions, as they are sequentially injected into the acceleration stage by the fast beam bouncing system.

If a charge exchange process 2⁺→1⁺ of those ions happens at the appropriate distance in the acceleration field (e.g., by collisional process with residual gas atoms/molecules), they will reach exactly the same momentum/charge (p/q) ratio as the ¹⁴C ion to be identified. Consequently, the filtering power of the HE magnet will be ineffective, and these parasitic ions will follow the ¹⁴C⁺ trajectories. Of course, they will have a different energy, but another collisional process further down the ion paths will create a certain probability that these ions will have a chance to reach the final detection system, mimic a false ¹⁴C ion, and create an elevated background. Such processes will happen in any AMS system exploiting a dual use of the acceleration voltage via the tandem principle. At the LEA system they might be enhanced due to the very low ion energy. To reduce this effect, the design of the LEA acceleration stage separates the exit of the conductance limiting aperture of the stripper housing from the acceleration gap. This reduces the density of the outflowing stripper gas in the critical region where the unwanted collisions can happen. Assuming a pressure distribution based on an error function at the exit of the conductance limiting aperture of the stripper housing, using the pressure inside the stripper housing and the base vacuum within the acceleration vessel as end members, the probability of parasitic charge exchange processes can be calculated. Based on this calculation, a reduction of background events by at least one order of magnitude can be expected. Combined with the achromatic combination of p/q (magnetic), and E/q (electrostatic) filtering elements enables ¹⁴C detection limits of better than 50,000 yr BP corresponding to ¹⁴C/¹²C ratio of less than 2 × 10^–15 for processed blank materials.

¹⁴C Detector

A Bragg-type gas ionization detector run with isobutane 3.5 is used to detect the ¹⁴C ions. Since the energy of the ¹⁴C ions is significantly lower than in the MICADAS system (less than 150 keV), the detector (Müller et al. Reference Müller, Döbeli, Seiler and Synal2015) is operated in the proportional counting region instead of the ion chamber region. Several test measurements taken with the LEA system showed that values of 450 V for the applied voltage and a gas pressure of 9.5 mbar provide the most accurate results in separating the background from the real ¹⁴C events. Since the ¹⁴C isotope energy is only 140 keV, the detector signal is amplified by a factor of approximately 3, resulting in a signal level of 3 V. By comparison, the MICADAS uses 300 V detector voltage at an isobutane gas pressure of 20 mbar. With the same settings of the amplifier electronics and total ¹⁴C isotope energy of 420 keV and an amplification factor of 1, the signal level is also equal to 3 V.

The thickness of the entrance window separating the vacuum and the isobutane gas of the detector also plays an important role in ensuring a clean division between background noise and the ¹⁴C events, as seen in Figure 3. Two different Silicon Nitride membrane detector windows were tested with nominal thicknesses of d₁ = 30 nm and d₂ = 50 nm, respectively. Test measurements were conducted using graphitized phthalic acid (PhA) blank samples as target materials. They are presumably free of ¹⁴C due to their petrochemical origin but usually contain a ¹⁴C contamination record from the preparation process which is typically visible at a low 10^–15 ratio with respect to ¹²C. Therefore, the obtained spectra show a distinct ¹⁴C peak and background events which predominantly dissipate lower energy signals in the active detector volume. There is no evidence that these background events are related to the detector itself, but are due to scattered particles. The background events and the ¹⁴C events in the energy spectrum of the 50 nm window, indicated as a red line in Figure 3, overlap and cannot be properly separated. Conversely, due to the lower stopping energy and energy straggling (Sun et al. Reference Sun, Döbeli, Müller, Stocker, Suter and Wacker2007; Suter et al. Reference Suter, Döbeli, Grajcar, Müller, Stocker, Sun, Synal and Wacker2007) in the thinner 30 nm membrane window, the energy spectrum recorded, marked with a blue line in Figure 3, shows two well-separated peaks that clearly distinguish the ¹⁴C events from other background events.

Figure 3

Two energy spectra of a PhA blank sample taken with an isobutane gas detector through 30 nm (blue lines) and 50 nm (red lines) Silicon Nitride membrane windows respectively. The horizontal axis refers to the energy level of the detected particles given in arbitrary units (au). Each spectrum is measured with the same blank sample for 30 min at a HE ¹²C current of >10 μA. The gap between the background peak and the ¹⁴C peak is clearly visible in the measurement taken with the 30 nm window, while the two peaks overlap in the spectrum with the 50 nm window.

