|  | | | | |
| Company | Nu Instruments | Nu Instruments | Nu Instruments | Nu Instruments | Nu Instruments |
| Item | Nu Sapphire XD MC-ICP-MS/MS | Attom ES ICP-MS | Nu Plasma 1700 HR-MC-ICP-MS | Nu Sapphire MC-ICP-MS | Vitesse ICP-MS |
| Price | | | | | |
| Description | Sapphire XD is a dual-path MC-ICP-MS/MS that extends the Sapphire platform with a fully retractable Double Wien mass filter (permanent magnets + lens field arrays) and an Xtra Dispersion (XD) fixed collector array. The mass filter can be inserted prior to the hexapole collision/reaction cell for MS/Sapphire XD is a dual-path MC-ICP-MS/MS that extends the Sapphire platform with a fully retractable Double Wien mass filter (permanent magnets + lens field arrays) and an Xtra Dispersion (XD) fixed collector array. The mass filter can be inserted prior to the hexapole collision/reaction cell for MS/MS operation (e.g. Rb-SrF mass shifting) or used alone to suppress space-charge effects. The XD collector provides 25% natural dispersion and accommodates up to 28 Faraday cups and 6 ion-counting detectors.... Read More | The Attom ES is a double-focusing, single-collector HR-ICP-MS with the analyser and sample introduction system at ground potential. It uses a laminated magnet with FastScan electrostatic deflector optics to cover up to 40% of a given mass range without changing the magnetic field. A unique patented The Attom ES is a double-focusing, single-collector HR-ICP-MS with the analyser and sample introduction system at ground potential. It uses a laminated magnet with FastScan electrostatic deflector optics to cover up to 40% of a given mass range without changing the magnetic field. A unique patented detector attenuation system extends the pulse-counting multiplier to 9 orders of magnitude dynamic range; an optional Faraday detector extends this to 12 orders.... Read More | Nu Plasma 1700 is a large-geometry, double-focusing HR-MC-ICP-MS with ~1,700 mm mass dispersion. The large geometry raises the base resolving power to >800 (10% valley definition) at full sensitivity, and edge resolving power reaches >30,000 (5–95% edge definition) by narrowing the continuously Nu Plasma 1700 is a large-geometry, double-focusing HR-MC-ICP-MS with ~1,700 mm mass dispersion. The large geometry raises the base resolving power to >800 (10% valley definition) at full sensitivity, and edge resolving power reaches >30,000 (5–95% edge definition) by narrowing the continuously adjustable source entrance slit. Each of the 16 Faraday detectors and up to 5 ion-counting detectors carries an independently adjustable high-resolution collector slit, enabling simultaneous true high-resolution operation across the entire array.... Read More | Nu Sapphire is a dual-path MC-ICP-MS that combines a double-focusing magnetic sector mass analyser with a hexapole collision/reaction cell on a separate low-energy ion path (patented GB 2535826). The high-energy path provides classical MC-ICP-MS operation; the low-energy path decelerates ions into Nu Sapphire is a dual-path MC-ICP-MS that combines a double-focusing magnetic sector mass analyser with a hexapole collision/reaction cell on a separate low-energy ion path (patented GB 2535826). The high-energy path provides classical MC-ICP-MS operation; the low-energy path decelerates ions into the hexapole CRC for removal of Ar-based and polyatomic interferences. Variable-dispersion Zoom Optics allow instantaneous switching between collector configurations.... Read More | The Vitesse is a Time-of-Flight (TOF) ICP-MS designed for simultaneous full-spectrum acquisition at acquisition rates of 33 kHz (full mass range) up to 160 kHz (reduced mass range via over-pulsing). It incorporates a segmented hexapole reaction cell for interference removal and a patented physical The Vitesse is a Time-of-Flight (TOF) ICP-MS designed for simultaneous full-spectrum acquisition at acquisition rates of 33 kHz (full mass range) up to 160 kHz (reduced mass range via over-pulsing). It incorporates a segmented hexapole reaction cell for interference removal and a patented physical ion beam attenuator. An optional full-sized quadrupole pre-cell (QCT configuration) provides additional selectivity for reaction chemistry.... Read More |
