1 00:00:01,000 --> 00:00:07,770 The 7000 triple quadrupole GC/MS is the first quadrupole MS/MS system 2 00:00:07,770 --> 00:00:13,000 designed specifically for the unique requirements of gas chromatography applications. 3 00:00:13,000 --> 00:00:22,000 These requirements include: enhanced selectivity, consistent low detection limits, and robust day-to-day operation. 4 00:00:25,000 --> 00:00:31,000 The typical MS/MS description focuses on the extraction of ions from the source 5 00:00:32,000 --> 00:00:35,600 isolation of the precursor ion in the first quadrupole 6 00:00:37,000 --> 00:00:40,000 dissociation of precursor ion in collision cell 7 00:00:41,000 --> 00:00:46,000 and mass filtering of the product ions in the second quadrupole before detection. 8 00:00:47,000 --> 00:00:52,000 But let’s return to the ion source to discuss processes that are often overlooked. 9 00:00:54,000 --> 00:01:01,000 Even for a high performance source, ionization efficiency - as a percentage of molecules entering the source - is very low. 10 00:01:02,000 --> 00:01:08,700 This means there are many more neutrals than ions exiting the source, so a thorough description must include: 11 00:01:09,000 --> 00:01:11,000 Analytes neutrals . . . and ions 12 00:01:12,010 --> 00:01:14,000 Helium neutrals . . . and ions 13 00:01:15,000 --> 00:01:17,000 Column bleed neutrals and ions 14 00:01:18,000 --> 00:01:23,000 And many more neutrals and ions from the matrix – at concentrations typically higher than the analyte. 15 00:01:24,000 --> 00:01:28,000 To simplify the description, let’s start with the analyte molecules and ions 16 00:01:29,000 --> 00:01:36,600 Analyte molecules enter the vacuum source from the GC capillary column and begin bouncing off the hot surfaces of the source 17 00:01:36,600 --> 00:01:43,540 Analyte ions are immediately extracted from the source and focused into the quadrupole mass filter. 18 00:01:45,420 --> 00:01:47,700 But what about the non-ionized molecules? 19 00:01:48,660 --> 00:01:53,420 The electrical fields within the MS have no influence on these molecules. 20 00:01:54,140 --> 00:01:58,500 They follow rapid, random motion until removed by the vacuum pump. 21 00:02:00,740 --> 00:02:05,620 Parallel processes are occurring simultaneously for the molecules from the sample matrix 22 00:02:06,540 --> 00:02:09,260 and instrument background like column bleed. 23 00:02:10,140 --> 00:02:14,620 The quadrupole analyzer performs the critical task of mass filtering 24 00:02:14,620 --> 00:02:18,260 to isolate the analytes ions from the majority of these ions. 25 00:02:18,860 --> 00:02:26,780 Chemical noise often remains after the first quadruple, but the selectivity of MS/MS removes this final source of interference. 26 00:02:28,380 --> 00:02:33,100 Again we ask, what about the large population of non-ionized molecules. 27 00:02:33,940 --> 00:02:40,060 Although the turbo pump removes many neutrals quickly, some will randomly diffuse into the quadrupole. 28 00:02:41,100 --> 00:02:47,940 At the end of the GC separation, the EI source will be flooded with the highest boiling molecules from the sample matrix 29 00:02:48,620 --> 00:02:54,740 Even in a vacuum, these high boiling molecules can contaminate surfaces in the mass spectrometer. 30 00:02:54,860 --> 00:02:58,860 A cool surface will accelerate this contamination process. 31 00:03:00,540 --> 00:03:05,100 As we think about the potential for contamination, we must not forget helium. 32 00:03:05,980 --> 00:03:11,420 The intense flux - high flow - of helium ions helps to ‘burn’ the high boiling molecules 33 00:03:11,420 --> 00:03:14,580 onto the surfaces of the source and the analyzer. 34 00:03:15,060 --> 00:03:20,860 The cooler the surfaces the faster the rate of contamination and the faster performance is lost. 35 00:03:21,780 --> 00:03:24,700 For a LC atmospheric pressure source like ESI, 36 00:03:24,700 --> 00:03:32,140 metal quadrupoles at a temperature of 100 C are perfectly adequate and commonly used. 37 00:03:32,140 --> 00:03:38,940 But for GC/MS/MS analyses, metal surfaces at this temperature will quickly become contaminated. 38 00:03:40,380 --> 00:03:46,540 The Agilent 7000 uses a combination of proprietary and patented technologies 39 00:03:46,540 --> 00:03:51,940 to avoid contamination problems and ensure robust,high performance operation. 40 00:03:52,820 --> 00:04:02,820 These include: an inert source operating at up to 350 C and quartz quadrupole operating at up to 200 C. 41 00:04:02,820 --> 00:04:12,340 With 35 years of MS experience, Agilent built the 7000 around the unique, hot quartz analyzer of the MSD, 42 00:04:12,340 --> 00:04:17,930 not the cooler metal quadrupole rods used for LC/MS/MS. 43 00:04:20,050 --> 00:04:24,460 Before continuing to the collision cell, one more process must be mentioned. 44 00:04:24,460 --> 00:04:30,660 An EI source produces a large number of highly energetic, metastable helium atoms. 45 00:04:30,660 --> 00:04:38,340 These highly energetic atoms follows a random path like any other neutral until removed by the pump. 46 00:04:38,340 --> 00:04:43,340 Some will follow a path parallel to the analyzer and have a high probability 47 00:04:43,340 --> 00:04:48,620 of traversing the entire analyzer assembly to the HED-EM detector. 48 00:04:49,700 --> 00:04:58,660 During the development of the 7000, Agilent engineers realized a small flow of helium added to the nitrogen collision gas 49 00:04:58,660 --> 00:05:04,260 was very effective way to reduce the transmission of metastable helium through the collision cell. 50 00:05:04,260 --> 00:05:08,660 We call this patent-pending solution: “Helium Quenching”. 51 00:05:10,380 --> 00:05:16,780 A comparison of signal to noise ratio with and without Helium Quenching shows to benefit of this technology. 52 00:05:18,060 --> 00:05:26,180 Helium Quenching has no affect on Product Ion signal, but the neutral noise component is reduced by a factor of four. 53 00:05:26,180 --> 00:05:31,700 This technical breakthrough means lower limits of detection and quantitation. 54 00:05:33,220 --> 00:05:39,500 The 7000 MS/MS, an MS/MS system optimized for gas chromatography 55 00:05:40,620 --> 00:05:45,340 from the classical distribution of ions produced in the inert, high performance source 56 00:05:45,340 --> 00:05:51,940 to the precise isolation of the precursor ion through the path of the hot, quartz, hyperbolic quadrupole 57 00:05:52,820 --> 00:05:57,980 into the high pressure, hexapole collision cell for efficient precursor dissociation, 58 00:05:57,980 --> 00:06:03,980 product ion transmission and simultaneous reduction of metastables with “Helium Quenching” 59 00:06:04,260 --> 00:06:12,260 To the final, accurate mass analysis in a second, hyperbolic quadrupole field before ion collection at the Triple-Axis detector 60 00:06:12,260 --> 00:06:20,100 The 7000 system has been carefully designed to deliver robust sensitivity and reliable quantitative results 61 00:06:21,260 --> 00:06:25,660 The Agilent 7000 quadrupole GC/MS/MS system 62 00:06:25,660 --> 00:06:31,740 an MS/MS optimized for trace analysis of your most complex GC samples 63 00:06:31,740 --> 00:06:35,220 the new standard for GC/MS/MS performance