Beam Optimization

In order to achieve reliable and stable results, each isotope beam has to be adjusted with the fast-bouncing system in such a way that beam scans performed with the low energy (LE) magnet as well as with the high energy (HE) magnet are depicted as shown in Figure 4. The detailed description of the adjustment technique can be found elsewhere (De Maria Reference De Maria2021). The LE and HE magnet scans are perfect tools to check the performance of the different isotope beams and to ensure stable long-term measurements. After the scans are taken, the magnetic fields are adjusted accordingly, as in our case B_LE = 428 mT for the low energy magnet and B_HE = 847.2 mT for the high energy magnet, indicated by blue lines in Figure 4. With these settings a transmission of 56% is achieved. The transmission is determined by the ratio of the $^{12}C_{HE}^ + $ beam current after the accelerator divided by the ${}_{}^{12}C_{LE}^ - $ beam current before the accelerator or ${}_{}^{12}C_{HE}^ + /{}_{}^{12}C_{LE}^ - $ . In comparison to the expected charge state yield of about 70% of the 1⁺ charge state at 92 keV (Maxeiner et al. Reference Maxeiner, Suter, Christl and Synal2015b) this corresponds to $ \approx $ 80% ion optical transmission of the LEA accelerator.

Figure 4

Low energy magnet (a) and high energy magnet (b) beam scans taken after optimizing the different isotopic beams. Black squares indicate normalized ¹²C ion currents, green ¹³C currents and red ¹⁴C normalized counts. The ¹³C/¹²C ratio is indicated by yellow circles. Please note the flat region of the ¹³C/¹²C isotope ratio in both scans ensuring long-term stable performance of the LEA system. Transparent green areas show possible magnetic field values for a stable measurement, while the blue lines indicate the values we chose for the measurements, B_LE = 428.0 mT for the low energy magnet and B_HE = 847.2 mT for the high energy magnet. Please note that since the isotopic beams are not perfectly Gaussian, the ¹⁴C peak in the HE-magnet scan is chosen slightly left to optimize the transmission. The rather narrow ¹⁴C scan is caused by another filter (electrostatic, E/q filter) that the ¹⁴C isotopes have to pass (see Figure 2).

Performance Tests

For the performance test a series of two PhA blanks as well as five Oxalic Acid II (Oxa2; SRM-4990C) standards (Mann 1983) are introduced to the LEA system, where each sample is analyzed in 23 runs of 300 s testing time. All samples are measured sequentially for a total of 23 runs. The measurements of two well prepared blanks are shown in Figure 5(a), blank 1 with a measured radiocarbon age of 52,900 yr ± 250 yr and blank 2 with 54,700 yr ± 280 yr, which are exceptionally good results in terms of both the quality of the measurements and the sample preparation. The blanks measured on LEA tend to be even older than measured on the MICADAS (Sookdeo et al. Reference Sookdeo, Kromer, Büntgen, Friedrich, Friedrich, Helle, Pauly, Nievergelt, Reinig and Treydte2019), likely due to the implementation of an electrical field-free gap separating the conductance aperture at the exit of the stripper housing form the electric field section at the HE acceleration stage (see Figure 2).

Figure 5

(a) ¹⁴C/¹²C ratios measured for two phthalic acid blanks. Each run has a testing time of 300 s and 23 runs are taken of each sample. Statistical uncertainties are indicated by error bars, while mean values and their uncertainties are indicated by solid and dashed black lines, respectively. The radiocarbon age of blank 1 is more than 52,900 years (F¹⁴C = 0.00138) and blank 2 more than 54,600 years (F¹⁴C = 0.00110), which is not only a strong indication of a good measuring system, but also of clean sample preparation. (b) ¹⁴C/¹²C ratios (¹³C/¹²C fractionation corrected) measured for five Oxalic Acid II standards. Each run has a testing time of 300 s and 23 runs are taken of each sample. The total number of ¹⁴C events detected is 10⁶ counts per sample. Statistical uncertainties are indicated by error bars, while mean values and their uncertainties are indicated by solid and dashed black lines, respectively.

The ¹⁴C/¹²C ratio of five Oxa2 standards are given in Figure 5(b). The measured ¹⁴C/¹²C ratios are normalized to a δ¹³C of –25‰ according to (Stuiver and Polach Reference Stuiver and Polach1977). While the raw data of ¹⁴C/¹²C change by about 1% over the course of the measurement, there is no discernible trend in the fractionation-corrected ¹⁴C/¹²C data. Notable here is the precision of the mean value of each sample, which is less than 1‰ for all samples. The mean of the means is (1.44191 ± 0.00063) * 10^–12 (i.e., the statistical uncertainty of these measurements is less than 0.5‰). The standard deviation of 1.0‰ of the 5 measured standards is in good agreement with the uncertainty of the counting statistics of the individual measurements 0.9‰.