| Optical System | Double-focusing magnetic sector; dual-path transfer optics (high-energy path and low-energy path with hexapole CRC); fully retractable Double Wien mass filter (permanent magnets + lens field arrays); variable-dispersion Zoom Optics; Enhanced Sensitivity Interface as standard; up to 4 mass-flow-controlled reaction gas inlets; software-selectable standard, medium, and high-resolution modes | Double-focusing magnetic sector (electrostatic analyser + laminated magnet); forward Nier-Johnson geometry; ground-potential analyser; FastScan electrostatic deflector optics covering up to 40% of mass range; three fixed-slit resolution modes: low (~300 M/?M), medium (~4,000 M/?M), high (>10,000 M/?M) | Double-focusing large-geometry MC-ICP-MS; ~1,700 mm mass dispersion; continuously adjustable source entrance slit; independently adjustable high-resolution collector slit per detector; base resolving power >800 (10% valley); peak-flat resolving power >5,000; edge resolving power >30,000 (5–95% edge); Enhanced Sensitivity Interface as standard; variable-dispersion Zoom Optics; optional EATO; optional hexapole collision/reaction cell (Sapphire 1700 variant) with dual-path transfer optics | Double-focusing magnetic sector; dual-path transfer optics (high-energy path for classical MC-ICP-MS; low-energy path with hexapole collision/reaction cell, patented GB 2535826); variable-dispersion Zoom Optics; Enhanced Sensitivity Interface as standard; up to 4 independently controlled reaction gas inlets | Time-of-Flight (TOF) mass spectrometer with segmented hexapole reaction cell; Bradbury-Nielsen gate for mass range selection; optional full-sized quadrupole pre-cell (QCT option); patented ion beam attenuator |
| Mass Analyzer | Multi-collector double-focusing magnetic sector with MS/MS capability; XD collector array with up to 28 Faraday cups + up to 6 ion-counting detectors (SEM or Daly); mass range Li to U and beyond; 25% natural dispersion; dynamic range 0–75 Gcps (SEM to 10^10 O pre-amplifier) | Single-collector double-focusing magnetic sector; mass range 1–260 u | Multi-collector double-focusing magnetic sector; 16 Faraday cups + up to 5 ion-counting detectors (SEM or Daly); mass range lithium to actinide series | Multi-collector double-focusing magnetic sector; 16 Faraday cups + up to 6 ion-counting detectors (SEM or Daly); high-resolution and pseudo-high-resolution modes | Time-of-Flight (TOF); simultaneous full-spectrum acquisition; acquisition rate 33 kHz (full mass range) to 160 kHz (reduced mass range); spectrum readout time as low as 80 µs |
| Dynamic Range | 0–75 Gcps (0–1200 V) from SEM to 10^10 O resistor pre-amplifier | 9 orders of magnitude (pulse-counting multiplier with patented beam attenuation); 12 orders of magnitude with optional Faraday detector | Inquire | Inquire | 10 orders of magnitude (patented ion beam attenuation system combined with MagneTOF detector) |
| Applications | Geochronology (Rb-Sr, Lu-Hf, Re-Os, U-Th-Pb), stable isotope analysis (Mg, Si, S, K, Ca, Ti, V, Cr, Fe, Ni, Se), laser ablation in situ dating, nuclear safeguarding, environmental monitoring, forensics, life sciences | Laser ablation imaging, nanoparticle analysis, isotope ratio measurements, trace element quantification, nuclear analysis, geochemistry, environmental monitoring | High-resolution isotope ratio analysis, non-traditional stable isotopes (Mg, Si, S, K, Ca, Ti, V, Cr, Fe, Ni, Se), geochronology, geochemistry, cosmochemistry, nuclear research, life sciences | Non-traditional stable isotope analysis (Mg, Si, S, K, Ca, Ti, V, Cr, Fe, Ni, Se), geochemistry, cosmochemistry, life sciences, nuclear research | Laser ablation elemental imaging, nanoparticle analysis, single-cell analysis, single-particle ICP-MS, nuclear forensics, geochemistry, environmental monitoring |
| Get Quote | | | | | |